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We introduce the concept of Spin^G-structure in a SO-bundle, where $G\subset U(V)$ is a compact Lie group containing $-id_V$. We study and classify $Spin^G(4)$-structures on 4-manifolds, we introduce the G-Monopole equations associated with…

alg-geom · Mathematics 2008-02-03 Andrei Teleman

We study the topology of compact manifolds with a Lie group action for which there are only finitely many non-principal orbits, and describe the possible orbit spaces which can occur. If some non-principal orbit is singular, we show that…

Differential Geometry · Mathematics 2011-06-20 Stefan Bechtluft-Sachs , David J. Wraith

The geometry of the total space of a principal bundle with regard to the action of the bundle's structure group is elegantly described by the bundle's operation, a collection of derivations consisting of the de Rham differential and the…

Mathematical Physics · Physics 2019-07-02 Roberto Zucchini

The action of Ashtekar's generalized gauge group $\Gb$ on the space $\Ab$ of generalized connections is investigated for compact structure groups $\LG$. First a stratum is defined to be the set of all connections of one and the same gauge…

Mathematical Physics · Physics 2009-10-31 Christian Fleischhack

An orbitope is the convex hull of an orbit of a compact group acting linearly on a vector space. These highly symmetric convex bodies lie at the crossroads of several fields, in particular convex geometry, optimization, and algebraic…

Algebraic Geometry · Mathematics 2013-01-21 Raman Sanyal , Frank Sottile , Bernd Sturmfels

We construct a compactification of the heterotic string on an orbifold T^6/Z_6 leading to the standard model spectrum plus vector--like matter. The standard model gauge group is obtained as an intersection of three SO(10) subgroups of E_8.…

High Energy Physics - Phenomenology · Physics 2010-11-19 Wilfried Buchmuller , Koichi Hamaguchi , Oleg Lebedev , Michael Ratz

A real form $G_0$ of a complex semisimple Lie group $G$ has only finitely many orbits in any given compact $G$-homogeneous projective algebraic manifold $Z=G/Q$. A maximal compact subgroup $K_0$ of $G_0$ has special orbits $C$ which are…

Representation Theory · Mathematics 2017-10-03 Faten S. Abu-Shoga

If P, B, H are the algebras of the total space, the base space, and the structure group of a locally trivial principal fibre bundle (QPFB), left (right) gauge transformations are defined as automorphisms of the left (right) B-module P which…

Quantum Algebra · Mathematics 2007-05-23 Dirk Calow , Rainer Matthes

Motivated by the simplicity and direct phenomenological applicability of field-theoretic orbifold constructions in the context of grand unification, we set out to survey the immensely rich group-theoretical possibilities open to this type…

High Energy Physics - Phenomenology · Physics 2010-04-05 Arthur Hebecker , Michael Ratz

Using geometric arguments, we compute the group of homotopy classes of maps from a closed $(n+1)$-dimensional manifold to the $n$-sphere for $n \geq 3$. Our work extends results from Kirby, Melvin and Teichner for closed oriented…

Geometric Topology · Mathematics 2025-10-15 Michael Jung , Thomas O. Rot

We propose a conceptually economical and computationally tractable completion of the foundations of gauge theory on quantum principal bundles \`{a} la Brzezi\'{n}ski--Majid to the case of general differential calculi and strong bimodule…

Mathematical Physics · Physics 2021-09-01 Branimir Ćaćić

Let $G$ be a compact Lie group of Lie type $B_{n},$ such as $SO(2n+1)$. We characterize the tuples\ $(x_{1},...,x_{L})$ of the elements $x_{j}\in G$ which have the property that the product of their conjugacy classes has non-empty interior.…

Functional Analysis · Mathematics 2021-10-14 Kathryn E. Hare

It is widely understood that the quotient space of a topological group action can have a complicated combinatorial structure, indexed somehow by the sotropy groups of the action, but how best to record this structure seems unclear. This…

Algebraic Topology · Mathematics 2014-05-20 Jack Morava

Four dimensional heterotic SO(32) orbifold models are classified systematically with model building applications in mind. We obtain all Z3, Z7 and Z2N models based on vectorial gauge shifts. The resulting gauge groups are reminiscent of…

High Energy Physics - Theory · Physics 2010-02-03 Kang-Sin Choi , Stefan Groot Nibbelink , Michele Trapletti

An approach to gauge theory in the context of locally conformally flat space-time is described. It is discussed how there are a number of natural principal bundles associated with any given locally conformally flat space-time $X$. The…

Mathematical Physics · Physics 2025-06-25 John Mashford

We consider the problem of existence of representations of topological groupoids on a principal bundle and the classification of such representations up to gauge transformation. Such representations naturally occur in various contexts such…

Differential Geometry · Mathematics 2007-05-23 Jean-Claude Hausmann

Geodesic orbit manifolds (or g.o. manifolds) are those Riemannian manifolds $(M,g)$ whose geodesics are integral curves of Killing vector fields. Equivalently, there exists a Lie group $G$ of isometries of $(M,g)$ such that any geodesic…

Differential Geometry · Mathematics 2024-09-13 Andreas Arvanitoyeorgos , Nikolaos Panagiotis Souris , Marina Statha

We classify SO(n)-equivariant principal bundles over $S^n$ in terms of their isotropy representations over the north and south poles. This is an example of a general result classifying equivariant $(\Pi, G)$-bundles over cohomogeneity one…

Geometric Topology · Mathematics 2013-02-12 Ian Hambleton , Jean-Claude Hausmann

Let $\mathcal{G}_k$ be the gauge group of the principal $SU(4)$-bundle over $S^4$ with second Chern class $k$ and let $p$ be a prime. We show that there is a rational or $p$-local homotopy equivalence…

Algebraic Topology · Mathematics 2022-06-28 Tyrone Cutler , Stephen Theriault

Higgs fields are attributes of classical gauge theory on a principal bundle $P\to X$ whose structure Lie group $G$ if is reducible to a closed subgroup $H$. They are represented by sections of the quotient bundle $P/H\to X$. A problem lies…

Mathematical Physics · Physics 2015-03-16 G. Sardanashvily , A. Kurov