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<style> /* Style Definitions */ table.MsoNormalTable {mso-style-name:"Table Normal"; mso-tstyle-rowband-size:0; mso-tstyle-colband-size:0; mso-style-noshow:yes; mso-style-priority:99; mso-style-parent:""; mso-padding-alt:0in 5.4pt 0in 5.4pt; mso-para-margin:0in; mso-pagination:widow-orphan; font-size:12.0pt; font-family:"Aptos",sans-serif;} </style> <![endif]--><!--[if gte mso 9]><xml> <o:shapedefaults v:ext="edit" spidmax="1026"/> </xml><![endif]--><!--[if gte mso 9]><xml> <o:shapelayout v:ext="edit"> <o:idmap v:ext="edit" data="1"/> </o:shapelayout></xml><![endif]--> </head> <body lang=EN-US link="#467886" vlink="#96607D" style='tab-interval:.5in; word-wrap:break-word'> <div class=WordSection1> <h1 style='margin:0in'><b><span style='font-size:18.0pt;line-height:115%; font-family:"Times New Roman",serif;mso-fareast-font-family:"Times New Roman"'>Papers by </span></b><span style='mso-fareast-font-family:"Times New Roman"'><a href="https://pages.uoregon.edu/arkadiy/"><b><span style='font-size:18.0pt; line-height:115%;font-family:"Times New Roman",serif;color:blue'>Arkady <span class=SpellE>Berenstein</span></span></b></a><o:p></o:p></span></h1> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>If you have problems downloading any of these <b>PDF </b>files<b>,</b> please email me at: </span><a href="mailto:arkadiy@uoregon.edu"><span style='font-family:"Times New Roman",serif;color:blue'>arkadiy@uoregon.edu</span></a><span style='font-family:"Times New Roman",serif'> </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/hecke.hom.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Hecke monoids, their homomorphisms and parabolicity</span></b></a><span style='font-family:"Times New Roman",serif; color:black'> (with </span><a href="http://front.math.ucdavis.edu/author/J.Greenstein"><span style='font-family:"Times New Roman",serif;color:blue'>J. Greenstein</span></a><span style='font-family:"Times New Roman",serif;color:black'> and </span><a href="https://sites.google.com/view/jianrong-li"><span style='font-family:"Times New Roman",serif; color:blue'>J.-R.</span></a><u><span style='font-family:"Times New Roman",serif; color:blue'> Li</span></u><span style='font-family:"Times New Roman",serif; color:black'>),</span></p> <p class=MsoNoSpacing><span style='font-family:"Times New Roman",serif'>We study homomorphisms of Hecke <span class=GramE>monoids,&nbsp; notably</span> parabolic homomorphisms, which map parabolic elements to parabolic elements, and injective ones. The importance of the <span class=GramE>first class</span> stems from the fact that parabolic elements form a rather mysterious <span class=SpellE>submonoid</span> of the Hecke monoid, and we found a plethora of parabolic homomorphisms. Concerning injective ones, as a first step towards their classification, we classified all locally injective connected homomorphisms between Hecke monoids of classical types and expect all of them to be injective. As a surprising byproduct of our study of parabolic and injective <a name="_Int_ttC4SRGi">homomorphisms</a> we described, to some extent, all homomorphisms between Hecke monoids</span>.</p> <p class=MsoNoSpacing>&nbsp;</p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/monom.bialg.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Monomial <span class=SpellE>bialgebras</span></span></b></a><span style='font-family:"Times New Roman",serif; color:black'> (with </span><a href="http://front.math.ucdavis.edu/author/J.Greenstein"><span style='font-family:"Times New Roman",serif;color:blue'>J. Greenstein</span></a><span style='font-family:"Times New Roman",serif;color:black'> and </span><a href="https://sites.google.com/view/jianrong-li"><span style='font-family:"Times New Roman",serif; color:blue'>J.-R.</span></a><u><span style='font-family:"Times New Roman",serif; color:blue'> Li</span></u><span style='font-family:"Times New Roman",serif; color:black'>),</span><span style='font-size:10.0pt;line-height:115%; font-family:"Times New Roman",serif;color:black'> </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>Starting from a single solution of QYBE (or CYBE) we produce an infinite family of solutions of QYBE (or CYBE) parametrized by transitive arrays and<span class=GramE>, in particular, by</span> signed permutations. We are especially interested in cases when such solutions yield quasi-triangular structures on direct powers of Lie <span class=SpellE>bialgebras</span> and tensor powers of <span class=SpellE>Hopf</span> algebras. We obtain infinite families of such structures as well and study the corresponding Poisson-Lie structures and co-quasi-triangular algebras.</span></p> <p class=MsoNormal align=center style='margin-bottom:0in;text-align:center'><span style='font-family:"Times New Roman",serif'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="https://pages.uoregon.edu/arkadiy/Expansionformula.final.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Noncommutative marked surfaces II: tagged triangulations, clusters, and their symmetries</span></b></a><span style='font-family:"Times New Roman",serif'> <b>&nbsp;</b><span style='color:#333333'>(with </span></span><a href="http://www.math.rutgers.edu/~vretakh/"><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>V. <span class=SpellE>Retakh</span></span></a><span style='font-family:"Times New Roman",serif'> and </span><a href="https://mathzh.sysu.edu.cn/zh-hans/teacher/115"><span style='font-family: "Times New Roman",serif'>M. Huang</span></a><span style='font-family:"Times New Roman",serif; color:#333333'>), </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:#333333'>The aim of the paper is to define noncommutative cluster structure on several algebras&nbsp;<i>A</i>&nbsp;related to marked surfaces possibly with orbifold points of various orders, which includes noncommutative clusters, i.e., embeddings of a given group&nbsp;G&nbsp;into the multiplicative monoid&nbsp;<i>A</i></span><i><sup><span style='font-family:"Times New Roman",serif; color:black'>�</span></sup></i><span style='font-family:"Times New Roman",serif; color:#333333'> and an action of a certain braid-like group&nbsp;<span class=SpellE><i>Br</i><i><sub><span style='color:black'>A</span></sub></i></span>&nbsp;by automorphisms of each cluster group in a compatible way. For punctured surfaces we construct new symmetries, noncommutative tagged clusters and establish a noncommutative Laurent Phenomenon.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="https://pages.uoregon.edu/arkadiy/mhorn.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Multiple Horn problems for planar networks and invertible matrices</span></b></a><span style='font-family:"Times New Roman",serif'> <span style='color:black'>(with </span></span><a href="https://www.unige.ch/math/en/section/enseignants-et-chercheurs-2/anton-alekseev"><span style='font-family:"Times New Roman",serif;color:blue'>A. Alekseev</span></a><span style='font-family:"Times New Roman",serif;color:black'>, </span><span style='font-family:"Times New Roman",serif'>A. <span class=SpellE>Gurenkova</span><span style='color:black'>, </span></span><a href="https://www.researchgate.net/scientific-contributions/Yanpeng-Li-2133340975"><span style='font-family:"Times New Roman",serif;color:blue'>Y. Li</span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="https://www.journals.elsevier.com/advances-in-mathematics"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Advances in Mathematics</span></i></a><i><span style='font-family:"Times New Roman",serif;color:black'>,</span></i><span style='font-family:"Times New Roman",serif;color:black'> Vol. <b>478</b>, 2025.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>The multiplicative multiple Horn problem is asking to determine possible singular values of the combinations <i>AB</i>, <i>BC</i> and <i>ABC</i> for a triple of invertible matrices <span class=GramE><i>A</i>,<i>B</i></span>,<i>C</i> with given singular values. There are similar problems for eigenvalues of sums of Hermitian matrices (the additive problem), and for maximal weights of multi-paths in concatenations of planar networks (the tropical problem). For the planar network multiple Horn problem, we establish necessary conditions, and we conjecture that for large enough networks they are also sufficient. These conditions are given by the trace equalities and rhombus inequalities (familiar from the hive description of the classical Horn problem), and by the new set of tetrahedron equalities. Furthermore, if one imposes Gelfand-Zeitlin conditions on weights of planar networks, tetrahedron equalities turn into the octahedron recurrence from the theory of crystals. We give a geometric interpretation of our results in terms of positive varieties with potential. In this approach, rhombus inequalities follow from the inequality �</span><i><sup><span style='font-size:14.0pt;line-height:115%;font-family:"Times New Roman",serif'>t</span></sup></i><span style='font-family:"Times New Roman",serif'>d"0 for the tropicalized potential, and tetrahedron equalities are obtained as tropicalization of certain Pl�cker relations. For the multiplicative problem, we introduce a scaling parameter s, and we show that for s large enough (corresponding to exponentially large/small singular values) the <span class=SpellE>Duistermaat</span>-Heckman measure associated to the multiplicative problem concentrates in a small neighborhood of the octahedron recurrence locus.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/hecke.artin.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Hecke and <span class=SpellE>Artin</span> monoids and their homomorphisms</span></b></a><span style='font-family:"Times New Roman",serif;color:black'> (with </span><a href="http://front.math.ucdavis.edu/author/J.Greenstein"><span style='font-family:"Times New Roman",serif;color:blue'>J. Greenstein</span></a><span style='font-family:"Times New Roman",serif;color:black'> and </span><a href="https://sites.google.com/view/jianrong-li"><span style='font-family:"Times New Roman",serif; color:blue'>J.-R.</span></a><u><span style='font-family:"Times New Roman",serif; color:blue'> Li</span></u><span style='font-family:"Times New Roman",serif; color:black'>),</span><span style='font-family:"Times New Roman",serif'> <i>submitted</i>. </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>This work was motivated by a striking observation that parabolic projections of Hecke monoids map respect all parabolic elements. We found other classes of homomorphisms of Hecke monoids with the same property and discovered that many of them lift to homomorphisms of covering <span class=SpellE>Artin</span> monoids with a similar property. It turned out that they belong to a much larger class (in fact, a category) of homomorphisms of <span class=SpellE>Artin</span> monoids, most of which appear to be new.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal><a href="http://pages.uoregon.edu/arkadiy/general.electric.new.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Generalized electrical Lie algebras</span></b></a><b><span style='font-family:"Times New Roman",serif'> </span></b><span style='font-family:"Times New Roman",serif'>(with </span><a href="https://www.researchgate.net/profile/Azat-Gainutdinov-2"><span style='font-family:"Times New Roman",serif;color:blue'>A. <span class=SpellE>Gainutdinov</span></span></a><span style='font-family:"Times New Roman",serif'>, </span><a href="https://www.hse.ru/en/org/persons/216359816"><span style='font-family: "Times New Roman",serif;color:blue'>V. Gorbunov</span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="https://www.journals.elsevier.com/advances-in-mathematics"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Advances in Mathematics</span></i></a><span style='font-family:"Times New Roman",serif;color:black'>, Vol. <b>478</b>, 2025.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>We generalize the electrical Lie algebras originally introduced by Lam and <span class=SpellE>Pylyavskyy</span> in several ways. To each Kac-Moody Lie algebra <b><i><span style='color:black'>g</span></i></b> we associate two types (vertex type and edge type) of the generalized electrical algebras. The electrical Lie algebras of vertex type are always subalgebras of <b><i><span style='color:black'>g</span></i></b> and are flat deformations of the nilpotent Lie subalgebra of <b><i><span style='color:black'>g</span></i></b>. In many cases including <span class=SpellE>sl<i><sub>n</sub></i></span>, so<i><sub>n</sub></i>, and sp<sub>2<i>n</i></sub> we find new (edge) models for our generalized electrical Lie algebras of vertex type. Finding an edge model in general is an interesting an open problem.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:blue'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/valuation.jh.bases.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Valuations, bijections, and bases</span></b></a><b><span style='font-family:"Times New Roman",serif'> </span></b><span style='font-family:"Times New Roman",serif'>(with </span><a href="https://en.wikipedia.org/wiki/Dima_Grigoriev"><span style='font-family: "Times New Roman",serif;color:blue'>D. Grigoriev</span></a><span style='font-family:"Times New Roman",serif;color:black'>), submitted.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>The aim of this paper is to build a theory of commutative and noncommutative <i>injective</i> valuations of various algebras (including algebras with zero divisors). The targets of our valuations are (well-)ordered commutative and noncommutative (partial or entire) semigroups including any sub-semigroups of the free monoid <span class=SpellE><i>F<sub>n</sub></i></span> on <i>n</i> generators and various quotients. In the case when the (partial) valuation semigroup is finitely generated, we construct a generalization of the standard monomial bases for the so-valued algebra, which seems to be new in noncommutative case. Quite remarkably, for any pair of well-ordered valuations one has canonical bijections between the valuation semigroups, which serve as analogs of the celebrated Jordan-H�lder <span class=GramE>correspondences</span> and these bijections are  almost homomorphisms of the involved (partial and entire) semigroups.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>A spectacular demonstration of this remarkable property of JH-bijections for quantum Schubert cells <i>A=<span class=SpellE>U<sub><span style='color:black'>q</span></sub></span>(w)</i> results in mysterious &quot;<span class=SpellE>symplectomorphisms</span>&quot; of involved skew symmetric forms.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/transitive.gallai.complete.graphs.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Transitive and <span class=SpellE>Gallai</span> colorings of the complete graphs</span></b></a><b><span style='font-family:"Times New Roman",serif'> </span></b><span style='font-family: "Times New Roman",serif'>(with </span><a href="https://u.math.biu.ac.il/~radin/"><span style='font-family:"Times New Roman",serif;color:blue'>R. M. Adin</span></a><span style='font-family:"Times New Roman",serif'> , </span><a href="http://front.math.ucdavis.edu/author/J.Greenstein"><span style='font-family:"Times New Roman",serif;color:blue'>J. Greenstein</span></a><span style='font-family:"Times New Roman",serif;color:black'>, </span><a href="https://sites.google.com/view/jianrong-li"><span style='font-family:"Times New Roman",serif; color:blue'>J-R Li</span></a><span style='font-family:"Times New Roman",serif'>, </span><a href="https://arxiv.org/search/math?searchtype=author&amp;query=Marmor,+A"><span style='font-family:"Times New Roman",serif;color:blue'>A. <span class=SpellE>Marmor</span></span></a><span style='font-family:"Times New Roman",serif'>, </span><a href="https://u.math.biu.ac.il/~yuval/"><span style='font-family:"Times New Roman",serif; color:blue'>Y. <span class=SpellE>Roichman</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="https://www.sciencedirect.com/journal/european-journal-of-combinatorics"><span style='font-family:"Times New Roman",serif;color:blue'>European Journal of Combinatorics</span></a><span style='font-family:"Times New Roman",serif; color:black'>, Vol. <b>130</b>,&nbsp; 2025 (the journal version is different from the </span><a href="http://pages.uoregon.edu/arkadiy/transitive.pdf"><span class=SpellE><span style='font-family:"Times New Roman",serif'>ArXiv</span></span></a><span style='font-family:"Times New Roman",serif;color:black'> one).