Dynamics of the Multifragmentation of 1 A GeV Gold on Carbon
An exclusive study of the interaction of 1{ital A}GeV Au with C shows a separability into two stages: a prompt stage involving emission of most {ital Z}=1 and some {ital Z}=2 particles and a second stage involving the decay of an equilibrated remnant, which typically undergoes multifragmentation. Th...
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Veröffentlicht in: | Physical Review Letters 1996-07, Vol.77 (2), p.235-238 |
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creator | Hauger, J. A. Albergo, S. Bieser, F. Brady, F. P. Caccia, Z. Cebra, D. A. Chacon, A. D. Chance, J. L. Choi, Y. Costa, S. Elliott, J. B. Gilkes, M. L. Hirsch, A. S. Hjort, E. L. Insolia, A. Justice, M. Keane, D. Kintner, J. C. Lindenstruth, V. Lisa, M. A. Lynen, U. Matis, H. S. McMahan, M. McParland, C. Müller, W. F. J. Olson, D. L. Partlan, M. D. Porile, N. T. Potenza, R. Rai, G. Rasmussen, J. Ritter, H. G. Romanski, J. Romero, J. L. Russo, G. V. Sann, H. Scharenberg, R. Scott, A. Shao, Y. Srivastava, B. K. Symons, T. J. M. Tincknell, M. Tuvé, C. Wang, S. Warren, P. Wieman, H. H. Wienold, T. Wolf, K. |
description | An exclusive study of the interaction of 1{ital A}GeV Au with C shows a separability into two stages: a prompt stage involving emission of most {ital Z}=1 and some {ital Z}=2 particles and a second stage involving the decay of an equilibrated remnant, which typically undergoes multifragmentation. The mean mass, charge, excitation energy, and the initial temperature {ital T}{sub {ital i}} of the remnant have been determined as a function of the total charge multiplicity, {ital m}, as has the freeze-out temperature {ital T}{sub {ital f}}. Both {ital T}{sub {ital i}} and {ital T}{sub {ital f}} increase linearly with {ital m} and their values at the critical point have been determined. {ital T}{sub {ital f}} rises monotonically with excitation energy as expected for a continuous phase transition. {copyright} {ital 1996 The American Physical Society.} |
doi_str_mv | 10.1103/PhysRevLett.77.235 |
format | Article |
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A. ; Albergo, S. ; Bieser, F. ; Brady, F. P. ; Caccia, Z. ; Cebra, D. A. ; Chacon, A. D. ; Chance, J. L. ; Choi, Y. ; Costa, S. ; Elliott, J. B. ; Gilkes, M. L. ; Hirsch, A. S. ; Hjort, E. L. ; Insolia, A. ; Justice, M. ; Keane, D. ; Kintner, J. C. ; Lindenstruth, V. ; Lisa, M. A. ; Lynen, U. ; Matis, H. S. ; McMahan, M. ; McParland, C. ; Müller, W. F. J. ; Olson, D. L. ; Partlan, M. D. ; Porile, N. T. ; Potenza, R. ; Rai, G. ; Rasmussen, J. ; Ritter, H. G. ; Romanski, J. ; Romero, J. L. ; Russo, G. V. ; Sann, H. ; Scharenberg, R. ; Scott, A. ; Shao, Y. ; Srivastava, B. K. ; Symons, T. J. M. ; Tincknell, M. ; Tuvé, C. ; Wang, S. ; Warren, P. ; Wieman, H. H. ; Wienold, T. ; Wolf, K.