Light dark matter and Z′ dark force at colliders
A bstract Light DM, < 10 GeV, with sizeable direct detection rate is an interesting and less explored scenario. Collider searches can be very powerful, such as through the channel in which a pair of dark matter particle is produced in association with a jet. It is a generic possibility that the m...
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Veröffentlicht in: | The journal of high energy physics 2012-07, Vol.2012 (7), Article 182 |
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container_title | The journal of high energy physics |
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creator | An, Haipeng Ji, Xiangdong Wang, Lian-Tao |
description | A
bstract
Light DM, < 10 GeV, with sizeable direct detection rate is an interesting and less explored scenario. Collider searches can be very powerful, such as through the channel in which a pair of dark matter particle is produced in association with a jet. It is a generic possibility that the mediator of the interaction between dark matter and the nucleus will also be accessible at the Tevatron and the LHC. Therefore, collider search of the mediator can provide a more comprehensive probe of the dark matter and its interactions. In this article, to demonstrate the complementarity of these two approaches, we focus on the possibility of the mediator being a new U(1)′ gauge boson, which is probably the simplest model which allows a large direct detection cross section for a light dark matter candidate. We combine searches in the monojet + MET channel and dijet resonance search for the mediator. We find that for the mass of
Z
′ between 250 GeV and 4 TeV, resonance searches at the colliders provide stronger constraints on this model than the monojet + MET searches. |
doi_str_mv | 10.1007/JHEP07(2012)182 |
format | Article |
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bstract
Light DM, < 10 GeV, with sizeable direct detection rate is an interesting and less explored scenario. Collider searches can be very powerful, such as through the channel in which a pair of dark matter particle is produced in association with a jet. It is a generic possibility that the mediator of the interaction between dark matter and the nucleus will also be accessible at the Tevatron and the LHC. Therefore, collider search of the mediator can provide a more comprehensive probe of the dark matter and its interactions. In this article, to demonstrate the complementarity of these two approaches, we focus on the possibility of the mediator being a new U(1)′ gauge boson, which is probably the simplest model which allows a large direct detection cross section for a light dark matter candidate. We combine searches in the monojet + MET channel and dijet resonance search for the mediator. We find that for the mass of
Z
′ between 250 GeV and 4 TeV, resonance searches at the colliders provide stronger constraints on this model than the monojet + MET searches.</description><identifier>ISSN: 1029-8479</identifier><identifier>EISSN: 1029-8479</identifier><identifier>DOI: 10.1007/JHEP07(2012)182</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer-Verlag</publisher><subject>Classical and Quantum Gravitation ; Constraint modelling ; Dark matter ; Elementary Particles ; High energy physics ; Large Hadron Collider ; Physics ; Physics and Astronomy ; Quantum Field Theories ; Quantum Field Theory ; Quantum Physics ; Relativity Theory ; Resonance ; Searching ; String Theory</subject><ispartof>The journal of high energy physics, 2012-07, Vol.2012 (7), Article 182</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-c2912-3e3bce2ed95fa49d9847206d3d2677d89dbc0c5ff77bf203dbb6e5e4d5c98ea23</citedby><cites>FETCH-LOGICAL-c2912-3e3bce2ed95fa49d9847206d3d2677d89dbc0c5ff77bf203dbb6e5e4d5c98ea23</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/JHEP07(2012)182$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/JHEP07(2012)182$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,778,782,27911,27912,41107,41475,42176,42544,51306,51563</link.rule.ids><linktorsrc>$$Uhttps://doi.org/10.1007/JHEP07(2012)182$$EView_record_in_Springer_Nature$$FView_record_in_$$GSpringer_Nature</linktorsrc></links><search><creatorcontrib>An, Haipeng</creatorcontrib><creatorcontrib>Ji, Xiangdong</creatorcontrib><creatorcontrib>Wang, Lian-Tao</creatorcontrib><title>Light dark matter and Z′ dark force at colliders</title><title>The journal of high energy physics</title><addtitle>J. High Energ. Phys</addtitle><description>A
bstract
