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Does the Excited Cluster 14N Exist in the 15O Nucleus?
On the basis of the modified potential two-cluster model with forbidden state which effectively take the Pauli principle into account, calculations have been performed of the astrophysical S-factor of radiative p 14 N capture to the ground state of the 15 O nucleus at proton energies up to 5 MeV in...
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Published in: | Russian physics journal 2019-03, Vol.61 (11), p.2105-2112 |
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creator | Dubovichenko, S. B. Burkova, N. A. |
description | On the basis of the modified potential two-cluster model with forbidden state which effectively take the Pauli principle into account, calculations have been performed of the astrophysical S-factor of radiative
p
14
N capture to the ground state of the
15
O nucleus at proton energies up to 5 MeV in the center-of-mass system (c.m.s.) with allowance for wide resonances up to 3.4 MeV in the c.m.s. For an acceptable explanation of the available experimental data it is necessary to allow the existence of the
14
N cluster in the excited state
14
N
*
at an excitation energy of 5.69 MeV and angular momentum
J
π
= 1
–
. It is assumed that in such a case it is possible to use the wave function of the
4
D
1/2
state with respect to the relative motion of the
p
14
N
*
clusters. It is also shown that a description of the S-factor of
p
14
N capture in the resonance region is possible only under the assumption that all of the low-lying resonances at 260(1/2
+
), 987(3/2
+
), 1447(1/2
+
), 2187(3/2
+
), and 3211(3/2
+
) keV in the c.m.s. are
4
D
1/2
and
4
D
3/2
scattering waves. |
doi_str_mv | 10.1007/s11182-019-01643-w |
format | article |
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p
14
N capture to the ground state of the
15
O nucleus at proton energies up to 5 MeV in the center-of-mass system (c.m.s.) with allowance for wide resonances up to 3.4 MeV in the c.m.s. For an acceptable explanation of the available experimental data it is necessary to allow the existence of the
14
N cluster in the excited state
14
N
*
at an excitation energy of 5.69 MeV and angular momentum
J
π
= 1
–
. It is assumed that in such a case it is possible to use the wave function of the
4
D
1/2
state with respect to the relative motion of the
p
14
N
*
clusters. It is also shown that a description of the S-factor of
p
14
N capture in the resonance region is possible only under the assumption that all of the low-lying resonances at 260(1/2
+
), 987(3/2
+
), 1447(1/2
+
), 2187(3/2
+
), and 3211(3/2
+
) keV in the c.m.s. are
4
D
1/2
and
4
D
3/2
scattering waves.</description><identifier>ISSN: 1064-8887</identifier><identifier>EISSN: 1573-9228</identifier><identifier>DOI: 10.1007/s11182-019-01643-w</identifier><language>eng</language><publisher>New York: Springer US</publisher><subject>Angular momentum ; Clusters ; Condensed Matter Physics ; Hadrons ; Heavy Ions ; Lasers ; Mathematical and Computational Physics ; Nuclear Physics ; Nuclei (nuclear physics) ; Optical Devices ; Optics ; Photonics ; Physics ; Physics and Astronomy ; Theoretical</subject><ispartof>Russian physics journal, 2019-03, Vol.61 (11), p.2105-2112</ispartof><rights>Springer Science+Business Media, LLC, part of Springer Nature 2019</rights><rights>Copyright Springer Nature B.V. 2019</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c249t-c328a1cfdf7c7d9c2647dbae48f6e9ee31992b235c010a378af97b5166dcbc443</citedby><cites>FETCH-LOGICAL-c249t-c328a1cfdf7c7d9c2647dbae48f6e9ee31992b235c010a378af97b5166dcbc443</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Dubovichenko, S. B.</creatorcontrib><creatorcontrib>Burkova, N. A.</creatorcontrib><title>Does the Excited Cluster 14N Exist in the 15O Nucleus?</title><title>Russian physics journal</title><addtitle>Russ Phys J</addtitle><description>On the basis of the modified potential two-cluster model with forbidden state which effectively take the Pauli principle into account, calculations have been performed of the astrophysical S-factor of radiative
p
14
N capture to the ground state of the
15
O nucleus at proton energies up to 5 MeV in the center-of-mass system (c.m.s.) with allowance for wide resonances up to 3.4 MeV in the c.m.s. For an acceptable explanation of the available experimental data it is necessary to allow the existence of the
14
N cluster in the excited state
14
N
*
at an excitation energy of 5.69 MeV and angular momentum
J
π
= 1
–
. It is assumed that in such a case it is possible to use the wave function of the
