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We use instanton numbers to: (i) stratify moduli of vector bundles, (ii) calculate relative homology of moduli spaces and (iii) distinguish curve singularities.

Mathematical Physics · Physics 2008-11-26 Elizabeth Gasparim , Pedro Ontaneda

Atiyah and Manton have outlined a scheme to obtain approximations to the SU(2) skyrmions from instantons in $\R^4$. In this paper we apply this scheme to construct, in an explicit form, approximations to static spherically symmetric SU(N)…

High Energy Physics - Theory · Physics 2009-10-31 Theodora Ioannidou

We derive the general equations of motion for a braneworld containing a (localized) domain wall. Euclideanization gives the geometry for braneworld false vacuum decay. We explicitly derive these instantons and compute the amplitude for…

High Energy Physics - Theory · Physics 2011-08-12 Ruth Gregory , Antonio Padilla

We elaborate on the quantization of toric varieties by combining techniques from toric geometry, isospectral deformations and noncommutative geometry in braided monoidal categories, and the construction of instantons thereon by combining…

High Energy Physics - Theory · Physics 2012-12-17 Lucio S. Cirio , Giovanni Landi , Richard J. Szabo

The Yang-Mills (YM) and self-dual Yang-Mills (SDYM) equations on the noncommutative Euclidean four-dimensional space are considered. We introduce an ansatz for a gauge potential reducing the noncommutative SDYM equations to a difference…

High Energy Physics - Theory · Physics 2008-11-26 Filip Franco-Sollova , Tatiana A. Ivanova

Explicit construction of the basic SU(2) anti-instantons over the multi-Taub--NUT geometry via the classical conformal rescaling method is exhibited. These anti-instantons satisfiy the so-called weak holonomy condition at infinity with…

Differential Geometry · Mathematics 2011-01-05 Gabor Etesi , Szilard Szabo

We review the theory and phenomenology of instantons in QCD. After a general overview, we provide a pedagogical introduction to semi-classical methods in quantum mechanics and field theory. The main part of the review summarizes our…

High Energy Physics - Phenomenology · Physics 2008-11-26 T. Schaefer , E. Shuryak

The moduli space of k G-instantons on R^4 for a classical gauge group G is known to be given by the Higgs branch of a supersymmetric gauge theory that lives on Dp branes probing D(p + 4) branes in Type II theories. For p = 3, these (3 + 1)…

High Energy Physics - Theory · Physics 2015-03-17 Sergio Benvenuti , Amihay Hanany , Noppadol Mekareeya

Generalized Fourier transformation between the position and the momentum representation of a quantum state is constructed in a coordinate independent way. The only ingredient of this construction is the symplectic (canonical) geometry of…

Quantum Physics · Physics 2012-03-14 Witold Chmielowiec , Jerzy Kijowski

Instantons play a crucial role in understanding non-perturbative dynamics in quantum field theories, including those with spontaneously broken gauge symmetries. In the broken phase, finite-size instanton-like configurations are no longer…

High Energy Physics - Theory · Physics 2026-04-06 Takafumi Aoki , Masahiro Ibe , Satoshi Shirai

We study $SU(2)$ calorons, also known as periodic instantons, and consider invariance under isometries of $S^1\times\mathbb{R}^3$ coupled with a non-spatial isometry called the rotation map. In particular, we investigate the fixed points…

High Energy Physics - Theory · Physics 2018-06-22 Josh Cork

We embed the multi-fractional instantons of $SU(N)$ gauge theories on $\mathbb T^4$ with 't Hooft twisted boundary conditions into $U(N)$ bundles and use the Nahm transform to study the corresponding configurations on the dual…

High Energy Physics - Theory · Physics 2024-11-20 Mohamed M. Anber , Erich Poppitz

We generalize Nakajima-Yoshioka blowup equations to arbitrary gauge group with hypermultiplets in arbitrary representations. Using our blowup equations, we compute the instanton partition functions for 4d N=2 and 5d N=1 gauge theories for…

High Energy Physics - Theory · Physics 2020-01-08 Joonho Kim , Sung-Soo Kim , Ki-Hong Lee , Kimyeong Lee , Jaewon Song

We present a construction of framed torsion free instanton sheaves on a projective variety containing a fixed line which further generalizes the one on projective spaces. This is done by generalizing the so called ADHM variety. We show that…

Algebraic Geometry · Mathematics 2015-08-05 Abdelmoubine Amar Henni , Marcos Jardim , Renato Vidal Martins

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 study U(1) and U(2) instanton solutions on noncommutative R^4 based on the noncommutative version of ADHM equation proposed by Nekrasov and Schwarz. It is shown that the anti-self-dual gauge fields on self-dual noncommutative R^4…

High Energy Physics - Theory · Physics 2008-11-26 Keun-Young Kim , Bum-Hoon Lee , Hyun Seok Yang

We employ the ADHM method to derive the moduli space of two instantons in U(1) gauge theory on a noncommutative space. We show by an explicit hyperK\"ahler quotient construction that the relative metric of the moduli space of two instantons…

High Energy Physics - Theory · Physics 2009-10-31 Kimyeong Lee , David Tong , Sangheon Yi

For the system with one-dimensional spatially periodic potential we demonstrate that small periodic in time perturbation results in appearance of chaotic instanton solutions. We estimate parameter of local instability, width of stochastic…

Chaotic Dynamics · Physics 2009-11-10 V. I. Kuvshinov , A. V. Kuzmin , R. G. Shulyakovsky

The thermal instanton determinant for the gauge group $SU(2)$ can be reduced to a form involving two simple functions. Various boundary conditions can easily incorporated. Only a two dimensional integral has to be done numerically. As an…

High Energy Physics - Theory · Physics 2014-12-02 Chris. P. Korthals Altes , Alfonso Sastre

A general formula for bound-continuous transition form factors is derived. It is shown that these form factors can be represented in the form of finite sum of terms with simple analytical structure.

High Energy Physics - Phenomenology · Physics 2007-05-23 O. Voskresenskaya
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