Optical molasses loaded from a low-velocity intense source of atoms: an atom source for improved atomic fountains
We demonstrate the efficient capture of cesium atoms from a low-velocity intense source (LVIS) of atoms into an optical molasses. The high load rates that are achievable with the technique can potentially improve the stability of and reduce collisional shifts in atomic fountain clocks. An LVIS is an...
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creator | Donley, E.A. Heavner, T.P. Jefferts, S.R. |
description | We demonstrate the efficient capture of cesium atoms from a low-velocity intense source (LVIS) of atoms into an optical molasses. The high load rates that are achievable with the technique can potentially improve the stability of and reduce collisional shifts in atomic fountain clocks. An LVIS is an atomic beam created from a small hole in one of the retroreflectors in an otherwise ordinary magnetooptical trap (MOT). Our typical LVIS flux was 10/sup 10/ atoms/s. The asymptotic value for the number of atoms captured in the optical molasses was 1.1(1) /spl times/ 10/sup 9/ atoms, and the fill time constant was /spl tau/ = 290(30) ms. The initial molasses fill rate was R/sub t=0/ = 3.8(5) /spl times/ 10/sup 6/ atoms/ms. At this rate, it would require 24 ms to capture and launch 10/sup 7/ state-selected atoms in an atomic fountain. The fill rate at short times indicates that approximately 40% of the LVIS atoms were being captured in the optical molasses. |
doi_str_mv | 10.1109/TIM.2005.853218 |
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The high load rates that are achievable with the technique can potentially improve the stability of and reduce collisional shifts in atomic fountain clocks. An LVIS is an atomic beam created from a small hole in one of the retroreflectors in an otherwise ordinary magnetooptical trap (MOT). Our typical LVIS flux was 10/sup 10/ atoms/s. The asymptotic value for the number of atoms captured in the optical molasses was 1.1(1) /spl times/ 10/sup 9/ atoms, and the fill time constant was /spl tau/ = 290(30) ms. The initial molasses fill rate was R/sub t=0/ = 3.8(5) /spl times/ 10/sup 6/ atoms/ms. At this rate, it would require 24 ms to capture and launch 10/sup 7/ state-selected atoms in an atomic fountain. The fill rate at short times indicates that approximately 40% of the LVIS atoms were being captured in the optical molasses.</description><identifier>ISSN: 0018-9456</identifier><identifier>EISSN: 1557-9662</identifier><identifier>DOI: 10.1109/TIM.2005.853218</identifier><identifier>CODEN: IEIMAO</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Asymptotic properties ; Atom optics ; Atomic beams ; Atomic clocks ; Atomic measurements ; Atomic properties ; Clocks ; Flux ; Frequency ; Instrumentation ; Magnetic resonance ; Microwave ovens ; Molasses ; NIST ; Stability ; Time constant ; Uncertainty</subject><ispartof>IEEE transactions on instrumentation and measurement, 2005-10, Vol.54 (5), p.1905-1910</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2005</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c392t-1cfa1d3d647bd488331715a773d4721ea545c1c16b578b0e5a0d3639a202ef403</citedby><cites>FETCH-LOGICAL-c392t-1cfa1d3d647bd488331715a773d4721ea545c1c16b578b0e5a0d3639a202ef403</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/1514641$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,27924,27925,54758</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/1514641$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Donley, E.A.</creatorcontrib><creatorcontrib>Heavner, T.P.</creatorcontrib><creatorcontrib>Jefferts, S.R.</creatorcontrib><title>Optical molasses loaded from a low-velocity intense source of atoms: an atom source for improved atomic fountains</title><title>IEEE transactions on instrumentation and measurement</title><addtitle>TIM</addtitle><description>We demonstrate the efficient capture of cesium atoms from a low-velocity intense source (LVIS) of atoms into an optical molasses. The high load rates that are achievable with the technique can potentially improve the stability of and reduce collisional shifts in atomic fountain clocks. An LVIS is an atomic beam created from a small hole in one of the retroreflectors in an otherwise ordinary magnetooptical trap (MOT). Our typical LVIS flux was 10/sup 10/ atoms/s. The asymptotic value for the number of atoms captured in the optical molasses was 1.1(1) /spl times/ 10/sup 9/ atoms, and the fill time constant was /spl tau/ = 290(30) ms. The initial molasses fill rate was R/sub t=0/ = 3.8(5) /spl times/ 10/sup 6/ atoms/ms. At this rate, it would require 24 ms to capture and launch 10/sup 7/ state-selected atoms in an atomic fountain. The fill rate at short times indicates that approximately 40% of the LVIS atoms were being captured in the optical molasses.