</creator><creatorcontrib>Hauger, J. A. ; Albergo, S. ; Bieser, F. ; Brady, F. P. ; Caccia, Z. ; Cebra, D. A. ; Chacon, A. D. ; Chance, J. L. ; Choi, Y. ; Costa, S. ; Elliott, J. B. ; Gilkes, M. L. ; Hirsch, A. S. ; Hjort, E. L. ; Insolia, A. ; Justice, M. ; Keane, D. ; Kintner, J. C. ; Lindenstruth, V. ; Lisa, M. A. ; Lynen, U. ; Matis, H. S. ; McMahan, M. ; McParland, C. ; Müller, W. F. J. ; Olson, D. L. ; Partlan, M. D. ; Porile, N. T. ; Potenza, R. ; Rai, G. ; Rasmussen, J. ; Ritter, H. G. ; Romanski, J. ; Romero, J. L. ; Russo, G. V. ; Sann, H. ; Scharenberg, R. ; Scott, A. ; Shao, Y. ; Srivastava, B. K. ; Symons, T. J. M. ; Tincknell, M. ; Tuvé, C. ; Wang, S. ; Warren, P. ; Wieman, H. H. ; Wienold, T. ; Wolf, K. ; Lawrence Berkeley National Laboratory</creatorcontrib><description>An exclusive study of the interaction of 1{ital A}GeV Au with C shows a separability into two stages: a prompt stage involving emission of most {ital Z}=1 and some {ital Z}=2 particles and a second stage involving the decay of an equilibrated remnant, which typically undergoes multifragmentation. The mean mass, charge, excitation energy, and the initial temperature {ital T}{sub {ital i}} of the remnant have been determined as a function of the total charge multiplicity, {ital m}, as has the freeze-out temperature {ital T}{sub {ital f}}. Both {ital T}{sub {ital i}} and {ital T}{sub {ital f}} increase linearly with {ital m} and their values at the critical point have been determined. {ital T}{sub {ital f}} rises monotonically with excitation energy as expected for a continuous phase transition. {copyright} {ital 1996 The American Physical Society.}</description><identifier>ISSN: 0031-9007</identifier><identifier>EISSN: 1079-7114</identifier><identifier>DOI: 10.1103/PhysRevLett.77.235</identifier><language>eng</language><publisher>United States</publisher><subject>CARBON 12 TARGET ; CHARGES ; DECAY ; DYNAMICS ; EMISSION ; EXCITATION ; FRAGMENTATION ; FREEZING OUT ; GEV RANGE 100-1000 ; GOLD 197 REACTIONS ; MULTIPLICITY ; PHASE TRANSFORMATIONS ; PHYSICS</subject><ispartof>Physical Review Letters, 1996-07, Vol.77 (2), p.235-238</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c1186-26eead93fc21aa8cb2dd5f5e850ad5524cb04193fef2efb5739cd23d65b661e73</citedby><cites>FETCH-LOGICAL-c1186-26eead93fc21aa8cb2dd5f5e850ad5524cb04193fef2efb5739cd23d65b661e73</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>315,782,786,887,2878,2879,27931,27932</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/288756$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Hauger, J. A.</creatorcontrib><creatorcontrib>Albergo, S.</creatorcontrib><creatorcontrib>Bieser, F.</creatorcontrib><creatorcontrib>Brady, F. P.</creatorcontrib><creatorcontrib>Caccia, Z.</creatorcontrib><creatorcontrib>Cebra, D. A.</creatorcontrib><creatorcontrib>Chacon, A. D.</creatorcontrib><creatorcontrib>Chance, J. L.</creatorcontrib><creatorcontrib>Choi, Y.</creatorcontrib><creatorcontrib>Costa, S.</creatorcontrib><creatorcontrib>Elliott, J. B.</creatorcontrib><creatorcontrib>Gilkes, M. L.</creatorcontrib><creatorcontrib>Hirsch, A. S.</creatorcontrib><creatorcontrib>Hjort, E. L.</creatorcontrib><creatorcontrib>Insolia, A.</creatorcontrib><creatorcontrib>Justice, M.</creatorcontrib><creatorcontrib>Keane, D.</creatorcontrib><creatorcontrib>Kintner, J. C.</creatorcontrib><creatorcontrib>Lindenstruth, V.</creatorcontrib><creatorcontrib>Lisa, M. A.</creatorcontrib><creatorcontrib>Lynen, U.</creatorcontrib><creatorcontrib>Matis, H. S.</creatorcontrib><creatorcontrib>McMahan, M.</creatorcontrib><creatorcontrib>McParland, C.</creatorcontrib><creatorcontrib>Müller, W. F. J.</creatorcontrib><creatorcontrib>Olson, D. L.