We compute the reduced electric-dipole matrix elements〈 n S 1/2|| D|| n′ PJ〉 with n= 6, 7
and n′= 6, 7,..., 12 in cesium using the most complete to date ab initio relativistic coupled …

Our improved calculation of the nuclear spin-independent parity violating electric dipole
transition amplitude (E 1 PV) for 6 s S 2 1/2-7 s S 2 1/2 in Cs 133 in combination with the …

Using recent high-precision measurements of electric dipole matrix elements of atomic
cesium, we make an improved determination of the scalar (α) and vector (β) polarizabilities …

Motivated by recent measurements for several alkali-metal atoms and alkali-metal-like ions,
we perform a detailed study of electric dipole (E 1) transition amplitudes in K, Ca+, Rb, Sr+ …

We use the radiative potential method to perform a detailed study of quantum
electrodynamics (QED) radiative corrections to electric dipole (E1) transition amplitudes in …

We consider the implications of the recent measurement of the W-boson mass MW=
80,433.5±9.4 MeV/c 2 for atomic parity violation experiments. We show that the change in …

We report measurements of the electric dipole matrix elements of the Cs 133 6 s S 1/2 2→ 7
p P 1/2 2 and 6 s S 1/2 2→ 7 p P 3/2 2 transitions. Each of these determinations is based on …

We demonstrate the state-of-the-art technique of an active clock to provide a continuous
superradiant lasing signal using an ensemble of trapped Cs atoms in an optical lattice. A …

We report a new precision measurement of the dc Stark shift of the 6 s S 2 1/2→ 7 s S 2 1/2
transition in atomic cesium-133. Our result is 0.72246 (29) Hz (V/cm)-2. This result differs …

The static and dynamic electric-dipole polarizabilities and tune-out wavelengths for the
ground state of Cs atoms are calculated by using a semiempirical relativistic configuration …