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Linked-Cluster Expansions for the Nuclear Many-Body Problem
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Citations
155
References
1967
Year
Spectral TheoryTransition-amplitude ExpansionsEngineeringNuclear PhysicsLinked-cluster ExpansionsStatistical Field TheoryQuantum MaterialsQuantum TheoryGoldstone ExpansionCluster ScienceQuantum SciencePhysicsQuantum Field TheoryNuclear TheoryQuantum ChemistryCondensed Matter TheoryPerturbation TheoryNatural SciencesApplied PhysicsCondensed Matter PhysicsNuclear Many-body PhysicsMany-body Problem
The Goldstone expansion is rederived from Brillouin‑Wigner perturbation theory using elementary time‑independent methods, and similar algebraic techniques yield linked expansions for the total wave function (Hugenholtz) and general operator expectation values (Thouless). The authors propose the linked‑cluster expansions as a tool for studying superfluid phenomena in nuclear matter and connecting to Landau Fermi‑liquid theory, while also addressing the definition of the shell‑model potential and presenting a specific.
The Goldstone expansion is rederived by elementary time-independent methods, starting from Brillouin-Wigner (BW) perturbation theory. Interaction energy terms $\ensuremath{\Delta}E$ are expanded out of the BW energy denominators, and the series is then rearranged to obtain the linked-cluster result. Similar algebraic methods lead to the linked expansions for the total wave function (Hugenholtz) and the expectation value of a general operator (Thouless). Starting again with a degenerate version of BW perturbation theory, these methods are used to obtain the Bloch-Horowitz energy expansion, as well as the corresponding wave function, expectation-value, and transition-amplitude expansions. A "reduced" form of the Block-Horowitz expansion is described, and also a "completely linked" version. The latter is suggested as a tool for investigating superfiuid phenomena in nuclear matter, and for establishing contact with the Landau theory of Fermi liquids. The physical interpretation of these expansions is carefully studied, especially with regard to nuclear applications, to determine how they handle such "physical" features as antisymmetry, self-energy effects, wave-function renormalizations, and the distinction between "true" and "model" single-particle occupation probabilities. The problem of a correct theoretical definition for the shell-model potential is carefully examined, and a specific theory is presented. These expansions are seen to form a convenient and very powerful set of tools for studying the structure of actual nuclei.
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