Results 31 to 40 of about 1,481,386 (231)

Adjoint-based optimization of a source-term representation of vortex generators

, 2017
Liesbeth Florentie, Steven J. Hulshoff, A.H. van Zuijlen   +2 more
openalex   +2 more sources

SELF-ADJOINT REPRESENTATIONS OF BRAID GROUPS [PDF]

Journal of Knot Theory and Its Ramifications, 2012
We give a method to construct new self-adjoint representations of 𝔹n of finite dimension. In particular, we give a family of irreducible self-adjoint representations of dimension arbitrarily large. Moreover we give sufficient condition for a representation to be constructed with this method.
Esther Galina, Claudia Maria Egea
openaire   +3 more sources

Correction to: Representations are adjoint to endomorphisms [PDF]

Journal of Homotopy and Related Structures, 2020
The first equation under section “Remark 3” was processed and published incorrectly. The correct equation should read as follows:
Damien Lejay, Joseph Hirsh, Gabriel C. Drummond-Cole   +2 more
openaire   +1 more source

On Adjoint Dynamical Systems [PDF]

, 1973
Transformations of dynamical systems and organismic structures are discussed in terms of adjoint, simple adjoint and weak adjoint functors of organismic supercategories during development and evolution of organisms on markedly different timescales.
Baianu, Prof. Dr. I. C., Scripcariu, Prof.Dr. Dragos   +1 more
core   +1 more source

Simultaneous representation by adjoint quadratic forms [PDF]

Acta Arithmetica, 1964
Gordon Pall
openalex   +3 more sources

Analysis of the vacuum solution of the five-dimensional Einstein field equations with negative cosmological constant via variational symmetries [PDF]

AUT Journal of Mathematics and Computing
The Kaluza-Klein theory can be reckoned as a classical unified field theory of two of the significant forces of nature gravitation and electromagnetism.
Fatemeh Ahangari
doaj   +1 more source

A 6D nonabelian (1, 0) theory

Journal of High Energy Physics, 2018
We construct a 6D nonabelian N=1,0 $$ \mathcal{N}=\left(1,\ 0\right) $$ theory by coupling an N=1,0 $$ \mathcal{N}=\left(1,\ 0\right) $$ tensor multiplet to an N=1,0 $$ \mathcal{N}=\left(1,\ 0\right) $$ hypermultiplet.
Fa-Min Chen
doaj   +1 more source

Perturbative improvement of SU(2) gauge theory with two Wilson fermions in the adjoint representation [PDF]

, 2010
We present a perturbative calculation of the improvement coefficients of SU(2) gauge theory with adjoint representation Wilson-clover fermions and using Schrodinger functional boundary conditions.
Tuomas Karavirta, Anne Mykkanen, J. Rantaharju, K. Rummukainen, K. Tuominen   +4 more
semanticscholar   +1 more source

VB-groupoids and representation theory of Lie groupoids [PDF]

, 2016
A VB-groupoid is a Lie groupoid equipped with a compatible linear structure. In this paper, we describe a correspondence, up to isomorphism, between VB-groupoids and 2-term representations up to homotopy of Lie groupoids.
Gracia-Saz, Alfonso, Mehta, Rajan Amit
core   +3 more sources

Asymptotic formulas for a scalar linear delay differential equation

Electronic Journal of Qualitative Theory of Differential Equations, 2016
The linear delay differential equation $$ x'(t)=p(t)x(t-r) $$ is considered, where $r>0$ and the coefficient $p:[t_0,\infty)\to\mathbb{R}$ is a continuous function such that $p(t)\to0$ as $t\to\infty$. In a recent paper [M. Pituk, G. Röst, Bound.
István Győri, Mihály Pituk
doaj   +1 more source