</span></p> <p class=MsoNormal style='margin-bottom:0in'><span class=SpellE><span style='font-family:"Times New Roman",serif;color:black'>Gallai</span></span><span style='font-family:"Times New Roman",serif;color:black'> coloring of the complete graph is an edge-coloring with no rainbow triangle. This concept first appeared in the study of comparability graphs and anti-Ramsey theory. We introduce a transitive analogue for acyclic directed graphs, and generalize both notions to <span class=SpellE>Coxeter</span> systems, matroids and commutative algebras. It is shown that for any finite matroid (or oriented matroid), the maximal number of colors is equal to the matroid rank. This generalizes a result of <span class=SpellE>ErdQs-Simonovits-S�s</span> for complete graphs. The number of <span class=SpellE>Gallai</span> (or transitive) colorings of the matroid that use at most </span><i><span style='font-family: "Times New Roman",serif'>k</span></i><span style='font-family:"Times New Roman",serif'> colors is a polynomial in<span style='color:blue'> </span><i><span style='color:black'>k</span></i>. Also, for any acyclic oriented matroid, represented over the real numbers, the number of transitive colorings using at most 2 colors is equal to the number of chambers in the dual hyperplane arrangement. We count <span class=SpellE>Gallai</span> and transitive colorings of the root system of type A using the maximal number of colors, and show that, when equipped with a natural descent set map, the resulting <span class=SpellE>quasisymmetric</span> function is symmetric and Schur-positive.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="https://u.math.biu.ac.il/~yuval/"><b><span style='font-family:"Times New Roman",serif; color:blue'>Twists on rational <span class=SpellE>Cherednik</span> algebras</span></b></a><span style='font-family:"Times New Roman",serif;color:black'> (with </span><a href="http://www.maths.manchester.ac.uk/~ybazlov/"><span style='font-family: "Times New Roman",serif;color:blue'>Y. <span class=SpellE>Bazlov</span></span></a><span style='font-family:"Times New Roman",serif'>, </span><a href="https://research.manchester.ac.uk/en/persons/edward.jones-healey"><span style='font-family:"Times New Roman",serif;color:blue'>E. Jones-Healey</span></a><span style='font-family:"Times New Roman",serif'>, A. McGaw),<span style='color: black'> </span></span><a href="https://academic.oup.com/qjmath"><span style='font-family:"Times New Roman",serif;color:blue'>Quarterly Journal of Mathematics</span></a><span style='font-family:"Times New Roman",serif; color:black'>,&nbsp; <b>74</b> (2), 2022.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>We show that braided <span class=SpellE>Cherednik</span> algebras introduced by the first two authors are cocycle twists of rational <span class=SpellE>Cherednik</span> algebras of the imprimitive complex reflection groups G(<span class=SpellE><span class=GramE><i>m</i>,<i>p</i></span>,<i>n</i></span></span><span style='font-family:"Times New Roman",serif'>), when <i>m</i> is even. This gives a new construction of mystic reflection groups which have <span class=SpellE>Artin-Schelter</span> regular rings of quantum polynomial invariants. As an application of this result, we show that a braided <span class=SpellE>Cherednik</span> algebra has a finite-dimensional representation if and only if its rational counterpart has one.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:blue'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in;background:white'><span style='color:black'><a href="https://pages.uoregon.edu/arkadiy/symp.groups.noncom.pdf"><span class=SpellE><b><span style='font-family:"Times New Roman",serif;color:blue'>Symplectic</span></b></span><b><span style='font-family:"Times New Roman",serif;color:blue'> groups over noncommutative algebras</span></b></a></span><span style='font-family:"Times New Roman",serif; color:black'> (with </span><span style='color:black'><a href="https://www.math.columbia.edu/~alessandrini/"><span style='font-family: "Times New Roman",serif;color:black'>D. <span class=SpellE>Alessandrini</span></span></a></span><span style='font-family:"Times New Roman",serif;color:black'>, </span><span style='color:black'><a href="https://sites.math.rutgers.edu/~vretakh/"><span style='font-family:"Times New Roman",serif;color:black'>V. <span class=SpellE>Retakh</span></span></a></span><span style='font-family:"Times New Roman",serif;color:black'>, </span><span style='color:black'><a href="https://www.researchgate.net/profile/Eugen-Rogozinnikov"><span style='font-family:"Times New Roman",serif;color:black'>E. <span class=SpellE>Rogozinnikov</span></span></a></span><span style='font-family:"Times New Roman",serif;color:black'>, </span><span style='color:black'><a href="https://www.mpg.de/19381685/mathematics-in-the-sciences-wienhard"><span style='font-family:"Times New Roman",serif;color:black'>A. <span class=SpellE>Wienhard</span></span></a></span><span style='font-family:"Times New Roman",serif;color:black'>) </span><span style='color:black'><a href="https://www.springer.com/journal/29"><i><span style='font-family:"Times New Roman",serif;color:blue'>Selecta Mathematica</span></i></a></span><span style='font-family:"Times New Roman",serif;color:black'>, <b>28</b>,&nbsp; 82 (2022)</span></p> <p class=MsoNormal style='margin-bottom:0in;background:white'><span style='font-family:"Times New Roman",serif;color:black'>We introduce the <span class=SpellE>symplectic</span> group Sp<sub>2</sub>(<span class=GramE>A,<span lang=RU style='mso-ansi-language:RU'>�</span></span>) over a noncommutative algebra A with an anti-involution </span><span lang=RU style='font-family:"Times New Roman",serif; color:black;mso-ansi-language:RU'>�</span><span style='font-family:"Times New Roman",serif; color:black'>. We realize several classical Lie groups as Sp<sub>2</sub> over various noncommutative algebras, which provide new insights into their structure theory. We construct several geometric spaces, on which the groups Sp<sub>2</sub>(<span class=GramE>A,<span lang=RU style='mso-ansi-language:RU'>�</span></span>) act. We introduce the space of isotropic A-lines, which generalizes the projective line. We describe the action of Sp<sub>2</sub>(<span class=GramE>A,<span lang=RU style='mso-ansi-language:RU'>�</span></span>) on isotropic A-lines, generalize the <span class=SpellE>Kashiwara</span>-Maslov index of triples and the cross ratio of quadruples of isotropic A-lines as invariants of this action. When the algebra A is Hermitian or the complexification of a Hermitian algebra, we introduce the symmetric space XSp<sub>2</sub>(<span class=GramE>A,<span lang=RU style='mso-ansi-language:RU'>�</span></span>), and construct different models of this space. Applying this to classical Hermitian Lie groups of tube type (realized as Sp<sub>2</sub>(<span class=GramE>A,<span lang=RU style='mso-ansi-language:RU'>�</span></span>)) and their complexifications, we obtain different models of the symmetric space as noncommutative generalizations of models of the hyperbolic plane and of the three-dimensional hyperbolic space. We also provide a partial classification of Hermitian algebras in Appendix A.</span></p> <p class=MsoNormal style='margin-bottom:0in;background:white'><span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="https://pages.uoregon.edu/arkadiy/geom.mult.pdf"><b><span style='font-family:"Times New Roman",serif;color:#0070C0'>Geometric multiplicities</span></b></a><b><span style='font-family:"Times New Roman",serif'> </span></b><span style='font-family:"Times New Roman",serif'>(with </span><a href="https://www.researchgate.net/scientific-contributions/Yanpeng-Li-2133340975"><span style='font-family:"Times New Roman",serif'>Y. Li</span></a><span style='font-family:"Times New Roman",serif'>),<b> </b>preprint <span style='color:black'>&nbsp;</span></span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>In this paper, we introduce geometric multiplicities, which are positive varieties with potential fibered over the <span class=SpellE>Cartan</span> subgroup <i>H</i> of a reductive group <i>G</i>. They form a monoidal <span class=GramE>category</span> and we construct a monoidal functor from this category to the representations of the <span class=SpellE>Langlands</span> dual group <span class=SpellE><i>Gv</i></span> of <i>G</i>. Using this, we explicitly compute various multiplicities in <span class=SpellE><i>G<sup>v</sup></i></span></span><span style='font-family:"Times New Roman",serif'>-modules in many ways. <span class=GramE>In particular, we</span> recover the formulas for tensor product multiplicities of <span class=SpellE>Berenstein-Zelevinsky</span> and generalize them in several directions. In the case when our geometric multiplicity <i>X</i> is a monoid, i.e., the corresponding <span class=SpellE><i>G<sup>v</sup></i></span>-module is an algebra, we expect that in many cases, the spectrum of this algebra is an affine <span class=SpellE><i>G<sup>v</sup></i></span>-variety <span class=SpellE><i>X<sup>v</sup></i></span>, and thus the correspondence <span class=SpellE><i>X<span style='color:black'>�X<sup>v</sup></span></i></span><span style='color:black'> has a flavor of both the <span class=SpellE>Langlands</span> duality and mirror symmetry.</span></span><br> <span style='font-size:6.0pt;line-height:115%;font-family:"Times New Roman",serif; color:black'>&nbsp; </span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="https://pages.uoregon.edu/arkadiy/langlands.poisson.cluster.pdf"><span class=SpellE><b><span style='font-family:"Times New Roman",serif;color:blue'>Langlands</span></b></span><b><span style='font-family:"Times New Roman",serif;color:blue'> Duality and Poisson-Lie Duality via Cluster Theory and Tropicalization</span></b></a><b><span style='font-family:"Times New Roman",serif;color:black'> </span></b><span style='font-family:"Times New Roman",serif;color:black'>(with </span><a href="https://www.unige.ch/math/en/section/enseignants-et-chercheurs"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>A. Alekseev</span></a><span style='font-family:"Times New Roman",serif; color:black'>, </span><a href="http://www.math.cornell.edu/~bsh68/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>B. Hoffman</span></a><span style='font-family:"Times New Roman",serif; color:black'>, </span><a href="https://www.researchgate.net/scientific-contributions/Yanpeng-Li-2133340975"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Y. Li</span><span style='font-family:"Times New Roman",serif; color:windowtext;text-decoration:none;text-underline:none'>)</span></a><span style='font-family:"Times New Roman",serif;color:black'> </span><a href="https://www.springer.com/journal/29"><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>Selecta Mathematica</span></a><span style='font-family:"Times New Roman",serif;color:black'>, <b>27</b>, 69 (2021) </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>Let<i> G</i> be a connected <span class=SpellE>semisimple</span> Lie group. There are two natural duality constructions that assign to it the <span class=SpellE>Langlands</span> dual group <span class=SpellE><i>G<sup>v</sup></i></span> and the Poisson-Lie dual group <i>G</i>*. The main result of this paper is the following relation between these two objects: the integral cone defined by the cluster structure and the <span class=SpellE>Berenstein-Kazhdan</span> potential on the double <span class=SpellE>Bruhat</span> cell <span class=SpellE><span class=GramE><i>G<sup>v;w</sup></i><i><sup><span style='font-size:8.0pt;line-height:115%'>o</span></sup></i></span><i><sup>,e</sup></i></span>. is isomorphic to the integral Bohr-Sommerfeld cone defined by the Poisson structure on the partial tropicalization of <i>K</i>*</span><span style='font-family:"Cambria Math",serif;mso-bidi-font-family:"Cambria Math"; color:black'>�"</span><span style='font-family:"Times New Roman",serif; color:black'>G* (the Poisson-Lie dual of the compact form <i>K</i></span><span style='font-family:"Cambria Math",serif;mso-bidi-font-family:"Cambria Math"; color:black'>�"</span><i><span style='font-family:"Times New Roman",serif; color:black'>G</span></i><span style='font-family:"Times New Roman",serif; color:black'>). The first cone parametrizes the canonical bases of irreducible <i>G</i>-modules. The corresponding points in the second cone belong to integral <span class=SpellE>symplectic</span> leaves of the partial tropicalization labeled by the highest weight of the representation. As a by-product of our construction, we show that <span class=SpellE>symplectic</span> volumes of generic <span class=SpellE>symplectic</span> leaves in the partial tropicalization of <i>K</i>* are equal to <span class=SpellE>symplectic</span> volumes of the corresponding coadjoint orbits in <b><i>k</i></b>*. To achieve these goals, we use (<span class=SpellE>Langlands</span> dual) double cluster varieties defined by <span class=SpellE>Fock</span> and Goncharov. These are pairs of cluster varieties whose seed matrices are transpose to each other. There is a naturally defined isomorphism between their tropicalizations. The isomorphism between the cones described above is a particular instance of such an isomorphism associated to the double <span class=SpellE>Bruhat</span> cells <i>G<sup> <span class=SpellE>w<span style='font-size:8.0pt;line-height:115%'>o</span>,e</span></sup></i> </span><span style='font-family:"Cambria Math",serif;mso-bidi-font-family:"Cambria Math"; color:black'>�"</span><span style='font-family:"Times New Roman",serif; color:black'> <i>G</i> and <span class=SpellE><i>G<sup>v;w</sup></i><i><sup><span style='font-size:8.0pt;line-height:115%'>o</span>,e</sup></i></span>.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/cacti.crystals.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>On cacti and crystals</span></b></a><span style='font-family:"Times New Roman",serif;color:black'> (with </span><a href="http://front.math.ucdavis.edu/author/J.Greenstein"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>J. Greenstein</span></a><span style='font-family:"Times New Roman",serif; color:black'> and </span><a href="https://sites.google.com/view/jianrong-li"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>J.-R. Li</span></a><span style='font-family:"Times New Roman",serif; color:black'>) <i>Representations and Nilpotent Orbits of Lie Algebraic Systems: in honor of the 75th Birthday of Tony Joseph</i>,&nbsp; </span><a href="https://www.springer.com/series/4848"><i><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>Progress in Mathematic</span></i></a><i><span style='font-family:"Times New Roman",serif;color:black'>s</span></i><span style='font-family:"Times New Roman",serif;color:black'>,&nbsp;&nbsp; <b>330</b>, 2019. </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>In the present work we study actions of various groups generated by involutions on the category <span class=SpellE><i>O<sub>q</sub><sup>int</sup></i></span>(</span><b><i><span style='font-family:"Times New Roman",serif'>g</span></i></b><span style='font-family:"Times New Roman",serif'>) of integrable highest weight <span class=SpellE><i><span style='color:black'>U<sub>q</sub></span></i></span><i><span style='color:black'>(<b>g</b>)</span></i><span style='color:black'>-modules and their crystal bases for any <span class=SpellE>symmetrizable</span> Kac-Moody algebra <b><i>g</i></b>. The most notable of them are the cactus group and (yet conjectural) Weyl group action on any highest weight integrable module and its lower and upper crystal bases. Surprisingly, some generators of cactus groups are anti-involutions of the Gelfand-Kirillov model for <span class=SpellE><i>O<sub>q</sub><sup>int</sup></i></span>(</span><b><i>g</i></b>) closely related to the remarkable quantum twists discovered by Kimura and Oya.