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B-param eters ofthe com plete set ofm atrix elem ents ofB = 2 operators from the lattice

D. Berevi

Published Jan 1, 2001• 0 citations
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Using a family of coherent state representations we obtain in a natural and coordinate independent wayan explicit realization of a projective unitary representation of the symplectic group. Dequantization of these operators gives us the corresponding classical functions.

Ingrid C. Daubechies, Theoretische Natuurkunde

cause the substitution has taken us out of it) is, up to some constant factor, a unitary operator. The family of these oper­ ators gives us our projective representation. We work with intrinsic and coordinate-free notations differing from the no­ tations used in Refs. 2, 3, or 4. At the end of the paper we rewrite some of the results in the more familiar x-p notations. Following the prescription given in Ref. 11 for the de­ quantization of these operators, we proceed then to compute the classical functions corresponding to the symplectic transformations. This calculation of classical functions for symplectic transformations has been done for one-param­ eter subgroups of the symplectic group.8.9 One then only

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Strengthened Hyper-Raman Lines with the Coherent Superposition State

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当在它的地面 andfirst 之间的协调重叠使状态激动,从与起始的状态计算的一个维的库仑潜在的 atomare 的高顺序的泛音代准备了。当二个状态的精力差别是小的时,我们装 shoose properlaser 脉搏以便第一个激动的状态能相反对另外的界限状态仅仅激动 ofbeing 电离了。我们证明仅仅 hyper-Raman 线是看得见的而不是泛音。地面和第一个激动的状态的 Theenergy 差别能从最高的山峰 ofthe hyper-Raman 线被推出。我们进一步证明类似的结果能被使用二激光脉搏的 acombination,不同频率开始与原子交往获得 atthe 地面状态。

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Short‐range ±J interaction Ising spin glass in a transverse field on a Bethe lattice: a quantum‐spherical approach

T. K. Kopeć, Klaus D. Usadel

Abstract We consider the short‐range interaction disordered quantum Ising model with symmetric binary ±J bond distribution on the Bethe lattice (with coordination number z). The system exhibits quantum phase transition separating the spin glass and disordered phases where the quantum effect are regulated by a param‐ eter Δ describing the transverse field. By introducing a mapping of the quantum Hamiltonian of the model onto a soft‐spin action we consider it truncated version in a form of the solvable quantized spherical model. Quantum dynamics is examined via various correlation functions on the infinite tree which are evaluated in a closed form. (© 2006 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)

physica status solidi (b)•Dec 8, 2005•10 citations
cause the substitution has taken us out of it) is, up to some constant factor, a unitary operator. The family of these oper­ ators gives us our projective representation. We work with intrinsic and coordinate-free notations differing from the no­ tations used in Refs. 2, 3, or 4. At the end of the paper we rewrite some of the results in the more familiar x-p notations. Following the prescription given in Ref. 11 for the de­ quantization of these operators, we proceed then to compute the classical functions corresponding to the symplectic transformations. This calculation of classical functions for symplectic transformations has been done for one-param­ eter subgroups of the symplectic group.8.9 One then only
当在它的地面 andfirst 之间的协调重叠使状态激动,从与起始的状态计算的一个维的库仑潜在的 atomare 的高顺序的泛音代准备了。当二个状态的精力差别是小的时,我们装 shoose properlaser 脉搏以便第一个激动的状态能相反对另外的界限状态仅仅激动 ofbeing 电离了。我们证明仅仅 hyper-Raman 线是看得见的而不是泛音。地面和第一个激动的状态的 Theenergy 差别能从最高的山峰 ofthe hyper-Raman 线被推出。我们进一步证明类似的结果能被使用二激光脉搏的 acombination,不同频率开始与原子交往获得 atthe 地面状态。
Abstract We consider the short‐range interaction disordered quantum Ising model with symmetric binary ±J bond distribution on the Bethe lattice (with coordination number z). The system exhibits quantum phase transition separating the spin glass and disordered phases where the quantum effect are regulated by a param‐ eter Δ describing the transverse field. By introducing a mapping of the quantum Hamiltonian of the model onto a soft‐spin action we consider it truncated version in a form of the solvable quantized spherical model. Quantum dynamics is examined via various correlation functions on the infinite tree which are evaluated in a closed form. (© 2006 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)