Search results for "Commutative property"

showing 10 items of 34 documents

Some aspects of deformations of supersymmetric field theories

2000

We investigate some aspects of Moyal-Weyl deformations of superspace and their compatibility with supersymmetry. For the simplest case, when only bosonic coordinates are deformed, we consider a four dimensional supersymmetric field theory which is the deformation of the Wess-Zumino renormalizable theory of a chiral superfield. We then consider the deformation of a free theory of an abelian vector multiplet, which is a non commutative version of the rank one Yang-Mills theory. We finally give the supersymmetric version of the $\alpha'\mapsto 0$ limit of the Born-Infeld action with a B-field turned on, which is believed to be related to the non commutative U(1) gauge theory.

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSupersymmetrySuperspaceTheoretical physicsHigh Energy Physics::TheoryChiral superfieldHigh Energy Physics - Theory (hep-th)Compatibility (mechanics)Mathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)Gauge theoryAbelian groupMultipletCommutative propertyParticle Physics - Theory
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Non-commutative geometry and supersymmetry II

1991

Abstract Extending results of a previous work [Phys. Lett. B 260 (1991) 359], we establis that anothe non-commutative model proposed by Balakrishna, Gursey and Wali may be expressed as a Yang-Mills theory of a graded Lie group.

PhysicsNuclear and High Energy PhysicsTheoretical physicsWork (thermodynamics)Quantum mechanicsLie groupSupersymmetryQuantum field theoryCommutative propertyPhysics Letters B
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Perturbative BF-Yang–Mills theory on noncommutative

2000

A U(1) BF-Yang-Mills theory on noncommutative ${\mathbb{R}}^4$ is presented and in this formulation the U(1) Yang-Mills theory on noncommutative ${\mathbb{R}}^4$ is seen as a deformation of the pure BF theory. Quantization using BRST symmetry formalism is discussed and Feynman rules are given. Computations at one-loop order have been performed and their renormalization studied. It is shown that the U(1) BFYM on noncommutative ${\mathbb{R}}^4$ is asymptotically free and its UV-behaviour in the computation of the $\beta$-function is like the usual SU(N) commutative BFYM and Yang Mills theories.

PhysicsNuclear and High Energy PhysicsYang–Mills existence and mass gapYang–Mills theoryNoncommutative geometryBRST quantizationRenormalizationHigh Energy Physics::Theorysymbols.namesakeFormalism (philosophy of mathematics)Mathematics::Quantum AlgebrasymbolsFeynman diagramCommutative propertyMathematical physicsNuclear Physics B
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A pointwise selection principle for metric semigroup valued functions

2008

Abstract Let ∅ ≠ T ⊂ R , ( X , d , + ) be an additive commutative semigroup with metric d satisfying d ( x + z , y + z ) = d ( x , y ) for all x , y , z ∈ X , and X T the set of all functions from T into X . If n ∈ N and f , g ∈ X T , we set ν ( n , f , g , T ) = sup ∑ i = 1 n d ( f ( t i ) + g ( s i ) , g ( t i ) + f ( s i ) ) , where the supremum is taken over all numbers s 1 , … , s n , t 1 , … , t n from T such that s 1 ⩽ t 1 ⩽ s 2 ⩽ t 2 ⩽ ⋯ ⩽ s n ⩽ t n . We prove the following pointwise selection theorem: If a sequence of functions { f j } j ∈ N ⊂ X T is such that the closure in X of the set { f j ( t ) } j ∈ N is compact for each t ∈ T , and lim n → ∞ ( 1 n lim N → ∞ sup j , k ⩾ N , j…

PointwisePointwise convergenceDiscrete mathematicsSequenceSemigroupApplied MathematicsPointwise productInfimum and supremumPointwise convergenceSelection principleMetric semigroupJoint modulus of variationCombinatoricsSubsequenceCommutative propertyDouble sequenceAnalysisMathematicsJournal of Mathematical Analysis and Applications
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Matrix algebras with degenerate traces and trace identities

2022

In this paper we study matrix algebras with a degenerate trace in the framework of the theory of polynomial identities. The first part is devoted to the study of the algebra $D_n$ of $n \times n$ diagonal matrices. We prove that, in case of a degenerate trace, all its trace identities follow by the commutativity law and by pure trace identities. Moreover we relate the trace identities of $D_{n+1}$ endowed with a degenerate trace, to those of $D_n$ with the corresponding trace. This allows us to determine the generators of the trace T-ideal of $D_3$. In the second part we study commutative subalgebras of $M_k(F)$, denoted by $C_k$ of the type $F + J$ that can be endowed with the so-called st…

PolynomialAlgebra and Number TheoryTrace (linear algebra)Trace algebrasDiagonal matricesDegenerate energy levelsMathematics - Rings and AlgebrasType (model theory)Polynomial identitiesStirling numbersCombinatoricsMatrix (mathematics)Settore MAT/02 - Algebra16R10 16R30 16R50Rings and Algebras (math.RA)Diagonal matrixFOS: MathematicsDegenerate tracesAlgebra over a fieldCommutative propertyTrace algebras; Polynomial identities; Diagonal matrices; Degenerate traces; Stirling numbersMathematics
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Trace identities and almost polynomial growth

2021

In this paper we study algebras with trace and their trace polynomial identities over a field of characteristic 0. We consider two commutative matrix algebras: $D_2$, the algebra of $2\times 2$ diagonal matrices and $C_2$, the algebra of $2 \times 2$ matrices generated by $e_{11}+e_{22}$ and $e_{12}$. We describe all possible traces on these algebras and we study the corresponding trace codimensions. Moreover we characterize the varieties with trace of polynomial growth generated by a finite dimensional algebra. As a consequence, we see that the growth of a variety with trace is either polynomial or exponential.