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="https://pages.uoregon.edu/arkadiy/double.bruhat.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Poisson structures and potentials</span></b></a><b><span style='font-family:"Times New Roman",serif; color:black'> </span></b><span style='font-family:"Times New Roman",serif; color:black'>(with </span><a href="https://www.unige.ch/math/en/section/enseignants-et-chercheurs"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>A. Alekseev</span></a><span style='font-family:"Times New Roman",serif; color:black'>, </span><a href="http://www.math.cornell.edu/~bsh68/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>B. Hoffman</span></a><span style='font-family:"Times New Roman",serif; color:black'>, </span><a href="https://www.researchgate.net/scientific-contributions/Yanpeng-Li-2133340975"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Y. Li</span></a><span style='font-family:"Times New Roman",serif; color:black'>) <i>Lie Groups, Geometry, and Representation Theory: A Tribute to the Life and Work of Bertram <span class=SpellE>Kostant</span></i>, </span><a href="https://www.springer.com/gp/book/9783030021900"><span class=SpellE><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Birkhauser</span></span></a><span style='font-family:"Times New Roman",serif; color:black'>, 2018.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>We introduce a notion of weakly log-canonical Poisson structures on positive varieties with potentials. Such a Poisson structure is log-canonical up to terms dominated by the potential. To a compatible real form of a weakly log-canonical Poisson variety we assign an integrable system on the product of a certain real convex polyhedral cone (the tropicalization of the variety) and a compact torus. We apply this theory to the dual Poisson-Lie group G* of a <span class=GramE>simply-connected</span> <span class=SpellE>semisimple</span> complex Lie group G. We define a positive structure and potential on <i>G</i>* and show that the natural Poisson-Lie structure on <i>G</i>* is weakly log-canonical with respect to this positive structure and potential. For <i>K</i></span><span style='font-family:"Cambria Math",serif;mso-bidi-font-family:"Cambria Math"; color:black'>�"</span><i><span style='font-family:"Times New Roman",serif; color:black'>G</span></i><span style='font-family:"Times New Roman",serif; color:black'> the compact real form, we show that the real form <i>K</i>*</span><span style='font-family:"Cambria Math",serif;mso-bidi-font-family:"Cambria Math"; color:black'>�"</span><i><span style='font-family:"Times New Roman",serif; color:black'>G</span></i><span style='font-family:"Times New Roman",serif; color:black'>* is compatible and prove that the corresponding integrable system is defined on the product of the decorated string cone and the compact torus of dimension 1/2(dim <i>G -</i> rank <i>G</i>).</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/noncomm.catalan.pub.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Noncommutative Catalan numbers</span></b></a><b><span style='font-family:"Times New Roman",serif; color:black'> </span></b><span style='font-family:"Times New Roman",serif; color:black'>(with </span><a href="https://sites.math.rutgers.edu/~vretakh/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>V. <span class=SpellE>Retakh</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>) </span><a href="https://www.springer.com/journal/26"><i><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>Annals of Combinatorics</span></i></a><span style='font-family:"Times New Roman",serif;color:black'>, Vol. 23, Issue 3 4 (2019), 527 547.</span></p> <p class=MsoNormal style='margin-bottom:12.0pt'><span style='font-family:"Times New Roman",serif; color:black'>The goal of this paper is to introduce and study noncommutative Catalan numbers <i>C<sub>n</sub></i> which belong to the free Laurent polynomial algebra in <i>n</i> generators. Our noncommutative numbers admit interesting (commutative and noncommutative) specializations, one of them related to <span class=SpellE>Garsia-Haiman</span> (<span class=SpellE><span class=GramE><i>q</i>,<i>t</i></span></span>)-versions, another -- to solving noncommutative quadratic equations. We also establish total positivity of the corresponding (noncommutative) Hankel matrices <span class=SpellE><i>H<sub>n</sub></i></span> and introduce accompanying noncommutative binomial coefficients.</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/factorizable.module.algebras.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Factorizable module algebras</span></b></a><b><span style='font-family:"Times New Roman",serif; color:black'> </span></b><span style='font-family:"Times New Roman",serif; color:black'>(with </span><a href="https://www.researchgate.net/profile/Karl-Schmidt-10"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>K. Schmidt</span></a><span style='font-family:"Times New Roman",serif; color:black'>) <i>&nbsp;</i></span><a href="https://academic.oup.com/imrn"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Int. Math. Res. Not</span></i></a><i><span style='font-family:"Times New Roman",serif;color:blue'>.</span></i><span style='font-family:"Times New Roman",serif;color:black'> <b>2019</b> (21), 6711 6764 (2019).</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>The aim of this paper is to introduce and study a large class of <b><i>g</i></b>-module algebras which we call factorizable by generalizing the Gauss factorization of (square or rectangular) matrices. This class includes coordinate algebras of corresponding reductive groups <i>G</i>, their parabolic subgroups, basic affine spaces and many others. It turns out that tensor products of factorizable algebras are also factorizable and it is easy to create a factorizable algebra out of virtually any <b><i>g</i></b>-module algebra. We also have quantum versions of all these constructions in the category of <span class=SpellE><i>U<sub>q</sub></i></span><i>(<b>g</b>)</i>-module algebras. Quite surprisingly, our quantum factorizable algebras are naturally acted on by the quantized enveloping algebra <span class=SpellE><i>U<sub>q</sub></i></span><i>(<b>g</b>*)</i> of the dual Lie <span class=SpellE>bialgebra</span> <b><i>g</i></b><i>*</i> of <b><i>g</i></b>.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/hecke.hopf.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Hecke-<span class=SpellE>Hopf</span> algebras</span></b></a><span style='font-family:"Times New Roman",serif; color:black'> (with </span><a href="http://www.ma.huji.ac.il/~kazhdan/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>D. <span class=SpellE>Kazhdan</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>)&nbsp; </span><a href="https://www.journals.elsevier.com/advances-in-mathematics"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Advances in Mathematics</span></i></a><span style='font-family:"Times New Roman",serif;color:black'>, Vol. 353 (2019), 312 395.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;Let <i>W</i> be a <span class=SpellE>Coxeter</span> group. The goal of the paper is to construct new <span class=SpellE>Hopf</span> algebras contain Hecke algebras </span><span class=SpellE><i><span style='font-size:10.0pt;line-height:115%;font-family: "Times New Roman",serif;color:black'>H</span></i><b><i><sub><span style='font-size:13.5pt;line-height:115%;font-family:"Times New Roman",serif; color:black'>q</span></sub></i></b></span><i><span style='font-family:"Times New Roman",serif; color:black'>(W)</span></i><span style='font-family:"Times New Roman",serif; color:black'> as (left) coideal subalgebras. Our <i>Hecke-<span class=SpellE>Hopf</span> <span class=GramE>algebras<span style='font-style:normal'>&nbsp; </span><b>H</b></span>(W)</i> have a number of applications. <span class=GramE>In particular they</span> provide new solutions of quantum Yang-Baxter equation and lead to a construction of a new family of endo-functors of the category of </span><span class=SpellE><i><span style='font-size:10.0pt;line-height:115%;font-family: "Times New Roman",serif;color:black'>H</span></i><b><i><sub><span style='font-size:13.5pt;line-height:115%;font-family:"Times New Roman",serif; color:black'>q</span></sub></i></b></span><i><span style='font-family:"Times New Roman",serif; color:black'>(W)</span></i><span style='font-family:"Times New Roman",serif; color:black'>-modules. Hecke-<span class=SpellE>Hopf</span> algebras for the symmetric group are related to Fomin-Kirillov algebras; for an arbitrary <span class=SpellE>Coxeter</span> group <span class=GramE><i>W</i>&nbsp; the</span>  <span class=SpellE>Demazure</span> part of <b><i>H</i></b>(<i>W</i>) is being acted upon by generalized braided derivatives which generate the corresponding (generalized) Nichols algebra. </span><br> <b><span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span></b></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/schubbas.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Canonical bases of quantum Schubert cells and their symmetries</span></b></a><span style='font-family:"Times New Roman",serif; color:black'> (with </span><a href="https://profiles.ucr.edu/app/home/profile/jacobg"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>J. Greenstein</span></a><span style='font-family:"Times New Roman",serif; color:black'>),&nbsp;&nbsp; </span><a href="http://link.springer.com/journal/29"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Selecta Mathematica</span></i></a><span style='font-family: "Times New Roman",serif;color:black'>, </span><b><span style='font-family:"Times New Roman",serif; color:#333333'>23</span></b><span style='font-family:"Times New Roman",serif; color:#333333'>, pages 2755 2799 (2017</span><span style='font-family:"Times New Roman",serif'>)<span style='color:black'>.</span></span><br> <span style='font-family:"Times New Roman",serif;color:#333333'>&nbsp;</span><span style='font-family:"Times New Roman",serif;color:black'>The goal of this work is to provide an elementary construction of the canonical basis <i>B(w)</i> in each quantum Schubert cell </span><span class=SpellE><i><span style='font-family: "Times New Roman",serif'>U<sub>q</sub></span></i></span><span style='font-family: "Times New Roman",serif'>(w) and to establish its invariance under modified <span class=SpellE>Lusztig s</span> symmetries. To that effect, we obtain a direct characterization of the upper global basis <span class=SpellE><b><i>B</i></b><i><sup>u<b>p</b></sup></i></span> in terms of a suitable bilinear form and show that <b><i>B</i></b><i>(w)</i> is contained in <span class=SpellE><b><i>B</i></b><i><sup>u<b>p</b></sup></i></span> and its large part is preserved by modified <span class=SpellE>Lusztig s</span> symmetries.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="https://pages.uoregon.edu/arkadiy/noncomtriangsurf.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Noncommutative marked surfaces</span></b></a><b><span style='font-family:"Times New Roman",serif'> </span></b><span style='font-family:"Times New Roman",serif;color:#333333'>(with </span><a href="http://www.math.rutgers.edu/~vretakh/"><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>V. <span class=SpellE>Retakh</span></span></a><span style='font-family:"Times New Roman",serif;color:#333333'>), </span><a href="https://www.journals.elsevier.com/advances-in-mathematics"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Advances in Mathematics</span></i></a><span style='font-family:"Times New Roman",serif;color:#333333'>, </span><span style='font-family:"Times New Roman",serif;color:black'>Vol 328 (2018), pages 1010 1087.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>The aim of the paper is to attach a noncommutative cluster-like structure to each marked surface �. This is a noncommutative algebra A<sub>�</sub> generated by  noncommutative geodesics between marked points subject to certain triangular relations and noncommutative analogues of Ptolemy-<span class=SpellE>Plucker</span> relations. It turns out that the algebra A<sub>�</sub> exhibits a noncommutative Laurent Phenomenon with respect to any triangulation of �, which confirms its  cluster nature. As a surprising byproduct, we obtain a new topological invariant of �, which is a free or a 1-relator group easily computable in terms of any triangulation of �.&nbsp;&nbsp; Another application is the proof of <span class=SpellE>Laurentness</span> and positivity of certain discrete noncommutative integrable systems.</span><span style='font-family: "Times New Roman",serif'> </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/generalized.adjoint.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Generalized adjoint actions</span></b></a><span style='font-family:"Times New Roman",serif; color:black'> (with </span><a href="https://sites.math.rutgers.edu/~vretakh/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>V. <span class=SpellE>Retakh</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="http://www.emis.de/journals/JLT/"><i><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>Journal of Lie Theory</span></i></a><span style='font-family:"Times New Roman",serif;color:black'>, 26 (2016), No. 1, pages 219 225.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>The aim of this paper is to generalize the classical formula <span class=SpellE>e<sup>x</sup>ye</span><sup>-x</sup>=�<sub>ke"0</sub> 1/k! (ad <span class=GramE>x)<sup>k</sup></span>(y). We also obtain combinatorial applications to <b><i>q</i></b>-exponentials, <b><i>q</i></b>-binomials, and Hall-Littlewood polynomials.</span><br> <span style='font-family:"Times New Roman",serif'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/joseph.decomp.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Generalized Joseph s decompositions</span></b></a><span style='font-family:"Times New Roman",serif; color:black'> (with </span><a href="https://profiles.ucr.edu/app/home/profile/jacobg"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>J. Greenstein</span></a><span style='font-family:"Times New Roman",serif; color:black'>), </span><a href="https://www.sciencedirect.com/journal/comptes-rendus-mathematique"><span class=SpellE><i><span style='font-family:"Times New Roman",serif'>Comptes</span></i></span><span style='font-family:"Times New Roman",serif'> <span class=SpellE><i>Rendus</i></span> </span><span class=SpellE><i><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>Mathematique</span></i></span></a><span style='font-family:"Times New Roman",serif;color:black'>, Doi : 10.1016/j.crma.2015.07.002.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;We generalize the decomposition of <span class=SpellE><i>U<sub>q</sub></i></span><i>(<b>g</b>)</i> introduced by A. Joseph and relate it, for g <span class=SpellE>semisimple</span>, to the celebrated computation of central elements due to V. <span class=SpellE>Drinfeld</span>. In that case we construct a natural basis in the center of <span class=SpellE><i>U<sub>q</sub></i></span><i>(<b>g</b>)</i> whose elements behave as Schur polynomials and thus explicitly identify the center with the ring of symmetric functions.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/integrableclusters.