Light DM, < 10 GeV, with sizeable direct detection rate is an interesting and less explored scenario. Collider searches can be very powerful, such as through the channel in which a pair of dark matter particle is produced in association with a jet. It is a generic possibility that the mediator of the interaction between dark matter and the nucleus will also be accessible at the Tevatron and the LHC. Therefore, collider search of the mediator can provide a more comprehensive probe of the dark matter and its interactions. In this article, to demonstrate the complementarity of these two approaches, we focus on the possibility of the mediator being a new U(1)′ gauge boson, which is probably the simplest model which allows a large direct detection cross section for a light dark matter candidate. We combine searches in the monojet + MET channel and dijet resonance search for the mediator. We find that for the mass of
Z
′ between 250 GeV and 4 TeV, resonance searches at the colliders provide stronger constraints on this model than the monojet + MET searches.</description><subject>Classical and Quantum Gravitation</subject><subject>Constraint modelling</subject><subject>Dark matter</subject><subject>Elementary Particles</subject><subject>High energy physics</subject><subject>Large Hadron Collider</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>Resonance</subject><subject>Searching</subject><subject>String Theory</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>eNp1kL9OwzAQxi0EEqUws0ZigSH0fE7ieERVoaBKMMDCYjn2ubS0TbHTgY1n4pF4EhIFCRam-3T6_kg_xk45XHIAObqbTh5AniNwvOAl7rEBB1RpmUm1_0cfsqMYlwA85woGDGeL-UuTOBNek7VpGgqJ2bjk-evjs3_6OlhKTJPYerVaOArxmB14s4p08nOH7Ol68jieprP7m9vx1Sy1qDimgkRlCcmp3JtMOdWuIxROOCykdKVylQWbey9l5RGEq6qCcspcblVJBsWQnfW921C_7Sg2elnvwqad1ChUKbI8w8416l021DEG8nobFmsT3jUH3YHRPRjdgdEtmDYBfSK2zs2cwm_vf5Fvb-BkwQ</recordid><startdate>20120701</startdate><enddate>20120701</enddate><creator>An, Haipeng</creator><creator>Ji, Xiangdong</creator><creator>Wang, Lian-Tao</creator><general>Springer-Verlag</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>20120701</creationdate><title>Light dark matter and Z′ dark force at colliders</title><author>An, Haipeng ; Ji, Xiangdong ; Wang, Lian-Tao</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c2912-3e3bce2ed95fa49d9847206d3d2677d89dbc0c5ff77bf203dbb6e5e4d5c98ea23</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Classical and Quantum Gravitation</topic><topic>Constraint modelling</topic><topic>Dark matter</topic><topic>Elementary Particles</topic><topic>High energy physics</topic><topic>Large Hadron Collider</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>Resonance</topic><topic>Searching</topic><topic>String Theory</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>An, Haipeng</creatorcontrib><creatorcontrib>Ji, Xiangdong</creatorcontrib><creatorcontrib>Wang, Lian-Tao</creatorcontrib><collection>CrossRef</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni Edition)</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 (ProQuest)</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>Advanced Technologies & Aerospace Database</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>An, Haipeng</au><au>Ji, Xiangdong</au><au>Wang, Lian-Tao</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Light dark matter and Z′ dark force at colliders</atitle><jtitle>The journal of high energy physics</jtitle><stitle>J. High Energ. Phys</stitle><date>2012-07-01</date><risdate>2012</risdate><volume>2012</volume><issue>7</issue><artnum>182</artnum><issn>1029-8479</issn><eissn>1029-8479</eissn><abstract>A
bstract
Light DM, < 10 GeV, with sizeable direct detection rate is an interesting and less explored scenario. Collider searches can be very powerful, such as through the channel in which a pair of dark matter particle is produced in association with a jet. It is a generic possibility that the mediator of the interaction between dark matter and the nucleus will also be accessible at the Tevatron and the LHC. Therefore, collider search of the mediator can provide a more comprehensive probe of the dark matter and its interactions. In this article, to demonstrate the complementarity of these two approaches, we focus on the possibility of the mediator being a new U(1)′ gauge boson, which is probably the simplest model which allows a large direct detection cross section for a light dark matter candidate. We combine searches in the monojet + MET channel and dijet resonance search for the mediator. We find that for the mass of
Z
′ between 250 GeV and 4 TeV, resonance searches at the colliders provide stronger constraints on this model than the monojet + MET searches.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer-Verlag</pub><doi>10.1007/JHEP07(2012)182</doi><oa>free_for_read</oa></addata></record> |
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subjects | Classical and Quantum Gravitation Constraint modelling Dark matter Elementary Particles High energy physics Large Hadron Collider Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Quantum Physics Relativity Theory Resonance Searching String Theory |
title | Light dark matter and Z′ dark force at colliders |
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