Our previous measurements in the P and D series in 133 Cs have been extended to a number of higher lying levels, populated in a two-step excitation process involving an rf lamp and a CW dye laser. The D states were studied with the level-crossing technique, while the optical-double-resonance method was used for the investigation of the P states. For the magnetic dipole interaction constant a , the Landé g J factor, and the tensor polarizability α 2 we obtain 12 2 P 3/2 : a = 1.10(3) MHz, g J = 1.3340(15) 13 2 P 3/2 : a = 0.77(5) MHz, g J = 1.3337(20) 7 2 D 3/2 : | a | = 7.4(2) MHz 14 2 D 3/2 : | a | = 0.425(7) MHz 15 2 D 3/2 : | a | = 0.325(8) MHz 16 2 D 3/2 : | a | = 0.255(12) MHz 17 2 D 3/2 : | a | = 0.190(12) MHz 18 2 D 3/2 : | a | = 0....
The scalar polarizability constanta0 for excitedS- andD-states in rubidium and cesium was measured u...
The level crossing method has been used for the investigation of the hyperfine structure of the 6p2P...
We have measured the ratio M1/β of the M 1 amplitude to the vector polarizability β of the 6S1/2-7S ...
The scalar polarizability constant [alpha]0 for the 10, 11 2S1/2 and 9 2D5/2 states of 133Cs was mea...
We report the measurement of hyperfine splitting in the $7d$ $^{2}D_{3/2}$ state of $^{133}$Cs using...
Using the optical double resonance and level crossing methods, properties of several excited S , P ,...
By combining recent level crossing data with the results from a modified atomic beam experiment by B...
We present an experimental and theoretical investigation of the polarizabilities and hyperfine const...
Accurate measurements of hyperfine constants have revealed effects that can not be explained by a si...
We report measurements of absolute transition frequencies and hyperfine coupling constants for the ...
We report the magnetic dipole and electric quadrupole hyperfine coupling constants of 6 P_{3/2} stat...
Our previous level crossing measurements in the 6, 7, and 8 p 2 P 3/2 levels of Cs 133 have been ext...
The finite distribution of the nuclear magnetic moment across the nucleus gives a contribution to th...
The magnitudes and signs of the hyperfine interaction constants for 133Cs19F in the J = 1, v = 0, 1,...
We report measurements of the hyperfine coupling constant for the $8p \ ^2P_{1/2}$ level of atomic c...
The scalar polarizability constanta0 for excitedS- andD-states in rubidium and cesium was measured u...
The level crossing method has been used for the investigation of the hyperfine structure of the 6p2P...
We have measured the ratio M1/β of the M 1 amplitude to the vector polarizability β of the 6S1/2-7S ...
The scalar polarizability constant [alpha]0 for the 10, 11 2S1/2 and 9 2D5/2 states of 133Cs was mea...
We report the measurement of hyperfine splitting in the $7d$ $^{2}D_{3/2}$ state of $^{133}$Cs using...
Using the optical double resonance and level crossing methods, properties of several excited S , P ,...
By combining recent level crossing data with the results from a modified atomic beam experiment by B...
We present an experimental and theoretical investigation of the polarizabilities and hyperfine const...
Accurate measurements of hyperfine constants have revealed effects that can not be explained by a si...
We report measurements of absolute transition frequencies and hyperfine coupling constants for the ...
We report the magnetic dipole and electric quadrupole hyperfine coupling constants of 6 P_{3/2} stat...
Our previous level crossing measurements in the 6, 7, and 8 p 2 P 3/2 levels of Cs 133 have been ext...
The finite distribution of the nuclear magnetic moment across the nucleus gives a contribution to th...
The magnitudes and signs of the hyperfine interaction constants for 133Cs19F in the J = 1, v = 0, 1,...
We report measurements of the hyperfine coupling constant for the $8p \ ^2P_{1/2}$ level of atomic c...
The scalar polarizability constanta0 for excitedS- andD-states in rubidium and cesium was measured u...
The level crossing method has been used for the investigation of the hyperfine structure of the 6p2P...
We have measured the ratio M1/β of the M 1 amplitude to the vector polarizability β of the 6S1/2-7S ...