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Integrable clusters</span></b></a><span style='font-family:"Times New Roman",serif;color:black'> (with </span><a href="https://profiles.ucr.edu/app/home/profile/jacobg"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>J. Greenstein</span></a><span style='font-family:"Times New Roman",serif; color:black'>, </span><a href="http://www.ma.huji.ac.il/~kazhdan/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>D. <span class=SpellE>Kazhdan</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="https://www.sciencedirect.com/journal/comptes-rendus-mathematique"><span class=SpellE><i><span style='font-family:"Times New Roman",serif'>Comptes</span></i></span><span style='font-family:"Times New Roman",serif'> <span class=SpellE><i>Rendus</i></span> </span><span class=SpellE><i><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>Mathematique</span></i></span></a><span class=SpellE><span style='font-family:"Times New Roman",serif;color:#333333'>,Vol</span></span><span style='font-family:"Times New Roman",serif;color:#333333'> 353, <b>5</b></span><span style='font-family:"Times New Roman",serif;color:#2E2E2E'> (2015), pages 387 390</span><span style='font-family:"Times New Roman",serif;color:black'>.</span><br> <span style='font-family:"Times New Roman",serif;color:#333333'>&nbsp;The goal of this note is to study quantum clusters in which cluster variables (not coefficients) commute which each other. It turns out that this property is preserved by mutations. Remarkably, this is equivalent to the celebrated sign coherence conjecture recently proved by M. Gross, P. Hacking, S. Keel and M. <span class=SpellE>Kontsevich</span>.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="https://pages.uoregon.edu/arkadiy/doublecanbases.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Double canonical bases</span></b></a><span style='font-family:"Times New Roman",serif;color:black'> (with </span><a href="https://profiles.ucr.edu/app/home/profile/jacobg"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>J. Greenstein</span></a><span style='font-family:"Times New Roman",serif; color:black'>), </span><a href="https://www.sciencedirect.com/journal/advances-in-mathematics"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Advances in <span class=SpellE>Mathematics</span></span></i></a><span class=SpellE><span style='font-family:"Times New Roman",serif;color:black'>,Vol</span></span><span style='font-family:"Times New Roman",serif;color:black'>. 316 (2017), pages 54 111.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>We introduce a new class of bases for quantized universal enveloping algebras <span class=SpellE><i>U<sub>q</sub></i></span><i>(<b>g</b>) </i>and other doubles attached to <span class=SpellE>semisimple</span> and Kac-Moody Lie algebras. These bases contain dual canonical bases of upper and lower halves of <span class=SpellE><i>U<sub>q</sub></i></span><i>(<b>g</b>)</i> and are invariant under many symmetries including all <span class=SpellE>Lusztig s</span> symmetries if <b><i>g</i></b> is <span class=SpellE>semisimple</span>. It also turns out that a part of a double canonical basis of <span class=SpellE><i>U<sub>q</sub></i></span><i>(<b>g</b>)</i> spans its center.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/mystic.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Mystic reflection groups</span></b></a><span style='font-family:"Times New Roman",serif;color:black'> (with </span><a href="https://research.manchester.ac.uk/en/persons/yuri.bazlov"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Y. <span class=SpellE>Bazlov</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="http://www.emis.de/journals/SIGMA/"><i><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>SIGMA</span></i></a><span style='font-family:"Times New Roman",serif;color:black'> 10 (2014), 040, 11 pages.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>This paper aims to systematically study mystic reflection groups that emerged independently in a paper by the authors and in a paper by Kirkman, <span class=SpellE>Kuzmanovich</span>, and Zhang. A detailed analysis of this class of groups reveals that they are in a nontrivial correspondence with complex reflection groups <i>G(<span class=SpellE><span class=GramE>m,p</span>,n</span>)</i>. We also prove that the group algebras of corresponding groups are isomorphic and classify all such groups up to isomorphism.</span><span style='font-family: "Times New Roman",serif'> </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/feiginchar.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Quantum cluster characters of Hall algebras</span></b></a><span style='font-family:"Times New Roman",serif; color:blue'> (</span><span style='font-family:"Times New Roman",serif; color:black'>with </span><a href="https://scholar.google.com/citations?user=u-_JDfcAAAAJ&amp;hl=en"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>D. Rupel</span></a><span style='font-family:"Times New Roman",serif; color:blue'>), </span><a href="http://link.springer.com/journal/29"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Selecta Mathematica</span></i></a><span style='font-family: "Times New Roman",serif;color:blue'>, </span><b><span style='font-family:"Times New Roman",serif; color:#333333'>21</span></b><span style='font-family:"Times New Roman",serif; color:#333333'>, pages</span><span style='font-family:"Times New Roman",serif; color:black'> 1121 1176 (2015).</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>The aim of the paper is to introduce a generalized quantum cluster character, which assigns to each object <i>V</i> of a finitary Abelian category <span class=SpellE><i>C</i> over</span> a finite field <span class=SpellE><i>F</i><i><sub><span style='font-size:14.0pt;line-height:115%'>q</span></sub></i></span> and any sequence <span class=SpellE>i</span> of simple objects in <i>C</i> the element <span class=SpellE><span class=GramE><i>X</i><i><sub><span style='font-size:14.0pt; line-height:115%'>V,<b>i</b></span></sub></i></span></span> of the corresponding algebra <span class=SpellE>P<i><sub><span style='font-size:14.0pt; line-height:115%'>C</span></sub></i><sub><span style='font-size:14.0pt; line-height:115%'>,<b><i>i</i></b></span></sub></span> of <b><i>q</i></b>-polynomials. We prove that if <i>C</i> was hereditary, then the assignments <span class=SpellE><span class=GramE><i>V�X</i><i><sub><span style='font-size:14.0pt; line-height:115%'>V,<b>i</b></span></sub></i></span></span></span><span style='font-size:14.0pt;line-height:115%;font-family:"Times New Roman",serif; color:black'> </span><span style='font-family:"Times New Roman",serif; color:black'>define algebra homomorphisms from the (dual) Hall-<span class=SpellE>Ringel</span> algebra of <i>C</i> to the <span class=SpellE>P<i><sub><span style='font-size:14.0pt;line-height:115%'>C</span></sub></i><sub><span style='font-size:14.0pt;line-height:115%'>,<b><i>i</i></b></span></sub></span>, which generalize the well-known <span class=SpellE>Feigin</span> homomorphisms from the upper half of a quantum group to <b><i>q</i></b>-polynomial algebras. If <i>C</i> is the representation category of an acyclic valued quiver <i>(<span class=SpellE><span class=GramE>Q,d</span></span>)</i> and <span class=SpellE>i</span>=(<span class=SpellE><b><i>i</i></b><sub><span style='font-size:14.0pt;line-height: 115%'>o</span></sub>,<b><i>i</i></b><sub><span style='font-size:14.0pt; line-height:115%'>o</span></sub></span>), where <b><i>i</i></b></span><sub><span style='font-size:14.0pt;line-height:115%;font-family:"Times New Roman",serif; color:black'>o</span></sub><span style='font-family:"Times New Roman",serif; color:black'> is a repetition-free source-adapted sequence, then we prove that the <span class=SpellE><b><i>i</i></b></span>-character <span class=SpellE><i>X</i><i><sub><span style='font-size:14.0pt;line-height:115%'>V,<b>i</b></span></sub></i></span>&nbsp; equals the quantum cluster character <i>X</i></span><i><sub><span style='font-size:14.0pt;line-height:115%;font-family:"Times New Roman",serif; color:black'>V</span></sub></i><span style='font-family:"Times New Roman",serif; color:black'> introduced earlier by the second author in [29] and [30]. Using this identification, we deduce a quantum cluster structure on the quantum unipotent cell corresponding to the square of a <span class=SpellE>Coxeter</span> element. As a corollary, we prove a conjecture from the joint paper [5] of the first author with A. <span class=SpellE>Zelevinsky</span> for such quantum unipotent cells. As a byproduct, we construct the quantum twist and prove that it preserves the triangular basis introduced by A. <span class=SpellE>Zelevinsky</span> and the first author in [6].</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/cocycle.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Cocycle twists and extensions of braided doubles</span></b></a><span style='font-family:"Times New Roman",serif; color:black'> (with </span><a href="https://research.manchester.ac.uk/en/persons/yuri.bazlov"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Y. <span class=SpellE>Bazlov</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="http://www.ams.org/publications/books/monographs/conm-home"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Contemp. Math.</span></i></a><span style='font-family: "Times New Roman",serif;color:black'>, <b>592</b> (2013), pages 19 70.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>It is well known that central extensions of a group <i>G</i> correspond to 2-cocycles on <i>G</i>. Cocycles can be used to construct extensions of <i>G</i>-graded algebras via a version of the <span class=SpellE>Drinfeld</span> twist introduced by Majid. We show how to define the second <span class=SpellE>cohomology</span> group of an abstract monoidal category <i>C</i>, <span class=SpellE>generalising</span> the Schur multiplier of a finite group and the lazy <span class=SpellE>cohomology</span> of a <span class=SpellE>Hopf</span> algebra, recently studied by <span class=SpellE>Schauenburg</span>, Bichon, <span class=SpellE>Carnovale</span> and others. A braiding on <i>C</i> leads to analogues of Nichols algebras in <i>C</i>, and we explain how the recent work on twists of Nichols algebras by <span class=SpellE>Andruskiewitsch</span>, Fantino, Garcia and <span class=SpellE>Vendramin</span> fits in our context. In the second part of the <span class=GramE>paper</span> we propose an approach to twisting the multiplication in braided doubles, which are a class of algebras with triangular decomposition over <i>G</i>. Braided doubles are not <i>G</i>-graded, but may be embedded in a double of a Nichols algebra, where a twist is carried out. This is a source of new algebras with triangular decomposition. As an example, we show how to twist the rational <span class=SpellE>Cherednik</span> algebra of the symmetric group by the cocycle arising from the Schur covering group, obtaining the spin <span class=SpellE>Cherednik</span> algebra introduced by Wang.</span><span style='font-family:"Times New Roman",serif'> </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/bbckl.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Macdonald Polynomials and BGG reciprocity for current algebras</span></b></a><b><span style='font-family:"Times New Roman",serif; color:black'> </span></b><span style='font-family:"Times New Roman",serif; color:black'>(with </span><a href="https://www.researchgate.net/profile/Matthew-Bennett-14"><span style='font-family:"Times New Roman",serif;color:blue'>M. Bennett</span></a><span style='font-family:"Times New Roman",serif;color:black'>, </span><a href="https://profiles.ucr.edu/app/home/profile/vyjayanc"><span style='font-family:"Times New Roman",serif;color:blue'>V. Chari</span></a><span style='font-family:"Times New Roman",serif;color:black'>, </span><a href="https://cris.haifa.ac.il/en/persons/anton-khoroshkin"><span style='font-family:"Times New Roman",serif;color:blue'>A. <span class=SpellE>Khoroshkin</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>, </span><a href="https://scholar.google.ru/citations?user=-oFg5VEAAAAJ&amp;hl=en"><span style='font-family:"Times New Roman",serif;color:blue'>S. <span class=SpellE>Loktev</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="https://www.springer.com/journal/29"><i><span style='font-family:"Times New Roman",serif; color:blue'>Selecta Mathematica</span></i></a><span style='font-family:"Times New Roman",serif; color:black'>,&nbsp; Vol. 20,&nbsp; <b>2</b> (2014),&nbsp; pages 585 607.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>We study the category of graded representations with finite-dimensional graded pieces for the current algebra associated to a simple Lie algebra. This category has many similarities with the category <i>O</i> of modules for <b><i>g</i></b> and in this paper, we use the combinatorics of Macdonald polynomials to prove an analogue of the famous BGG duality in the case of <i>sl</i></span><a href="http://www.ams.org/publications/books/monographs/conm-home"><i><sub><span style='font-size:14.0pt;line-height:115%;font-family:"Times New Roman",serif'>n+1</span></sub></i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>.</span></a></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/hallnichols.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Primitively generated Hall algebras</span></b></a><span style='font-family:"Times New Roman",serif; color:black'> (with </span><a href="https://profiles.ucr.edu/app/home/profile/jacobg"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>J. Greenstein</span></a><span style='font-family:"Times New Roman",serif; color:black'>),<b> </b></span><a href="http://msp.org/pjm"><i><span style='font-family:"Times New Roman",serif;color:blue'>Pacific Journal of Mathematics</span></i></a><span style='font-family:"Times New Roman",serif; color:black'>, Vol. 281, No. 2, 2016.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;The aim of the present paper is to demonstrate that Hall algebras of a large class of finitary exact categories behave like quantum nilpotent groups in the sense that they are generated by their primitive elements. Another goal is to construct analogues of quantum enveloping algebras as certain primitively generated subalgebras of the Hall algebras and conjecture an analogue of  Lie correspondence for those finitary categories.</span><br> <b><span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span></b><br> <a href="http://pages.uoregon.edu/arkadiy/bztriangbases.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Triangular bases in quantum cluster algebras</span></b></a><span style='font-family:"Times New Roman",serif; color:black'> (with </span><a href="http://www.math.neu.edu/~zelevinsky/mathindex.html"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>A. <span class=SpellE>Zelevinsky</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="http://imrn.oxfordjournals.org/"><i><span style='font-family:"Times New Roman",serif'>Int. Math. Res. N</span></i><i><span style='font-family:"Times New Roman",serif; color:blue'>o</span></i></a><a href="http://imrn.oxfordjournals.org/"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>t</span></i></a><a href="http://imrn.oxfordjournals.org/"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>.</span></i></a><span style='font-family:"Times New Roman",serif; color:black'> 2012, no. 21, pages 4821 4883.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>A lot of recent activity has been directed towards various constructions of  natural bases in cluster algebras. We develop a new approach to this problem which is close in spirit to <span class=SpellE>Lusztig s</span> construction of a canonical basis, and the pioneering construction of the <span class=SpellE>Kazhdan-Lusztig</span> basis in a Hecke algebra. The key ingredient of our approach is a new version of <span class=SpellE>Lusztig s</span> Lemma that we apply to all acyclic quantum cluster algebras. As a result, we construct the  canonical basis in every such algebra that we call the canonical triangular basis.