Diphoton excess at 750 GeV: gluon–gluon fusion or quark–antiquark annihilation?

Gao, Jun; Zhang, Hao; Zhu, Hua Xing

doi:10.1140/epjc/s10052-016-4200-z

Title: Diphoton excess at 750 GeV: gluon–gluon fusion or quark–antiquark annihilation?

Abstract

Recently, ATLAS and CMS collaborations reported an excess in the measurement of diphoton events, which can be explained by a new resonance with a mass around 750 GeV. In this work, we explored the possibility of identifying if the hypothetical new resonance is produced through gluon–gluon fusion or quark–antiquark annihilation, or tagging the beam. Three different observables for beam tagging, namely the rapidity and transverse-momentum distribution of the diphoton, and one tagged bottom-jet cross section, are proposed. Combining the information gained from these observables, a clear distinction of the production mechanism for the diphoton resonance is promising.

Authors:

Gao, Jun ^[1]; Zhang, Hao ^[2]; Zhu, Hua Xing ^[3]

Argonne National Lab. (ANL), Argonne, IL (United States)
Univ. of California, Santa Barbara, CA (United States)
Massachusetts Inst. of Technology (MIT), Cambridge, MA (United States)

Publication Date:: Thu Jun 23 00:00:00 EDT 2016

Research Org.:: Massachusetts Inst. of Technology (MIT), Cambridge, MA (United States); Univ. of California, Santa Barbara, CA (United States)

Sponsoring Org.:: USDOE Office of Science (SC), Nuclear Physics (NP); USDOE Office of Science (SC), High Energy Physics (HEP)

OSTI Identifier:: 1557587

Grant/Contract Number:: SC0011090; SC0011702; AC02-06CH11357

Resource Type:: Accepted Manuscript

Journal Name:: European Physical Journal. C, Particles and Fields

Additional Journal Information:: Journal Volume: 76; Journal Issue: 6; Journal ID: ISSN 1434-6044

Publisher:: Springer

Country of Publication:: United States

Language:: English

Subject:: 72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; Standard Model Background; Partonic Cross Section; Landau Pole; Gluon Scattering; Diphoton Excess

Citation Formats


                    Gao, Jun, Zhang, Hao, and Zhu, Hua Xing. Diphoton excess at 750 GeV: gluon–gluon fusion or quark–antiquark annihilation?.  United States: N. p., 2016. 
Web.  doi:10.1140/epjc/s10052-016-4200-z.

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                    Gao, Jun, Zhang, Hao, & Zhu, Hua Xing. Diphoton excess at 750 GeV: gluon–gluon fusion or quark–antiquark annihilation?.  United States.  https://doi.org/10.1140/epjc/s10052-016-4200-z

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                    Gao, Jun, Zhang, Hao, and Zhu, Hua Xing. Thu .  
"Diphoton excess at 750 GeV: gluon–gluon fusion or quark–antiquark annihilation?".  United States.  https://doi.org/10.1140/epjc/s10052-016-4200-z.  https://www.osti.gov/servlets/purl/1557587.

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@article{osti_1557587,

  title        = {Diphoton excess at 750 GeV: gluon–gluon fusion or quark–antiquark annihilation?},

  author       = {Gao, Jun and Zhang, Hao and Zhu, Hua Xing},

  abstractNote = {Recently, ATLAS and CMS collaborations reported an excess in the measurement of diphoton events, which can be explained by a new resonance with a mass around 750 GeV. In this work, we explored the possibility of identifying if the hypothetical new resonance is produced through gluon–gluon fusion or quark–antiquark annihilation, or tagging the beam. Three different observables for beam tagging, namely the rapidity and transverse-momentum distribution of the diphoton, and one tagged bottom-jet cross section, are proposed. Combining the information gained from these observables, a clear distinction of the production mechanism for the diphoton resonance is promising.},

  doi          = {10.1140/epjc/s10052-016-4200-z},

  journal      = {European Physical Journal. C, Particles and Fields},

  number       = 6,

  volume       = 76,

  place        = {United States},

  year         = {Thu Jun 23 00:00:00 EDT 2016},

  month        = {Thu Jun 23 00:00:00 EDT 2016}

}

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Journal Article:

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https://doi.org/10.1140/epjc/s10052-016-4200-z

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Cited by: 12 works

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Figures / Tables:

