R. K. Gardner, C. L. Cocke, T. K. Saylor, and B. Curnutte, "Lifetimes of some L-x-ray emitting levels in silicon, sulfur, and chlorine*," J. Opt. Soc. Am. 68, 830-835 (1978)
Lifetimes of several L -x-ray emitting levels in neon-like, fluorine-like, and oxygen-like sulfur and chlorine and in lithium-like and beryllium-like silicon have been measured. While L x rays from these levels have been previously observed, no prior measurements of decay curves for these transitions have been reported. The lifetimes as inferred from the measured decay curves are compared to calculated lifetimes.
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Calculated using the computer program given in Ref. 5. Fluorine-like case in intermediate coupling.
See Reference 4.
Nonrelativistic Hartree-Fock calculations, except as noted.
See Ref. 8.
See Ref. 2.
Relative intensity of fast decay to slow decay; at excitation point.
Calculated using the computer program given in Ref. 5. Fluorine-like case in intermediate coupling.
See Ref. 4.
Nonrelativistic Hartree-Fock calculations, except as noted.
See Ref. 8.
Relative intensity of fast decay to slow decay, at excitation point.
Calculated using the computer progam given in Ref. 5.
See Ref. 4.
Nonrelativistic Hartree-Fock calculations, except as noted.
Relative intensity of fast decay to slow decay, at excitation point.
See Ref. 8.
Not reliable, because of resolving time.
Calculated using the computer program given in Ref. 5. Fluorine-like case in intermediate coupling.
See Reference 4.
Nonrelativistic Hartree-Fock calculations, except as noted.
See Ref. 8.
See Ref. 2.
Relative intensity of fast decay to slow decay; at excitation point.
Calculated using the computer program given in Ref. 5. Fluorine-like case in intermediate coupling.
See Ref. 4.
Nonrelativistic Hartree-Fock calculations, except as noted.
See Ref. 8.
Relative intensity of fast decay to slow decay, at excitation point.
Calculated using the computer progam given in Ref. 5.
See Ref. 4.
Nonrelativistic Hartree-Fock calculations, except as noted.
Relative intensity of fast decay to slow decay, at excitation point.
See Ref. 8.
Not reliable, because of resolving time.