Antineutrino Spectra of U and Pu Taken from the Double Chooz Experiment
U, U, Pu, and Pu antineutrino spectra were obtained from the measurement done by the near detector in Double Chooz experiment. Method of converting the experimental positron spectrum into the antineutrino one has been developed. The spectrum conversion function obtained from Monte Carlo calculations...
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Veröffentlicht in: | Physics of atomic nuclei 2023-12, Vol.86 (6), p.1178-1188 |
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container_title | Physics of atomic nuclei |
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creator | Vlasenko, A. P. Ingerman, S. V. Naumov, P. Yu Sinev, V. V. |
description | U,
U,
Pu, and
Pu antineutrino spectra were obtained from the measurement done by the near detector in Double Chooz experiment. Method of converting the experimental positron spectrum into the antineutrino one has been developed. The spectrum conversion function obtained from Monte Carlo calculations is used. The experimental antineutrino spectrum taken by this method corresponds to a certain fuel composition of a nuclear reactor core in parts of fission. It is possible to split the experimental antineutrino spectrum on nuclear fuel components spectra. Nuclear fuel individual isotope antineutrino spectra from uranium and plutonium were fitted by the calculated ones obtained by summation of individual fragment spectra. In the calculation, a strength function was used to describe the probability distribution of beta transitions for unknown fragments. The most accurate experimental cross sections of inverse beta decay reaction measured in a number of experiments are consistent with sections calculated on base of our experimental and calculated
U,
U,
Pu, and
Pu antineutrino spectra. |
doi_str_mv | 10.1134/S1063778824010599 |
format | Article |
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U,
Pu, and
Pu antineutrino spectra were obtained from the measurement done by the near detector in Double Chooz experiment. Method of converting the experimental positron spectrum into the antineutrino one has been developed. The spectrum conversion function obtained from Monte Carlo calculations is used. The experimental antineutrino spectrum taken by this method corresponds to a certain fuel composition of a nuclear reactor core in parts of fission. It is possible to split the experimental antineutrino spectrum on nuclear fuel components spectra. Nuclear fuel individual isotope antineutrino spectra from uranium and plutonium were fitted by the calculated ones obtained by summation of individual fragment spectra. In the calculation, a strength function was used to describe the probability distribution of beta transitions for unknown fragments. The most accurate experimental cross sections of inverse beta decay reaction measured in a number of experiments are consistent with sections calculated on base of our experimental and calculated
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U,
Pu, and
Pu antineutrino spectra were obtained from the measurement done by the near detector in Double Chooz experiment. Method of converting the experimental positron spectrum into the antineutrino one has been developed. The spectrum conversion function obtained from Monte Carlo calculations is used. The experimental antineutrino spectrum taken by this method corresponds to a certain fuel composition of a nuclear reactor core in parts of fission. It is possible to split the experimental antineutrino spectrum on nuclear fuel components spectra. Nuclear fuel individual isotope antineutrino spectra from uranium and plutonium were fitted by the calculated ones obtained by summation of individual fragment spectra. In the calculation, a strength function was used to describe the probability distribution of beta transitions for unknown fragments. The most accurate experimental cross sections of inverse beta decay reaction measured in a number of experiments are consistent with sections calculated on base of our experimental and calculated
U,
U,
Pu, and
