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Second order per- turbation theory J er emy Faupin Regular Mourre On second order perturbation theory for embedded theory eigenvalues Nelson model Singular Mourre theory J er emy Faupin References Institut de Math


  1. Second order per- turbation theory J´ er´ emy Faupin Regular Mourre On second order perturbation theory for embedded theory eigenvalues Nelson model Singular Mourre theory J´ er´ emy Faupin References Institut de Math´ ematiques de Bordeaux Universit´ e de Bordeaux 1 Joint work with J.S. Møller and E. Skibsted 1 / 25

  2. Second order per- turbation Outline of the talk theory J´ er´ emy Faupin Regular Mourre theory Nelson 1 Regular Mourre theory with a self-adjoint conjugate operator model Singular Mourre theory References 2 The Nelson model 3 Singular Mourre theory with a non self-adjoint conjugate operator 2 / 25

  3. Second order per- turbation theory J´ er´ emy Faupin Regular Mourre theory Nelson model Part I Singular Mourre theory Regular Mourre theory with References a self-adjoint conjugate operator 3 / 25

  4. Second order per- turbation Regularity w.r.t. a self-adjoint operator theory J´ er´ emy Faupin • H complex Hilbert space Regular • H , A self-adjoint operators on H Mourre theory Nelson Definition model Singular Let n ∈ N . We say that H ∈ C n ( A ) if and only if ∀ z ∈ C \ σ ( H ), ∀ φ ∈ H , Mourre theory s �→ e isA ( H − z ) − 1 e − isA φ ∈ C n ( R ) References Remarks • H ∈ C 1 ( A ) if and only if ∀ z ∈ C \ σ ( H ), ( H − z ) − 1 D ( A ) ⊆ D ( A ), and ∀ φ ∈ D ( H ) ∩ D ( A ), |� A φ, H φ � − � H φ, A φ �| ≤ C ( � H φ � 2 + � φ � 2 ) • If H ∈ C 1 ( A ), then D ( H ) ∩ D ( A ) is a core for H , and the quadratic form [ H , A ] defined on ( D ( H ) ∩ D ( A )) × ( D ( H ) ∩ D ( A )) extend by continuity to a bounded quadratic form on D ( H ) × D ( H ) denoted [ H , A ] 0 4 / 25

  5. Second order per- turbation Regularity w.r.t. a self-adjoint operator theory J´ er´ emy Faupin • H complex Hilbert space Regular • H , A self-adjoint operators on H Mourre theory Nelson Definition model Singular Let n ∈ N . We say that H ∈ C n ( A ) if and only if ∀ z ∈ C \ σ ( H ), ∀ φ ∈ H , Mourre theory s �→ e isA ( H − z ) − 1 e − isA φ ∈ C n ( R ) References Remarks • H ∈ C 1 ( A ) if and only if ∀ z ∈ C \ σ ( H ), ( H − z ) − 1 D ( A ) ⊆ D ( A ), and ∀ φ ∈ D ( H ) ∩ D ( A ), |� A φ, H φ � − � H φ, A φ �| ≤ C ( � H φ � 2 + � φ � 2 ) • If H ∈ C 1 ( A ), then D ( H ) ∩ D ( A ) is a core for H , and the quadratic form [ H , A ] defined on ( D ( H ) ∩ D ( A )) × ( D ( H ) ∩ D ( A )) extend by continuity to a bounded quadratic form on D ( H ) × D ( H ) denoted [ H , A ] 0 4 / 25

