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Journal of Experimental and Theoretical Physics Letters

Fermionic atom laser

K. G. Petrosyan

Published Jul 1, 1999• 11 citations
Publisher

Abstract

An output coupling of a magnetically trapped two-species Fermi gas to a untrapped species is considered which can be implemented using rf or optical Raman transitions. The process can be used to produce an intense output beam of fermionic atoms once the device reaches a threshold in the zero-temperature case. For finite temperatures there is no threshold, as the output current grows smoothly. This behavior, which is reminiscent of conventional optical and cavity-QED lasers, suggests the name fermionic atom laser for this device.

DOI
10.1134/1.568122

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An output coupling of a magnetically trapped two-species Fermi gas to a untrapped species is considered which can be implemented using rf or optical Raman transitions. The process can be used to produce an intense output beam of fermionic atoms once the device reaches a threshold in the zero-temperature case. For finite temperatures there is no threshold, as the output current grows smoothly. This behavior, which is reminiscent of conventional optical and cavity-QED lasers, suggests the name fermionic atom laser for this device.
We consider a cold two-species atomic Fermi gas confined in a trap. We combine the Hermitian coupling between the states (we assume them to be the states with different spins) with the Cooper pairing of atoms with these different spins. This opens up a new prospect for investigation of interplay between various phenomena involving Raman coupling (e.g., atom lasers, dark-state polaritons) and effects caused by Cooper pairing of particles (e.g., superfluidity). We have obtained a threshold of transition from oscillatory to amplifying behavior of matter waves.
In this paper we present an atom laser scheme using a Raman transition for the output coupling of atoms. A beam of thermal atoms (bosons) in a metastable atomic state is pumped into a multimode atomic cavity. This cavity is coupled through spontaneous emission to another cavity for the atomic ground state. Above a certain threshold pumping rate a large number of atoms build up in the lowest energy state of the second cavity, while the higher energy states remain unpopulated. Atoms are then coupled to the outside of the cavity with a Raman transition. This changes the internal level of the atom and imparts a momentum kick, allowing the atoms to leave the system. We propose an implementation of our scheme using hollow optical-fiber atom waveguides.
We present a theory to derive the output rate of an atom laser consisting of an interacting Bose-Einstein condensate in a magnetic trap and two additional rf fields transferring trapped atoms to a repelled Zeeman sublevel via an intermediate untrapped Zeeman sublevel. We explicitly obtain the dependence of the output rate ${\ensuremath{\Gamma}}_{\mathrm{out}}$ on various characteristic parameters such as a coupling parameter (the Rabi frequency), the atom number density in the center of the condensate, and the strength of the atom-atom interaction.
We consider a cold two-species atomic Fermi gas confined in a trap. We combine the Hainan coupling between the states (we assume them to be the states with different spins) with the Cooper pairing of atoms with these different spins. This opens up a new prospect for investigation of interplay between various phenomena involving Raman coupling (e.g., atom lasers, dark-state polaritons) and effects caused by Cooper pairing of particles (e.g., superfluidity). We have obtained a threshold of transition from oscillatory to amplifying behavior of matter waves.