4
D
1/2
state with respect to the relative motion of the
p
14
N
*
clusters. It is also shown that a description of the S-factor of
p
14
N capture in the resonance region is possible only under the assumption that all of the low-lying resonances at 260(1/2
+
), 987(3/2
+
), 1447(1/2
+
), 2187(3/2
+
), and 3211(3/2
+
) keV in the c.m.s. are
4
D
1/2
and
4
D
3/2
scattering waves.</description><subject>Angular momentum</subject><subject>Clusters</subject><subject>Condensed Matter Physics</subject><subject>Hadrons</subject><subject>Heavy Ions</subject><subject>Lasers</subject><subject>Mathematical and Computational Physics</subject><subject>Nuclear Physics</subject><subject>Nuclei (nuclear physics)</subject><subject>Optical Devices</subject><subject>Optics</subject><subject>Photonics</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Theoretical</subject><issn>1064-8887</issn><issn>1573-9228</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNp9kE9PwzAMxSMEEmPwBThV4hyIkzR_TgiNDZCm7QLnqE1d6FTWkbQafHvCisSNg2XLer9n6xFyCewaGNM3EQAMpwxsKiUF3R-RCeRaUMu5OU4zU5IaY_QpOYtxw1jClJ4Qdd9hzPo3zOafvumxymbtEHsMGchV2jWxz5rtQQD5OlsNvsUh3p6Tk7poI1789il5WcyfZ490uX54mt0tqefS9tQLbgrwdVVrryvruZK6KguUplZoEQVYy0sucp_-KYQ2RW11mYNSlS-9lGJKrkbfXeg-Boy923RD2KaTjnPQec41sKTio8qHLsaAtduF5r0IXw6Y-8nHjfm4lI875OP2CRIjFJN4-4rhz_of6htsl2Zu</recordid><startdate>20190301</startdate><enddate>20190301</enddate><creator>Dubovichenko, S. B.</creator><creator>Burkova, N. A.</creator><general>Springer US</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20190301</creationdate><title>Does the Excited Cluster 14N Exist in the 15O Nucleus?</title><author>Dubovichenko, S. B. ; Burkova, N. A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c249t-c328a1cfdf7c7d9c2647dbae48f6e9ee31992b235c010a378af97b5166dcbc443</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Angular momentum</topic><topic>Clusters</topic><topic>Condensed Matter Physics</topic><topic>Hadrons</topic><topic>Heavy Ions</topic><topic>Lasers</topic><topic>Mathematical and Computational Physics</topic><topic>Nuclear Physics</topic><topic>Nuclei (nuclear physics)</topic><topic>Optical Devices</topic><topic>Optics</topic><topic>Photonics</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Theoretical</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Dubovichenko, S. B.</creatorcontrib><creatorcontrib>Burkova, N. A.</creatorcontrib><collection>CrossRef</collection><jtitle>Russian physics journal</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Dubovichenko, S. B.</au><au>Burkova, N. A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Does the Excited Cluster 14N Exist in the 15O Nucleus?</atitle><jtitle>Russian physics journal</jtitle><stitle>Russ Phys J</stitle><date>2019-03-01</date><risdate>2019</risdate><volume>61</volume><issue>11</issue><spage>2105</spage><epage>2112</epage><pages>2105-2112</pages><issn>1064-8887</issn><eissn>1573-9228</eissn><abstract>On the basis of the modified potential two-cluster model with forbidden state which effectively take the Pauli principle into account, calculations have been performed of the astrophysical S-factor of radiative
p
14
N capture to the ground state of the
15
O nucleus at proton energies up to 5 MeV in the center-of-mass system (c.m.s.) with allowance for wide resonances up to 3.4 MeV in the c.m.s. For an acceptable explanation of the available experimental data it is necessary to allow the existence of the
14
N cluster in the excited state
14
N
*
at an excitation energy of 5.69 MeV and angular momentum
J
π
= 1
–
. It is assumed that in such a case it is possible to use the wave function of the
4
D
1/2
state with respect to the relative motion of the
p
14
N
*
clusters. It is also shown that a description of the S-factor of
p
14
N capture in the resonance region is possible only under the assumption that all of the low-lying resonances at 260(1/2
+
), 987(3/2
+
), 1447(1/2
+
), 2187(3/2
+
), and 3211(3/2
+
) keV in the c.m.s. are
4
D
1/2
and
4
D
3/2
scattering waves.</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s11182-019-01643-w</doi><tpages>8</tpages></addata></record> |
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subjects | Angular momentum Clusters Condensed Matter Physics Hadrons Heavy Ions Lasers Mathematical and Computational Physics Nuclear Physics Nuclei (nuclear physics) Optical Devices Optics Photonics Physics Physics and Astronomy Theoretical |
title | Does the Excited Cluster 14N Exist in the 15O Nucleus? |
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