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Volumn 79, Issue 4, 2009, Pages

Directional effects due to quantum statistics in dissociation of elongated molecular condensates

Author keywords

[No Author keywords available]

Indexed keywords

ATOMIC FERMIONS; DIMERIC MOLECULES; DIRECTIONAL EFFECTS; GEOMETRIC STRUCTURE; LONG AXIS; MOLECULAR CONDENSATE; QUANTUM STATISTICS; ULTRA-COLD;

EID: 66049098097     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.79.043624     Document Type: Article
Times cited : (9)

References (35)
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    • For a given atom-molecule scattering length, the respective s -wave interaction energy per particle can be made negligible by operating at much higher absolute values of the dissociation detuning |Δ|. This would, however, imply a higher velocity of the atoms, which may leave the molecular condensate region well before the atomic mode population reaches one and the difference between bosonic and fermionic statistics starts to show up. To surpass this problem one would need to use species with stronger values of the dissociation coupling χ in order to speed up the conversion and see the effects discussed here. While physically not impossible, this parameter regime would require a much larger computational lattice which is currently not feasible with our numerical method.
    • For a given atom-molecule scattering length, the respective s -wave interaction energy per particle can be made negligible by operating at much higher absolute values of the dissociation detuning |Δ|. This would, however, imply a higher velocity of the atoms, which may leave the molecular condensate region well before the atomic mode population reaches one and the difference between bosonic and fermionic statistics starts to show up. To surpass this problem one would need to use species with stronger values of the dissociation coupling χ in order to speed up the conversion and see the effects discussed here. While physically not impossible, this parameter regime would require a much larger computational lattice which is currently not feasible with our numerical method.
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    • For these values of RTF,i = (2 U 22 (2D) ρM,0 / m2 ωi2) 1/2 (i=x,y), we have assumed the trap oscillation frequencies of ωx /2π=2 Hz and ωy /2π=20 Hz and used ρM,0 =3.2× 1012 m-2 as the 2D peak density of the molecular BEC. The effective 2D molecule-molecule interaction strength, U 22 (2D) = U 22 (3D) / (2π l2,z), where U 22 (3D) =4π 2 a22 / m2, a22 is the 3D molecule-molecule scattering length, and l2,z = / m2 ωz is the length of the harmonic-oscillator ground state for the molecules in the eliminated z direction, is evaluated assuming ωz /2π=500 Hz and a22 =1.4 nm.
    • For these values of RTF,i = (2 U 22 (2D) ρM,0 / m2 ωi2) 1/2 (i=x,y), we have assumed the trap oscillation frequencies of ωx /2π=2 Hz and ωy /2π=20 Hz and used ρM,0 =3.2× 1012 m-2 as the 2D peak density of the molecular BEC. The effective 2D molecule-molecule interaction strength, U 22 (2D) = U 22 (3D) / (2π l2,z), where U 22 (3D) =4π 2 a22 / m2, a22 is the 3D molecule-molecule scattering length, and l2,z = / m2 ωz is the length of the harmonic-oscillator ground state for the molecules in the eliminated z direction, is evaluated assuming ωz /2π=500 Hz and a22 =1.4 nm.
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.