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Volumn 60, Issue 2, 1999, Pages 1420-1428

Strongly perturbed Stark states and electron correlation in Ba

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EID: 0004789944     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.60.1420     Document Type: Article
Times cited : (15)

References (21)
  • 7
    • 5344267644 scopus 로고
    • Phys. Rev. AD. A. Harmin26, 2656 (1982).
    • (1982) , vol.26 , pp. 2656
    • Harmin, D.A.1
  • 17
    • 85037189448 scopus 로고    scopus 로고
    • We note that all channels have K-matrix elements that are nonzero. However, the size of the K-matrix elements decreases very rapidly with the orbital angular momentum of the Rydberg electron. For the level of accuracy desired in a particular problem, there is an effective maximum orbital angular momentum where K-matrix elements for higher angular momentum may be set identically to zero without affecting the calculation
    • We note that all channels have K-matrix elements that are nonzero. However, the size of the K-matrix elements decreases very rapidly with the orbital angular momentum of the Rydberg electron. For the level of accuracy desired in a particular problem, there is an effective maximum orbital angular momentum where K-matrix elements for higher angular momentum may be set identically to zero without affecting the calculation.
  • 19
    • 84926802670 scopus 로고
    • U.S. GPO, Washington, DC
    • Atomic Energy Levels, edited by C. E. Moore, Natl. Bur. Stand. (U.S.) Circ. No. 467 (U.S. GPO, Washington, DC, 1949).
    • (1949) Atomic Energy Levels
  • 21
    • 85037232078 scopus 로고    scopus 로고
    • The singlet and triplet partial cross sections are well defined because once the electron leaves the atom there is no interaction that changes the spin coupling since the core is left in an s state
    • The singlet and triplet partial cross sections are well defined because once the electron leaves the atom there is no interaction that changes the spin coupling since the core is left in an s state.


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