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/ncfps.pdf"><b><span style='font-family: "Times New Roman",serif;color:#0B769F'>The reciprocal of </span></b><i><span style='font-family:"Times New Roman",serif;color:#0B769F'>�</span></i><b><i><sub><span style='font-size:14.0pt;line-height:115%;font-family:"Times New Roman",serif; color:#0B769F'>ne"0</span></sub></i></b><b><span style='font-family:"Times New Roman",serif; color:#0B769F'> </span></b><span class=SpellE><i><span style='font-family:"Times New Roman",serif; color:#0B769F'>a<sup>n</sup>b<sup>n</sup></span></i></span><b><span style='font-family:"Times New Roman",serif;color:#0B769F'> for non-commuting <i>a</i> and <i>b</i>, </span></b><b><span style='font-family:"Times New Roman",serif; color:blue'>Catalan numbers and non-commutative quadratic <span class=SpellE>equations</span></span></b></a><span class=SpellE><b><i><sub><span style='font-size:14.0pt;line-height:115%; font-family:"Times New Roman",serif;color:#0B769F'>��</span></sub></i></b><i><span style='font-family:"Times New Roman",serif;color:#0B769F'>����<sub>�</sub><sup>n</sup></span></i></span><b><i><sub><span style='font-family:"Times New Roman",serif;color:#0B769F'>�</span></sub></i></b><b><span style='font-family:"Times New Roman",serif;color:#0B769F'> for non-commuting <i>a</i> and <i>b</i>, </span></b><b><span style='font-family:"Times New Roman",serif; color:blue'>Catalan numbers and non-commutative quadratic equations</span></b><span style='font-family:"Times New Roman",serif;color:black'> (with&nbsp; </span><a href="http://www.math.rutgers.edu/~vretakh/"><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>V. <span class=SpellE>Retakh</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>, </span><a href="https://professeurs.uqam.ca/professeur/reutenauer.christophe/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>C. <span class=SpellE>Reutenauer</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>, </span><a href="http://www.math.rutgers.edu/~zeilberg/"><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>D. <span class=SpellE>Zeilberger</span></span></a><span style='font-family:"Times New Roman",serif;color:black'> )<i>, </i></span><a href="http://www.ams.org/publications/books/monographs/conm-home"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Contemp. Math.</span></i></a><span style='font-family: "Times New Roman",serif;color:black'> <b>592</b> (2013), 103 109.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>The aim of this paper is to describe the inversion of the sum <i>�<sub>ne"0��</sub></i> <span class=SpellE><i>a����<sup>n</sup><sub>�</sub>b<sup>n</sup></i></span> where <i>a</i> and <i>b</i> are non-commuting variables as a formal series in <i>a</i> and <i>b</i>. We show that the inversion satisfies a non-commutative quadratic equation and that the number of certain monomials in its homogeneous components equals to a Catalan number. We also study general solutions of similar quadratic equations.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/qchevalley.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Quantum <span class=SpellE>Chevalley</span> groups</span></b></a><span style='font-family: "Times New Roman",serif;color:black'> (with </span><a href="https://profiles.ucr.edu/app/home/profile/jacobg"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>J. Greenstein</span></a><span style='font-family:"Times New Roman",serif; color:black'>), </span><a href="http://www.ams.org/publications/books/monographs/conm-home"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Contemp. Math.</span></i></a><span style='font-family: "Times New Roman",serif;color:black'>, <b>592</b> (2013), pages 71 102.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;The goal of this paper is to construct quantum analogues of <span class=SpellE>Chevalley</span> groups inside completions of quantum groups or, more precisely, inside completions of Hall algebras of finitary categories. In particular, we obtain pentagonal and other identities in the quantum <span class=SpellE>Chevalley</span> groups which generalize their classical counterparts and explain <span class=SpellE>Faddeev</span>-Volkov quantum <span class=SpellE>dilogarithmic</span> identities and their recent generalizations due to Keller.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/lr.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Littlewood-Richardson coefficients for reflection groups</span></b></a><span style='font-family:"Times New Roman",serif; color:black'> (with </span><a href="http://www.math.ubc.ca/~erichmond/"><span style='font-family:"Times New Roman",serif;color:blue'>E. Richmond</span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="https://www.sciencedirect.com/journal/advances-in-mathematics"><i><span style='font-family:"Times New Roman",serif;color:blue'>Advances in Mathematics</span></i></a><span style='font-family:"Times New Roman",serif;color:black'>, Vol 284 </span><span style='font-family:"Times New Roman",serif'>(2015), pages 54 111.</span><br> <b><span style='font-family:"Times New Roman",serif;color:blue'>&nbsp;</span></b><span style='font-family:"Times New Roman",serif;color:black'>In this paper we explicitly compute all Littlewood-Richardson coefficients for <span class=SpellE>semisimple</span> or Kac-Moody groups <i>G</i>, that is, the structure coefficients of the <span class=SpellE>cohomology</span> algebra <i>&nbsp;H*(G/P)</i>, where <i>P</i> is a parabolic subgroup of <i>G</i>. These coefficients are of importance in enumerative geometry, algebraic combinatorics and representation theory. Our formula for the Littlewood-Richardson coefficients is purely combinatorial and is given in terms of the <span class=SpellE>Cartan</span> matrix and the Weyl group of <i>G</i>. <span class=GramE>In particular, our</span> formula gives a combinatorial proof of positivity of the Littlewood-Richardson coefficients in the cases when off-diagonal <span class=SpellE>Cartan</span> matrix entries are less than or equal to <i>-2</i>. Moreover, all our results for the Littlewood-Richardson coefficients extend to the structure coefficients of the<i> T</i>-equivariant <span class=SpellE>cohomology</span> algebra <i>H*<sub>T</sub>(G/P)</i>.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/kontsevich.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>A short proof of <span class=SpellE>Kontsevich</span> cluster conjecture</span></b></a><b><span style='font-family:"Times New Roman",serif;color:black'> </span></b><span style='font-family:"Times New Roman",serif;color:black'>(with </span><a href="http://www.math.rutgers.edu/~vretakh/"><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>V. <span class=SpellE>Retakh</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="https://www.sciencedirect.com/journal/comptes-rendus-mathematique"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>C. R. Math. Acad. Sci.</span></i></a><span style='font-family:"Times New Roman",serif;color:black'>, Paris 349 (2011), no. 3 4, pages 119 122.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;We give an elementary proof of the <span class=SpellE>Kontsevich</span> conjecture that asserts that the iterations of the noncommutative rational map <i>K<sub>r</sub>:(<span class=SpellE>x,y</span>)�!(xyx<sup>-1</sup>,(1+y<sup>-r</sup>)x<sup>-1</sup>)</i> are given by noncommutative Laurent polynomials.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/berkap2.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Stability inequalities and universal Schubert calculus of rank 2</span></b></a><b><span style='font-family:"Times New Roman",serif;color:black'> (</span></b><span style='font-family:"Times New Roman",serif;color:black'>with </span><a href="https://www.math.ucdavis.edu/~kapovich/"><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>M. <span class=SpellE>Kapovich</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="https://www.springer.com/journal/31"><i><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>Transformation Groups</span></i></a><span style='font-family:"Times New Roman",serif;color:black'>, Vol.&nbsp; <b>16</b>, Issue 4 (2011), pages 955 1007.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;The goal of the paper is to introduce a version of Schubert calculus for each dihedral reflection group <i>W</i>. That is, to each  sufficiently rich spherical building <i>Y</i> of type <i>W</i> we associate a certain <span class=SpellE>cohomology</span> theory and verify that, first, it depends only on <i>W</i> (i.e., all such buildings are  <span class=SpellE>homotopy</span> equivalent ) and second, the <span class=SpellE>cohomology</span> ring is the associated graded of the <span class=SpellE>coinvariant</span> algebra of <i>W</i> under certain filtration. We also construct the dual homology  pre-ring of<i> Y</i>. The convex  stability cones defined via these (co)homology theories of<i> Y</i> are then shown to solve the problem of classifying weighted <span class=SpellE>semistable</span> <i>m</i>-tuples on <i>Y</i> in the sense of <span class=SpellE>Kapovich</span>, <span class=SpellE>Leeb</span> and <span class=SpellE>Millson</span> equivalently, they are cut out by the generalized triangle inequalities for thick Euclidean buildings with the Tits boundary <i>Y</i>. Quite remarkably, the <span class=SpellE>cohomology</span> ring is obtained from a certain universal algebra<i> A</i> by a kind of  crystal limit that has been previously introduced by <span class=SpellE>Belkale</span>-Kumar for the <span class=SpellE>cohomology</span> of flag varieties and Grassmannians. Another degeneration of <i>A</i> leads to the homology theory of<i> Y</i>.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/qfold.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Quantum folding</span></b></a><b><span style='font-family:"Times New Roman",serif;color:black'> </span></b><span style='font-family:"Times New Roman",serif;color:black'>(with </span><a href="https://profiles.ucr.edu/app/home/profile/jacobg"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>J. Greenstein</span></a><span style='font-family:"Times New Roman",serif; color:black'>), </span><a href="https://academic.oup.com/imrn"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Int. Math. Res. Not.</span></i></a><span style='font-family: "Times New Roman",serif;color:black'> 2011, no. 21, pages 4821 4883.</span><br> <b><span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span></b><span style='font-family:"Times New Roman",serif;color:black'>In the present paper we introduce a quantum analogue of the classical folding of a simply-laced Lie algebra <b><i>g</i></b> to the non-simply-laced algebra <span class=SpellE><b><i>g</i></b><sup>�</sup></span> along a <span class=SpellE>Dynkin</span> diagram automorphism � of <b><i>g</i></b>. For each quantum folding we replace <span class=SpellE><b><i>g</i></b><sup>�</sup></span> by its <span class=SpellE>Langlands</span> dual <i>(<span class=SpellE><b>g</b><span class=GramE><sup><span style='font-style:normal'>�</span></sup></span></span><span class=GramE>)<sup><span style='font-style:normal'>v</span></sup></span></i> and construct a nilpotent Lie algebra <b><i>n</i></b> which interpolates between the nilpotent parts of <b><i>g</i></b> and<i> (<span class=SpellE><b>g</b><sup><span style='font-style:normal'>�</span></sup></span>)</i><sup>v</sup>, together with its quantized enveloping algebra<i> <span class=SpellE>U<sub>q</sub></span>(<b>n</b>) </i>and a Poisson structure on S(<b><i>n</i></b>). Remarkably, for the pair<i> (<b>g</b>, (<span class=SpellE><b>g</b><span class=GramE><sup><span style='font-style:normal'>�</span></sup></span></span><span class=GramE>)<sup><span style='font-style:normal'>v</span></sup></span>)=(so<sub>2n+2</sub>,sp<sub>2n</sub>)</i>, the algebra <span class=SpellE><i>U<sub>q</sub></i></span></span><i><span style='font-size:11.0pt;line-height:115%;font-family:"Times New Roman",serif; color:black'>(<b>n</b>)</span></i><span style='font-size:11.0pt;line-height: 115%;font-family:"Times New Roman",serif;color:black'> admits an action of the <span class=SpellE>Artin</span> braid group<i> <span class=SpellE>Br<sub>n</sub></span></i> and contains a new algebra of quantum <i>n x n</i> matrices with an adjoint action of <span class=SpellE><i>U<sub>q</sub></i></span><i>(<span class=SpellE>sl<sub>n</sub></span>)</i>, which generalizes the algebras constructed by K. <span class=SpellE>Goodearl</span> and M. <span class=SpellE>Yakimov</span>. The hardest case of quantum folding is, quite expectably, the pair<i> (so</i></span><i><sub><span style='font-family: "Times New Roman",serif;color:black'>8</span></sub></i><i><span style='font-family:"Times New Roman",serif;color:black'>,G<sub>2</sub>)</span></i><span style='font-family:"Times New Roman",serif;color:black'> for which the PBW presentation of <span class=SpellE><i>U<sub>q</sub></i></span></span><i><span style='font-size:11.0pt;line-height:115%;font-family:"Times New Roman",serif; color:black'>(<b>n</b>)</span></i><span style='font-size:11.0pt;line-height: 115%;font-family:"Times New Roman",serif;color:black'> and the corresponding Poisson bracket on S(<b><i>n</i></b><i>)</i> contain more than 700 terms each.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/quasiharmonic.pdf"><span class=SpellE><b><span style='font-family:"Times New Roman",serif;color:blue'>Quasiharmonic</span></b></span><b><span style='font-family:"Times New Roman",serif;color:blue'> polynomials for <span class=SpellE>Coxeter</span> groups and representations of <span class=SpellE>Cherednik</span> algebras</span></b></a><b><span style='font-family:"Times New Roman",serif; color:black'> </span></b><span style='font-family:"Times New Roman",serif; color:black'>(with </span><a href="https://scholar.google.com/citations?user=r3oMgNgAAAAJ&amp;hl=en"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Yu. Burman</span></a><span style='font-family:"Times New Roman",serif; color:black'>),&nbsp; </span><a href="http://www.ams.org/publications/journals/journalsframework/tran"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Trans. Amer. Math. Soc.</span></i></a><span style='font-family:"Times New Roman",serif;color:black'>, 362 (2010), 229 260.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;We introduce and study deformations of finite-dimensional modules over rational <span class=SpellE>Cherednik</span> algebras. Our main tool is a generalization of usual harmonic polynomials for <span class=SpellE>Coxeter</span> groups  the so-called <span class=SpellE>quasiharmonic</span> polynomials. A surprising application of this approach is the construction of canonical elementary symmetric polynomials and their deformations for all <span class=SpellE>Coxeter</span> groups.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/berbur2.pdf"><span class=SpellE><b><span style='font-family:"Times New Roman",serif;color:blue'>Dunkl</span></b></span><b><span style='font-family:"Times New Roman",serif;color:blue'> Operators and Canonical Invariants of Reflection Groups</span></b></a><span style='font-family:"Times New Roman",serif; color:black'> (with </span><a href="https://scholar.google.com/citations?user=r3oMgNgAAAAJ&amp;hl=en"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Yu. Burman</span></a><span style='font-family:"Times New Roman",serif; color:black'>), </span><a href="https://www.emis.de/journals/SIGMA/"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>SIGMA</span></i></a><i><span style='font-family:"Times New Roman",serif; color:black'> </span></i><span style='font-family:"Times New Roman",serif; color:black'>5 (2009), 057, 18 pages.