P. G. Burkhalter, Leonard Cohen, Robert D. Cowan, and U. Feldman, "L-series satellite spectra in Ti xii and Fe xvi," J. Opt. Soc. Am. 69, 1133-1140 (1979)
Transitions in Na-like Ti and Fe ions, which appears as satellites to 2p-3s and 2p-3d transitions in Ne-like ions, were studied. The soft x-ray spectra produced by a focused-laser source and a vacuum-spark device were obtained with the same grazing-incidence spectrograph. Atomic structure calculations agreed with the observed 2p-3s spectral patterns and made possible line identifications in Ti xii and Fe xvi.
S. Ya. Khakhalin, V. M. Dyakin, A. Ya. Faenov, H. Fiedorowicz, A. Bartnik, P. Parys, A. L. Osterheld, and J. Nilsen J. Opt. Soc. Am. B 12(7) 1203-1210 (1995)
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The symbols J and J′ represent the total angular momentum of the lower and upper levels, respectively. The symbol E′ is the theoretical eigenvalue of the upper configuration.
Abbreviated notation (1/2,1P1) in place of 2p52P1/2, (3s3p) 1P1. The coefficient is the square of the eigenvector component for the indicated basis state; only the most important basis state is listed.
nd means not detected, sh means shoulder.
TABLE II
Experimental and calculated values for Na- and Mg-like transitions in Fe
The symbols J and J′ represent the total angular momentum of the lower and upper levels, respectively. The symbol E′ is the theoretical eigenvalue of the upper configuration.
Abbreviated notation (1/2,1P2) in place of 2p52P1/2,(3s3p)1P1. The coefficient is the square of the eigenvector component for the indicated basis state; only the most important basis state is listed.
nd means not detected.
Composition in LS coupling for both the lower and upper levels listed for Fe xv transitions.
Tables (2)
TABLE I
Experimental (exp) and calculated (calc) values for Na-like transitions in Ti xii
The symbols J and J′ represent the total angular momentum of the lower and upper levels, respectively. The symbol E′ is the theoretical eigenvalue of the upper configuration.
Abbreviated notation (1/2,1P1) in place of 2p52P1/2, (3s3p) 1P1. The coefficient is the square of the eigenvector component for the indicated basis state; only the most important basis state is listed.
nd means not detected, sh means shoulder.
TABLE II
Experimental and calculated values for Na- and Mg-like transitions in Fe
The symbols J and J′ represent the total angular momentum of the lower and upper levels, respectively. The symbol E′ is the theoretical eigenvalue of the upper configuration.
Abbreviated notation (1/2,1P2) in place of 2p52P1/2,(3s3p)1P1. The coefficient is the square of the eigenvector component for the indicated basis state; only the most important basis state is listed.
nd means not detected.
Composition in LS coupling for both the lower and upper levels listed for Fe xv transitions.