2003
DOI: 10.1088/0305-4470/36/29/302
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The structure of operators in effective particle-conserving models

Abstract: For many-particle systems defined on lattices we investigate the global structure of effective Hamiltonians and observables obtained by means of a suitable basis transformation. We study transformations which lead to effective Hamiltonians conserving the number of excitations. The same transformation must be used to obtain effective observables.The analysis of the structure shows that effective operators give rise to a simple and intuitive perspective on the initial problem. The systematic calculation of n-par… Show more

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Cited by 127 publications
(226 citation statements)
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References 29 publications
(100 reference statements)
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“…The results for the Mott phase are obtained for commensurate filling n = 1. For fillings n = 1 the reference state used for normal ordering before truncation should ideally be the disordered state at the lower filling n [7,26]. This requires to redo the whole CUT for each n. But the effect of a different reference state is not very large if t/U is small.…”
Section: Resultsmentioning
confidence: 99%
“…The results for the Mott phase are obtained for commensurate filling n = 1. For fillings n = 1 the reference state used for normal ordering before truncation should ideally be the disordered state at the lower filling n [7,26]. This requires to redo the whole CUT for each n. But the effect of a different reference state is not very large if t/U is small.…”
Section: Resultsmentioning
confidence: 99%
“…To capture the zero temperature quantum fluctuations quantitatively we apply a continuous unitary transformation [30][31][32][33][34] that conserves the number of triplons in the system. To first order in the parameter α the effective Hamiltonian is given by…”
Section: Theory: Diagrammatic Brückner Approachmentioning
confidence: 99%
“…The original Hamiltonian H can be replaced with an effective one H eff which conserves the number of quasiparticles. The Hamiltonian H eff is obtained by continuous unitary transformation; that is, H eff = H(∞) (satisfying [H(∞), Q] = 0) 12,13 . Because of the conservation relation, one can rewrite…”
Section: Perturbative Continuous Unitary Transformation (Pcut)mentioning
confidence: 99%
“…(4) keeps only those processes that conserve the number of quasiparticles and eliminates all parts of H changing the number of quasiparticles 12,13 . To obtain a final diagonalized Hamiltonian, the number of energy quanta created or annihilated at ℓ → ∞ must be zero.…”
Section: Perturbative Continuous Unitary Transformation (Pcut)mentioning
confidence: 99%