</creatorcontrib><creatorcontrib>Partlan, M. D.</creatorcontrib><creatorcontrib>Porile, N. T.</creatorcontrib><creatorcontrib>Potenza, R.</creatorcontrib><creatorcontrib>Rai, G.</creatorcontrib><creatorcontrib>Rasmussen, J.</creatorcontrib><creatorcontrib>Ritter, H. G.</creatorcontrib><creatorcontrib>Romanski, J.</creatorcontrib><creatorcontrib>Romero, J. L.</creatorcontrib><creatorcontrib>Russo, G. V.</creatorcontrib><creatorcontrib>Sann, H.</creatorcontrib><creatorcontrib>Scharenberg, R.</creatorcontrib><creatorcontrib>Scott, A.</creatorcontrib><creatorcontrib>Shao, Y.</creatorcontrib><creatorcontrib>Srivastava, B. K.</creatorcontrib><creatorcontrib>Symons, T. J. M.</creatorcontrib><creatorcontrib>Tincknell, M.</creatorcontrib><creatorcontrib>Tuvé, C.</creatorcontrib><creatorcontrib>Wang, S.</creatorcontrib><creatorcontrib>Warren, P.</creatorcontrib><creatorcontrib>Wieman, H. H.</creatorcontrib><creatorcontrib>Wienold, T.</creatorcontrib><creatorcontrib>Wolf, K.</creatorcontrib><creatorcontrib>Lawrence Berkeley National Laboratory</creatorcontrib><title>Dynamics of the Multifragmentation of 1 A GeV Gold on Carbon</title><title>Physical Review Letters</title><description>An exclusive study of the interaction of 1{ital A}GeV Au with C shows a separability into two stages: a prompt stage involving emission of most {ital Z}=1 and some {ital Z}=2 particles and a second stage involving the decay of an equilibrated remnant, which typically undergoes multifragmentation. The mean mass, charge, excitation energy, and the initial temperature {ital T}{sub {ital i}} of the remnant have been determined as a function of the total charge multiplicity, {ital m}, as has the freeze-out temperature {ital T}{sub {ital f}}. Both {ital T}{sub {ital i}} and {ital T}{sub {ital f}} increase linearly with {ital m} and their values at the critical point have been determined. {ital T}{sub {ital f}} rises monotonically with excitation energy as expected for a continuous phase transition. {copyright} {ital 1996 The American Physical Society.}</description><subject>CARBON 12 TARGET</subject><subject>CHARGES</subject><subject>DECAY</subject><subject>DYNAMICS</subject><subject>EMISSION</subject><subject>EXCITATION</subject><subject>FRAGMENTATION</subject><subject>FREEZING OUT</subject><subject>GEV RANGE 100-1000</subject><subject>GOLD 197 REACTIONS</subject><subject>MULTIPLICITY</subject><subject>PHASE TRANSFORMATIONS</subject><subject>PHYSICS</subject><issn>0031-9007</issn><issn>1079-7114</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1996</creationdate><recordtype>article</recordtype><recordid>eNpNkMFKAzEURYMoWKs_4Cp-wNS8ZJLMgJtS7ShUFFG3IZO82JF2IpMo9O-dUheuLtx7uItDyCWwGQAT18_rXXrBnxXmPNN6xoU8IhNgui40QHlMJowJKGrG9Ck5S-mTMQZcVRNyc7vr7bZzicZA8xrp4_cmd2GwH1vss81d7PcL0Dlt8J02cePpWC3s0Mb-nJwEu0l48ZdT8ra8e13cF6un5mExXxUOoFIFV4jW1yI4DtZWruXeyyCxksx6KXnpWlbCuGPgGFqpRe08F17JVilALabk6vAbU-5Mcl1Gt3ax79Flw6tKSzUy_MC4IaY0YDBfQ7e1w84AM3tH5p8jo7UZHYlf9rVcRw</recordid><startdate>199607</startdate><enddate>199607</enddate><creator>Hauger, J. 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A. ; Lynen, U. ; Matis, H. S. ; McMahan, M. ; McParland, C. ; Müller, W. F. J. ; Olson, D. L. ; Partlan, M. D. ; Porile, N. T. ; Potenza, R. ; Rai, G. ; Rasmussen, J. ; Ritter, H. G. ; Romanski, J. ; Romero, J. L. ; Russo, G. V. ; Sann, H. ; Scharenberg, R. ; Scott, A. ; Shao, Y. ; Srivastava, B. K. ; Symons, T. J. M. ; Tincknell, M. ; Tuvé, C. ; Wang, S. ; Warren, P. ; Wieman, H. 