0105143v1

related topics
{energy, state, states}
{vol, operators, histories}
{group, space, representation}
{spin, pulse, spins}
{energy, gaussian, time}
{force, casimir, field}
{equation, function, exp}
{level, atom, field}

Quantum algebraic symmetries in atomic clusters, molecules and nuclei

D. Bonatsos, N. Karoussos, P. P. Raychev, R. P. Roussev

abstract: Quantum algebras (also called quantum groups) are deformed versions of the usual Lie algebras, to which they reduce when the deformation parameter q is set equal to unity. From the mathematical point of view they are Hopf algebras. Their use in physics became popular with the introduction of the q-deformed harmonic oscillator as a tool for providing a boson realization of the quantum algebra SUq(2), although similar mathematical structures had already been known. Initially used for solving the quantum Yang-Baxter equation, quantum algebras have subsequently found applications in several branches of physics, as, for example, in the description of spin chains, squeezed states, hydrogen atom and hydrogen-like spectra, rotational and vibrational nuclear and molecular spectra, and in conformal field theories. By now much work has been done on the q-deformed oscillator and its relativistic extensions, and several kinds of generalized deformed oscillators and SU(2) algebras have been introduced. Here we shall confine ourselves to a list of applications of quantum algebras in nuclear structure physics and in molecular physics and, in addition, a recent application of quantum algebraic techniques to the structure of atomic clusters will be discussed in more detail.

oai_identifier:
oai:arXiv.org:quant-ph/0105143
categories:
quant-ph math-ph math.MP nucl-th physics.chem-ph
comments:
Plain TeX, 10 pages. Lecture given at the XXIII International Workshop on Condensed Matter Theories (Ithaca, Greece, 17-23/6/1999)
arxiv_id:
quant-ph/0105143
journal_ref:
Condensed Matter Theor. 15 (2000) 25
report_no:
DEM-NT-99-13
created:
2001-05-29

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