TY - JOUR
T1 - Nonlinear effects in optical pumping of a cold and slow atomic beam
AU - Porfido, N.
AU - Bezuglov, N. N.
AU - Bruvelis, M.
AU - Shayeganrad, G.
AU - Birindelli, S.
AU - Tantussi, F.
AU - Guerri, I.
AU - Viteau, M.
AU - Fioretti, A.
AU - Ciampini, D.
AU - Allegrini, M.
AU - Comparat, D.
AU - Arimondo, E.
AU - Ekers, Aigars
AU - Fuso, F.
N1 - KAUST Repository Item: Exported on 2020-10-01
PY - 2015/10/12
Y1 - 2015/10/12
N2 - By photoionizing hyperfine (HF) levels of the Cs state 62P3/2 in a slow and cold atom beam, we find how their population depends on the excitation laser power. The long time (around 180μs) spent by the slow atoms inside the resonant laser beam is large enough to enable exploration of a unique atom-light interaction regime heavily affected by time-dependent optical pumping. We demonstrate that, under such conditions, the onset of nonlinear effects in the population dynamics and optical pumping occurs at excitation laser intensities much smaller than the conventional respective saturation values. The evolution of population within the HF structure is calculated by numerical integration of the multilevel optical Bloch equations. The agreement between numerical results and experiment outcomes is excellent. All main features in the experimental findings are explained by the occurrence of “dark” and “bright” resonances leading to power-dependent branching coefficients.
AB - By photoionizing hyperfine (HF) levels of the Cs state 62P3/2 in a slow and cold atom beam, we find how their population depends on the excitation laser power. The long time (around 180μs) spent by the slow atoms inside the resonant laser beam is large enough to enable exploration of a unique atom-light interaction regime heavily affected by time-dependent optical pumping. We demonstrate that, under such conditions, the onset of nonlinear effects in the population dynamics and optical pumping occurs at excitation laser intensities much smaller than the conventional respective saturation values. The evolution of population within the HF structure is calculated by numerical integration of the multilevel optical Bloch equations. The agreement between numerical results and experiment outcomes is excellent. All main features in the experimental findings are explained by the occurrence of “dark” and “bright” resonances leading to power-dependent branching coefficients.
UR - http://hdl.handle.net/10754/579845
UR - http://link.aps.org/doi/10.1103/PhysRevA.92.043408
UR - http://www.scopus.com/inward/record.url?scp=84944414426&partnerID=8YFLogxK
U2 - 10.1103/PhysRevA.92.043408
DO - 10.1103/PhysRevA.92.043408
M3 - Article
SN - 1050-2947
VL - 92
JO - Physical Review A - Atomic, Molecular, and Optical Physics
JF - Physical Review A - Atomic, Molecular, and Optical Physics
IS - 4
ER -