Energy and angular distributions of neutrons from 90 MeV proton and 140 MeV alpha-particle bombardment of nuclei
We measured neutron time-of-flight spectra from 90 MeV protons and 140 MeV alpha particles bombarding thin targets of Al, Ni, Zr, and Bi at laboratory angles between 20/sup 0/ and 135/sup 0/. The low-energy (5 to 45 MeV) portions of the spectra were measured with 5 cm diameter by 5 cm deep NE-213 co...
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Veröffentlicht in: | Phys. Rev. C; (United States) 1983-07, Vol.28 (1), p.105-119 |
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creator | Kalend, A. M. Anderson, B. D. Baldwin, A. R. Madey, R. Watson, J. W. Chang, C. C. Holmgren, H. D. Koontz, R. W. Wu, J. R. Machner, H. |
description | We measured neutron time-of-flight spectra from 90 MeV protons and 140 MeV alpha particles bombarding thin targets of Al, Ni, Zr, and Bi at laboratory angles between 20/sup 0/ and 135/sup 0/. The low-energy (5 to 45 MeV) portions of the spectra were measured with 5 cm diameter by 5 cm deep NE-213 counters at 1 m flight paths with n-..gamma.. pulse-shape discrimination. The high-energy (35 to 150 MeV) portions of the spectra were measured with 12.7 cm diameter by 10.2 cm deep NE-102 counters at flight paths of 2.0 to 5.0 m. The proton-induced measured neutron spectra reveal three distinct energy regions: a low-energy evaporation region, a high-energy region dominated by the quasifree scattering process, and an intermediate-energy region dominated by multistep, preequilibrium processes. In the latter two regions, the spectra show strong angular dependence. The alpha-particle induced neutron spectra show these same distinct energy regions plus an exponential falloff above the beam energy per nucleon. The neutron spectra are compared with earlier proton spectra produced also by 90 MeV protons and 140 MeV alpha particles. It is observed that the high-energy portions of the forward-angle neutron and proton cross sections are in ratios consistent with the idea that single nucleon-nucleon scattering dominates. For the heavy-mass targets, the low-energy evaporation regions show neutron yields larger than proton yields. The proton-to-neutron ratios observed in the high-energy continua are interpreted with a quasifree calculation fitted simultaneously to the proton and the neutron spectra. Preequilibrium calculations with the exciton model and the hybrid model reproduce the shape of the experimental angle-integrated energy spectra down to lower energies than the quasifree calculations. The exciton model calculations underestimate the magnitudes of the cross sections, while the hybrid model provides better absolute agreement. |
doi_str_mv | 10.1103/PhysRevC.28.105 |
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fullrecord | <record><control><sourceid>crossref_osti_</sourceid><recordid>TN_cdi_crossref_primary_10_1103_PhysRevC_28_105</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>10_1103_PhysRevC_28_105</sourcerecordid><originalsourceid>FETCH-LOGICAL-c332t-db4bff4c7b50018f8958eb71227dd2d2f81e8cefb36ac939418a06243a372ea63</originalsourceid><addsrcrecordid>eNo1kEtLAzEUhbNQsFbXboP7afOYzGSWUqoWKoqo2yHPNjKTDElG6L932uqFyz18nHsWB4A7jBYYI7p82x_Su_lZLQhfYMQuwAwxVhWEY3oFrlP6RtNQWs3AsPYm7g5QeD3tbuxEhNqlHJ0csws-wWChN2OOR21j6GGD4Iv5gkMMOfjTIy7PSHTDXhSDiNmpzkAZeimi7o3Pp5Rxgu4GXFrRJXP7d-fg83H9sXoutq9Pm9XDtlCUklxoWUprS1VLhhDmljeMG1ljQmqtiSaWY8OVsZJWQjW0KTEXqCIlFbQmRlR0Du7PuSFl1yblslF7Fbw3KresQQ0v68m0PJtUDClFY9shul7EQ4tRe2yy_W-yJXxijP4CWZJrAg</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Energy and angular distributions of neutrons from 90 MeV proton and 140 MeV alpha-particle bombardment of nuclei</title><source>American Physical Society Journals</source><creator>Kalend, A. M. ; Anderson, B. D. ; Baldwin, A. R. ; Madey, R. ; Watson, J. W. ; Chang, C. C. ; Holmgren, H. D. ; Koontz, R. W. ; Wu, J. R. ; Machner, H.