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H.</creatorcontrib><creatorcontrib>Wienold, T.</creatorcontrib><creatorcontrib>Wolf, K.</creatorcontrib><creatorcontrib>Lawrence Berkeley National Laboratory</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Physical Review Letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Hauger, J. A.</au><au>Albergo, S.</au><au>Bieser, F.</au><au>Brady, F. P.</au><au>Caccia, Z.</au><au>Cebra, D. A.</au><au>Chacon, A. D.</au><au>Chance, J. L.</au><au>Choi, Y.</au><au>Costa, S.</au><au>Elliott, J. B.</au><au>Gilkes, M. L.</au><au>Hirsch, A. S.</au><au>Hjort, E. L.</au><au>Insolia, A.</au><au>Justice, M.</au><au>Keane, D.</au><au>Kintner, J. C.</au><au>Lindenstruth, V.</au><au>Lisa, M. A.</au><au>Lynen, U.</au><au>Matis, H. S.</au><au>McMahan, M.</au><au>McParland, C.</au><au>Müller, W. F. J.</au><au>Olson, D. L.</au><au>Partlan, M. D.</au><au>Porile, N. T.</au><au>Potenza, R.</au><au>Rai, G.</au><au>Rasmussen, J.</au><au>Ritter, H. G.</au><au>Romanski, J.</au><au>Romero, J. L.</au><au>Russo, G. V.</au><au>Sann, H.</au><au>Scharenberg, R.</au><au>Scott, A.</au><au>Shao, Y.</au><au>Srivastava, B. K.</au><au>Symons, T. J. M.</au><au>Tincknell, M.</au><au>Tuvé, C.</au><au>Wang, S.</au><au>Warren, P.</au><au>Wieman, H. H.</au><au>Wienold, T.</au><au>Wolf, K.</au><aucorp>Lawrence Berkeley National Laboratory</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Dynamics of the Multifragmentation of 1 A GeV Gold on Carbon</atitle><jtitle>Physical Review Letters</jtitle><date>1996-07</date><risdate>1996</risdate><volume>77</volume><issue>2</issue><spage>235</spage><epage>238</epage><pages>235-238</pages><issn>0031-9007</issn><eissn>1079-7114</eissn><abstract>An exclusive study of the interaction of 1{ital A}GeV Au with C shows a separability into two stages: a prompt stage involving emission of most {ital Z}=1 and some {ital Z}=2 particles and a second stage involving the decay of an equilibrated remnant, which typically undergoes multifragmentation. The mean mass, charge, excitation energy, and the initial temperature {ital T}{sub {ital i}} of the remnant have been determined as a function of the total charge multiplicity, {ital m}, as has the freeze-out temperature {ital T}{sub {ital f}}. Both {ital T}{sub {ital i}} and {ital T}{sub {ital f}} increase linearly with {ital m} and their values at the critical point have been determined. {ital T}{sub {ital f}} rises monotonically with excitation energy as expected for a continuous phase transition. {copyright} {ital 1996 The American Physical Society.}</abstract><cop>United States</cop><doi>10.1103/PhysRevLett.77.235</doi><tpages>4</tpages></addata></record> |
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source | American Physical Society Journals |
subjects | CARBON 12 TARGET CHARGES DECAY DYNAMICS EMISSION EXCITATION FRAGMENTATION FREEZING OUT GEV RANGE 100-1000 GOLD 197 REACTIONS MULTIPLICITY PHASE TRANSFORMATIONS PHYSICS |
title | Dynamics of the Multifragmentation of 1 A GeV Gold on Carbon |
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