THEORY OF RADIATIVE RECOMBINATION WITH STRONG LASER-PULSES AND THE FORMATION OF ULTRACOLD MOLECULES VIA STIMULATED PHOTO-RECOMBINATION OF COLD ATOMS

Citation
A. Vardi et al., THEORY OF RADIATIVE RECOMBINATION WITH STRONG LASER-PULSES AND THE FORMATION OF ULTRACOLD MOLECULES VIA STIMULATED PHOTO-RECOMBINATION OF COLD ATOMS, The Journal of chemical physics, 107(16), 1997, pp. 6166-6174
Citations number
37
Categorie Soggetti
Physics, Atomic, Molecular & Chemical
ISSN journal
00219606
Volume
107
Issue
16
Year of publication
1997
Pages
6166 - 6174
Database
ISI
SICI code
0021-9606(1997)107:16<6166:TORRWS>2.0.ZU;2-G
Abstract
A time dependent theory for radiative recombination induced by strong pulses is presented. Analytic solutions in the adiabatic limit are der ived and found to be in excellent agreement with exact numerical solut ions. Both the pump-before-dump ''intuitive'' and dump-before-pump ''c ounter-intuitive'' schemes are considered. Resonantly enhanced two-pho ton recombination of ultracold atoms is shown to be an efficient mecha nism for the production of ultracold molecules. We have performed deta iled calculations on the radiative recombination of cold Na atoms by s hort laser pulses. Our calculations show that, per pulse, it is possib le for up to 97% of all head-on Na-Na colliding pairs to end up as v=0 , J=0 translationally cold Na-2 molecules. We show that these findings , translated to thermally cooled ensemble conditions, mean that the fr action of Na atoms at mu Kelvin which can be recombined by a pulse of 20 ns duration and 10(8) W/cm(2) peak intensity, to form J=0 molecules is 6x10(-6) per pulse. With the above parameters, a laser operating a t 100 Hz can convert half of an ensemble of cold atoms to cold molecul es in similar to 25 min. The efficiency of the process can be increase d by going to longer pulses of lower intensity, by going to lower temp eratures or by increasing the density of the ensemble. In particular, the ''counter-intuitive'' scheme which allows for use of longer pulses of lower intensities, with no spontaneous emission losses, considerab ly increases the yield. (C) 1997 American Institute of Physics.