</creator><creatorcontrib>Kalend, A. M. ; Anderson, B. D. ; Baldwin, A. R. ; Madey, R. ; Watson, J. W. ; Chang, C. C. ; Holmgren, H. D. ; Koontz, R. W. ; Wu, J. R. ; Machner, H. ; Department of Physics, Kent State University, Kent, Ohio 44242</creatorcontrib><description>We measured neutron time-of-flight spectra from 90 MeV protons and 140 MeV alpha particles bombarding thin targets of Al, Ni, Zr, and Bi at laboratory angles between 20/sup 0/ and 135/sup 0/. The low-energy (5 to 45 MeV) portions of the spectra were measured with 5 cm diameter by 5 cm deep NE-213 counters at 1 m flight paths with n-..gamma.. pulse-shape discrimination. The high-energy (35 to 150 MeV) portions of the spectra were measured with 12.7 cm diameter by 10.2 cm deep NE-102 counters at flight paths of 2.0 to 5.0 m. The proton-induced measured neutron spectra reveal three distinct energy regions: a low-energy evaporation region, a high-energy region dominated by the quasifree scattering process, and an intermediate-energy region dominated by multistep, preequilibrium processes. In the latter two regions, the spectra show strong angular dependence. The alpha-particle induced neutron spectra show these same distinct energy regions plus an exponential falloff above the beam energy per nucleon. The neutron spectra are compared with earlier proton spectra produced also by 90 MeV protons and 140 MeV alpha particles. It is observed that the high-energy portions of the forward-angle neutron and proton cross sections are in ratios consistent with the idea that single nucleon-nucleon scattering dominates. For the heavy-mass targets, the low-energy evaporation regions show neutron yields larger than proton yields. The proton-to-neutron ratios observed in the high-energy continua are interpreted with a quasifree calculation fitted simultaneously to the proton and the neutron spectra. Preequilibrium calculations with the exciton model and the hybrid model reproduce the shape of the experimental angle-integrated energy spectra down to lower energies than the quasifree calculations. The exciton model calculations underestimate the magnitudes of the cross sections, while the hybrid model provides better absolute agreement.</description><identifier>ISSN: 0556-2813</identifier><identifier>DOI: 10.1103/PhysRevC.28.105</identifier><language>eng</language><publisher>United States</publisher><subject><![CDATA[651425 - Nuclear Properties & Reactions, A=20-38, Experimental- Nuclear Reactions & Scattering- (-1987) ; 651525 - Nuclear Properties & Reactions, A=39-58, Experimental- Nuclear Reactions & Scattering- (-1987) ; 651725 - Nuclear Properties & Reactions, A=90-149, Experimental- Nuclear Reactions & Scattering- (-1987) ; 651925 - Nuclear Properties & Reactions, A=190-219, Experimental- Nuclear Reactions & Scattering- (-1987) ; ALPHA REACTIONS ; ALUMINIUM 27 TARGET ; ANGULAR DISTRIBUTION ; BARYON REACTIONS ; BISMUTH 209 TARGET ; CHARGED-PARTICLE REACTIONS ; CROSS SECTIONS ; DATA ; DIFFERENTIAL CROSS SECTIONS ; DIRECT REACTIONS ; DISTRIBUTION ; ENERGY RANGE ; ENERGY SPECTRA ; EXPERIMENTAL DATA ; HADRON REACTIONS ; IMPULSE APPROXIMATION ; INFORMATION ; MEV RANGE ; MEV RANGE 10-100 ; MEV RANGE 100-1000 ; NEUTRON SPECTRA ; NICKEL 58 TARGET ; NUCLEAR CASCADES ; NUCLEAR PHYSICS AND RADIATION PHYSICS ; NUCLEAR REACTIONS ; NUCLEON REACTIONS ; NUMERICAL DATA ; PARTIAL WAVES ; PRECOMPOUND-NUCLEUS EMISSION ; PROTON REACTIONS ; QUASI-FREE REACTIONS ; SPECTRA ; TARGETS ; ZIRCONIUM 90 TARGET]]></subject><ispartof>Phys. Rev. C; (United States), 1983-07, Vol.28 (1), p.105-119</ispartof><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c332t-db4bff4c7b50018f8958eb71227dd2d2f81e8cefb36ac939418a06243a372ea63</citedby><cites>FETCH-LOGICAL-c332t-db4bff4c7b50018f8958eb71227dd2d2f81e8cefb36ac939418a06243a372ea63</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,881,2862,2863,27903,27904</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/5909847$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Kalend, A. M.</creatorcontrib><creatorcontrib>Anderson, B. D.</creatorcontrib><creatorcontrib>Baldwin, A. R.</creatorcontrib><creatorcontrib>Madey, R.</creatorcontrib><creatorcontrib>Watson, J. W.</creatorcontrib><creatorcontrib>Chang, C. C.</creatorcontrib><creatorcontrib>Holmgren, H. D.</creatorcontrib><creatorcontrib>Koontz, R. W.</creatorcontrib><creatorcontrib>Wu, J. R.</creatorcontrib><creatorcontrib>Machner, H.</creatorcontrib><creatorcontrib>Department of Physics, Kent State University, Kent, Ohio 44242</creatorcontrib><title>Energy and angular distributions of neutrons from 90 MeV proton and 140 MeV alpha-particle bombardment of nuclei</title><title>Phys. Rev. C; (United States)</title><description>We measured neutron time-of-flight spectra from 90 MeV protons and 140 MeV alpha particles bombarding thin targets of Al, Ni, Zr, and Bi at laboratory angles between 20/sup 0/ and 135/sup 0/. The low-energy (5 to 45 MeV) portions of the spectra were measured with 5 cm diameter by 5 cm deep NE-213 counters at 1 m flight paths with n-..gamma.. pulse-shape discrimination. The high-energy (35 to 150 MeV) portions of the spectra were measured with 12.7 cm diameter by 10.2 cm deep NE-102 counters at flight paths of 2.0 to 5.0 m. The proton-induced measured neutron spectra reveal three distinct energy regions: a low-energy evaporation region, a high-energy region dominated by the quasifree scattering process, and an intermediate-energy region dominated by multistep, preequilibrium processes. In the latter two regions, the spectra show strong angular dependence. The alpha-particle induced neutron spectra show these same distinct energy regions plus an exponential falloff above the beam energy per nucleon. The neutron spectra are compared with earlier proton spectra produced also by 90 MeV protons and 140 MeV alpha particles. It is observed that the high-energy portions of the forward-angle neutron and proton cross sections are in ratios consistent with the idea that single nucleon-nucleon scattering dominates. For the heavy-mass targets, the low-energy evaporation regions show neutron yields larger than proton yields. The proton-to-neutron ratios observed in the high-energy continua are interpreted with a quasifree calculation fitted simultaneously to the proton and the neutron spectra. Preequilibrium calculations with the exciton model and the hybrid model reproduce the shape of the experimental angle-integrated energy spectra down to lower energies than the quasifree calculations. The exciton model calculations underestimate the magnitudes of the cross sections, while the hybrid model provides better absolute agreement.