Microwave spectroscopic study of the hyperfine structure of antiprotonic super(3)He
In this work, we describe the latest results for the measurements of the hyperfine structure of antiprotonic super(3)He. Two out of four measurable super-super-hyperfine (SSHF) transition lines of the (n, L) = (36, 34) state of antiprotonic super(3)He were observed. The measured frequencies of the i...
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creator | Friedreich, S Barna, D Caspers, F Dax, A Hayano, R S Hori, M Horvath, D Juhasz, B Kobayashi, T Massiczek, O Soter, A Todoroki, K Widmann, E Zmeskal, J |
description | In this work, we describe the latest results for the measurements of the hyperfine structure of antiprotonic super(3)He. Two out of four measurable super-super-hyperfine (SSHF) transition lines of the (n, L) = (36, 34) state of antiprotonic super(3)He were observed. The measured frequencies of the individual transitions are 11.125 48 (08) GHz and 11.157 93 (13) GHz, with the increased precisions of about 43% and 25%, respectively, compared to our first measurements with antiprotonic super(3)He (Friedreich et al 2011 Phys. Lett. B 700 1-6). They are less than 0.5 MHz higher with respect to the most recent theoretical values, still within their estimated errors. Although the experimental uncertainty for the difference of 0.03245 (15) GHz between these frequencies is large as compared to that of theory, its measured value also agrees with theoretical calculations. The rates for collisions between antiprotonic helium and helium atoms have been assessed through comparison with simulations, resulting in an elastic collision rate of gamma e = 3.41 plus or minus 0.62 MHz and an inelastic collision rate of gamma i = 0.51 plus or minus 0.07 MHz. |
doi_str_mv | 10.1088/0953-4075/46/12/125003 |
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Two out of four measurable super-super-hyperfine (SSHF) transition lines of the (n, L) = (36, 34) state of antiprotonic super(3)He were observed. The measured frequencies of the individual transitions are 11.125 48 (08) GHz and 11.157 93 (13) GHz, with the increased precisions of about 43% and 25%, respectively, compared to our first measurements with antiprotonic super(3)He (Friedreich et al 2011 Phys. Lett. B 700 1-6). They are less than 0.5 MHz higher with respect to the most recent theoretical values, still within their estimated errors. Although the experimental uncertainty for the difference of 0.03245 (15) GHz between these frequencies is large as compared to that of theory, its measured value also agrees with theoretical calculations. The rates for collisions between antiprotonic helium and helium atoms have been assessed through comparison with simulations, resulting in an elastic collision rate of gamma e = 3.41 plus or minus 0.62 MHz and an inelastic collision rate of gamma i = 0.51 plus or minus 0.07 MHz.</description><identifier>ISSN: 0953-4075</identifier><identifier>DOI: 10.1088/0953-4075/46/12/125003</identifier><language>eng</language><subject>Collisions ; Elastic scattering ; Helium atoms ; Hyperfine structure ; Inelastic collisions ; Mathematical analysis ; Microwaves ; Simulation</subject><ispartof>Journal of physics. 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B, Atomic, molecular, and optical physics</title><description>In this work, we describe the latest results for the measurements of the hyperfine structure of antiprotonic super(3)He. Two out of four measurable super-super-hyperfine (SSHF) transition lines of the (n, L) = (36, 34) state of antiprotonic super(3)He were observed. The measured frequencies of the individual transitions are 11.125 48 (08) GHz and 11.157 93 (13) GHz, with the increased precisions of about 43% and 25%, respectively, compared to our first measurements with antiprotonic super(3)He (Friedreich et al 2011 Phys. Lett. B 700 1-6). They are less than 0.5 MHz higher with respect to the most recent theoretical values, still within their estimated errors. Although the experimental uncertainty for the difference of 0.03245 (15) GHz between these frequencies is large as compared to that of theory, its measured value also agrees with theoretical calculations. The rates for collisions between antiprotonic helium and helium atoms have been assessed through comparison with simulations, resulting in an elastic collision rate of gamma e = 3.41 plus or minus 0.62 MHz and an inelastic collision rate of gamma i = 0.51 plus or minus 0.07 MHz.