Ghost story. II. The midpoint ghost vertex
We construct the ghost number 9 three strings vertex for OSFT in the natural normal ordering. We find two versions, one with a ghost insertion at z=i and a twist-conjugate one with insertion at z=-i. For this reason we call them midpoint vertices. We show that the relevant Neumann matrices commute a...
Gespeichert in:
Veröffentlicht in: | arXiv.org 2009-11 |
---|---|
Hauptverfasser: | , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | |
---|---|
container_issue | |
container_start_page | |
container_title | arXiv.org |
container_volume | |
creator | Bonora, L Maccaferri, C Scherer Santos, R J Tolla, D D |
description | We construct the ghost number 9 three strings vertex for OSFT in the natural normal ordering. We find two versions, one with a ghost insertion at z=i and a twist-conjugate one with insertion at z=-i. For this reason we call them midpoint vertices. We show that the relevant Neumann matrices commute among themselves and with the matrix \(G\) representing the operator K1. We analyze the spectrum of the latter and find that beside a continuous spectrum there is a (so far ignored) discrete one. We are able to write spectral formulas for all the Neumann matrices involved and clarify the important role of the integration contour over the continuous spectrum. We then pass to examine the (ghost) wedge states. We compute the discrete and continuous eigenvalues of the corresponding Neumann matrices and show that they satisfy the appropriate recursion relations. Using these results we show that the formulas for our vertices correctly define the star product in that, starting from the data of two ghost number 0 wedge states, they allow us to reconstruct a ghost number 3 state which is the expected wedge state with the ghost insertion at the midpoint, according to the star recursion relation. |
doi_str_mv | 10.48550/arxiv.0908.0055 |
format | Article |
fullrecord | <record><control><sourceid>proquest_arxiv</sourceid><recordid>TN_cdi_arxiv_primary_0908_0055</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2090062002</sourcerecordid><originalsourceid>FETCH-LOGICAL-a512-eb2552bbd91f4c2edf21e1d23894de6ffca394d929d2d123321f922164a8b6f63</originalsourceid><addsrcrecordid>eNotj0FLAzEQhYMgWGrvniTgTdh1MtnEzVGK1oWCl70v2SaxW2yzJmlp_71p62kezMfjfYQ8MCirWgh40eE4HEpQUJcAQtyQCXLOirpCvCOzGDcAgPIVheAT8rxY-5hoTD6cSto0JW3Xlm4HM_phl-j35XuwIdnjPbl1-ifa2f-dkvbjvZ1_FsuvRTN_WxZaMCxsn4ux741irlqhNQ6ZZQZ5rSpjpXMrzXNSqAwalpchcwqRyUrXvXSST8njtfbi0Y1h2Opw6s4-3dknA09XYAz-d29j6jZ-H3Z5UoeZAonZj_8BrMlLeg</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2090062002</pqid></control><display><type>article</type><title>Ghost story. II. The midpoint ghost vertex</title><source>World Web Journals</source><source>arXiv.org</source><creator>Bonora, L ; Maccaferri, C ; Scherer Santos, R J ; Tolla, D D</creator><creatorcontrib>Bonora, L ; Maccaferri, C ; Scherer Santos, R J ; Tolla, D D</creatorcontrib><description>We construct the ghost number 9 three strings vertex for OSFT in the natural normal ordering. We find two versions, one with a ghost insertion at z=i and a twist-conjugate one with insertion at z=-i. For this reason we call them midpoint vertices. We show that the relevant Neumann matrices commute among themselves and with the matrix \(G\) representing the operator K1. We analyze the spectrum of the latter and find that beside a continuous spectrum there is a (so far ignored) discrete one. We are able to write spectral formulas for all the Neumann matrices involved and clarify the important role of the integration contour over the continuous spectrum. We then pass to examine the (ghost) wedge states. We compute the discrete and continuous eigenvalues of the corresponding Neumann matrices and show that they satisfy the appropriate recursion relations. Using these results we show that the formulas for our vertices correctly define the star product in that, starting from the data of two ghost number 0 wedge states, they allow us to reconstruct a ghost number 3 state which is the expected wedge state with the ghost insertion at the midpoint, according to the star recursion relation.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.0908.0055</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Apexes ; Eigenvalues ; Insertion ; Operators (mathematics) ; Physics - High Energy Physics - Theory ; Strings ; Wedges</subject><ispartof>arXiv.org, 2009-11</ispartof><rights>2009. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,776,780,881,27902</link.rule.ids><backlink>$$Uhttps://doi.org/10.48550/arXiv.0908.0055$$DView paper in arXiv$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.1088/1126-6708/2009/11/075$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink></links><search><creatorcontrib>Bonora, L</creatorcontrib><creatorcontrib>Maccaferri, C</creatorcontrib><creatorcontrib>Scherer Santos, R J</creatorcontrib><creatorcontrib>Tolla, D D</creatorcontrib><title>Ghost story. II. The midpoint ghost vertex</title><title>arXiv.org</title><description>We construct the ghost number 9 three strings vertex for OSFT in the natural normal ordering. We find two versions, one with a ghost insertion at z=i and a twist-conjugate one with insertion at z=-i. For this reason we call them midpoint vertices. We show that the