Fig. 1: Centrality ratio, defined as ratio of cross section in central rapidity region |y| < y_cut and the total cross section, as a function of y_cut

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margin-top: 0.5em; padding-left: 0; line-height:1.8em;"> <li> <span style="color:#5C7B2D;"> Ladinsky, G. 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margin-top:0px;">Works referencing / citing this record:</p> <div class="list"> <div> <h2 class="title" style="margin-bottom:0;" data-apporder=""> <a href="https://doi.org/10.1007/jhep11(2016)154" target="_blank" rel="noopener noreferrer" class="name">Implications of a high-mass diphoton resonance for heavy quark searches<span class="fa fa-external-link" aria-hidden="true"></span></a> <small class="text-muted" style="text-transform:uppercase; font-size:0.75rem;"><br/> <span class="type">journal</span>, <span class="date" data-date="2016-11-01">November 2016</span></small> </h2> <ul class="small references-list" style="list-style-type:none; margin-top: 0.5em; padding-left: 0; line-height:1.8em;"> <li> <span style="color:#5C7B2D;"> Banerjee, Shankha; Barducci, Daniele; Bélanger, Geneviève</span> </li> <li> Journal of High Energy Physics, Vol. 2016, Issue 11</li> <li> <span class="text-muted related-url">DOI: <a href="https://doi.org/10.1007/jhep11(2016)154" class="text-muted" target="_blank" rel="noopener noreferrer">10.1007/jhep11(2016)154<span class="fa fa-external-link" aria-hidden="true"></span></a></span> </li> </ul> <hr/> </div> <div> <h2 class="title" style="margin-bottom:0;" data-apporder=""> <a href="https://doi.org/10.1142/s0217751x17500142" target="_blank" rel="noopener noreferrer" class="name">Interpreting 750 GeV diphoton excess with R -parity violating supersymmetry<span class="fa fa-external-link" aria-hidden="true"></span></a> <small class="text-muted" style="text-transform:uppercase; 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float:none;">[ × clear filter / sort ]</a> </div> <input type="submit" id="sort_submit_citations" name="submit" aria-label="submit" style="display: none;"/> </form> </div> </div> </div> </section> <section id="biblio-images" class="tab-content tab-content-sec osti-curated" data-tab="biblio"> <div class="row"> <div class="col-sm-9 order-sm-9"> <div class="padding"> <p class="lead text-muted" style="font-size: 18px; margin-top:0px;"><span id="image-type-label">Figures / Tables</span> found in this record:</p> <div class="list clearfix"> <div class="col-sm-3 float-left biblio-image-tile" data-apporder="p. 4" data-order="1" data-imgid="1557587-img147029" data-imgsrc="/biblio/1557587/image/001/929/0019295/1/0147029.png" data-title="Fig. 1" data-desc="Centrality ratio, defined as ratio of cross section in central rapidity region |y| < ycut and the total cross section, as a function of ycut" data-ostiid="1557587" style="padding-bottom: 2em; border-bottom: 1px solid #ddd;"> <a href="#img" class="biblio-image-tile-a ga-click-event" data-imgid="1557587-img147029" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1557587-img147029"> <div style=" padding: .5em; border: 1px solid #eee; background-color: #fff; "> <small class="name">Fig. 1 <small class="pull-right" style="margin-right: .5em;color:#999;top: 3px;position: relative;">(p. 4)</small><span class="d-none type">figure</span></small> <div style=" background-image:url('/biblio/1557587/image/001/929/0019295/1/t0147029.png'); background-repeat:no-repeat; background-size:contain; background-position-x: center; width: 100%; height: 175px; margin-top:.5em; "> </div> </div> </a> </div> <div class="col-sm-3 float-left biblio-image-tile" data-apporder="p. 6" data-order="2" data-imgid="1557587-img147024" data-imgsrc="/biblio/1557587/image/001/929/0019295/1/0147024.png" data-title="Fig. 2" data-desc="QT distribution at small transverse momentum at NLL accuracy for the resonance production initiated by different parton flavors. The two plots show results obtained from two public codes, HqT and CuTe" data-ostiid="1557587" style="padding-bottom: 2em; border-bottom: 1px solid #ddd;"> <a href="#img" class="biblio-image-tile-a ga-click-event" data-imgid="1557587-img147024" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1557587-img147024"> <div style=" padding: .5em; border: 1px solid #eee; background-color: #fff; "> <small class="name">Fig. 2 <small class="pull-right" style="margin-right: .5em;color:#999;top: 3px;position: relative;">(p. 6)</small><span class="d-none type">figure</span></small> <div style=" background-image:url('/biblio/1557587/image/001/929/0019295/1/t0147024.png'); background-repeat:no-repeat; background-size:contain; background-position-x: center; width: 100%; height: 175px; margin-top:.5em; "> </div> </div> </a> </div> <div class="col-sm-3 float-left biblio-image-tile" data-apporder="p. 6" data-order="3" data-imgid="1557587-img147023" data-imgsrc="/biblio/1557587/image/001/929/0019295/1/0147023.png" data-title="Table 1" data-desc="Ratio R for a 750 GeV resonance produced at 13 TeV LHC, initiated by different parton flavors as predicted by two resummation codes, HqT and CuTe" data-ostiid="1557587" style="padding-bottom: 2em; border-bottom: 1px solid #ddd;"> <a href="#img" class="biblio-image-tile-a ga-click-event" data-imgid="1557587-img147023" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1557587-img147023"> <div style=" padding: .5em; border: 1px solid #eee; background-color: #fff; "> <small class="name">Table 1 <small class="pull-right" style="margin-right: .5em;color:#999;top: 3px;position: relative;">(p. 6)</small><span class="d-none type">table</span></small> <div style=" background-image:url('/biblio/1557587/image/001/929/0019295/1/t0147023.png'); background-repeat:no-repeat; background-size:contain; background-position-x: center; width: 100%; height: 175px; margin-top:.5em; "> </div> </div> </a> </div> <div class="col-sm-3 float-left biblio-image-tile" data-apporder="p. 7" data-order="4" data-imgid="1557587-img147026" data-imgsrc="/biblio/1557587/image/001/929/0019295/1/0147026.png" data-title="Fig. 3" data-desc="The Feynman diagrams of the resonance with one jet production process in gg scenario" data-ostiid="1557587" style="padding-bottom: 2em; border-bottom: 1px solid #ddd;"> <a href="#img" class="biblio-image-tile-a ga-click-event" data-imgid="1557587-img147026" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1557587-img147026"> <div style=" padding: .5em; border: 1px solid #eee; background-color: #fff; "> <small class="name">Fig. 3 <small class="pull-right" style="margin-right: .5em;color:#999;top: 3px;position: relative;">(p. 7)</small><span class="d-none type">figure</span></small> <div style=" background-image:url('/biblio/1557587/image/001/929/0019295/1/t0147026.png'); background-repeat:no-repeat; background-size:contain; background-position-x: center; width: 100%; height: 175px; margin-top:.5em; "> </div> </div> </a> </div> <div class="col-sm-3 float-left biblio-image-tile" data-apporder="p. 7" data-order="5" data-imgid="1557587-img147025" data-imgsrc="/biblio/1557587/image/001/929/0019295/1/0147025.png" data-title="Fig. 4" data-desc="The Feynman diagrams of the resonance with one jet production process. In this scenario, the new resonance is produced via the bb̄ initial state at the LHC" data-ostiid="1557587" style="padding-bottom: 2em; border-bottom: 1px solid #ddd;"> <a href="#img" class="biblio-image-tile-a ga-click-event" data-imgid="1557587-img147025" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1557587-img147025"> <div style=" padding: .5em; border: 1px solid #eee; background-color: #fff; "> <small class="name">Fig. 4 <small class="pull-right" style="margin-right: .5em;color:#999;top: 3px;position: relative;">(p. 7)</small><span class="d-none type">figure</span></small> <div style=" background-image:url('/biblio/1557587/image/001/929/0019295/1/t0147025.png'); background-repeat:no-repeat; background-size:contain; background-position-x: center; width: 100%; height: 175px; margin-top:.5em; "> </div> </div> </a> </div> <div class="col-sm-3 float-left biblio-image-tile" data-apporder="p. 8" data-order="6" data-imgid="1557587-img147028" data-imgsrc="/biblio/1557587/image/001/929/0019295/1/0147028.png" data-title="Fig. 5" data-desc="Transverse-momentum distribution of the leading-(b-)jet" data-ostiid="1557587" style="padding-bottom: 2em; border-bottom: 1px solid #ddd;"> <a href="#img" class="biblio-image-tile-a ga-click-event" data-imgid="1557587-img147028" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1557587-img147028"> <div