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>Using <span class=SpellE>Dunkl</span> operators, we introduce a continuous family of canonical invariants of finite reflection groups. We verify that the elementary canonical invariants of the symmetric group are deformations of the elementary symmetric polynomials. We also compute the canonical invariants for all dihedral groups as certain hypergeometric functions.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/berkap1.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Affine buildings for dihedral groups</span></b></a><b><span style='font-family:"Times New Roman",serif; color:black'>&nbsp; (</span></b><span style='font-family:"Times New Roman",serif; color:black'>with </span><a href="https://www.math.ucdavis.edu/~kapovich/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>M. <span class=SpellE>Kapovich</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>),&nbsp; </span><a href="https://www.springer.com/journal/10711"><span class=SpellE><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Geometriae</span></i></span><i><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'> <span class=SpellE>Dedicata</span></span></i></a><span style='font-family:"Times New Roman",serif; color:black'>, 156 (2012), pages 171 207.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;We construct rank 2 thick <span class=SpellE>nondiscrete</span> affine buildings associated with an arbitrary finite dihedral group.</span><br> <span style='font-size:10.0pt;line-height:115%;font-family:"Times New Roman",serif; color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/brcher.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Noncommutative <span class=SpellE>Dunkl</span> operators and braided <span class=SpellE>Cherednik</span> algebras</span></b></a><span style='font-family:"Times New Roman",serif; color:black'> (with </span><a href="https://research.manchester.ac.uk/en/persons/yuri.bazlov"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Y. <span class=SpellE>Bazlov</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>) <i>&nbsp;</i></span><a href="http://link.springer.com/journal/29"><i><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>Selecta Mathematica</span></i></a><span style='font-family:"Times New Roman",serif;color:black'>,&nbsp; <b>14</b>, (2009), pages 325 372.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;We introduce braided <span class=SpellE>Dunkl</span> operators that are acting on a <b><i>q</i></b>-polynomial algebra and <b><i>q</i></b>-commute. Generalizing the approach of <span class=SpellE>Etingof</span> and Ginzburg, we explain the <b><i>q</i></b>-commutation phenomenon by constructing braided <span class=SpellE>Cherednik</span> algebras for which the above operators form a representation. We classify all braided <span class=SpellE>Cherednik</span> algebras using the theory of braided doubles developed in our previous paper. Besides ordinary rational <span class=SpellE>Cherednik</span> algebras, our classification gives new algebras attached to an infinite family of subgroups of even elements in complex reflection groups, so that the corresponding braided <span class=SpellE>Dunkl</span> <span class=GramE>operators</span> pairwise anti-commute. We explicitly compute these new operators in terms of braided partial derivatives and divided differences. </span><br> <br> <a href="http://pages.uoregon.edu/arkadiy/doubles.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Braided Doubles and rational <span class=SpellE>Cherednik</span> algebras</span></b></a><span style='font-family:"Times New Roman",serif;color:black'> (with </span><a href="https://research.manchester.ac.uk/en/persons/yuri.bazlov"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Y. <span class=SpellE>Bazlov</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="https://www.journals.elsevier.com/advances-in-mathematics"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Advances in Mathematics</span></i></a><span style='font-family:"Times New Roman",serif;color:black'>, Vol. 220 (2009) <b>5</b>,&nbsp; pages 1466 1530.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;We introduce and study a large class of algebras with triangular decomposition which we call braided doubles. Braided doubles provide a unifying framework for classical and quantum universal enveloping algebras and rational <span class=SpellE>Cherednik</span> algebras. We classify braided doubles in terms of quasi-<span class=SpellE>Yetter</span>-<span class=SpellE>Drinfeld</span> (QYD) modules over <span class=SpellE>Hopf</span> algebras which turn out to be a <span class=SpellE>generalisation</span> of the ordinary <span class=SpellE>Yetter-Drinfeld</span> modules. To each braiding (a solution to the braid equation) we associate a QYD-module and the corresponding braided Heisenberg double  this is a quantum deformation of the Weyl algebra where the role of polynomial algebras is played by Nichols-<span class=SpellE>Woronowicz</span> algebras. Our main result is that any rational <span class=SpellE>Cherednik</span> algebra canonically embeds into the braided Heisenberg double attached to the corresponding complex reflection group. </span><br> <br> <a href="http://pages.uoregon.edu/arkadiy/noncomloopalg.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Lie algebras and Lie groups over noncommutative rings</span></b></a><b><span style='font-family: "Times New Roman",serif;color:black'> </span></b><span style='font-family:"Times New Roman",serif; color:black'>(with </span><a href="http://www.math.rutgers.edu/~vretakh/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>V. <span class=SpellE>Retakh</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="https://www.journals.elsevier.com/advances-in-mathematics"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Advances in Mathematics</span></i></a><span style='font-family:"Times New Roman",serif;color:black'>, Vol. 218, <b>6</b>, (2008), pages 1723 1758.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;The aim of this paper is to introduce and study Lie algebras over noncommutative rings. For any Lie algebra <i>g</i> sitting inside an associative algebra <i>A</i> and any associative algebra <i>F</i> we introduce and study the <i>F</i>-<i>current</i> Lie algebra <i>(<span class=SpellE><span class=GramE><b>g</b>,A</span></span>)(F)</i>, which is the Lie subalgebra of <i>F</i></span><span style='font-size:14.0pt; line-height:115%;font-family:"Cambria Math",serif;mso-bidi-font-family:"Cambria Math"; color:black'>�"</span><i><span style='font-family:"Times New Roman",serif; color:black'>A</span></i><span style='font-family:"Times New Roman",serif; color:black'> generated by <span class=SpellE><i>F</i><span style='font-size: 14.0pt;line-height:115%;font-family:"Cambria Math",serif;mso-bidi-font-family: "Cambria Math"'>�"</span><b><i>g</i></b></span>. In most examples <i>A</i> is the universal enveloping algebra of <b><i>g</i></b>. Our description of the current algebra has a striking resemblance to the commutator expansions of <i>F</i> used by M. <span class=SpellE>Kapranov</span> in his approach to noncommutative geometry. We also associate with each Lie algebra <i>(<span class=SpellE><b>g</b>,A</span>)(F)</i> a  noncommutative algebraic group <i>G</i> which naturally acts on <i>(<span class=SpellE><b>g</b>,A</span>)(F)</i> by conjugations and conclude the paper with a number of examples of such groups.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/braidedsymmextalg.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Braided symmetric and exterior algebras</span></b></a><b><span style='font-family:"Times New Roman",serif; color:black'> </span></b><span style='font-family:"Times New Roman",serif; color:black'>(with </span><a href="https://www.researchgate.net/scientific-contributions/Sebastian-Zwicknagl-73038482"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>S. <span class=SpellE>Zwicknagl</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="https://www.ams.org/publications/journals/journalsframework/tran"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Trans. Amer. Math. Soc.</span></i></a><span style='font-family:"Times New Roman",serif;color:black'>,&nbsp; <b>360</b>&nbsp; (2008), pages 3429 3472.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;We introduce and study symmetric and exterior algebras in braided monoidal categories such as the category <i>O</i> over quantum groups. We relate our braided symmetric algebras and braided exterior algebras with their classical counterparts.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;</span><br> <a href="http://pages.uoregon.edu/arkadiy/geomunipnotes.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Lecture notes on geometric crystals and their combinatorial analogues</span></b></a><span style='font-family:"Times New Roman",serif;color:black'> (with </span><a href="http://www.ma.huji.ac.il/~kazhdan/"><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>D. <span class=SpellE>Kazhdan</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), <i>Combinatorial aspect of integrable systems</i>, </span><a href="https://mathsoc.jp/publication/memoir/memoirs-e.html"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>MSJ Memoirs</span></i></a><span style='font-family:"Times New Roman",serif; color:black'>, 17, Mathematical Society of Japan,&nbsp; Tokyo, 2007.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;This is an exposition of the results on Geometric crystals and the associated <span class=SpellE>Kashiwara</span> crystal bases (presented by the first author in RIMS, August 2004). </span><br> <br> <a href="http://pages.uoregon.edu/arkadiy/bk2007.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Geometric and Unipotent Crystals II: From Unipotent <span class=SpellE>Bicrystals</span> to Crystal Bases</span></b></a><span style='font-family:"Times New Roman",serif; color:black'> (with </span><a href="http://www.ma.huji.ac.il/~kazhdan/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>D. <span class=SpellE>Kazhdan</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="http://www.ams.org/publications/books/monographs/conm-home"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Contemp. Math.</span></i></a><span style='font-family: "Times New Roman",serif;color:black'>, <b>433</b>, Amer. Math. Soc., Providence, RI, 2007, pages 13 88.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;For each reductive algebraic group <i>G</i>, we introduce and study <i>unipotent <span class=SpellE>bicrystals</span></i> which serve as a regular version of rational geometric and unipotent crystals introduced earlier by the authors. The framework of unipotent <span class=SpellE>bicrystals</span> allows, on the one hand, to study systematically such varieties as <span class=SpellE>Bruhat</span> cells in <i>G</i> and their convolution products and, on the other hand, to give a new construction of many normal <span class=SpellE>Kashiwara</span> crystals including those for <span class=SpellE><i>G</i><sup>v</sup></span>-modules, where <span class=SpellE><i>G</i><sup>v</sup></span> is the <span class=SpellE>Langlands</span> dual groups. In fact, <span class=GramE>our&nbsp; analogues</span> of crystal bases (which we refer to as crystals <i>associated</i> to <span class=SpellE><i>G</i><sup>v</sup></span>-modules) are associated to <span class=SpellE><i>G</i><sup>v</sup></span>-modules directly, i.e., without quantum deformations.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/ncbruhat.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Noncommutative Double <span class=SpellE>Bruhat</span> cells and their factorizations</span></b></a><b><span style='font-family:"Times New Roman",serif; color:black'> </span></b><span style='font-family:"Times New Roman",serif; color:black'>(with </span><a href="http://www.math.rutgers.edu/~vretakh/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>V. <span class=SpellE>Retakh</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>), </span><a href="https://academic.oup.com/imrn"><i><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>Int. Math.</span></i></a><i><span style='font-family:"Times New Roman",serif'> Res. Not<span class=GramE>.<span style='font-style:normal'>,&nbsp; <b>8</b></span></span></span></i><span style='font-family:"Times New Roman",serif;color:black'>&nbsp; (2005), pages 477 516. </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>In the present paper we study noncommutative double <span class=SpellE>Bruhat</span> cells. Our main results are explicit positive matrix factorizations in the cells via <span class=SpellE>quasiminors</span> of matrices with noncommutative coefficients.</span><span style='font-family:"Times New Roman",serif'> </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/bzqclust.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Quantum cluster algebras</span></b></a><span style='font-family:"Times New Roman",serif'> (with </span><a href="https://en.wikipedia.org/wiki/Andrei_Zelevinsky"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>A. <span class=SpellE>Zelevinsky</span></span></a><span style='font-family:"Times New Roman",serif'>)&nbsp; </span><a href="https://www.journals.elsevier.com/advances-in-mathematics"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Advances in Mathematics</span></i></a><span style='font-family:"Times New Roman",serif'>, vol. 195, <b>2</b> (2005),&nbsp; pages 405 455.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>Cluster algebras were introduced by S. Fomin and A. <span class=SpellE>Zelevinsky</span>; their study continued in a series of papers including </span><a href="http://pages.uoregon.edu/arkadiy/bfz-cluster.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Cluster algebras III: Upper bounds and double <span class=SpellE>Bruhat</span> cells</span></b></a><span style='font-family:"Times New Roman",serif;color:black'>. This is a family of commutative rings designed to serve as an algebraic framework for the theory of total positivity and canonical bases in <span class=SpellE>semisimple</span> groups and their quantum analogs. In this paper we introduce and study quantum deformations of cluster algebras.</span><span style='font-family:"Times New Roman",serif'> </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/bfz-cluster.pdf"><b><span style='font-family:"Times New Roman",serif;color:blue'>Cluster algebras III: Upper bounds and double <span class=SpellE>Bruhat</span> cells</span></b></a><span style='font-family:"Times New Roman",serif'> (with </span><a href="https://dept.math.lsa.umich.edu/~fomin/"><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>S. Fomin</span></a><span style='font-family:"Times New Roman",serif'> and </span><a href="https://en.wikipedia.org/wiki/Andrei_Zelevinsky"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>A. <span class=SpellE>Zelevinsky</span></span></a><span style='font-family:"Times New Roman",serif'>)&nbsp; </span><a href="https://www.dukeupress.edu/duke-mathematical-journal"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Duke Math. Journal</span></i></a><span style='font-family: "Times New Roman",serif'>, vol. 126, <b>1</b> (2005), pages 1 52.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>We continue the study of cluster algebras. We develop a new approach based on the notion of upper cluster algebra, defined as an intersection of certain Laurent polynomial rings. Strengthening the Laurent phenomenon, we show that, under an assumption of  acyclicity, a cluster algebra coincides with its  upper counterpart, and is finitely generated. In this case, we also describe its defining <span class=GramE>ideal, and</span> construct a standard monomial basis. We prove that the coordinate ring of any double <span class=SpellE>Bruhat</span> cell in a <span class=SpellE>semisimple</span> complex Lie group is naturally isomorphic to the upper cluster algebra explicitly defined in terms of relevant combinatorial data.