1,124 research outputs found
Altering the Symmetry of Wavefunctions in Quantum Algebras and Supersymmetry
The statistics-altering operators present in the limit of
multiparticle SU_q(2)-invariant subspaces parallel the action of such operators
which naturally occur in supersymmetric theories. We illustrate this
heuristically by comparison to a toy superymmetry algebra, and ask
whether there is a supersymmetry structure underlying SU(2)_q at that limit. We
remark on the relevance of such alternating-symmetry multiplets to the
construction of invariant hamiltonians.Comment: 6 page
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Dimensional Deconstruction and Wess-Zumino-Witten Terms
A new technique is developed for the derivation of the Wess-Zumino-Witten
terms of gauged chiral lagrangians. We start in D=5 with a pure (mesonless)
Yang-Mills theory, which includes relevant gauge field Chern-Simons terms. The
theory is then compactified, and the effective D=4 lagrangian is derived using
lattice techniques, or ``deconstruction,'' where pseudoscalar mesons arise from
the lattice Wilson links. This yields the WZW term with the correct Witten
coefficient by way of a simple heuristic argument. We discover a novel WZW term
for singlet currents, that yields the full Goldstone-Wilczek current, and a
U(1) axial current for the skyrmion, with the appropriate anomaly structures. A
more detailed analysis is presented of the dimensional compactification of
Yang-Mills in D=5 into a gauged chiral lagrangian in D=4, heeding the
consistency of the D=4 and D=5 Bianchi identities. These dictate a novel
covariant derivative structure in the D=4 gauge theory, yielding a field
strength modified by the addition of commutators of chiral currents. The
Chern-Simons term of the pure D=5 Yang-Mills theory then devolves into the
correct form of the Wess-Zumino-Witten term with an index (the analogue of
N_{colors}=3) of N=D=5. The theory also has a Skyrme term with a fixed
coefficient.Comment: 29 pages, no figures; replacement fixes a typographical minus sign
error in eq.(16), an errant normalization factor, and clarifies some
discussion issue
Umbral Vade Mecum
In recent years the umbral calculus has emerged from the shadows to provide
an elegant correspondence framework that automatically gives systematic
solutions of ubiquitous difference equations --- discretized versions of the
differential cornerstones appearing in most areas of physics and engineering
--- as maps of well-known continuous functions. This correspondence deftly
sidesteps the use of more traditional methods to solve these difference
equations. The umbral framework is discussed and illustrated here, with special
attention given to umbral counterparts of the Airy, Kummer, and Whittaker
equations, and to umbral maps of solitons for the Sine-Gordon, Korteweg--de
Vries, and Toda systems.Comment: arXiv admin note: text overlap with arXiv:0710.230
Deformation Quantization of Nambu Mechanics
Phase Space is the framework best suited for quantizing superintegrable
systems--systems with more conserved quantities than degrees of freedom. In
this quantization method, the symmetry algebras of the hamiltonian invariants
are preserved most naturally, as illustrated on nonlinear -models,
specifically for Chiral Models and de Sitter -spheres. Classically, the
dynamics of superintegrable models such as these is automatically also
described by Nambu Brackets involving the extra symmetry invariants of them.
The phase-space quantization worked out then leads to the quantization of the
corresponding Nambu Brackets, validating Nambu's original proposal, despite
excessive fears of inconsistency which have arisen over the years. This is a
pedagogical talk based on hep-th/0205063 and hep-th/0212267, stressing points
of interpretation and care needed in appreciating the consistency of Quantum
Nambu Brackets in phase space. For a parallel discussion in Hilbert space, see
T Curtright's contribution in these Proceedings [hep-th 0303088].Comment: Invited talk by the first author at the Coral Gables Conference
(C02/12/11.2), Ft Lauderdale, Dec 2002. 14p, LateX2e, aipproc, amsfont
Quantum Mechanics in Phase Space
Ever since Werner Heisenberg's 1927 paper on uncertainty, there has been
considerable hesitancy in simultaneously considering positions and momenta in
quantum contexts, since these are incompatible observables. But this persistent
discomfort with addressing positions and momenta jointly in the quantum world
is not really warranted, as was first fully appreciated by Hilbrand Groenewold
and Jos\'e Moyal in the 1940s. While the formalism for quantum mechanics in
phase space was wholly cast at that time, it was not completely understood nor
widely known --- much less generally accepted --- until the late 20th century.Comment: A brief history of deformation quantization, ca 1930-1960, with some
elementary illustrations of the theor
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