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We show that noncommutative gauge theory in two dimensions is an exactly solvable model. A cohomological formulation of gauge theory defined on the noncommutative torus is used to show that its quantum partition function can be written as a…

High Energy Physics - Theory · Physics 2009-11-07 L. D. Paniak , R. J. Szabo

We define and study natural $\mathrm{SU}(2)$-structures, in the sense of Conti-Salamon, on the total space $\cal S$ of the tangent sphere bundle of any given oriented Riemannian 3-manifold $M$. We recur to a fundamental exterior…

Differential Geometry · Mathematics 2020-10-19 R. Albuquerque

We recently defined invariants of contact 3-manifolds using a version of instanton Floer homology for sutured manifolds. In this paper, we prove that if several contact structures on a 3-manifold are induced by Stein structures on a single…

Symplectic Geometry · Mathematics 2018-12-19 John A. Baldwin , Steven Sivek

We consider generalized self-duality equations for U(2r) Yang-Mills theory on R^{4k} with quaternionic structure and self-dual Moyal deformation. We employ the extended ADHM method in 4k dimensions to construct new noncommutative…

High Energy Physics - Theory · Physics 2008-11-26 Johannes Broedel , Tatiana A. Ivanova , Olaf Lechtenfeld

We initiate the systematic study of $G_2$-instantons with $SU(2)^2$-symmetry. As well as developing foundational theory, we give existence, non-existence and classification results for these instantons. We particularly focus on…

Differential Geometry · Mathematics 2018-04-24 Jason D. Lotay , Goncalo Oliveira

We study the q-deformed fuzzy sphere, which is related to D-branes on SU(2) WZW models, for both real q and q a root of unity. We construct for both cases a differential calculus which is compatible with the star structure, study the…

High Energy Physics - Theory · Physics 2009-10-31 Harald Grosse , John Madore , Harold Steinacker

In applications that involve interactive curve and surface modeling, the intuitive manipulation of shapes is crucial. For instance, user interaction is facilitated if a geometrical object can be manipulated through control points that…

Functional Analysis · Mathematics 2017-10-11 Daniel Schmitter , Julien Fageot , Anaïs Badoual , Pablo Garcia-Amorena , Michael Unser

Using center manifolds and topological degree theory, we construct a new family of complete, $SU(2)$-invariant and steady gradient Ricci solitons on the four-dimensional non-compact cohomogeneity one manifold with group diagram…

Differential Geometry · Mathematics 2021-11-29 Timothy Buttsworth

In this paper, we continue the study of the category of functors Fquad, associated to F_2-vector spaces equipped with a nondegenerate quadratic form, initiated in two previous papers of the author. We define a filtration of the standard…

Algebraic Topology · Mathematics 2007-05-23 Christine Vespa

A fuzzy version of the ordinary round 2-sphere has been constructed with an invariant curvature. We here consider linear connections on arbitrary fuzzy surfaces of genus zero. We shall find as before that they are more or less rigidly…

General Relativity and Quantum Cosmology · Physics 2009-10-30 J. Madore

A detailed Monte Carlo calculation of the phase diagram of bosonic IKKT Yang-Mills matrix models in three and six dimensions with quartic mass deformations is given. Background emergent fuzzy geometries in two and four dimensions are…

High Energy Physics - Theory · Physics 2017-03-08 Badis Ydri , Rouag Ahlam , Ramda Khaled

We show that the moduli space of the $(2,0)$ and little-string theories compactified on $T^3$ with R-symmetry twists is equal to the moduli space of U(1) instantons on a non-commutative $T^4$. The moduli space of $U(q)$ instantons on a…

High Energy Physics - Theory · Physics 2007-05-23 Yeuk-Kwan E. Cheung , Ori J. Ganor , Morten Krogh , Andrei Yu. Mikhailov

In this note we prove that the moduli space of rank $2n$ symplectic instanton bundles on ${\PP^{2n+1}}$, defined from the well known monad condition, is affine. This result was not known even in the case $n=1$, where the real instanton…

Algebraic Geometry · Mathematics 2007-05-23 Laura Costa , Giorgio Ottaviani

Some one- and two-parametric deformations of U[sl(2)] and their representations are considered. Interestingly, a newly introduced two-parametric deformation admits a class of infinite - dimensional representations which have no classical…

Quantum Algebra · Mathematics 2007-05-23 Nguyen Anh Ky

We study, by means of mirror symmetry, the quantum geometry of the K\"ahler-class parameters of a number of Calabi-Yau manifolds that have $b_{11}=2$. Our main interest lies in the structure of the moduli space and in the loci corresponding…

High Energy Physics - Theory · Physics 2009-10-22 Philip Candelas , Xenia de la Ossa , Anamaria Font , Sheldon Katz , David R. Morrison

We suggest the exactly solvable model of the oscillator on a four-dimensional hyperboloid which interacts with a SU(2) instanton. We calculate its wavefunctions and spectrum.

High Energy Physics - Theory · Physics 2009-11-11 Stefano Bellucci , Levon Mardoyan , Armen Nersessian

A noncommutative algebra of the complex $q$-twistors and their differentials is considered on the basis of the quantum $GL_q (4)\times SL_q (2)$ group. Real and pseudoreal $q$-twistors are discussed too. We consider the quantum-group…

q-alg · Mathematics 2008-02-03 B. M. Zupnik

For a given smooth $2$-knot in $S^4$, we relate the existence of a smooth Seifert hypersurface of a certain class to the existence of irreducible $ SU(2)$-representations of its knot group. For example, we see that any smooth $2$-knot…

Geometric Topology · Mathematics 2022-01-28 Masaki Taniguchi

We describe explicitly the moduli spaces $M^{pst}_g(S,E)$ of polystable holomorphic structures $E$ with $\det E\cong K$ on a rank 2 vector bundle $E$ with $c_1(E)=c_1(K)$ and $c_2(E)=0$ for all minimal class VII surfaces $S$ with $b_2(S)=1$…

Differential Geometry · Mathematics 2013-11-14 Konrad Schöbel

We show that the knot group of any knot in any integer homology sphere admits a non-abelian representation into $SU(3)$ such that meridians are mapped to matrices whose eigenvalues are the three distinct third roots of unity. This answers…

Geometric Topology · Mathematics 2024-02-19 Aliakbar Daemi , Nobuo Iida , Christopher Scaduto