</description><subject>651425 - Nuclear Properties & Reactions, A=20-38, Experimental- Nuclear Reactions & Scattering- (-1987)</subject><subject>651525 - Nuclear Properties & Reactions, A=39-58, Experimental- Nuclear Reactions & Scattering- (-1987)</subject><subject>651725 - Nuclear Properties & Reactions, A=90-149, Experimental- Nuclear Reactions & Scattering- (-1987)</subject><subject>651925 - Nuclear Properties & Reactions, A=190-219, Experimental- Nuclear Reactions & Scattering- (-1987)</subject><subject>ALPHA REACTIONS</subject><subject>ALUMINIUM 27 TARGET</subject><subject>ANGULAR DISTRIBUTION</subject><subject>BARYON REACTIONS</subject><subject>BISMUTH 209 TARGET</subject><subject>CHARGED-PARTICLE REACTIONS</subject><subject>CROSS SECTIONS</subject><subject>DATA</subject><subject>DIFFERENTIAL CROSS SECTIONS</subject><subject>DIRECT REACTIONS</subject><subject>DISTRIBUTION</subject><subject>ENERGY RANGE</subject><subject>ENERGY SPECTRA</subject><subject>EXPERIMENTAL DATA</subject><subject>HADRON REACTIONS</subject><subject>IMPULSE APPROXIMATION</subject><subject>INFORMATION</subject><subject>MEV RANGE</subject><subject>MEV RANGE 10-100</subject><subject>MEV RANGE 100-1000</subject><subject>NEUTRON SPECTRA</subject><subject>NICKEL 58 TARGET</subject><subject>NUCLEAR CASCADES</subject><subject>NUCLEAR PHYSICS AND RADIATION PHYSICS</subject><subject>NUCLEAR REACTIONS</subject><subject>NUCLEON REACTIONS</subject><subject>NUMERICAL DATA</subject><subject>PARTIAL WAVES</subject><subject>PRECOMPOUND-NUCLEUS EMISSION</subject><subject>PROTON REACTIONS</subject><subject>QUASI-FREE REACTIONS</subject><subject>SPECTRA</subject><subject>TARGETS</subject><subject>ZIRCONIUM 90 TARGET</subject><issn>0556-2813</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1983</creationdate><recordtype>article</recordtype><recordid>eNo1kEtLAzEUhbNQsFbXboP7afOYzGSWUqoWKoqo2yHPNjKTDElG6L932uqFyz18nHsWB4A7jBYYI7p82x_Su_lZLQhfYMQuwAwxVhWEY3oFrlP6RtNQWs3AsPYm7g5QeD3tbuxEhNqlHJ0csws-wWChN2OOR21j6GGD4Iv5gkMMOfjTIy7PSHTDXhSDiNmpzkAZeimi7o3Pp5Rxgu4GXFrRJXP7d-fg83H9sXoutq9Pm9XDtlCUklxoWUprS1VLhhDmljeMG1ljQmqtiSaWY8OVsZJWQjW0KTEXqCIlFbQmRlR0Du7PuSFl1yblslF7Fbw3KresQQ0v68m0PJtUDClFY9shul7EQ4tRe2yy_W-yJXxijP4CWZJrAg</recordid><startdate>19830701</startdate><enddate>19830701</enddate><creator>Kalend, A. M.</creator><creator>Anderson, B. D.</creator><creator>Baldwin, A. R.</creator><creator>Madey, R.</creator><creator>Watson, J. W.</creator><creator>Chang, C. C.</creator><creator>Holmgren, H. D.</creator><creator>Koontz, R. W.</creator><creator>Wu, J. R.</creator><creator>Machner, H.</creator><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope></search><sort><creationdate>19830701</creationdate><title>Energy and angular distributions of neutrons from 90 MeV proton and 140 MeV alpha-particle bombardment of nuclei</title><author>Kalend, A. M. ; Anderson, B. D. ; Baldwin, A. R. ; Madey, R. ; Watson, J. W. ; Chang, C. C. ; Holmgren, H. D. ; Koontz, R. W. ; Wu, J. 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M.</creatorcontrib><creatorcontrib>Anderson, B. D.</creatorcontrib><creatorcontrib>Baldwin, A. R.</creatorcontrib><creatorcontrib>Madey, R.</creatorcontrib><creatorcontrib>Watson, J. W.</creatorcontrib><creatorcontrib>Chang, C. C.</creatorcontrib><creatorcontrib>Holmgren, H. D.</creatorcontrib><creatorcontrib>Koontz, R. W.</creatorcontrib><creatorcontrib>Wu, J. R.</creatorcontrib><creatorcontrib>Machner, H.</creatorcontrib><creatorcontrib>Department of Physics, Kent State University, Kent, Ohio 44242</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Phys. Rev. C; (United States)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kalend, A. M.</au><au>Anderson, B. D.</au><au>Baldwin, A. R.</au><au>Madey, R.</au><au>Watson, J. W.</au><au>Chang, C. C.</au><au>Holmgren, H. D.</au><au>Koontz, R. W.</au><au>Wu, J. R.</au><au>Machner, H.