M. G. Kozlov

Blackbody-radiation shift in the Sr optical atomic clock

We evaluated the static and dynamic polarizabilities of the

Development of a configuration-interaction plus all-order method for atomic calculations

5{s}^{2}phantom{rule{0.16em}{0ex}}{}^{1}{S}_{0}

Parity nonconservation in thallium

and

Electric dipole moment enhancement factor of thallium.

5s5pphantom{rule{0.16em}{0ex}}{}^{3}{P}_{0}^{o}

Precision Calculation of Blackbody Radiation Shifts for Optical Frequency Metrology

states of Sr using the high-precision relativistic configuration interaction combined with the all-order method. Our calculation explains the discrepancy between the recent experimental

High-precision calculations of In I and Sn II atomic properties

5{s}^{2}phantom{rule{0.16em}{0ex}}{}^{1}{S}_{0}ensuremath{-}5s5pphantom{rule{0.16em}{0ex}}{}^{3}{P}_{0}^{o}

Black-body radiation shifts and theoretical contributions to atomic clock research

dc Stark shift measurement

Correlation effects in Yb + and implications for parity violation

ensuremath{Delta}ensuremath{alpha}=247.379(7)

Blackbody radiation shifts in optical atomic clocks

[Middelmann et al., Phys. Rev. Lett. 109, 263004 (2012)] and the earlier theoretical result of 261(4) a.u. [Porsev and Derevianko, Phys. Rev. A 74, 020502(R) (2006)]. Our present value of 247.5 a.u. is in excellent agreement with the experimental result. We also evaluated the dynamic correction to the BBR shift with 1

Polarizabilities of Si 2+ : A benchmark test of theory and experiment

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