Date | Speaker | Title |
Feb 29 | Mike Miller University of Vermont |
TBA |
Feb 8 | Oleg Lazarev UMass Boston |
TBA |
Nov 16 * | Sergey Melikhov Steklov Mathematical Institute of the Russian Academy of Science, Moscow, Russia |
On the analogues of Cochran's derived invariants for links of linking number 1 |
Oct 26 | Ivan Dynnikov Steklov Mathematical Institute of the Russian Academy of Science and Moscow State University, Moscow, Russia |
Rectangular diagrams of taut foliations in knot complements |
Oct 12 | Matt Hogancamp Northeastern University |
Khovanov homology and handleslides |
Sep 28 | Matthew Harper UC Riverside |
Seifert-Torres Formulas for the Alexander Polynomial of Links from Quantum sl2 |
Sep 14 * | Evgeniy Scepin Steklov Mathematical Institute of the Russian Academy of Science, Moscow, Russia |
Application of topology to optical recognition of handwritten characters |
February 29, 2023: Mike Miller "TBA"
Abstract: TBA
February 8, 2023: Oleg Lazarev "TBA"
Abstract: TBA
November 16, 2023: Sergey Melikhov " On the analogues of Cochran's derived invariants for links of linking number 1"
Abstract:
Let L=(K_1,K_2) be a two-component smooth link in S^3. In the case
lk(L)=0, S. Kojima and M. Yamasaki (1979) introduced a useful
invariant \eta_L, namely, the generating function of the linking
numbers between a lift of a zero pushoff of K_2 and the various lifts
of K_2 itself in the infinite cyclic cover of S^3-K_1. (Here the
"linking number" has the usual meaning when K_1 is the unknot, and in
general it is defined using that every 1-cycle in \widetilde{S^3-K_1}
becomes a boundary upon being multiplied by some Laurent polynomial.)
T. Cochran (1985) discovered that \eta_L is equivalent by a change of
variable to a power series whose coefficients \beta^i(L) have a simple
and beautiful geometric description in terms of iterated intersections
of Seifert surfaces. It further turns out that these integers
\beta^i(L) are in fact some of the coefficients of the power series
\nabla_L(u,v,w)/\nabla_{K_1}(u), where \nabla_{K_1} is the Conway
polynomial and \nabla_L is the so-called two-variable Conway
polynomial. This observation of mine (2003) was originally a
consequence of a theorem of J. T. Jin (1988), who expressed \eta_L in
terms of the Alexander polynomials of L and K_1 by a clever argument
involving many surgeries of S^3.
But recently I found a simpler proof of this fact, in terms of Seifert matrices.
Cochran's derived invariants \beta^i(L), being coefficients of the
power series \nabla_L(u,v,w)/\nabla_{K_1}(u), are defined for
two-component smooth links of any linking number. But in the case
lk(L)\ne 0 their geometry was a complete mystery until recently. I
will discuss a theorem which sheds some light on their geometry in the
case lk(L)=1.
One reason to be concerned about the geometry of \beta^i(L) in the
case lk(L)=1 is that these invariants have been used in the recent
progress on Rolfsen's problem: "Is every knot isotopic to
the unknot? In particular, is the Bing sling isotopic (=homotopic
through embeddings) to the unknot (or, equivalently, to a smooth
knot)?". The theorem says that there exists no isotopy from
the Bing sling to the unknot that extends to an isotopy of a
two-component link with lk=1.
October 26, 2023: Ivan Dynnikov "Rectangular diagrams of taut foliations in knot complements"
Abstract: Taut foliations are an important instrument in low-dimensional topology. In particular, due to the works of W.Thurston and D.Gabai, they can be used to certify knot genus. Jointly with Mikhail Chernavskikh we have worked out a universal way to represent taut foliations in knot complements by using the formalism of rectangular diagrams, and shown that any finite depth taut foliation can be represented in this way. This will be explained in the talk. The work is supported by the Russian Science Foundation under grant 22-11-00299
October 12, 2023: Matt Hogancamp " Khovanov homology and handleslides "
Abstract: If K is a framed knot and X is a link in the solid torus, then the satellite operation produces a link K(X), obtained by embedding X (the "pattern") into a tubular neighborhood of K (the "companion"). In the context of Khovanov homology, the patterns can be thought of as objects of a category called the annular Bar-Natan category (ABN), and the satellite operation defines a functor from ABN to bigraded vector spaces, sending a pattern X to Kh(K(X)). In this talk I will discuss joint work with Dave Rose and Paul Wedrich, in which we construct an object Ω (which we call a "Kirby color") in ABN such that Kh(K(Ω)) is invariant under handleslides. As I will explain, the object Ω encodes the Manolescu-Neithalath 2-handle formula for the sl(2) skein lasagna modules (which was inspirational for our work). Time permitting, I will discuss an intriguing description of the Kirby object in terms of some special braids (positive braid lifts of n-cycles) that we speculate may be more amenable for computation.
September 28, 2023: Matthew Harper "Seifert-Torres Formulas for the Alexander Polynomial of Links from Quantum sl2"
Abstract: In this talk, I will recall how the Alexander polynomial, a classical knot invariant, can be constructed as a quantum invariant from quantum sl2 at a fourth root of unity. I will then discuss the development of a diagrammatic calculus based on further investigation of quantum sl2 representations. Applying this calculus in the context of the Alexander polynomial allows us to compute the invariant for certain families of links using quantum algebraic methods, rather than using methods of classical topology.
September 14, 2023: Evgeniy Scepin "Application of topology to optical recognition of handwritten characters"
Abstract: Every handwritten symbol consists of several lines. These lines may intersect. Therefore, each symbol corresponds to a graph whose vertices correspond to the intersection points of the lines and their ends, and the edges correspond to the line segments enclosed between the vertices. A scanned image of a symbol representing a Boolean matrix is fed to the input of the recognition program. On the image matrix, the lines become "thick", interference also occurs there. The report will tell you how to reduce the image so as to get a correct graph of the symbol, whose edges on the matrix are represented by thin (pixel-thick) lines that preserve the shape of the original ones.