Inducing Resonant Interactions in Ultracold Atoms with a Modulated Magnetic Field
In systems of ultracold atoms, pairwise interactions can be resonantly enhanced by a new mechanism that does not rely upon a magnetic Feshbach resonance. In this mechanism, interactions are controlled by tuning the frequency of an oscillating parallel component of the magnetic field close to the tra...
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Veröffentlicht in: | Physical review letters 2015-11, Vol.115 (19), p.193002-193002, Article 193002 |
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description | In systems of ultracold atoms, pairwise interactions can be resonantly enhanced by a new mechanism that does not rely upon a magnetic Feshbach resonance. In this mechanism, interactions are controlled by tuning the frequency of an oscillating parallel component of the magnetic field close to the transition frequency between the scattering atoms and a two-atom bound state. The real part of the resulting s-wave scattering length a is resonantly enhanced when the oscillation frequency is close to the transition frequency. The resonance parameters can be controlled by varying the amplitude of the oscillating field. The amplitude also controls the imaginary part of a, which arises because the oscillating field converts atom pairs into molecules. The real part of a can be made much larger than the background scattering length without introducing catastrophic atom losses from the imaginary part. For the case of a shallow bound state in the scattering channel, the dimensionless resonance parameters are universal functions of the dimensionless oscillation amplitude. |
doi_str_mv | 10.1103/PhysRevLett.115.193002 |
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In this mechanism, interactions are controlled by tuning the frequency of an oscillating parallel component of the magnetic field close to the transition frequency between the scattering atoms and a two-atom bound state. The real part of the resulting s-wave scattering length a is resonantly enhanced when the oscillation frequency is close to the transition frequency. The resonance parameters can be controlled by varying the amplitude of the oscillating field. The amplitude also controls the imaginary part of a, which arises because the oscillating field converts atom pairs into molecules. The real part of a can be made much larger than the background scattering length without introducing catastrophic atom losses from the imaginary part. For the case of a shallow bound state in the scattering channel, the dimensionless resonance parameters are universal functions of the dimensionless oscillation amplitude.</description><identifier>ISSN: 0031-9007</identifier><identifier>EISSN: 1079-7114</identifier><identifier>DOI: 10.1103/PhysRevLett.115.193002</identifier><identifier>PMID: 26588376</identifier><language>eng</language><publisher>United States</publisher><subject>Amplitudes ; Channels ; Magnetic fields ; Magnetic resonance ; Oscillating ; Resonance scattering ; Scattering ; Tuning</subject><ispartof>Physical review letters, 2015-11, Vol.115 (19), p.193002-193002, Article 193002</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c445t-9475978979929883b12327845bfe8d5bf00f0d194592399e7ff68eae480031e73</citedby><cites>FETCH-LOGICAL-c445t-9475978979929883b12327845bfe8d5bf00f0d194592399e7ff68eae480031e73</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,2876,2877,27924,27925</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/26588376$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Smith, D Hudson</creatorcontrib><title>Inducing Resonant Interactions in Ultracold Atoms with a Modulated Magnetic Field</title><title>Physical review letters</title><addtitle>Phys Rev Lett</addtitle><description>In systems of ultracold atoms, pairwise interactions can be resonantly enhanced by a new mechanism that does not rely upon a magnetic Feshbach resonance. In this mechanism, interactions are controlled by tuning the frequency of an oscillating parallel component of the magnetic field close to the transition frequency between the scattering atoms and a two-atom bound state. The real part of the resulting s-wave scattering length a is resonantly enhanced when the oscillation frequency is close to the transition frequency. The resonance parameters can be controlled by varying the amplitude of the oscillating field. The amplitude also controls the imaginary part of a, which arises because the oscillating field converts atom pairs into molecules. The real part of a can be made much larger than the background scattering length without introducing catastrophic atom losses from the imaginary part. For the case of a shallow bound state in the scattering channel, the dimensionless resonance parameters are universal functions of the dimensionless oscillation amplitude.</description><subject>Amplitudes</subject><subject>Channels</subject><subject>Magnetic fields</subject><subject>Magnetic resonance</subject><subject>Oscillating</subject><subject>Resonance scattering</subject><subject>Scattering</subject><subject>Tuning</subject><issn>0031-9007</issn><issn>1079-7114</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNqNUMFOwzAMjRCIjcEvTDly6XCatEmO08Rg0hAwsXOVNe5W1KWjSUH7ezptII5cbPnpPT_7ETJkMGIM-N3LZu8X-DnHEDogGTHNAeIz0mcgdSQZE-ekD8BZpAFkj1x5_w4ALE7VJenFaaIUl2mfvM6cbfPSrekCfe2MC3TmAjYmD2XtPC0dXVahG-vK0nGot55-lWFDDX2qbVuZgJY-mbXDUOZ0WmJlr8lFYSqPN6c-IMvp_dvkMZo_P8wm43mUC5GESAuZaKm01DrW3TErFvNYKpGsClS2qwAFWKZFomOuNcqiSBUaFOrwFUo-ILfHvbum_mjRh2xb-hyryjisW58xqXksUiHSf1B5cjAH1lHTIzVvau8bLLJdU25Ns88YZIfksz_Jd0CSHZPvhMOTR7vaov2V_UTNvwELgIBx</recordid><startdate>20151106</startdate><enddate>20151106</enddate><creator>Smith, D Hudson</creator><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20151106</creationdate><title>Inducing Resonant Interactions in Ultracold Atoms with a Modulated Magnetic Field</title><author>Smith, D Hudson</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c445t-9475978979929883b12327845bfe8d5bf00f0d194592399e7ff68eae480031e73</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Amplitudes</topic><topic>Channels</topic><topic>Magnetic fields</topic><topic>Magnetic resonance</topic><topic>Oscillating</topic><topic>Resonance scattering</topic><topic>Scattering</topic><topic>Tuning</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Smith, D Hudson</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physical review letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Smith, D Hudson</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Inducing Resonant Interactions in Ultracold Atoms with a Modulated Magnetic Field</atitle><jtitle>Physical review letters</jtitle><addtitle>Phys Rev Lett</addtitle><date>2015-11-06</date><risdate>2015</risdate><volume>115</volume><issue>19</issue><spage>193002</spage><epage>193002</epage><pages>193002-193002</pages><artnum>193002</artnum><issn>0031-9007</issn><eissn>1079-7114</eissn><abstract>In systems of ultracold atoms, pairwise interactions can be resonantly enhanced by a new mechanism that does not rely upon a magnetic Feshbach resonance. 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title | Inducing Resonant Interactions in Ultracold Atoms with a Modulated Magnetic Field |
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