PolynomialPure mathematicsTrace (linear algebra)Trace algebrasField (mathematics)01 natural sciencesPolynomial identitiesMatrix (mathematics)16R10 16R30 16R50Polynomial identitieCodimensions growth Polynomial identities Trace algebras0103 physical sciencesDiagonal matrixFOS: Mathematics0101 mathematicsCommutative propertyMathematicsCodimensions growth; Polynomial identities; Trace algebrasAlgebra and Number TheoryCodimensions growth010102 general mathematicsTrace algebraMathematics - Rings and AlgebrasExponential functionSettore MAT/02 - AlgebraRings and Algebras (math.RA)010307 mathematical physicsVariety (universal algebra)
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Extensions of the Noncommutative Integration

2016

In this paper we will continue the analysis undertaken in Bagarello et al. (Rend Circ Mat Palermo (2) 55:21–28, 2006), Bongiorno et al. (Rocky Mt J Math 40(6):1745–1777, 2010), Triolo (Rend Circ Mat Palermo (2) 60(3):409–416, 2011) on the general problem of extending the noncommutative integration in a *-algebra of measurable operators. As in Aiena et al. (Filomat 28(2):263–273, 2014), Bagarello (Stud Math 172(3):289–305, 2006) and Bagarello et al. (Rend Circ Mat Palermo (2) 55:21–28, 2006), the main problem is to represent different types of partial *-algebras into a *-algebra of measurable operators in Segal’s sense, provided that these partial *-algebras posses a sufficient family of pos…

Pure mathematicsApplied MathematicsGeneral problem010102 general mathematicsMeasurable operatorOperator theory01 natural sciencesNoncommutative geometryNoncommutative integrationPartial algebras of operator010101 applied mathematicsComputational MathematicsComputational Theory and MathematicsSettore MAT/05 - Analisi MatematicaComputational Theory and MathematicComputational Mathematic0101 mathematicsAlgebra over a fieldCommutative propertyMathematicsComplex Analysis and Operator Theory
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Extended pseudo-fermions from non commutative bosons

2013

We consider some modifications of the two dimensional canonical commutation relations, leading to {\em non commutative bosons} and we show how biorthogonal bases of the Hilbert space of the system can be obtained out of them. Our construction extends those recently introduced by one of us (FB), modifying the canonical anticommutation relations. We also briefly discuss how bicoherent states, producing a resolution of the identity, can be defined.

Pure mathematicsFOS: Physical sciences01 natural sciencessymbols.namesakeIdentity (mathematics)Theoretical physicsMeasurement theory0103 physical sciences010306 general physicsSettore MAT/07 - Fisica MatematicaCommutative propertyMathematical PhysicsComputer Science::DatabasesComputingMilieux_MISCELLANEOUSMathematicsBoson[PHYS]Physics [physics]010308 nuclear & particles physicsHilbert spaceStatistical and Nonlinear PhysicsFermionMathematical Physics (math-ph)16. Peace & justiceBiorthogonal systemsymbolspseudo-bosons[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]Resolution (algebra)
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Identities of sums of commutative subalgebras

1994

SiaR un'algebra associativa tale cheR=A+B conA, B sottoalgebre commutative. Si dimostra cheR soddisfa l'identita polinomiale [[x,y],[z,t]]≡0 e che, seV e la varieta determinata da questa identita,V e la piu piccola varieta contenente tutte le algebre somma di sottoalgebre commutative. Si determina inoltre la struttura delle algebre libere diV.

Pure mathematicsGeneral MathematicsAlgebra over a fieldCommutative propertyMathematicsRendiconti del Circolo Matematico di Palermo
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Commutativity conditions on rings

1991

We prove the following result: let R be an arbitrary ring with centre Z such that for every x, y ∈ R, there exists a positive integer n = n(x, y) ≥ 1 such that (xy)n − ynxn ∈ Z and (yx)n − xnyn ∈ Z; then, if R has no non-zero nil ideals, R is commutative. We also prove a result on commutativity of general rings: if R is r!-torsion free and for all x, y ∈ R, [xr, ys] = 0 for fixed integers r ≥ s ≥ 1, then R is commutative. As a corollary we obtain that if R is (n + 1)!-torsion free and there exists a fixed n ≥ 1 such that (xy)n − ynxn = (yx)n − xnyn ∈ Z for all x, y ∈ R, then R is commutative.

Pure mathematicsGeneral MathematicsCommutative propertyMathematicsBulletin of the Australian Mathematical Society
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