Qed Calculation of Heavy Multicharged Ions With Account for Correlation, Radiative and Nuclear Effects

SENSING THE OPTIMAL PLASMA PARAMETERS FOR X-RAY LASING: CALCULATION OF ELECTRON-COLLISION STRENGTHS FOR Ar-LIKE PLASMA

“…The expression for the cross-section of the collisional excited-excited IK-IF transition can be found in [13]. The details of the whole numerical procedure of calculation of the collisional crosssection and strength can be found in [11][12][13][14][15][16][17]. It is worthwhile to indicate that the energy approach with using the optimal one-electron basis of PT first is used by us for description of elementary electron processes in collisionally pumped plasma.…”

“…It bases on the gauge invariant QED energy approach to construsction of the relativictic functions basis s [15,16] and using the Green s function method for accounting of the complex exchange-correlation, radiation and others corrections. Within the Gell-Mann and Low approach with the QED scattering matrix (c.f.…”

“…Usually the experimental one-quasi-particle energies are used for determination of parameters of the model potential (c.f. [8][9][10]15,16]). …”

“…In the zeroth order of QED PT we use the one-electron bare potential V N (r) + V C (r) . The core potential V C (r) is related to the core electron density r C (r) in a standard way [15,16]. Moreover, all the results of the approximate calculations are the functionals of the density r C (r).…”

An Advanced Laser Photoionization Separation Scheme for Radioactive Isotopes and Products of Atomic Energetics: Uranium and the Transuranium Elementsv.

“…This issue is being dedicated to a great number of works, because, obviously, the fundamental solution to the problem of destruction of long-lived radioactive waste fission products from spent nuclear fuel will undoubtedly contribute to further development of safe nuclear energy. In a light of saying, the effective technologies of detection and separation of the heavy radioactive isotopes are critically important [1][2][3][4][5][6][7][8][9][10]. The basis for its successful realization is, at first, carrying out the optimal multi stepped photo-ionization schemes for different elements and, at second, availability of enough effective UV and visible range lasers with high average power (Letokhov, 1977(Letokhov, , 1979(Letokhov, , 1983etc) [2,3].…”