Khovanov–Rozansky cycle calculus for bipartite links

Abstract Bipartite calculus is a direct generalization of Kauffman planar expansion from $$N=2$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>N</mml:mi> <mml:mo>=</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:math> to arbitrary N , applicable to the restricted class of knots which are entirely made of antiparallel lock tangles. Whenever applicable, it allows a straightforward generalization of the Khovanov calculus without a need of the technically complicated matrix factorization used for arbitrary N in the Khovanov–Rozansky (KR) approach. The main object here is the $$3^{n}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mn>3</mml:mn> <mml:mi>n</mml:mi> </mml:msup> </mml:math> -dimensional hypercube with n being the number of bipartite vertices. Maps, differentials, complex and Poincaré polynomials are straightforward and indeed reproduce the Khovanov–Rozansky polynomials in the known cases. This provides a great simplification of the Khovanov–Rozansky calculus on the bipartite locus, what can make it an accessible tool for the study of superpolynomials.

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Publication Details

Journal
The European Physical Journal C
Published
2025-10-22
DOI
https://doi.org/10.1140/epjc/s10052-025-14854-y
Citations
2
Primary Topic
Geometric and Algebraic Topology
Type
article
Field-Weighted Citation Impact
8.18

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article

Khovanov–Rozansky cycle calculus for bipartite links

E. Lanina, A. Morozov, A. Anokhina
2 citations
The European Physical Journal C
Geometric and Algebraic Topology
8.18
article

Khovanov–Rozansky cycle calculus for bipartite links

E. Lanina, A. Morozov, A. Anokhina
article en
2 citations

Abstract

Abstract Bipartite calculus is a direct generalization of Kauffman planar expansion from $$N=2$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>N</mml:mi> <mml:mo>=</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:math> to arbitrary N , applicable to the restricted class of knots which are entirely made of antiparallel lock tangles. Whenever applicable, it allows a straightforward generalization of the Khovanov calculus without a need of the technically complicated matrix factorization used for arbitrary N in the Khovanov–Rozansky (KR) approach. The main object here is the $$3^{n}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mn>3</mml:mn> <mml:mi>n</mml:mi> </mml:msup> </mml:math> -dimensional hypercube with n being the number of bipartite vertices. Maps, differentials, complex and Poincaré polynomials are straightforward and indeed reproduce the Khovanov–Rozansky polynomials in the known cases. This provides a great simplification of the Khovanov–Rozansky calculus on the bipartite locus, what can make it an accessible tool for the study of superpolynomials.

The European Physical Journal CVol. 85(10)
Moscow Institute of Physics and Technology (RU), Kurchatov Institute (RU), Institute for Information Transmission Problems (RU), Institute for Theoretical and Experimental Physics (RU)
Ministry of Science and Higher Education of the Russian Federation, Foundation for the Advancement of Theoretical Physics and Mathematics
Openalex Percentile: Top 2%
Geometric and Algebraic Topology
8.18
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