relevant Neumann matrices commute among themselves and with the matrix \(G\) representing the operator K1. We analyze the spectrum of the latter and find that beside a continuous spectrum there is a (so far ignored) discrete one. We are able to write spectral formulas for all the Neumann matrices involved and clarify the important role of the integration contour over the continuous spectrum. We then pass to examine the (ghost) wedge states. We compute the discrete and continuous eigenvalues of the corresponding Neumann matrices and show that they satisfy the appropriate recursion relations. Using these results we show that the formulas for our vertices correctly define the star product in that, starting from the data of two ghost number 0 wedge states, they allow us to reconstruct a ghost number 3 state which is the expected wedge state with the ghost insertion at the midpoint, according to the star recursion relation.</description><subject>Apexes</subject><subject>Eigenvalues</subject><subject>Insertion</subject><subject>Operators (mathematics)</subject><subject>Physics - High Energy Physics - Theory</subject><subject>Strings</subject><subject>Wedges</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2009</creationdate><recordtype>article</recordtype><sourceid>BENPR</sourceid><sourceid>GOX</sourceid><recordid>eNotj0FLAzEQhYMgWGrvniTgTdh1MtnEzVGK1oWCl70v2SaxW2yzJmlp_71p62kezMfjfYQ8MCirWgh40eE4HEpQUJcAQtyQCXLOirpCvCOzGDcAgPIVheAT8rxY-5hoTD6cSto0JW3Xlm4HM_phl-j35XuwIdnjPbl1-ifa2f-dkvbjvZ1_FsuvRTN_WxZaMCxsn4ux741irlqhNQ6ZZQZ5rSpjpXMrzXNSqAwalpchcwqRyUrXvXSST8njtfbi0Y1h2Opw6s4-3dknA09XYAz-d29j6jZ-H3Z5UoeZAonZj_8BrMlLeg</recordid><startdate>20091105</startdate><enddate>20091105</enddate><creator>Bonora, L</creator><creator>Maccaferri, C</creator><creator>Scherer Santos, R J</creator><creator>Tolla, D D</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20091105</creationdate><title>Ghost story. II. The midpoint ghost vertex</title><author>Bonora, L ; Maccaferri, C ; Scherer Santos, R J ; Tolla, D D</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a512-eb2552bbd91f4c2edf21e1d23894de6ffca394d929d2d123321f922164a8b6f63</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2009</creationdate><topic>Apexes</topic><topic>Eigenvalues</topic><topic>Insertion</topic><topic>Operators (mathematics)</topic><topic>Physics - High Energy Physics - Theory</topic><topic>Strings</topic><topic>Wedges</topic><toplevel>online_resources</toplevel><creatorcontrib>Bonora, L</creatorcontrib><creatorcontrib>Maccaferri, C</creatorcontrib><creatorcontrib>Scherer Santos, R J</creatorcontrib><creatorcontrib>Tolla, D D</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>ProQuest Engineering Database</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><collection>Engineering collection</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bonora, L</au><au>Maccaferri, C</au><au>Scherer Santos, R J</au><au>Tolla, D D</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Ghost story. II. The midpoint ghost vertex</atitle><jtitle>arXiv.org</jtitle><date>2009-11-05</date><risdate>2009</risdate><eissn>2331-8422</eissn><abstract>We construct the ghost number 9 three strings vertex for OSFT in the natural normal ordering. We find two versions, one with a ghost insertion at z=i and a twist-conjugate one with insertion at z=-i. For this reason we call them midpoint vertices. We show that the relevant Neumann matrices commute among themselves and with the matrix \(G\) representing the operator K1. We analyze the spectrum of the latter and find that beside a continuous spectrum there is a (so far ignored) discrete one. We are able to write spectral formulas for all the Neumann matrices involved and clarify the important role of the integration contour over the continuous spectrum. We then pass to examine the (ghost) wedge states. We compute the discrete and continuous eigenvalues of the corresponding Neumann matrices and show that they satisfy the appropriate recursion relations. Using these results we show that the formulas for our vertices correctly define the star product in that, starting from the data of two ghost number 0 wedge states, they allow us to reconstruct a ghost number 3 state which is the expected wedge state with the ghost insertion at the midpoint, according to the star recursion relation.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.0908.0055</doi><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | EISSN: 2331-8422 |
ispartof | arXiv.org, 2009-11 |
issn | 2331-8422 |
language | eng |
recordid | cdi_arxiv_primary_0908_0055 |
source | World Web Journals; arXiv.org |
subjects | Apexes Eigenvalues Insertion Operators (mathematics) Physics - High Energy Physics - Theory Strings Wedges |
title | Ghost story. II. The midpoint ghost vertex |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-29T08%3A26%3A49IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_arxiv&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Ghost%20story.%20II.%20The%20midpoint%20ghost%20vertex&rft.jtitle=arXiv.org&rft.au=Bonora,%20L&rft.date=2009-11-05&rft.eissn=2331-8422&rft_id=info:doi/10.48550/arxiv.0908.0055&rft_dat=%3Cproquest_arxiv%3E2090062002%3C/proquest_arxiv%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=2090062002&rft_id=info:pmid/&rfr_iscdi=true |