Abstract

The dynamic dipole polarizabilities at real and imaginary frequencies have been determined for the helium atom in its lowest singlet and triplet 2P states, using our time-dependent gauge-invariant method. Contributions of the 2S states to static polarizabilities are strong and negative, particularly in the case of the singlet 2 $^{1}$P state, for which the static scalar polarizability ${\mathrm{\ensuremath{\alpha}}}_{0}$ is negative. The tensor polarizability ${\mathrm{\ensuremath{\alpha}}}_{2}$ corresponding to the differential Stark shift between the m Zeeman sublevels was also calculated and compared to previous theoretical and experimental results for the singlet 2 $^{1}$P state. An evaluation of the ${\mathit{C}}_{6}$ dispersion coefficients for the 2 $^{1}$P--2 $^{1}$P and 2 $^{3}$P--2 $^{3}$P systems is also given, derived from the dynamic polarizabilities at imaginary pulsations \ensuremath{\omega}.

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