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Volumn 54, Issue 6, 1996, Pages 4789-4801

Rydberg states about dipolar cores: The quantum dynamics of the long-range anisotropic interaction

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EID: 5544261147     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.54.4789     Document Type: Article
Times cited : (20)

References (73)
  • 14
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    • Adv. Chem. Phys. (to be published)
    • R. D. Levine, Adv. Chem. Phys. (to be published).
    • Levine, R.D.1
  • 30
    • 0004285220 scopus 로고
    • Cambridge University Press, Cambridge
    • T. F. Gallagher, Rydberg Atoms (Cambridge University Press, Cambridge, 1994).
    • (1994) Rydberg Atoms
    • Gallagher, T.F.1
  • 42
    • 85037178027 scopus 로고    scopus 로고
    • The extra power of r causes a quadratically faster decrease of the matrix elements with l, as can be seen from the analytical expression 31 of the radial diagonal matrix elements of (Formula presented)
    • The extra power of r causes a quadratically faster decrease of the matrix elements with l, as can be seen from the analytical expression 31 of the radial diagonal matrix elements of (Formula presented).
  • 43
    • 85037204380 scopus 로고    scopus 로고
    • See Ref. 31, Sec. 60, Eqs. (60.7) and (60.11) in particular
    • See Ref. 31, Sec. 60, Eqs. (60.7) and (60.11) in particular.
  • 53
    • 85037241715 scopus 로고    scopus 로고
    • The distance of closest approach at high n's is l(l+1)/2
    • The distance of closest approach at high n's is l(l+1)/2.
  • 54
    • 85037199284 scopus 로고    scopus 로고
    • When, for a neutral molecule, additional, dipole bound states are possible 55,56
    • When, for a neutral molecule, additional, dipole bound states are possible 55,56.
  • 58
    • 85037188701 scopus 로고    scopus 로고
    • Since the difference between the two-density of states is a function of the rotational constant B of the core, we can use one coupling constant and B
    • Since the difference between the two-density of states is a function of the rotational constant B of the core, we can use one coupling constant and B.
  • 59
    • 85037219949 scopus 로고    scopus 로고
    • The only way to further increase the density of accessible states is to break M as a good quantum number by imposition of an external magnetic field 17–19 or by the presence of other ions 12,20,23
    • The only way to further increase the density of accessible states is to break M as a good quantum number by imposition of an external magnetic field 17–19 or by the presence of other ions 12,20,23.
  • 60
    • 85037200519 scopus 로고    scopus 로고
    • To see the transition from local to average behavior of the coupling constant, consider the density of states within a Stark manifold. Then δE=3nF. At the Inglis-Teller limit γ=(Formula presented)
    • To see the transition from local to average behavior of the coupling constant, consider the density of states within a Stark manifold. Then δE=3nF. At the Inglis-Teller limit γ=(Formula presented).
  • 61
    • 85037216366 scopus 로고    scopus 로고
    • The variation in the weight from one eigenstate to another is what one would expect for quantum fluctuations in the strong-coupling limit in the two-series problem 62
    • The variation in the weight from one eigenstate to another is what one would expect for quantum fluctuations in the strong-coupling limit in the two-series problem 62.
  • 65
    • 85037184047 scopus 로고    scopus 로고
    • This means that the Hamiltonian is symmetric and can be diagonalized by an orthogonal transformation, unlike the situation when the continuum is energetically accessible. One can then use an effective Hamiltonian within the bound subspace 63,64, which needs to be diagonalized in a biorthogonal basis
    • This means that the Hamiltonian is symmetric and can be diagonalized by an orthogonal transformation, unlike the situation when the continuum is energetically accessible. One can then use an effective Hamiltonian within the bound subspace 63,64, which needs to be diagonalized in a biorthogonal basis.
  • 68
    • 85037183713 scopus 로고    scopus 로고
    • This delay is necessary to remove the promptly produced ions
    • This delay is necessary to remove the promptly produced ions.
  • 70
  • 73
    • 84935857484 scopus 로고    scopus 로고
    • Ann. Phys. 2, 1031 (Leipzig) (1929)
    • W. Gordon, Ann. Phys. 2, 1031 (Leipzig) (1929).
    • Gordon, W.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.