Feshbach resonance in atomic binary collisions in the Wigner threshold law regime
We analyze, within the generalized multichannel quantum defect theory framework, atomic binary collision cross sections over the 1 {mu}K to 10 mK energy range just above the entrance channel threshold, a domain where the Wigner threshold law should apply. By adjusting the strength of a constant exte...
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description | We analyze, within the generalized multichannel quantum defect theory framework, atomic binary collision cross sections over the 1 {mu}K to 10 mK energy range just above the entrance channel threshold, a domain where the Wigner threshold law should apply. By adjusting the strength of a constant external magnetic field a Feshbach resonance is tuned at will over this energy range. In the threshold regime, the quasibound state interacts with an opening continuum whose wave function presents a strong energy dependence which reflects the breakdown of the WKB approximation. The effective discrete-continuum interactions become very sensitive to the energy. The consequences of these variations have been investigated by including threshold effects in the analysis of the Fano configuration-interaction theory [Phys. Rev. 124, 1866 (1961)] in terms of quantum defect theory quantities proposed by [Lecomte J. Phys. B 20, 3645 (1987)]. This analysis shows that the energy variations are in general so important that it becomes meaningless to associate a width with a Feshbach resonance. However, it is still possible to define the resonance energy, as long as the energy variation of the shift of the resonance, induced by the effective discrete-continuum interaction, remains linear over an energy range corresponding to the magnitude of the shift. |
doi_str_mv | 10.1103/PhysRevA.70.012710 |
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B 20, 3645 (1987)]. This analysis shows that the energy variations are in general so important that it becomes meaningless to associate a width with a Feshbach resonance. However, it is still possible to define the resonance energy, as long as the energy variation of the shift of the resonance, induced by the effective discrete-continuum interaction, remains linear over an energy range corresponding to the magnitude of the shift.</description><identifier>ISSN: 1050-2947</identifier><identifier>EISSN: 1094-1622</identifier><identifier>DOI: 10.1103/PhysRevA.70.012710</identifier><language>eng</language><publisher>United States</publisher><subject>ATOM COLLISIONS ; ATOMIC AND MOLECULAR PHYSICS ; BOUND STATE ; CONFIGURATION INTERACTION ; CROSS SECTIONS ; ENERGY DEPENDENCE ; ENERGY LEVELS ; MAGNETIC FIELDS ; QUASIBOUND STATE ; RESONANCE ; WAVE FUNCTIONS ; WKB APPROXIMATION</subject><ispartof>Physical review. 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A, Atomic, molecular, and optical physics</title><description>We analyze, within the generalized multichannel quantum defect theory framework, atomic binary collision cross sections over the 1 {mu}K to 10 mK energy range just above the entrance channel threshold, a domain where the Wigner threshold law should apply. By adjusting the strength of a constant external magnetic field a Feshbach resonance is tuned at will over this energy range. In the threshold regime, the quasibound state interacts with an opening continuum whose wave function presents a strong energy dependence which reflects the breakdown of the WKB approximation. The effective discrete-continuum interactions become very sensitive to the energy. The consequences of these variations have been investigated by including threshold effects in the analysis of the Fano configuration-interaction theory [Phys. Rev. 124, 1866 (1961)] in terms of quantum defect theory quantities proposed by [Lecomte J. Phys. B 20, 3645 (1987)]. This analysis shows that the energy variations are in general so important that it becomes meaningless to associate a width with a Feshbach resonance. However, it is still possible to define the resonance energy, as long as the energy variation of the shift of the resonance, induced by the effective discrete-continuum interaction, remains linear over an energy range corresponding to the magnitude of the shift.