</description><subject>Asymptotic properties</subject><subject>Atom optics</subject><subject>Atomic beams</subject><subject>Atomic clocks</subject><subject>Atomic measurements</subject><subject>Atomic properties</subject><subject>Clocks</subject><subject>Flux</subject><subject>Frequency</subject><subject>Instrumentation</subject><subject>Magnetic resonance</subject><subject>Microwave ovens</subject><subject>Molasses</subject><subject>NIST</subject><subject>Stability</subject><subject>Time constant</subject><subject>Uncertainty</subject><issn>0018-9456</issn><issn>1557-9662</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNp9kbtv2zAQh4kiBeq4nTt0ITqkk2we38oWGGkSwEWWdCZo6gTQkERblB3kvw9dtwiQodO9vnvhR8hXYAsAVi-fHn4tOGNqYZXgYD-QGShlqlprfkFmjIGtaqn0J3KZ85YxZrQ0M7J_3E0x-I72qfM5Y6Zd8g02tB1TT32JnqsjdinE6YXGYcIhI83pMAakqaV-Sn2-pn744_0rtGmksd-N6VgGnQoxlNxhmHwc8mfysfVdxi9_7Zz8_nn7tLqv1o93D6ubdRVEzacKQuuhEU25ctNIa4UAA8obIxppOKBXUgUIoDfK2A1D5VkjtKg9ZxxbycSc_DjPLXfsD5gn18ccsOv8gOmQna0154pJW8ir_5LcMmNqZQr4_R24LQ8P5QtnbW05aHHauzxDYUw5j9i63Rh7P744YO6klCtKuZNS7qxU6fh27oiI-EYrkFqCeAVCBo87</recordid><startdate>20051001</startdate><enddate>20051001</enddate><creator>Donley, E.A.</creator><creator>Heavner, T.P.</creator><creator>Jefferts, S.R.</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</general><scope>97E</scope><scope>RIA</scope><scope>RIE</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope><scope>7SC</scope><scope>JQ2</scope><scope>L~C</scope><scope>L~D</scope><scope>F28</scope><scope>FR3</scope></search><sort><creationdate>20051001</creationdate><title>Optical molasses loaded from a low-velocity intense source of atoms: an atom source for improved atomic fountains</title><author>Donley, E.A. ; Heavner, T.P. ; Jefferts, S.R.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c392t-1cfa1d3d647bd488331715a773d4721ea545c1c16b578b0e5a0d3639a202ef403</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2005</creationdate><topic>Asymptotic properties</topic><topic>Atom optics</topic><topic>Atomic beams</topic><topic>Atomic clocks</topic><topic>Atomic measurements</topic><topic>Atomic properties</topic><topic>Clocks</topic><topic>Flux</topic><topic>Frequency</topic><topic>Instrumentation</topic><topic>Magnetic resonance</topic><topic>Microwave ovens</topic><topic>Molasses</topic><topic>NIST</topic><topic>Stability</topic><topic>Time constant</topic><topic>Uncertainty</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Donley, E.A.</creatorcontrib><creatorcontrib>Heavner, T.P.</creatorcontrib><creatorcontrib>Jefferts, S.R.</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 2005-present</collection><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE Electronic Library (IEL)</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Computer and Information Systems Abstracts</collection><collection>ProQuest Computer Science Collection</collection><collection>Computer and Information Systems Abstracts Academic</collection><collection>Computer and Information Systems Abstracts Professional</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><jtitle>IEEE transactions on instrumentation and measurement</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Donley, E.A.</au><au>Heavner, T.P.</au><au>Jefferts, S.R.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Optical molasses loaded from a low-velocity intense source of atoms: an atom source for improved atomic fountains</atitle><jtitle>IEEE transactions on instrumentation and measurement</jtitle><stitle>TIM</stitle><date>2005-10-01</date><risdate>2005</risdate><volume>54</volume><issue>5</issue><spage>1905</spage><epage>1910</epage><pages>1905-1910</pages><issn>0018-9456</issn><eissn>1557-9662</eissn><coden>IEIMAO</coden><abstract>We demonstrate the efficient capture of cesium atoms from a low-velocity intense source (LVIS) of atoms into an optical molasses. The high load rates that are achievable with the technique can potentially improve the stability of and reduce collisional shifts in atomic fountain clocks. An LVIS is an atomic beam created from a small hole in one of the retroreflectors in an otherwise ordinary magnetooptical trap (MOT). Our typical LVIS flux was 10/sup 10/ atoms/s. The asymptotic value for the number of atoms captured in the optical molasses was 1.1(1) /spl times/ 10/sup 9/ atoms, and the fill time constant was /spl tau/ = 290(30) ms. The initial molasses fill rate was R/sub t=0/ = 3.8(5) /spl times/ 10/sup 6/ atoms/ms. At this rate, it would require 24 ms to capture and launch 10/sup 7/ state-selected atoms in an atomic fountain. The fill rate at short times indicates that approximately 40% of the LVIS atoms were being captured in the optical molasses.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TIM.2005.853218</doi><tpages>6</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Asymptotic properties Atom optics Atomic beams Atomic clocks Atomic measurements Atomic properties Clocks Flux Frequency Instrumentation Magnetic resonance Microwave ovens Molasses NIST Stability Time constant Uncertainty |
title | Optical molasses loaded from a low-velocity intense source of atoms: an atom source for improved atomic fountains |
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