Pu antineutrino spectra.</description><subject>Beta decay</subject><subject>Detectors</subject><subject>ELEMENTARY PARTICLES AND FIELDS/Experiment</subject><subject>Mathematical analysis</subject><subject>Monte Carlo method</subject><subject>Nuclear energy</subject><subject>Nuclear facilities</subject><subject>Nuclear fuels</subject><subject>Nuclear reactors</subject><subject>Particle and Nuclear Physics</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Plutonium</subject><subject>Reactor cores</subject><subject>Spectra</subject><subject>Uranium</subject><issn>1063-7788</issn><issn>1562-692X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNp1kUtLAzEQgBdRsD5-gLeAJw9b89g89lhq1UJBsQreljQ7abe2SU12ofrrTakgIpJDQub7JpmZLLsguE8IK66nBAsmpVK0wATzsjzIeoQLmouSvh6mcwrnu_hxdhLjEmNCFMe97G7g2sZB14bGeTTdgGmDRt6iF6RdjR479KzfwCEb_Bq1C0A3vputAA0X3n-i0XYDoVmDa8-yI6tXEc6_99Ps5Xb0PLzPJw934-FgkhvKRZkXFCwoLkUtqOVCMkNnWIJljFtbq9pYboDjQnPKCS8wV0LjkgmprObScHaaXe7zboJ_7yC21dJ3waUnK1qyVDhPbUhUf0_N9QqqxlmfqjJp1bBujHdgm3Q_kIpJrEq5E65-CYlpYdvOdRdjNZ4-_WbJnjXBxxjAVpvUAx0-KoKr3TCqP8NIDt07MbFuDuHn2_9LX45jiEc</recordid><startdate>20231201</startdate><enddate>20231201</enddate><creator>Vlasenko, A. P.</creator><creator>Ingerman, S. V.</creator><creator>Naumov, P. Yu</creator><creator>Sinev, V. V.</creator><general>Pleiades Publishing</general><general>Springer</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>ISR</scope></search><sort><creationdate>20231201</creationdate><title>Antineutrino Spectra of U and Pu Taken from the Double Chooz Experiment</title><author>Vlasenko, A. P. ; Ingerman, S. V. ; Naumov, P. Yu ; Sinev, V. V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c2569-42efe8576d62f5673c2b07ef335ffd8dcf5ce504a5251540586a093678fa57c53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Beta decay</topic><topic>Detectors</topic><topic>ELEMENTARY PARTICLES AND FIELDS/Experiment</topic><topic>Mathematical analysis</topic><topic>Monte Carlo method</topic><topic>Nuclear energy</topic><topic>Nuclear facilities</topic><topic>Nuclear fuels</topic><topic>Nuclear reactors</topic><topic>Particle and Nuclear Physics</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Plutonium</topic><topic>Reactor cores</topic><topic>Spectra</topic><topic>Uranium</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Vlasenko, A. P.</creatorcontrib><creatorcontrib>Ingerman, S. V.</creatorcontrib><creatorcontrib>Naumov, P. Yu</creatorcontrib><creatorcontrib>Sinev, V. V.</creatorcontrib><collection>CrossRef</collection><collection>Gale In Context: Science</collection><jtitle>Physics of atomic nuclei</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Vlasenko, A. P.</au><au>Ingerman, S. V.</au><au>Naumov, P. Yu</au><au>Sinev, V. V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Antineutrino Spectra of U and Pu Taken from the Double Chooz Experiment</atitle><jtitle>Physics of atomic nuclei</jtitle><stitle>Phys. Atom. Nuclei</stitle><date>2023-12-01</date><risdate>2023</risdate><volume>86</volume><issue>6</issue><spage>1178</spage><epage>1188</epage><pages>1178-1188</pages><issn>1063-7788</issn><eissn>1562-692X</eissn><abstract>U,
U,
Pu, and
Pu antineutrino spectra were obtained from the measurement done by the near detector in Double Chooz experiment. Method of converting the experimental positron spectrum into the antineutrino one has been developed. The spectrum conversion function obtained from Monte Carlo calculations is used. The experimental antineutrino spectrum taken by this method corresponds to a certain fuel composition of a nuclear reactor core in parts of fission. It is possible to split the experimental antineutrino spectrum on nuclear fuel components spectra. Nuclear fuel individual isotope antineutrino spectra from uranium and plutonium were fitted by the calculated ones obtained by summation of individual fragment spectra. In the calculation, a strength function was used to describe the probability distribution of beta transitions for unknown fragments. The most accurate experimental cross sections of inverse beta decay reaction measured in a number of experiments are consistent with sections calculated on base of our experimental and calculated
U,
U,
Pu, and
Pu antineutrino spectra.</abstract><cop>Moscow</cop><pub>Pleiades Publishing</pub><doi>10.1134/S1063778824010599</doi><tpages>11</tpages></addata></record> |
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source | Springer Online Journals Complete |
subjects | Beta decay Detectors ELEMENTARY PARTICLES AND FIELDS/Experiment Mathematical analysis Monte Carlo method Nuclear energy Nuclear facilities Nuclear fuels Nuclear reactors Particle and Nuclear Physics Physics Physics and Astronomy Plutonium Reactor cores Spectra Uranium |
title | Antineutrino Spectra of U and Pu Taken from the Double Chooz Experiment |
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