2009
DOI: 10.1007/s00023-009-0417-9
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Analytic Perturbation Theory and Renormalization Analysis of Matter Coupled to Quantized Radiation

Abstract: Abstract.For a large class of quantum mechanical models of matter and radiation we develop an analytic perturbation theory for non-degenerate ground states. This theory is applicable, for example, to models of matter with static nuclei and non-relativistic electrons that are coupled to the UV-cutoff quantized radiation field in the dipole approximation. If the lowest point of the energy spectrum is a non-degenerate eigenvalue of the Hamiltonian, we show that this eigenvalue is an analytic function of the nucle… Show more

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Cited by 41 publications
(67 citation statements)
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“…In Appendix A we recall some properties of the Feshbach-Schur map and in Appendix B we prove the main result of Section VI. The results of both appendices are close to certain results from [4,34,29], but there are a few important differences. The main ones are that we have to deal with unbounded interactions and, more importantly, with momentum-anisotropic spaces.…”
Section: Discussionsupporting
confidence: 74%
See 1 more Smart Citation
“…In Appendix A we recall some properties of the Feshbach-Schur map and in Appendix B we prove the main result of Section VI. The results of both appendices are close to certain results from [4,34,29], but there are a few important differences. The main ones are that we have to deal with unbounded interactions and, more importantly, with momentum-anisotropic spaces.…”
Section: Discussionsupporting
confidence: 74%
“…As was mentioned in Section VII, the proof follows the lines of the proof of Theorem IV.3 of [29] (cf. Theorem 3.8 of [4] and Theorem 28 of [34]). It is similar to the proofs of related results of [10,11].…”
Section: Appendix B Proof Of Theorem Vii1mentioning
confidence: 96%
“…(A.4) The function ω is continuous on R ν with lim |k|→∞ ω(k) = ∞ and there exist constants γ > 0 and C > 0 such that 12) where n 0 := max{n ≥ 0|E n < E 0 + ω 0 }. In particular, if the boson is massless, then σ(H 0 ) = [E 0 , ∞), which shows that all the eigenvalues of H 0 are embedded eigenvalues of H 0 .…”
Section: Remark 52mentioning
confidence: 99%
“…For the latter, Bach, Fröhlich and Sigal [8,9]) have developed a method exploring a renormalization group idea combined with the Feshbach map. Recently analyticity in the coupling constant for the ground state energy 1 for some concrete models of massless quantum fields (in which the ground state energy of the unperturbed system under consideration is an embedded eigenvalue) has been proved [1,2,12,13]. These results are very nice, but, they may be model-dependent.…”
Section: Introductionmentioning
confidence: 99%
“…This generalization is needed, for example, in the analysis of resonances, and in the perturbation theory of the ground state of models of matter and quantized radiation [4,6]. In the course of modifying the proof of Theorem II.1 [3], we closely examined all of its parts.…”
Section: Introductionmentioning
confidence: 98%