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Volumn 81, Issue 4, 2010, Pages

Three-body problem in heteronuclear mixtures with resonant interspecies interaction

Author keywords

[No Author keywords available]

Indexed keywords

ALTERNATIVE APPROACH; ANALYTIC SOLUTION; BODY PARAMETERS; BOSE-FERMI ATOMIC MIXTURE; COORDINATE REPRESENTATIONS; EFFECTIVE FIELD THEORY; HETERONUCLEAR; IDENTICAL BOSONS; INTERSPECIES INTERACTIONS; MASS RATIO; MOLECULAR STATE; RECOMBINATION LOSS; RELATIVE POSITIONS; SCATTERING LENGTH; THREE-BODY PROBLEM; THREE-BODY RECOMBINATION; TOTAL ENERGY; ZERO-RANGE APPROXIMATION;

EID: 77951742012     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.81.042715     Document Type: Article
Times cited : (107)

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    • In momentum space we have to work with an integral operator, the kernel of which is given by Eq. (5) with E=0. This operator possesses a property similar to Eq. (39), but the region of convergence in that case is narrower.
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    • Note that the coefficient C(δ) has the same dependence on δ as the term proportional to lnp in the definition of the infrared subtracted amplitude Ā in Eq. (15). This term arises from two-loop diagrams at fourth order in the two-body coupling g2 (see Sec. 8.5 in Ref. [1] and references therein).
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    • Note that our rate constant α is half the three-body loss coefficient K3 defined in Ref. [28].
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.