The phantom term in open string field theory
A bstract We show that given any two classical solutions in open string field theory and a singular gauge transformation relating them, it is possible to write the second solution as a gauge transformation of the first plus a singular, projector-like state which describes the shift in the open strin...
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creator | Erler, Theodore Maccaferri, Carlo |
description | A
bstract
We show that given any two classical solutions in open string field theory and a singular gauge transformation relating them, it is possible to write the second solution as a gauge transformation of the first plus a singular, projector-like state which describes the shift in the open string background between the two solutions. This is the “phantom term.” We give some applications in the computation of gauge invariant observables. |
doi_str_mv | 10.1007/JHEP06(2012)084 |
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bstract
We show that given any two classical solutions in open string field theory and a singular gauge transformation relating them, it is possible to write the second solution as a gauge transformation of the first plus a singular, projector-like state which describes the shift in the open string background between the two solutions. This is the “phantom term.” We give some applications in the computation of gauge invariant observables.</description><identifier>ISSN: 1029-8479</identifier><identifier>EISSN: 1029-8479</identifier><identifier>DOI: 10.1007/JHEP06(2012)084</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer Berlin Heidelberg</publisher><subject>Classical and Quantum Gravitation ; Elementary Particles ; Field theory ; High energy physics ; Physics ; Physics and Astronomy ; Quantum Field Theories ; Quantum Field Theory ; Quantum Physics ; Relativity Theory ; String Theory ; Strings</subject><ispartof>The journal of high energy physics, 2012-06, Vol.2012 (6), Article 84</ispartof><rights>SISSA, Trieste, Italy 2012</rights><rights>SISSA, Trieste, Italy 2012.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c376t-40e636d40a77db2e3feb0097aeffe8dc2c49945babb001407b26fba9ec9e67a23</citedby><cites>FETCH-LOGICAL-c376t-40e636d40a77db2e3feb0097aeffe8dc2c49945babb001407b26fba9ec9e67a23</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/JHEP06(2012)084$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://doi.org/10.1007/JHEP06(2012)084$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,776,780,27903,27904,41099,41467,42168,42536,51297,51554</link.rule.ids><linktorsrc>$$Uhttps://doi.org/10.1007/JHEP06(2012)084$$EView_record_in_Springer_Nature$$FView_record_in_$$GSpringer_Nature</linktorsrc></links><search><creatorcontrib>Erler, Theodore</creatorcontrib><creatorcontrib>Maccaferri, Carlo</creatorcontrib><title>The phantom term in open string field theory</title><title>The journal of high energy physics</title><addtitle>J. High Energ. Phys</addtitle><description>A
bstract
We show that given any two classical solutions in open string field theory and a singular gauge transformation relating them, it is possible to write the second solution as a gauge transformation of the first plus a singular, projector-like state which describes the shift in the open string background between the two solutions. This is the “phantom term.” We give some applications in the computation of gauge invariant observables.</description><subject>Classical and Quantum Gravitation</subject><subject>Elementary Particles</subject><subject>Field theory</subject><subject>High energy physics</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Field Theories</subject><subject>Quantum Field Theory</subject><subject>Quantum Physics</subject><subject>Relativity Theory</subject><subject>String Theory</subject><subject>Strings</subject><issn>1029-8479</issn><issn>1029-8479</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNp1kM1Lw0AQxRdRsFbPXhe8KBg7-5Fs9iilWqWgh3peNsmsSWk-3E0P_e9NiKAXTzMM773h_Qi5ZvDAANTidb16h-SWA-N3kMoTMmPAdZRKpU__7OfkIoQdAIuZhhm535ZIu9I2fVvTHn1Nq4a2HTY09L5qPqmrcF_QvsTWHy_JmbP7gFc_c04-nlbb5TravD2_LB83US5U0kcSMBFJIcEqVWQchcMMQCuLzmFa5DyXWss4s9lwZhJUxhOXWY25xkRZLubkZsrtfPt1wNCbXXvwzfDScKFTIZmK2aBaTKrctyF4dKbzVW390TAwIxIzITEjEjMgGRwwOUI3dkP_m_uf5RtRGmI_</recordid><startdate>20120601</startdate><enddate>20120601</enddate><creator>Erler, Theodore</creator><creator>Maccaferri, Carlo</creator><general>Springer Berlin Heidelberg</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>P5Z</scope><scope>P62</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope></search><sort><creationdate>20120601</creationdate><title>The phantom term in open string field theory</title><author>Erler, Theodore ; Maccaferri, Carlo</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c376t-40e636d40a77db2e3feb0097aeffe8dc2c49945babb001407b26fba9ec9e67a23</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Classical and Quantum Gravitation</topic><topic>Elementary Particles</topic><topic>Field theory</topic><topic>High energy physics</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Quantum Field Theories</topic><topic>Quantum Field Theory</topic><topic>Quantum Physics</topic><topic>Relativity Theory</topic><topic>String Theory</topic><topic>Strings</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Erler, Theodore</creatorcontrib><creatorcontrib>Maccaferri, Carlo</creatorcontrib><collection>CrossRef</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central UK/Ireland</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest advanced technologies & aerospace journals</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><jtitle>The journal of high energy physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Erler, Theodore</au><au>Maccaferri, Carlo</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The phantom term in open string field theory</atitle><jtitle>The journal of high energy physics</jtitle><stitle>J. High Energ. Phys</stitle><date>2012-06-01</date><risdate>2012</risdate><volume>2012</volume><issue>6</issue><artnum>84</artnum><issn>1029-8479</issn><eissn>1029-8479</eissn><abstract>A
bstract
We show that given any two classical solutions in open string field theory and a singular gauge transformation relating them, it is possible to write the second solution as a gauge transformation of the first plus a singular, projector-like state which describes the shift in the open string background between the two solutions. This is the “phantom term.” We give some applications in the computation of gauge invariant observables.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1007/JHEP06(2012)084</doi><oa>free_for_read</oa></addata></record> |
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subjects | Classical and Quantum Gravitation Elementary Particles Field theory High energy physics Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Quantum Physics Relativity Theory String Theory Strings |
title | The phantom term in open string field theory |
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