</description><subject>ATOM COLLISIONS</subject><subject>ATOMIC AND MOLECULAR PHYSICS</subject><subject>BOUND STATE</subject><subject>CONFIGURATION INTERACTION</subject><subject>CROSS SECTIONS</subject><subject>ENERGY DEPENDENCE</subject><subject>ENERGY LEVELS</subject><subject>MAGNETIC FIELDS</subject><subject>QUASIBOUND STATE</subject><subject>RESONANCE</subject><subject>WAVE FUNCTIONS</subject><subject>WKB APPROXIMATION</subject><issn>1050-2947</issn><issn>1094-1622</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2004</creationdate><recordtype>article</recordtype><recordid>eNo1UE1LAzEUDKJgrf4BTwHPW1-yyaZ7LMWqUPADxWPIZzeyTWSzKP33Zqm-yxt4M8O8QeiawIIQqG-fu0N-dd-rhYAFECoInKAZgZZVpKH0dMIcKtoycY4ucv6EMmzZztDLxuVOK9PhweUUVTQOh4jVmPbBYB2iGg7YpL4POaSYp9vYOfwRdtENBRZVl3qLe_VTHHZh7y7RmVd9dld_e47eN3dv64dq-3T_uF5tK1NTNlZLQ21NmqUF7jm0mpfYjHnlueDWkpZZrxkXjaaMOkaIhtaCb3TdciKYdfUc3Rx9Ux6DzCaMznQmxejMKCk0kxgKix5ZZkg5D87LryHsy1OSgJyqk__VSQHyWF39C4yFYyw</recordid><startdate>200407</startdate><enddate>200407</enddate><creator>Raoult, M.</creator><creator>Mies, F. 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H.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c324t-8c2d3168d05f509b501244faf575dd194dfb4576b242e411b09d0f6b395174de3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2004</creationdate><topic>ATOM COLLISIONS</topic><topic>ATOMIC AND MOLECULAR PHYSICS</topic><topic>BOUND STATE</topic><topic>CONFIGURATION INTERACTION</topic><topic>CROSS SECTIONS</topic><topic>ENERGY DEPENDENCE</topic><topic>ENERGY LEVELS</topic><topic>MAGNETIC FIELDS</topic><topic>QUASIBOUND STATE</topic><topic>RESONANCE</topic><topic>WAVE FUNCTIONS</topic><topic>WKB APPROXIMATION</topic><toplevel>online_resources</toplevel><creatorcontrib>Raoult, M.</creatorcontrib><creatorcontrib>Mies, F. H.</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Physical review. A, Atomic, molecular, and optical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Raoult, M.</au><au>Mies, F. H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Feshbach resonance in atomic binary collisions in the Wigner threshold law regime</atitle><jtitle>Physical review. A, Atomic, molecular, and optical physics</jtitle><date>2004-07</date><risdate>2004</risdate><volume>70</volume><issue>1</issue><artnum>012710</artnum><issn>1050-2947</issn><eissn>1094-1622</eissn><abstract>We analyze, within the generalized multichannel quantum defect theory framework, atomic binary collision cross sections over the 1 {mu}K to 10 mK energy range just above the entrance channel threshold, a domain where the Wigner threshold law should apply. By adjusting the strength of a constant external magnetic field a Feshbach resonance is tuned at will over this energy range. In the threshold regime, the quasibound state interacts with an opening continuum whose wave function presents a strong energy dependence which reflects the breakdown of the WKB approximation. The effective discrete-continuum interactions become very sensitive to the energy. The consequences of these variations have been investigated by including threshold effects in the analysis of the Fano configuration-interaction theory [Phys. Rev. 124, 1866 (1961)] in terms of quantum defect theory quantities proposed by [Lecomte J. Phys. B 20, 3645 (1987)]. This analysis shows that the energy variations are in general so important that it becomes meaningless to associate a width with a Feshbach resonance. 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subjects | ATOM COLLISIONS ATOMIC AND MOLECULAR PHYSICS BOUND STATE CONFIGURATION INTERACTION CROSS SECTIONS ENERGY DEPENDENCE ENERGY LEVELS MAGNETIC FIELDS QUASIBOUND STATE RESONANCE WAVE FUNCTIONS WKB APPROXIMATION |
title | Feshbach resonance in atomic binary collisions in the Wigner threshold law regime |
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