</description><subject>Collisions</subject><subject>Elastic scattering</subject><subject>Helium atoms</subject><subject>Hyperfine structure</subject><subject>Inelastic collisions</subject><subject>Mathematical analysis</subject><subject>Microwaves</subject><subject>Simulation</subject><issn>0953-4075</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNqVy70KwjAUBeAMCv6-gmTUQXvTNBpnUVycdC8l3mKkNjU3UXx7K4i7cOAM5zuMTQQsBGidwFrJeQYrlWTLRKRtFIDssP5v6LEB0RVACJ1Cnx0P1nj3LB7IqUETvCPjGms4hXh-cVfycEF-eTXoS1u3KPhoQvT4mYo62Ma74OrPIbZmKmd7HLFuWVSE428P2XS3PW3289beI1LIb5YMVlVRo4uUiyxday1VquQf9A1cBEpY</recordid><startdate>20130628</startdate><enddate>20130628</enddate><creator>Friedreich, S</creator><creator>Barna, D</creator><creator>Caspers, F</creator><creator>Dax, A</creator><creator>Hayano, R S</creator><creator>Hori, M</creator><creator>Horvath, D</creator><creator>Juhasz, B</creator><creator>Kobayashi, T</creator><creator>Massiczek, O</creator><creator>Soter, A</creator><creator>Todoroki, K</creator><creator>Widmann, E</creator><creator>Zmeskal, J</creator><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20130628</creationdate><title>Microwave spectroscopic study of the hyperfine structure of antiprotonic super(3)He</title><author>Friedreich, S ; Barna, D ; Caspers, F ; Dax, A ; Hayano, R S ; Hori, M ; Horvath, D ; Juhasz, B ; Kobayashi, T ; Massiczek, O ; Soter, A ; Todoroki, K ; Widmann, E ; Zmeskal, J</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_miscellaneous_14298835253</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Collisions</topic><topic>Elastic scattering</topic><topic>Helium atoms</topic><topic>Hyperfine structure</topic><topic>Inelastic collisions</topic><topic>Mathematical analysis</topic><topic>Microwaves</topic><topic>Simulation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Friedreich, S</creatorcontrib><creatorcontrib>Barna, D</creatorcontrib><creatorcontrib>Caspers, F</creatorcontrib><creatorcontrib>Dax, A</creatorcontrib><creatorcontrib>Hayano, R S</creatorcontrib><creatorcontrib>Hori, M</creatorcontrib><creatorcontrib>Horvath, D</creatorcontrib><creatorcontrib>Juhasz, B</creatorcontrib><creatorcontrib>Kobayashi, T</creatorcontrib><creatorcontrib>Massiczek, O</creatorcontrib><creatorcontrib>Soter, A</creatorcontrib><creatorcontrib>Todoroki, K</creatorcontrib><creatorcontrib>Widmann, E</creatorcontrib><creatorcontrib>Zmeskal, J</creatorcontrib><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of physics. B, Atomic, molecular, and optical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Friedreich, S</au><au>Barna, D</au><au>Caspers, F</au><au>Dax, A</au><au>Hayano, R S</au><au>Hori, M</au><au>Horvath, D</au><au>Juhasz, B</au><au>Kobayashi, T</au><au>Massiczek, O</au><au>Soter, A</au><au>Todoroki, K</au><au>Widmann, E</au><au>Zmeskal, J</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Microwave spectroscopic study of the hyperfine structure of antiprotonic super(3)He</atitle><jtitle>Journal of physics. B, Atomic, molecular, and optical physics</jtitle><date>2013-06-28</date><risdate>2013</risdate><volume>46</volume><issue>12</issue><spage>125003</spage><epage>1-9</epage><pages>125003-1-9</pages><issn>0953-4075</issn><abstract>In this work, we describe the latest results for the measurements of the hyperfine structure of antiprotonic super(3)He. Two out of four measurable super-super-hyperfine (SSHF) transition lines of the (n, L) = (36, 34) state of antiprotonic super(3)He were observed. The measured frequencies of the individual transitions are 11.125 48 (08) GHz and 11.157 93 (13) GHz, with the increased precisions of about 43% and 25%, respectively, compared to our first measurements with antiprotonic super(3)He (Friedreich et al 2011 Phys. Lett. B 700 1-6). They are less than 0.5 MHz higher with respect to the most recent theoretical values, still within their estimated errors. Although the experimental uncertainty for the difference of 0.03245 (15) GHz between these frequencies is large as compared to that of theory, its measured value also agrees with theoretical calculations. The rates for collisions between antiprotonic helium and helium atoms have been assessed through comparison with simulations, resulting in an elastic collision rate of gamma e = 3.41 plus or minus 0.62 MHz and an inelastic collision rate of gamma i = 0.51 plus or minus 0.07 MHz.</abstract><doi>10.1088/0953-4075/46/12/125003</doi></addata></record> |
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subjects | Collisions Elastic scattering Helium atoms Hyperfine structure Inelastic collisions Mathematical analysis Microwaves Simulation |
title | Microwave spectroscopic study of the hyperfine structure of antiprotonic super(3)He |
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