</au><aucorp>Department of Physics, Kent State University, Kent, Ohio 44242</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Energy and angular distributions of neutrons from 90 MeV proton and 140 MeV alpha-particle bombardment of nuclei</atitle><jtitle>Phys. Rev. C; (United States)</jtitle><date>1983-07-01</date><risdate>1983</risdate><volume>28</volume><issue>1</issue><spage>105</spage><epage>119</epage><pages>105-119</pages><issn>0556-2813</issn><abstract>We measured neutron time-of-flight spectra from 90 MeV protons and 140 MeV alpha particles bombarding thin targets of Al, Ni, Zr, and Bi at laboratory angles between 20/sup 0/ and 135/sup 0/. The low-energy (5 to 45 MeV) portions of the spectra were measured with 5 cm diameter by 5 cm deep NE-213 counters at 1 m flight paths with n-..gamma.. pulse-shape discrimination. The high-energy (35 to 150 MeV) portions of the spectra were measured with 12.7 cm diameter by 10.2 cm deep NE-102 counters at flight paths of 2.0 to 5.0 m. The proton-induced measured neutron spectra reveal three distinct energy regions: a low-energy evaporation region, a high-energy region dominated by the quasifree scattering process, and an intermediate-energy region dominated by multistep, preequilibrium processes. In the latter two regions, the spectra show strong angular dependence. The alpha-particle induced neutron spectra show these same distinct energy regions plus an exponential falloff above the beam energy per nucleon. The neutron spectra are compared with earlier proton spectra produced also by 90 MeV protons and 140 MeV alpha particles. It is observed that the high-energy portions of the forward-angle neutron and proton cross sections are in ratios consistent with the idea that single nucleon-nucleon scattering dominates. For the heavy-mass targets, the low-energy evaporation regions show neutron yields larger than proton yields. The proton-to-neutron ratios observed in the high-energy continua are interpreted with a quasifree calculation fitted simultaneously to the proton and the neutron spectra. Preequilibrium calculations with the exciton model and the hybrid model reproduce the shape of the experimental angle-integrated energy spectra down to lower energies than the quasifree calculations. The exciton model calculations underestimate the magnitudes of the cross sections, while the hybrid model provides better absolute agreement.</abstract><cop>United States</cop><doi>10.1103/PhysRevC.28.105</doi><tpages>15</tpages></addata></record> |
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subjects | 651425 - Nuclear Properties & Reactions, A=20-38, Experimental- Nuclear Reactions & Scattering- (-1987) 651525 - Nuclear Properties & Reactions, A=39-58, Experimental- Nuclear Reactions & Scattering- (-1987) 651725 - Nuclear Properties & Reactions, A=90-149, Experimental- Nuclear Reactions & Scattering- (-1987) 651925 - Nuclear Properties & Reactions, A=190-219, Experimental- Nuclear Reactions & Scattering- (-1987) ALPHA REACTIONS ALUMINIUM 27 TARGET ANGULAR DISTRIBUTION BARYON REACTIONS BISMUTH 209 TARGET CHARGED-PARTICLE REACTIONS CROSS SECTIONS DATA DIFFERENTIAL CROSS SECTIONS DIRECT REACTIONS DISTRIBUTION ENERGY RANGE ENERGY SPECTRA EXPERIMENTAL DATA HADRON REACTIONS IMPULSE APPROXIMATION INFORMATION MEV RANGE MEV RANGE 10-100 MEV RANGE 100-1000 NEUTRON SPECTRA NICKEL 58 TARGET NUCLEAR CASCADES NUCLEAR PHYSICS AND RADIATION PHYSICS NUCLEAR REACTIONS NUCLEON REACTIONS NUMERICAL DATA PARTIAL WAVES PRECOMPOUND-NUCLEUS EMISSION PROTON REACTIONS QUASI-FREE REACTIONS SPECTRA TARGETS ZIRCONIUM 90 TARGET |
title | Energy and angular distributions of neutrons from 90 MeV proton and 140 MeV alpha-particle bombardment of nuclei |
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