  6. Second order per- turbation Regularity w.r.t. a self-adjoint operator theory J´ er´ emy Faupin • H complex Hilbert space Regular • H , A self-adjoint operators on H Mourre theory Nelson Definition model Singular Let n ∈ N . We say that H ∈ C n ( A ) if and only if ∀ z ∈ C \ σ ( H ), ∀ φ ∈ H , Mourre theory s �→ e isA ( H − z ) − 1 e − isA φ ∈ C n ( R ) References Remarks • H ∈ C 1 ( A ) if and only if ∀ z ∈ C \ σ ( H ), ( H − z ) − 1 D ( A ) ⊆ D ( A ), and ∀ φ ∈ D ( H ) ∩ D ( A ), |� A φ, H φ � − � H φ, A φ �| ≤ C ( � H φ � 2 + � φ � 2 ) • If H ∈ C 1 ( A ), then D ( H ) ∩ D ( A ) is a core for H , and the quadratic form [ H , A ] defined on ( D ( H ) ∩ D ( A )) × ( D ( H ) ∩ D ( A )) extend by continuity to a bounded quadratic form on D ( H ) × D ( H ) denoted [ H , A ] 0 4 / 25

  7. Second order per- turbation Mourre estimate theory J´ er´ emy Faupin Definition Regular Mourre Let I be a bounded open interval, I ⊂ σ ( H ). We say that H satisfies a Mourre theory estimate on I with A as conjugate operator if ∃ c 0 > 0 and K 0 compact such Nelson model that Singular 1 I ( H )[ H , iA ] 0 1 I ( H ) ≥ c 0 1 I ( H ) − K 0 , Mourre theory in the sense of quadratic forms on H × H References Remarks • An equivalent formulation is [ H , iA ] 0 ≥ c ′ 0 − c ′ 1 1 R \ I ( H ) � H � − K ′ 0 , in the sense of quadratic forms on D ( H ) × D ( H ), with c ′ 0 > 0, c ′ 1 ∈ R , and K ′ 0 compact • If K 0 = 0, we say that H satisfies a strict Mourre estimate on I 5 / 25

  8. Second order per- turbation Mourre estimate theory J´ er´ emy Faupin Definition Regular Mourre Let I be a bounded open interval, I ⊂ σ ( H ). We say that H satisfies a Mourre theory estimate on I with A as conjugate operator if ∃ c 0 > 0 and K 0 compact such Nelson model that Singular 1 I ( H )[ H , iA ] 0 1 I ( H ) ≥ c 0 1 I ( H ) − K 0 , Mourre theory in the sense of quadratic forms on H × H References Remarks • An equivalent formulation is [ H , iA ] 0 ≥ c ′ 0 − c ′ 1 1 R \ I ( H ) � H � − K ′ 0 , in the sense of quadratic forms on D ( H ) × D ( H ), with c ′ 0 > 0, c ′ 1 ∈ R , and K ′ 0 compact • If K 0 = 0, we say that H satisfies a strict Mourre estimate on I 5 / 25

  9. Second order per- turbation The Virial Theorem theory J´ er´ emy Faupin Regular Mourre theory Nelson Theorem ([Mo ’81], [ABG ’96], [GG ’99]) model Let φ be an eigenstate of H . If H ∈ C 1 ( A ), then Singular Mourre theory � φ, [ H , iA ] 0 φ � = 0 References Corollary Assume that H ∈ C 1 ( A ) and that H satisfies a Mourre estimate on I . Then the number of eigenvalues of H in I is finite, and each such eigenvalue has a finite multiplicity 6 / 25

  10. Second order per- turbation The Virial Theorem theory J´ er´ emy Faupin Regular Mourre theory Nelson Theorem ([Mo ’81], [ABG ’96], [GG ’99]) model Let φ be an eigenstate of H . If H ∈ C 1 ( A ), then Singular Mourre theory � φ, [ H , iA ] 0 φ � = 0 References Corollary Assume that H ∈ C 1 ( A ) and that H satisfies a Mourre estimate on I . Then the number of eigenvalues of H in I is finite, and each such eigenvalue has a finite multiplicity 6 / 25

