1,542 research outputs found

    Hopf algebras and characters of classical groups

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    Schur functions provide an integral basis of the ring of symmetric functions. It is shown that this ring has a natural Hopf algebra structure by identifying the appropriate product, coproduct, unit, counit and antipode, and their properties. Characters of covariant tensor irreducible representations of the classical groups GL(n), O(n) and Sp(n) are then expressed in terms of Schur functions, and the Hopf algebra is exploited in the determination of group-subgroup branching rules and the decomposition of tensor products. The analysis is carried out in terms of n-independent universal characters. The corresponding rings, CharGL, CharO and CharSp, of universal characters each have their own natural Hopf algebra structure. The appropriate product, coproduct, unit, counit and antipode are identified in each case.Comment: 9 pages. Uses jpconf.cls and jpconf11.clo. Presented by RCK at SSPCM'07, Myczkowce, Poland, Sept 200

    Hermitian Young Operators

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    Starting from conventional Young operators we construct Hermitian operators which project orthogonally onto irreducible representations of the (special) unitary group.Comment: 15 page

    Parafermions, parabosons and representations of so(\infty) and osp(1|\infty)

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    The goal of this paper is to give an explicit construction of the Fock spaces of the parafermion and the paraboson algebra, for an infinite set of generators. This is equivalent to constructing certain unitary irreducible lowest weight representations of the (infinite rank) Lie algebra so(\infty) and of the Lie superalgebra osp(1|\infty). A complete solution to the problem is presented, in which the Fock spaces have basis vectors labelled by certain infinite but stable Gelfand-Zetlin patterns, and the transformation of the basis is given explicitly. We also present expressions for the character of the Fock space representations

    SU(3) Quantum Interferometry with single-photon input pulses

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    We develop a framework for solving the action of a three-channel passive optical interferometer on single-photon pulse inputs to each channel using SU(3) group-theoretic methods, which can be readily generalized to higher-order photon-coincidence experiments. We show that features of the coincidence plots vs relative time delays of photons yield information about permanents, immanants, and determinants of the interferometer SU(3) matrix

    Mixed Symmetry Solutions of Generalized Three-Particle Bargmann-Wigner Equations in the Strong-Coupling Limit

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    Starting from a nonlinear isospinor-spinor field equation, generalized three-particle Bargmann-Wigner equations are derived. In the strong-coupling limit, a special class of spin 1/2 bound-states are calculated. These solutions which are antisymmetric with respect to all indices, have mixed symmetries in isospin-superspin space and in spin orbit space. As a consequence of this mixed symmetry, we get three solution manifolds. In appendix \ref{b}, table 2, these solution manifolds are interpreted as the three generations of leptons and quarks. This interpretation will be justified in a forthcoming paper.Comment: 17 page

    Dipolar superfluidity in electron-hole bilayer systems

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    Bilayer electron-hole systems, where the electrons and holes are created via doping and confined to separate layers, undergo excitonic condensation when the distance between the layers is smaller than typical distance between particles within a layer. We argue that the excitonic condensate is a novel dipolar superfluid in which the phase of the condensate couples to the {\it gradient} of the vector potential. We predict the existence of dipolar supercurrent which can be tuned by an in-plane magnetic field and detected by independent contacts to the layers. Thus the dipolar superfluid offers an example of excitonic condensate in which the {\it composite} nature of its constituent excitons is manifest in the macroscopic superfluid state. We also discuss various properties of this superfluid including the role of vortices.Comment: 5 pages, 1 figure, minor changes and added few references; final published versio

    Energy evolution in time-dependent harmonic oscillator

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    The theory of adiabatic invariants has a long history, and very important implications and applications in many different branches of physics, classically and quantally, but is rarely founded on rigorous results. Here we treat the general time-dependent one-dimensional harmonic oscillator, whose Newton equation q¨+ω2(t)q=0\ddot{q} + \omega^2(t) q=0 cannot be solved in general. We follow the time-evolution of an initial ensemble of phase points with sharply defined energy E0E_0 at time t=0t=0 and calculate rigorously the distribution of energy E1E_1 after time t=Tt=T, which is fully (all moments, including the variance μ2\mu^2) determined by the first moment E1ˉ\bar{E_1}. For example, μ2=E02[(E1ˉ/E0)2(ω(T)/ω(0))2]/2\mu^2 = E_0^2 [(\bar{E_1}/E_0)^2 - (\omega (T)/\omega (0))^2]/2, and all higher even moments are powers of μ2\mu^2, whilst the odd ones vanish identically. This distribution function does not depend on any further details of the function ω(t)\omega (t) and is in this sense universal. In ideal adiabaticity E1ˉ=ω(T)E0/ω(0)\bar{E_1} = \omega(T) E_0/\omega(0), and the variance μ2\mu^2 is zero, whilst for finite TT we calculate E1ˉ\bar{E_1}, and μ2\mu^2 for the general case using exact WKB-theory to all orders. We prove that if ω(t)\omega (t) is of class Cm{\cal C}^{m} (all derivatives up to and including the order mm are continuous) μT(m+1)\mu \propto T^{-(m+1)}, whilst for class C{\cal C}^{\infty} it is known to be exponential μexp(αT)\mu \propto \exp (-\alpha T).Comment: 26 pages, 5 figure

    Integrity bases for local invariants of composite quantum systems

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    Unitary group branchings appropriate to the calculation of local invariants of density matrices of composite quantum systems are formulated using the method of SS-function plethysms. From this, the generating function for the number of invariants at each degree in the density matrix can be computed. For the case of two two-level systems the generating function is F(q)=1+q+4q2+6q3+16q4+23q5+52q6+77q7+150q8+224q9+396q10+583q11+O(q12)F(q) = 1 + q + 4q^{2} + 6 q^{3} + 16 q^{4} + 23 q^{5} + 52 q^{6} + 77 q^{7} + 150 q^{8} + 224 q^{9} + 396 q^{10} + 583 q^{11}+ O(q^{12}). Factorisation of such series leads in principle to the identification of an integrity basis of algebraically independent invariants. This note replaces Appendix B of our paper\cite{us} J Phys {\bf A33} (2000) 1895-1914 (\texttt{quant-ph/0001076}) which is incorrect.Comment: Latex, 4 pages, correcting Appendix B of quant-ph/0001076 Error in F(q)F(q) corrected and conclusions modified accordingl
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