</span><span style='font-family:"Times New Roman",serif'> </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/bz99.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Tensor product multiplicities, canonical bases and totally positive varieties</span></b></a><span style='font-family: "Times New Roman",serif'> (with&nbsp; </span><a href="https://en.wikipedia.org/wiki/Andrei_Zelevinsky"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>A. <span class=SpellE>Zelevinsky</span></span></a><span style='font-family:"Times New Roman",serif'>) <i>&nbsp;</i></span><a href="http://www.springer.com/mathematics/journal/222"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Invent. Math.</span></i></a><span style='font-family:"Times New Roman",serif'>, vol. 143, <b>1</b> (2001), pages 77 128. </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>We obtain a family of explicit  polyhedral combinatorial expressions for multiplicities in the tensor product of two simple finite-dimensional modules over a complex <span class=SpellE>semisimple</span> Lie algebra. Here  polyhedral means that the multiplicity in question is expressed as the number of lattice points in some convex polytope. Our answers use a new combinatorial concept of <span class=SpellE><b><i>i</i></b></span>-trails which resemble <span class=SpellE>Littelmann s</span> paths but seem to be more tractable. We also study combinatorial structure of <span class=SpellE>Lusztig s</span> canonical bases or, equivalently of <span class=SpellE>Kashiwara s</span> global bases. Although <span class=SpellE>Lusztig s</span> and <span class=SpellE>Kashiwara s</span> approaches were shown by <span class=SpellE>Lusztig</span> to be equivalent to each other, they lead to different combinatorial parametrizations of the canonical bases. One of our main results is an explicit description of the relationship between these parametrizations. Our approach to the above problems is based on a remarkable observation by G. <span class=SpellE>Lusztig</span> that combinatorics of the canonical basis is closely related to geometry of the totally positive varieties. We formulate this relationship in terms of two mutually inverse transformations:  tropicalization and  geometric lifting. </span><span style='font-family:"Times New Roman",serif'> <o:p></o:p></span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'><o:p>&nbsp;</o:p></span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/rsk.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>The Robinson-<span class=SpellE>Schensted</span>-Knuth bijection, quantum matrices and piece-wise linear combinatorics</span></b></a> (with <a href="https://www.kurims.kyoto-u.ac.jp/~kirillov/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Anatol Kirillov</span></a><span style='font-family:"Times New Roman",serif'>) <a href="http://math.la.asu.edu/~fpsac01/PROGRAM/5.html">FPSAC 2001</a>, Arizona State University, May 20-26, 2001.<o:p></o:p></span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; mso-ascii-theme-font:minor-bidi;mso-hansi-theme-font:minor-bidi;mso-bidi-theme-font: minor-bidi'>We explicitly compute the celebrated Robinson-<span class=SpellE>Schensted</span>-Knuth bijection (RSK) between the set of the matrices with non-negative integer entries, and the set of the plane partitions. More precisely, in suitable linear coordinates on both sets, the RSK is expressed via minima of linear forms, <span class=SpellE>i.e</span>, in piece-wise linear terms. <span class=GramE>In particular, we</span> answer the following question by C. Greene and G. <span class=SpellE>Viennot</span>:  What shape corresponds to a given matrix under the Robinson-<span class=SpellE>Schensted</span>-Knuth correspondence? Our main tools in establishing these formulae are the quantum matrices and crystal bases. As a byproduct of our approach, we compute the corresponding crystal equivalence in terms of  generalized <span class=SpellE>Kazhdan-Lusztig</span> polynomials.<o:p></o:p></span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/bka99.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Geometric and unipotent crystals</span></b></a><span style='font-family:"Times New Roman",serif;color:black'> (with </span><a href="http://www.ma.huji.ac.il/~kazhdan/"><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>D. <span class=SpellE>Kazhdan</span></span></a><span style='font-family:"Times New Roman",serif;color:black'>)&nbsp; </span><a href="http://www.springer.com/birkhauser/mathematics/journal/39"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Geom. <span class=SpellE>Funct</span>. Anal.</span></i></a><span style='font-family:"Times New Roman",serif;color:black'>, Special Volume, Part I (2000), pages 188 236.</span><br> <span style='font-family:"Times New Roman",serif;color:black'>&nbsp;We introduce geometric crystals and unipotent crystals which are <span class=SpellE>algebro</span>-geometric analogues of <span class=SpellE>Kashiwara s</span> crystal bases. Given a reductive group <i>G</i>, let <i>I</i> be the set of vertices of the <span class=SpellE>Dynkin</span> diagram of <i>G</i> and <i>T</i> be the maximal torus of <i>G</i>. The structure of a geometric <i>G</i>-crystal on <span class=GramE>an&nbsp; algebraic</span> variety <i>X</i> consists of a rational morphism <i>�:X�T</i> and a compatible family <span class=SpellE><i>e<sub>i</sub></i>:<b><i>G<sub>m</sub></i></b>�<i>X�X</i></span>, <span class=SpellE><i>i</i></span><i> </i>in <i>I</i>&nbsp; of rational actions of the&nbsp; multiplicative group <b><i>G<sub>m</sub></i> </b>&nbsp;satisfying certain braid-like relations.&nbsp; Such a structure induces a rational action of <i>W </i>on <i>X</i>. Surprisingly many interesting rational actions of the group <i>W</i> <span class=GramE>come&nbsp; from</span> geometric crystals. Also all the known examples of the action of <i>W</i> <span class=GramE>which&nbsp; appear</span> in the construction of Gamma-functions for the representations of&nbsp; the <span class=SpellE>Langlands</span> dual group <span class=SpellE><i>G</i><sup>v</sup></span> in the recent work by A. Braverman and D. <span class=SpellE>Kazhdan</span> come from&nbsp; geometric&nbsp; crystals. There are many examples of positive geometric crystals on (<b><i>G<sub>m</sub></i></b>)<i><sup>l</sup></i>, i.e., those geometric crystals for which the actions <span class=SpellE><i>e<sub>i</sub></i></span> and the morphism<i> gamma</i> are given by positive rational expressions.&nbsp; One can associate to each positive geometric crystal <i>X</i> the <span class=SpellE><span class=GramE>Kashiwara s</span></span><span class=GramE>&nbsp; crystal</span> corresponding to the <span class=SpellE>Langlands</span> dual group <span class=SpellE><i>G</i><sup>v</sup></span>.&nbsp; An emergence of <span class=SpellE><i>G</i><sup>v</sup></span> in the  crystal world was observed earlier by G. <span class=SpellE>Lusztig</span>. Another application of geometric crystals is a construction of trivialization which is <span class=GramE>an</span> <i>W</i>-equivariant isomorphism <span class=SpellE>X�</span>&gt;<i>�<sup>-1</sup>(e)�T</i> for any geometric <span class=SpellE><i>SL<sub>n</sub></i></span>-crystal. Unipotent crystals are geometric analogues of normal <span class=SpellE>Kashiwara</span> crystals. They form a strict monoidal category. To any unipotent crystal built on a variety <i>X</i> we associate a certain geometric crystal.</span><span style='font-family:"Times New Roman",serif'> </span></p> <p class=MsoNormal style='margin-bottom:0in'><b><span style='font-family:"Times New Roman",serif'>&nbsp;</span></b></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/bs.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Coadjoint orbits, moment polytopes, and the Hilbert-Mumford criterion</span></b></a><span style='font-family:"Times New Roman",serif'> (with </span><a href="http://www.math.cornell.edu/~sjamaar/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>R. <span class=SpellE>Sjamaar</span></span></a><span style='font-family:"Times New Roman",serif'>), </span><a href="http://www.ams.org/jams/"><i><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>J. Amer. Math. Soc.</span></i></a><i><span style='font-family:"Times New Roman",serif'>,</span></i><span style='font-family: "Times New Roman",serif'> 13 (2000), no. 2, pages 433 466.</span><br> <span style='font-family:"Times New Roman",serif'>&nbsp;In this paper we solve of the following problem: Given a reductive group <i>G</i>, and its reductive subgroup <i>H</i>, describe the <i>momentum cone</i> <span class=SpellE><i>�</i><i><sub><span style='font-size:13.5pt;line-height:115%'>o</span></sub></i></span>. This is a rational polyhedral cone spanned by all those dominant <i>G</i>-weights <i>� </i>for which the simple <i>G</i>-module <span class=SpellE><i>V<sub>�</sub></i></span> contains a non-trivial <i>H</i>-invariant. Our result generalizes the result by <span class=SpellE>Klyachko</span> who has solved this problem for <i>G</i>=<i> </i></span><span class=SpellE><i><span style='font-size:13.5pt;line-height: 115%;font-family:"Times New Roman",serif'>GL<sub>n</sub></span></i><span style='font-family:"Times New Roman",serif'>�</span><i><span style='font-size: 13.5pt;line-height:115%;font-family:"Times New Roman",serif'>GL<sub>n</sub></span></i><span style='font-family:"Times New Roman",serif'>�</span><i><span style='font-size: 13.5pt;line-height:115%;font-family:"Times New Roman",serif'>GL<sub>n</sub></span></i></span><span style='font-family:"Times New Roman",serif'> with the subgroup <i>H</i>=<span class=SpellE><i>GL</i><i><sub><span style='font-size:13.5pt;line-height:115%'>n</span></sub></i></span> embedded diagonally into <i>G</i>. We describe the facets of the cone <span class=SpellE><i>�</i><i><sub><span style='font-size:13.5pt;line-height:115%'>o</span></sub></i></span> in terms of the  relative Schubert calculus of the flag varieties of the two groups. Another formulation of the result is the description of the relative momentum cone <i>�</i>, which is spanned by those pairs <i>(<span class=SpellE><span class=GramE>�<span style='font-style:normal'>,</span>�</span></span></i>'<i>)</i> for which the&nbsp; restriction to <i>H</i> of the simple <i>G</i>-module <span class=SpellE><i>V<sub>�</sub></i></span> contains a simple <i>H</i>-module <span class=SpellE><i>V'<sub>�</sub></i></span><i><sub>'</sub></i>. </span></p> <p class=MsoNormal style='margin-bottom:0in'><b><span style='font-family:"Times New Roman",serif'>&nbsp;</span></b></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/bk2.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Domino tableaux, <span class=SpellE>Schutzenberger</span> involution and action of the symmetric group</span></b></a><span style='font-family:"Times New Roman",serif'> (with </span><a href="https://www.kurims.kyoto-u.ac.jp/~kirillov/"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>Anatol Kirillov</span></a><span style='font-family:"Times New Roman",serif'>), <i>Proceedings of the 10th International Conference on </i></span><a href="https://fpsac.org/"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Formal Power Series and Algebraic Combinatorics</span></i></a><span style='font-family:"Times New Roman",serif'>, Fields Institute, Toronto, 1998,&nbsp; </span><a href="https://www.sciencedirect.com/journal/discrete-mathematics"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Discrete Math.</span></i></a><span style='font-family: "Times New Roman",serif'>, vol. 225, <b>1 3</b> (2000),&nbsp; pages 5 24. </span></p> <p class=MsoNormal style='margin-bottom:0in'><b><span style='font-family:"Times New Roman",serif'>&nbsp;</span></b></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/alek.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Concavity of weighted arithmetic means with applications</span></b></a><span style='font-family:"Times New Roman",serif'> (with </span><a href="https://cris.haifa.ac.il/en/persons/alek-vainshtein"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Alek <span class=SpellE>Vainshtein</span></span></a><span style='font-family:"Times New Roman",serif'>), </span><a href="https://www.springer.com/journal/13"><i><span style='font-family:"Times New Roman",serif'>Arch. Math</span></i><span style='font-family:"Times New Roman",serif;color:blue; text-decoration:none;text-underline:none'>.</span></a><span style='font-family: "Times New Roman",serif'> (1997) 69, pages 120 126. </span></p> <p class=MsoNormal style='margin-bottom:0in'><b><span style='font-family:"Times New Roman",serif'>&nbsp;</span></b></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/ansgen1.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Total positivity in Schubert varieties</span></b></a><b><span style='font-family:"Times New Roman",serif'> </span></b><span style='font-family: "Times New Roman",serif'>(with </span><a href="https://en.wikipedia.org/wiki/Andrei_Zelevinsky"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>A. <span class=SpellE>Zelevinsky</span></span></a><span style='font-family:"Times New Roman",serif'>) </span><a href="https://www.ems-ph.org/journals/journal.php?jrn=cmh"><i><span style='font-family:"Times New Roman",serif'>Comment. Math.</span></i><span style='font-family:"Times New Roman",serif'> </span><span class=SpellE><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Helv</span></i></span><i><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>.</span></i></a><span style='font-family:"Times New Roman",serif'> <b>72 </b>(1997),<i> </i>no. 1, pages 128 166.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>In this paper we further develop the remarkable parallelism discovered by <span class=SpellE>Lusztig</span> between the canonical basis and the variety of totally positive elements in the unipotent group. </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/bfz.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Parametrizations of canonical bases and totally positive matrices</span></b></a><span style='font-family:"Times New Roman",serif'> (with </span><a href="https://dept.math.lsa.umich.edu/~fomin/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>S. Fomin</span></a><span style='font-family:"Times New Roman",serif'> and </span><a href="https://en.wikipedia.org/wiki/Andrei_Zelevinsky"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>A. <span class=SpellE>Zelevinsky</span></span></a><span style='font-family:"Times New Roman",serif'>), </span><a href="https://www.journals.elsevier.com/advances-in-mathematics"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Advances in Mathematics</span></i></a><b><span style='font-family:"Times New Roman",serif'> 122</span></b><span style='font-family:"Times New Roman",serif'> (1996), pages 49 149.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>We provide: (<span class=SpellE>i</span>) explicit formulas for <span class=SpellE>Lusztig s</span> transition maps related to the canonical basis of the quantum group of type A; (ii) formulas for the factorizations of a square matrix into elementary Jacobi matrices; (iii) a family of new total positivity criteria. </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/qufpub.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Group-like elements in quantum groups and <span class=SpellE>Feigin s</span> conjecture</span></b></a><span style='font-family: "Times New Roman",serif'>, preprint.