  11. Second order per- turbation Limiting Absorption Principle theory J´ er´ emy Faupin Theorem ([Mo ’81], [ABG ’96], [Ge ’08]) Regular Assume that H ∈ C 2 ( A ) and that H satisfies a strict Mourre estimate on I . Mourre theory Then for all closed interval J ⊂ I and s > 1 / 2, Nelson model z ∈ J ± �� A � − s ( H − z ) − 1 � A � − s � < ∞ , sup Singular Mourre theory where J ± = { z ∈ C , Re z ∈ J , ± Im z > 0 } and � A � = (1 + A 2 ) 1 / 2 . In References particular the spectrum of H in I is purely absolutely continuous. Moreover for 1 / 2 < s ≤ 1, the maps J ± ∋ z �→ �� A � − s ( H − z ) − 1 � A � − s � ∈ B ( H ) are H¨ older continuous of order s − 1 / 2. In particular, for λ ∈ J , the limits � A � − s ( H − λ ± i 0) − 1 � A � − s := lim ǫ ↓ 0 � A � − s ( H − λ ± i ǫ ) − 1 � A � − s exist in the norm topology of B ( H ), and the corresponding functions of λ are H¨ older continuous of order s − 1 / 2 7 / 25

  12. Second order per- turbation Fermi Golden Rule criterion theory J´ er´ emy Theorem ([AHS ’89], [HuSi ’00]) Faupin Suppose Regular Mourre theory 1) (Regularity of H ) H ∈ C 2 ( A ) and the quadratic forms [ H , iA ] and Nelson [[ H , iA ] , iA ] extend by continuity to H -bounded operators model 2) (Mourre estimate) H satisfies a Mourre estimate on I Singular Mourre theory Let λ ∈ I be an eigenvalue of H . Let P = 1 { λ } ( H ) be the associated eigenprojection and ¯ References P = I − P . Let J ⊂ I be a closed interval such that σ pp ( H ) ∩ J = { λ } . Let W be a symmetric and H -bounded operator. Suppose 3) (Regularity of eigenstates) Ran ( P ) ⊆ D ( A 2 ) 4) (Regularity of the perturbation) [ W , iA ] and [[ W , iA ] , iA ] extend by continuity to H -bounded operators If the Fermi Golden Rule criterion is satisfied, i.e. PW Im (( H − λ − i 0) − 1 ¯ P ) WP ≥ cP with c > 0, then ∃ σ 0 > 0 such that ∀ 0 < | σ | ≤ σ 0 , σ pp ( H + σ W ) ∩ J = ∅ 8 / 25

  13. Second order per- turbation Regularity of bound states theory J´ er´ emy Faupin Regular Mourre theory Theorem ([Ca ’05], [CGH ’06]) Nelson model Let n ∈ N . Assume that H ∈ C n +2 ( A ) and that ad k A ( H ) are H -bounded for all Singular 1 ≤ k ≤ n + 2. Assume that H satisfies a Mourre estimate on I . Let λ ∈ I be Mourre theory an eigenvalue of H and let P = 1 { λ } ( H ) be the associated eigenprojection. References Then we have that Ran ( P ) ⊆ D ( A n ) Remark In fact H ∈ C n +1 ( A ) is sufficient for the conclusion of the previous theorem to hold and this is optimal ([FMS’ 10], [MW’ 10]). 9 / 25

  14. Second order per- turbation Regularity of bound states theory J´ er´ emy Faupin Regular Mourre theory Theorem ([Ca ’05], [CGH ’06]) Nelson model Let n ∈ N . Assume that H ∈ C n +2 ( A ) and that ad k A ( H ) are H -bounded for all Singular 1 ≤ k ≤ n + 2. Assume that H satisfies a Mourre estimate on I . Let λ ∈ I be Mourre theory an eigenvalue of H and let P = 1 { λ } ( H ) be the associated eigenprojection. References Then we have that Ran ( P ) ⊆ D ( A n ) Remark In fact H ∈ C n +1 ( A ) is sufficient for the conclusion of the previous theorem to hold and this is optimal ([FMS’ 10], [MW’ 10]). 9 / 25

  15. Second order per- turbation theory J´ er´ emy Faupin Regular Mourre theory Nelson model Part II Singular Mourre theory The Nelson model References 10 / 25

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