The Hagedorn transition in noncommutative open string theory
The Hagedorn transition in noncommutative open string theory (NCOS) is relatively simple because gravity decouples. For NCOS theories in no more than five space–time dimensions, the Hagedorn transition is second order, and the high temperature phase involves long, nearly straight fundamental strings...
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Veröffentlicht in: | Journal of mathematical physics 2001-07, Vol.42 (7), p.2749-2764 |
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creator | Gubser, S. S. Gukov, S. Klebanov, I. R. Rangamani, M. Witten, E. |
description | The Hagedorn transition in noncommutative open string theory (NCOS) is relatively simple because gravity decouples. For NCOS theories in no more than five space–time dimensions, the Hagedorn transition is second order, and the high temperature phase involves long, nearly straight fundamental strings separating from the D-brane on which the NCOS theory is defined. Above five spacetime dimensions interaction effects become important below the Hagedorn temperature. Although this complicates studies of the transition, we believe that the high temperature phase again involves long strings liberated from the bound state. |
doi_str_mv | 10.1063/1.1372176 |
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S.</creatorcontrib><creatorcontrib>Gukov, S.</creatorcontrib><creatorcontrib>Klebanov, I. R.</creatorcontrib><creatorcontrib>Rangamani, M.</creatorcontrib><creatorcontrib>Witten, E.</creatorcontrib><creatorcontrib>Princeton Univ., NJ (United States)</creatorcontrib><title>The Hagedorn transition in noncommutative open string theory</title><title>Journal of mathematical physics</title><description>The Hagedorn transition in noncommutative open string theory (NCOS) is relatively simple because gravity decouples. For NCOS theories in no more than five space–time dimensions, the Hagedorn transition is second order, and the high temperature phase involves long, nearly straight fundamental strings separating from the D-brane on which the NCOS theory is defined. Above five spacetime dimensions interaction effects become important below the Hagedorn temperature. Although this complicates studies of the transition, we believe that the high temperature phase again involves long strings liberated from the bound state.</description><subject>BOUND STATE</subject><subject>CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS</subject><subject>DIFFERENTIAL GEOMETRY</subject><subject>DIMENSIONS</subject><subject>FIELD THEORIES</subject><issn>0022-2488</issn><issn>1089-7658</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2001</creationdate><recordtype>article</recordtype><recordid>eNqd0EFLAzEQBeAgCtbqwX-w4ElhaybZ3WTBixS1QsFLPYc0mbQRNylJLPTf29KCd09z-Xi8eYTcAp0A7fgjTIALBqI7IyOgsq9F18pzMqKUsZo1Ul6Sq5y_KAWQTTMiT4s1VjO9QhtTqErSIfviY6h8qEIMJg7DT9HFb7GKGwxVLsmHVVXWGNPumlw4_Z3x5nTH5PP1ZTGd1fOPt_fp87w2DetKbRxF6VojJKW610bikltLGW8dX4rOLlEgGJAt6B73vYy1HKF1xnaGNk7wMbk75sZcvMrGFzRrE0NAU1RDmRCih726PyqTYs4JndokP-i0U0DVYRwF6jTO3j4c7SFMHx7-H97G9AfVxjr-Cw23c1Y</recordid><startdate>200107</startdate><enddate>200107</enddate><creator>Gubser, S. 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R.</creatorcontrib><creatorcontrib>Rangamani, M.</creatorcontrib><creatorcontrib>Witten, E.</creatorcontrib><creatorcontrib>Princeton Univ., NJ (United States)</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Journal of mathematical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Gubser, S. S.</au><au>Gukov, S.</au><au>Klebanov, I. R.</au><au>Rangamani, M.</au><au>Witten, E.</au><aucorp>Princeton Univ., NJ (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The Hagedorn transition in noncommutative open string theory</atitle><jtitle>Journal of mathematical physics</jtitle><date>2001-07</date><risdate>2001</risdate><volume>42</volume><issue>7</issue><spage>2749</spage><epage>2764</epage><pages>2749-2764</pages><issn>0022-2488</issn><eissn>1089-7658</eissn><coden>JMAPAQ</coden><abstract>The Hagedorn transition in noncommutative open string theory (NCOS) is relatively simple because gravity decouples. For NCOS theories in no more than five space–time dimensions, the Hagedorn transition is second order, and the high temperature phase involves long, nearly straight fundamental strings separating from the D-brane on which the NCOS theory is defined. Above five spacetime dimensions interaction effects become important below the Hagedorn temperature. Although this complicates studies of the transition, we believe that the high temperature phase again involves long strings liberated from the bound state.</abstract><cop>United States</cop><pub>The American Physical Society</pub><doi>10.1063/1.1372176</doi><tpages>16</tpages><oa>free_for_read</oa></addata></record> |
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subjects | BOUND STATE CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS DIFFERENTIAL GEOMETRY DIMENSIONS FIELD THEORIES |
title | The Hagedorn transition in noncommutative open string theory |
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