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>In this paper analogue of the Gelfand-Kirillov conjecture for any simple quantum group </span><span class=SpellE><i><span style='font-size:13.5pt;line-height: 115%;font-family:"Times New Roman",serif'>G<sub>q</sub></span></i></span><span style='font-family:"Times New Roman",serif'> is proved (here </span><span class=SpellE><i><span style='font-size:13.5pt;line-height:115%;font-family: "Times New Roman",serif'>G<sub>q</sub></span></i></span><span style='font-family: "Times New Roman",serif'> is the <i>q</i>-deformed coordinate ring of a simple algebraic group <i>G</i>). Namely, the field of fractions of </span><span class=SpellE><i><span style='font-size:13.5pt;line-height:115%;font-family: "Times New Roman",serif'>G<sub>q</sub></span></i></span><span style='font-family: "Times New Roman",serif'> is isomorphic to the field of fractions of a certain skew-polynomial ring. The proof is based on a construction of some group-like elements in </span><span class=SpellE><i><span style='font-size:13.5pt; line-height:115%;font-family:"Times New Roman",serif'>G<sub>q</sub></span></i></span><i><span style='font-family:"Times New Roman",serif'> </span></i><span style='font-family: "Times New Roman",serif'>(which are <i>q</i>-analogs of elements in <i>G</i>). </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="https://pages.uoregon.edu/arkadiy/zel.pdf"><b><span style='font-family: "Times New Roman",serif'>Canonical bases for the quantum group of type <i>A</i></span></b><b><i><sub><span style='font-size:14.0pt;line-height:115%;font-family:"Times New Roman",serif'>r</span></sub></i></b><b><span style='font-family:"Times New Roman",serif;color:blue'> and piecewise-linear combinatorics</span></b></a><span style='font-family:"Times New Roman",serif'> (with </span><a href="https://en.wikipedia.org/wiki/Andrei_Zelevinsky"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>A. <span class=SpellE>Zelevinsky</span></span></a><span style='font-family:"Times New Roman",serif'>), </span><a href="https://www.dukeupress.edu/Duke-Mathematical-Journal/"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Duke Math. J.</span></i></a><i><span style='font-family: "Times New Roman",serif'> </span></i><b><span style='font-family:"Times New Roman",serif'>82 </span></b><span style='font-family:"Times New Roman",serif'>(1996), no. 3, pages 473 502.</span><br> <span style='font-family:"Times New Roman",serif'>&nbsp;We use the structure theory of the dual canonical basis <b><i>B</i></b> is to obtain a direct representation-theoretic proof of the Littlewood-Richardson rule (or rather, its piecewise-linear versions discussed above). Another application of string technique is an explicit formula for the action of the longest element </span><i><span style='font-size:13.5pt;line-height:115%;font-family:"Times New Roman",serif'>w</span></i><i><span style='font-size:10.0pt;line-height:115%;font-family:"Times New Roman",serif'>o</span></i><i><span style='font-family:"Times New Roman",serif'> </span></i><span style='font-family: "Times New Roman",serif'>in </span><i><span style='font-size:13.5pt;line-height: 115%;font-family:"Times New Roman",serif'>S<sub>r</sub></span></i><i><sub><span style='font-family:"Times New Roman",serif'>+1</span></sub></i><span style='font-family:"Times New Roman",serif'> on the dual canonical basis in each simple </span><i><span style='font-size:13.5pt;line-height:115%; font-family:"Times New Roman",serif'>sl<sub>r</sub></span></i><i><sub><span style='font-family:"Times New Roman",serif'>+1</span></sub></i><span style='font-family:"Times New Roman",serif'>-module. Having been translated into the language of Gelfand-<span class=SpellE>Tsetlin</span> patterns and <span class=GramE>Young</span> tableaux, this involution coincides with the <span class=SpellE>Sch�tzenberger</span> involution. </span></p> <p class=MsoNormal style='margin-bottom:0in'><b><span style='font-family:"Times New Roman",serif'>&nbsp;</span></b></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/andrei.pdf"><b><span style='font-family: "Times New Roman",serif'>String bases for quantum groups of type <i>A</i></span></b><b><i><sub><span style='font-size:14.0pt;line-height:115%;font-family:"Times New Roman",serif; color:blue'>r</span></sub></i></b></a><span style='font-family:"Times New Roman",serif'> (with </span><a href="https://en.wikipedia.org/wiki/Andrei_Zelevinsky"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>A. <span class=SpellE>Zelevinsky</span></span></a><span style='font-family:"Times New Roman",serif'>) <i>I. M. Gelfand Seminar, 51 89, </i></span><a href="http://www.ams.org/publications/ebooks/advsov-coll"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Adv. Soviet Math.</span></i></a><i><span style='font-family: "Times New Roman",serif'>, 16, Part 1, </span></i><span style='font-family: "Times New Roman",serif'>Amer. Math. Soc., Providence, RI, 1993.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>We introduce and study a family of <i>string bases</i> for the quantum groups of type <i>A<sub>r</sub></i> (which includes the dual canonical basis). These bases are defined axiomatically and possess many interesting properties, e.g., they all are <i>good</i> in the sense of Gelfand and <span class=SpellE>Zelevinsky</span>. For every string basis, we construct a family of combinatorial <span class=SpellE>labelings</span> by <i>strings</i>. These <span class=SpellE>labelings</span> in a different context appeared in more recent works by M. <span class=SpellE>Kashiwara</span> and by P. <span class=SpellE>Littelmann</span>. We expect that <b><i>B</i> </b>has a nice multiplicative structure. Namely, we conjecture in [8] that <b><i>B</i></b> contains all products of pairwise <b><i>q</i></b>-commuting elements of <b><i>B</i></b>. The conjecture <span class=GramE>was&nbsp; proved</span> in [8] for <i>A<sub>2</sub></i> and <i>A<sub>3</sub></i>. In fact, for <i>r</i>&lt; 4, the dual canonical basis <b><i>B</i></b> is the only string <span class=GramE>basis</span> and it consists of all <b><i>q</i></b>-commuting products of quantum minors (for <i>r </i>arbitrary, we proved that any string basis contains all quantum minors). </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/bk1.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Groups generated by involutions, <span class=SpellE>Gel fand-Tsetlin</span> patterns, and combinatorics of Young tableaux</span></b></a><span style='font-family:"Times New Roman",serif'> (with </span><a href="https://www.kurims.kyoto-u.ac.jp/~kirillov/"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Anatol Kirillov</span></a><span style='font-family:"Times New Roman",serif'>), </span><a href="http://www.mathnet.ru/php/journal.phtml?jrnid=aa&amp;option_lang=eng"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Algebra <span class=SpellE>i</span> Analiz</span></i></a><span style='font-family:"Times New Roman",serif'> <b>7</b> (1995), no. 1, 92 152 (Russian). Translation in: </span><a href="https://www.ams.org/publications/journals/journalsframework/spmj"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>St. Petersburg Math. J.</span></i></a><span style='font-family:"Times New Roman",serif'>, 7 (1996), no. 1, pages 77 127.</span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif'>The original motivation of this paper was to understand a rather mysterious action of the symmetric group <i>S<sub>n</sub></i> on Young tableaux, discovered by <span class=SpellE>Lascoux</span> and <span class=SpellE>Schutzenberger</span>. We introduced an action of <i>S<sub>n</sub></i> by piecewise-linear transformations on the space of Gelfand-<span class=SpellE>Tsetlin</span> patterns. In our approach, this group appears as a subgroup of the infinite group <span class=SpellE><i>G<sub>n</sub></i></span>, generated by quite simple piecewise-linear involutions (these involutions are continuous analogues of Bender-Knuth involutions acting on <span class=GramE>Young</span> tableaux). The structure of <span class=SpellE><i>G<sub>n</sub></i></span> is not yet completely understood. Some relations were given in [7]; they involve the famous <span class=SpellE>Sch�tzenberger</span> involution which also belongs to <i>G<sub>n</sub></i>.&nbsp;Another result of [7] is a conjectural description of <span class=SpellE>Kashiwara s</span> crystal operators for type <i>A</i>, in terms of <i>G<sub>n</sub></i>. </span></p> <p class=MsoNormal style='margin-bottom:0in'><span style='font-family:"Times New Roman",serif; color:black'>&nbsp;</span></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/triple.pdf"><b><span style='font-family: "Times New Roman",serif'>Triple multiplicities for <span class=SpellE><i>sl</i></span><i>(r+1)</i></span></b><b><span style='font-family:"Times New Roman",serif;color:blue'> and the spectrum of the exterior algebra of the adjoint representation</span></b></a><span style='font-family:"Times New Roman",serif'> (with </span><a href="https://en.wikipedia.org/wiki/Andrei_Zelevinsky"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>A. <span class=SpellE>Zelevinsky</span></span></a><span style='font-family:"Times New Roman",serif'>), </span><a href="https://www.springer.com/journal/10801"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>J. Algebraic <span class=SpellE>Combin</span>.</span></i></a><i><span style='font-family:"Times New Roman",serif'> </span></i><b><span style='font-family:"Times New Roman",serif'>1 </span></b><span style='font-family:"Times New Roman",serif'>(1992), no. 1, pages 7 22. </span></p> <p class=MsoNormal style='margin-bottom:0in'><b><span style='font-family:"Times New Roman",serif'>&nbsp;</span></b></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/mult1.pdf"><b><span style='font-family: "Times New Roman",serif'>When is the weight multiplicity equal to </span></b><b><i><span style='font-family:"Times New Roman",serif;color:blue'>1</span></i></b></a><b><i><span style='font-family:"Times New Roman",serif'>&nbsp; </span></i></b><span style='font-family:"Times New Roman",serif'>(Russian) (with&nbsp; </span><a href="https://en.wikipedia.org/wiki/Andrei_Zelevinsky"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>A. <span class=SpellE>Zelevinsky</span></span></a><span style='font-family:"Times New Roman",serif'>) </span><a href="https://www.mathnet.ru/php/archive.phtml?jrnid=faa&amp;wshow=IF_details&amp;year=2014&amp;IFTYPE=2&amp;option_lang=eng&amp;goto=e91adfeb0e359902752e30611c752262_0"><span class=SpellE><i><span style='font-family:"Times New Roman",serif;color:blue; text-decoration:none;text-underline:none'>Funkc</span></i></span><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>. Anal. <span class=SpellE>Pril</span>.</span></i></a><i><span style='font-family:"Times New Roman",serif'> <b>24 </b>(1990), no. 4, 1 13; </span></i><span style='font-family:"Times New Roman",serif'>translation:<i> </i></span><a href="https://www.springer.com/journal/10688"><span class=SpellE><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Funct</span></i></span><i><span style='font-family:"Times New Roman",serif; color:blue;text-decoration:none;text-underline:none'>. Anal. Appl.</span></i></a><i><span style='font-family:"Times New Roman",serif'> </span></i><b><span style='font-family:"Times New Roman",serif'>24 </span></b><span style='font-family:"Times New Roman",serif'>(1990), no. 4, pages 259 269. </span></p> <p class=MsoNormal style='margin-bottom:0in'><b><span style='font-family:"Times New Roman",serif'>&nbsp;</span></b></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/tensor.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>Tensor product multiplicities and convex polytopes in partition space</span></b></a><b><span style='font-family:"Times New Roman",serif'> </span></b><span style='font-family:"Times New Roman",serif'>(with </span><a href="https://en.wikipedia.org/wiki/Andrei_Zelevinsky"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>A. <span class=SpellE>Zelevinsky</span></span></a><span style='font-family:"Times New Roman",serif'>) </span><a href="https://www.journals.elsevier.com/journal-of-geometry-and-physics"><i><span style='font-family:"Times New Roman",serif'>J.</span></i><span style='font-family:"Times New Roman",serif'> </span><i><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>Geom. Phys.</span></i></a><span style='font-family:"Times New Roman",serif'> 5 (1988), no. 3, pages 453 472. </span></p> <p class=MsoNormal style='margin-bottom:0in'><b><span style='font-family:"Times New Roman",serif'>&nbsp;</span></b></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/alek0.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>A multiplicative analogue of the Bergstrom inequality for a matrix product in the sense of Hadamard</span></b></a><span style='font-family:"Times New Roman",serif'> (with </span><a href="https://cris.haifa.ac.il/en/persons/alek-vainshtein"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Alek <span class=SpellE>Vainshtein</span></span></a><span style='font-family:"Times New Roman",serif'>) (Russian) </span><a href="http://www.mathnet.ru/php/journal.phtml?jrnid=rm&amp;option_lang=eng"><span class=SpellE><i><span style='font-family:"Times New Roman",serif;color:blue; text-decoration:none;text-underline:none'>Uspekhi</span></i></span><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'> Mat. <span class=SpellE>Nauk</span></span></i></a><span style='font-family:"Times New Roman",serif'> <b>42</b> (1987), no. 6 (258), pages 181 182. Translation: </span><a href="https://iopscience.iop.org/journal/0036-0279"><i><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>Russian Mathematical Surveys</span></i></a><span style='font-family:"Times New Roman",serif'>.</span></p> <p class=MsoNormal style='margin-bottom:0in'><b><span style='font-family:"Times New Roman",serif'>&nbsp;</span></b></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/alek85.pdf"><b><span style='font-family: "Times New Roman",serif;color:blue'>The convexity property of the Poisson distribution and its applications in queueing theory</span></b></a><b><span style='font-family:"Times New Roman",serif'> </span></b><span style='font-family: "Times New Roman",serif'>(with </span><a href="https://cris.haifa.ac.il/en/persons/alek-vainshtein"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Alek <span class=SpellE>Vainshtein</span></span></a><span style='font-family:"Times New Roman",serif'> and </span><a href="https://scholar.google.com/citations?user=v9RrV4gAAAAJ&amp;hl=en"><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>A. <span class=SpellE>Kreinin</span></span></a><span style='font-family:"Times New Roman",serif'>)&nbsp; (Russian). Translation: </span><a href="https://journals.scholarsportal.info/browse/00904104"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>J. Soviet Math.</span></i></a><span style='font-family: "Times New Roman",serif'> <b>47</b> (1989), no. 1. </span></p> <p class=MsoNormal style='margin-bottom:0in'><b><span style='font-family:"Times New Roman",serif'>&nbsp;</span></b></p> <p class=MsoNormal style='margin-bottom:0in'><a href="http://pages.uoregon.edu/arkadiy/bz87.pdf"><b><span style='font-family: "Times New Roman",serif'>Involutions on Gelfand-<span class=SpellE>Tsetlin</span> patterns and multiplicities in skew <i>GL(n)</i></span></b><b><span style='font-family:"Times New Roman",serif;color:blue'>-modules</span></b></a><b><span style='font-family:"Times New Roman",serif'> </span></b><span style='font-family: "Times New Roman",serif'>(with </span><a href="https://en.wikipedia.org/wiki/Andrei_Zelevinsky"><span style='font-family: "Times New Roman",serif;color:blue;text-decoration:none;text-underline:none'>A. <span class=SpellE>Zelevinsky</span></span></a><span style='font-family:"Times New Roman",serif'>) </span><a href="https://www.springer.com/journal/11472"><i><span style='font-family:"Times New Roman",serif;color:blue;text-decoration:none; text-underline:none'>Soviet Math. <span class=SpellE>Dokl</span>.</span></i></a><span style='font-family:"Times New Roman",serif'> 37 (1988), no. 3, 799 802 <b>592</b> (2013), pages 71 102.</span></p> <p class=MsoNormal><span lang=RU style='font-family:"Times New Roman",serif; mso-ansi-language:RU'>&nbsp;</span></p> </div> </body> </html>