[1] Bauche J, Arnoult C B, Klapisch M. Transition arrays in the spectra of ionized atoms[J]. Advances in Atomic and Molecular Physics, 1987, 23: 131.
[2] Colombant D, Klapisch M, Bar-Shalom A. Increase in Rosseland mean opacity for inertial fusion hohlraum walls[J]. Phys. Rev. E, 1998, 57 (3, Part B): 3411.
[3] Joseph Abdallah Jr, Robert E H Clark. X-ray transmission calculations for an aluminum plasma[J]. Appl. Phys., 1991, 69: 23.
[4] Wang P, MacFarlane J J, Orzechowski T J. An investigation of the opacity of high-Z mixture and implications for inertial confinement fusion hohlraum design[J]. Rev. Sci. Instrum., 1997, 68 (1): 1107.
[5] Yan J, Wu Z Q, Pang J Q, et al. Theoretical study of the opacity for mixture at high temperture[J]. Phys. Rev. Lett., 2002, 19 (6): 818.
[6] Rozsnyai B F. Relativistic hartree-fock-slater calculations for arbitrary temperature and matter density[J]. Phys. Rev. A, 1972, 5(3): 1137.
[7] Perrot F. Fast calculation of electronic structure in plasmas: the screened hydrogenic model with L-splitting[J]. Physica spcripta, 1989, 39 (3): 332.
[8] Rickert A, Meyer-ter-vehn J. Frequency-dependent opacity calculations for light-Z plasma including splitting[J]. Laser and Particle Beams, 1990, 8 (4): 715.
[9] 闫安英, 姜明, 程新路, 等. Au混合物Rosseland平均不透明度的计算[J].核聚变与等离子体物理, 2006, 26(1): 42.
[10] Rosseland S. Note on the absorption of radiation within a star[J]. Mon. Not. R. Astron. Soc., 1924, 84(7): 525. |