The blackbody radiation shift of the Al+ 3s2 1Se0 ↦ 3s3p 3P○0 clock transition is evaluated. The polarizabilities of the two states are determined by means of configuration interaction calculations in conjunction with oscillator strength sum rules. The ground state polarizability was 24.14 ±0.12 a.u. while the metastable state polarizability was 24.62 ±0.25 a.u. The derived frequency shift at 300 K was Δν= -0.0042 ±0.0032 Hz. Some auxiliary sum rules are evaluated that allow for the conversion of a finite frequency polarizability difference to a static polarizability difference
The blackbody-radiation (BBR) shift of the 5s–4d5/2 clock transition in 88Sr+ is calculated to be 0....
<p><b>Table 3.</b> Absorption oscillator strengths for some low-lying transitions of Ga<sup>+</sup>....
The dipole polarizabilities of the ground state ns(2) (1)S(0) and the metastable state nsnp (3)P(0) ...
We report the theoretical evaluations of the static scalar polarizability of the 133Cs ground state ...
We report the theoretical evaluations of the static scalar polarizability of the 133Cs ground state ...
Abstract—We developed a theoretical method within the framework of relativistic many-body theory to ...
<p><b>Table 6.</b> Breakdown of the contributions to the dipole polarizabilities of the Ga<sup>+</su...
We present precise values of the dipole polarizabilities (alpha) of the ground [4f(14)6s] S-2(1/2) a...
We present preliminary results on a method used to determine the differential scalar polarizability ...
<p><b>Table 2.</b> Absorption oscillator strengths for some low-lying transitions of Ga<sup>2 +</sup...
Measurements of the scalar and tensor differential atomic polarisabilities have been made for two op...
We report a high-accuracy measurement of the differential static scalar polarizability \u394\u3b10 o...
The interaction between light and an atom causes perturbations in the atom’s energy levels, known as...
We used a Cs fountain to measure the Stark shift of the ground-state hyperfine transition frequency ...
We used a Cs fountain to measure the Stark shift of the ground-state hyperfine transition frequency ...
The blackbody-radiation (BBR) shift of the 5s–4d5/2 clock transition in 88Sr+ is calculated to be 0....
<p><b>Table 3.</b> Absorption oscillator strengths for some low-lying transitions of Ga<sup>+</sup>....
The dipole polarizabilities of the ground state ns(2) (1)S(0) and the metastable state nsnp (3)P(0) ...
We report the theoretical evaluations of the static scalar polarizability of the 133Cs ground state ...
We report the theoretical evaluations of the static scalar polarizability of the 133Cs ground state ...
Abstract—We developed a theoretical method within the framework of relativistic many-body theory to ...
<p><b>Table 6.</b> Breakdown of the contributions to the dipole polarizabilities of the Ga<sup>+</su...
We present precise values of the dipole polarizabilities (alpha) of the ground [4f(14)6s] S-2(1/2) a...
We present preliminary results on a method used to determine the differential scalar polarizability ...
<p><b>Table 2.</b> Absorption oscillator strengths for some low-lying transitions of Ga<sup>2 +</sup...
Measurements of the scalar and tensor differential atomic polarisabilities have been made for two op...
We report a high-accuracy measurement of the differential static scalar polarizability \u394\u3b10 o...
The interaction between light and an atom causes perturbations in the atom’s energy levels, known as...
We used a Cs fountain to measure the Stark shift of the ground-state hyperfine transition frequency ...
We used a Cs fountain to measure the Stark shift of the ground-state hyperfine transition frequency ...
The blackbody-radiation (BBR) shift of the 5s–4d5/2 clock transition in 88Sr+ is calculated to be 0....
<p><b>Table 3.</b> Absorption oscillator strengths for some low-lying transitions of Ga<sup>+</sup>....
The dipole polarizabilities of the ground state ns(2) (1)S(0) and the metastable state nsnp (3)P(0) ...