TY - JOUR
T1 - Stochastic laser cooling enabled by many-body effects
AU - Dann, Roie
AU - Kosloff, Ronnie
N1 - Publisher Copyright:
© 2018 IOP Publishing Ltd.
PY - 2018/6/7
Y1 - 2018/6/7
N2 - A novel laser cooling mechanism based on many-body effects is presented. The method can be applied to the cooling of a large class of atoms and molecules at a higher density than commonly excepted by existing methods. The cooling mechanism relies on the collective encounter of particles and light. Stochastic events between the particles and photons, as well as a collective effect, give rise to energy transfer between these media. Such a mechanism relies on multiple light-matter encounters, therefore requiring a sufficient particle density, ρ ∼ 1014 cm-3. This is an advantage for experiments where a high phase space density is required. A second tuning laser can be added, increasing the applicability to many types of atoms and molecules. This tuning laser changes the inter-particle potential by inducing an AC Stark effect. As a result, the required trapping density can be reduced to ρ ∼ 106 cm-3. Simulations of phase space distributions were performed, comparing different particle densities, trap potentials and light field intensity profiles. The modelling shows efficient cooling rates up to 10 2K s-1 for a dense ensemble of 87Rb atoms, and cooling rates of up to 6 • 10 2 K s-1 when adding an additional tuning source.
AB - A novel laser cooling mechanism based on many-body effects is presented. The method can be applied to the cooling of a large class of atoms and molecules at a higher density than commonly excepted by existing methods. The cooling mechanism relies on the collective encounter of particles and light. Stochastic events between the particles and photons, as well as a collective effect, give rise to energy transfer between these media. Such a mechanism relies on multiple light-matter encounters, therefore requiring a sufficient particle density, ρ ∼ 1014 cm-3. This is an advantage for experiments where a high phase space density is required. A second tuning laser can be added, increasing the applicability to many types of atoms and molecules. This tuning laser changes the inter-particle potential by inducing an AC Stark effect. As a result, the required trapping density can be reduced to ρ ∼ 106 cm-3. Simulations of phase space distributions were performed, comparing different particle densities, trap potentials and light field intensity profiles. The modelling shows efficient cooling rates up to 10 2K s-1 for a dense ensemble of 87Rb atoms, and cooling rates of up to 6 • 10 2 K s-1 when adding an additional tuning source.
KW - cooling
KW - high-density gas
KW - laser
UR - http://www.scopus.com/inward/record.url?scp=85049404431&partnerID=8YFLogxK
U2 - 10.1088/1361-6455/aac3bd
DO - 10.1088/1361-6455/aac3bd
M3 - ???researchoutput.researchoutputtypes.contributiontojournal.article???
AN - SCOPUS:85049404431
SN - 0953-4075
VL - 51
JO - Journal of Physics B: Atomic, Molecular and Optical Physics
JF - Journal of Physics B: Atomic, Molecular and Optical Physics
IS - 13
M1 - 135002
ER -