style=" padding: .5em; border: 1px solid #eee; background-color: #fff; "> <small class="name">Fig. 5 <small class="pull-right" style="margin-right: .5em;color:#999;top: 3px;position: relative;">(p. 8)</small><span class="d-none type">figure</span></small> <div style=" background-image:url('/biblio/1557587/image/001/929/0019295/1/t0147028.png'); background-repeat:no-repeat; background-size:contain; background-position-x: center; width: 100%; height: 175px; margin-top:.5em; "> </div> </div> </a> </div> <div class="col-sm-3 float-left biblio-image-tile" data-apporder="p. 8" data-order="7" data-imgid="1557587-img147027" data-imgsrc="/biblio/1557587/image/001/929/0019295/1/0147027.png" data-title="Table 2" data-desc="The fraction of the background events with at least one additional hard jet. The fraction of the events with the leading jet is tagged as a b-jet in these events. In the last line, we show the N+b event number with the assumption that all background events are from the corresponding process" data-ostiid="1557587" style="padding-bottom: 2em; border-bottom: 1px solid #ddd;"> <a href="#img" class="biblio-image-tile-a ga-click-event" data-imgid="1557587-img147027" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1557587-img147027"> <div style=" padding: .5em; border: 1px solid #eee; background-color: #fff; "> <small class="name">Table 2 <small class="pull-right" style="margin-right: .5em;color:#999;top: 3px;position: relative;">(p. 8)</small><span class="d-none type">table</span></small> <div style=" background-image:url('/biblio/1557587/image/001/929/0019295/1/t0147027.png'); background-repeat:no-repeat; background-size:contain; background-position-x: center; width: 100%; height: 175px; margin-top:.5em; "> </div> </div> </a> </div> <div class="col-sm-3 float-left biblio-image-tile" data-apporder="p. 9" data-order="8" data-imgid="1557587-img147030" data-imgsrc="/biblio/1557587/image/001/929/0019295/1/0147030.png" data-title="Fig. 6" data-desc="The ability of distinguishing the gg (bb) scenario from the bb (gg) scenario. The solid lines are with the assumption that all of the background events are from the irreducible γγ background. The dashed lines are with the assumption that all of the background events are from the reducible jj background with two jets are faked as photon" data-ostiid="1557587" style="padding-bottom: 2em; border-bottom: 1px solid #ddd;"> <a href="#img" class="biblio-image-tile-a ga-click-event" data-imgid="1557587-img147030" data-lityx data-category="Extracted Images" data-label="biblio: image thumbnail" data-value="1557587-img147030"> <div style=" padding: .5em; border: 1px solid #eee; background-color: #fff; "> <small class="name">Fig. 6 <small class="pull-right" style="margin-right: .5em;color:#999;top: 3px;position: relative;">(p. 9)</small><span class="d-none type">figure</span></small> <div style=" background-image:url('/biblio/1557587/image/001/929/0019295/1/t0147030.png'); background-repeat:no-repeat; background-size:contain; background-position-x: center; width: 100%; height: 175px; margin-top:.5em; "> </div> </div> </a> </div> </div> <div class="pagination-container small"> <a class="pure-button prev page" href="#" rel="prev"><span class="fa fa-angle-left"></span></a><ul class="pagination d-inline-block" style="padding-left:.2em;"></ul><a class="pure-button next page" href="#" rel="next"><span class="fa fa-angle-right"></span></a> </div> </div> </div> <div class="col-sm-3 order-sm-3"> <ul class="nav nav-stacked"> <li class="active"><a href="" class="reference-type-filter tab-nav" data-tab="biblio-images" data-filter="type" data-pattern="*"><span class="fa fa-angle-right"></span> All Images</a></li> <li class="small" style="margin-left:.75em; 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padding:1em;"> <em>Figures/Tables have been extracted from DOE-funded journal article accepted manuscripts.</em> </div> </div> </div> </section> <section id="biblio-related" class="tab-content tab-content-sec " data-tab="biblio"> <div class="row"> <div class="col-sm-9 order-sm-9"> <section id="biblio-similar" class="tab-content tab-content-sec active" data-tab="related"> <div class="padding"> <p class="lead text-muted" style="font-size: 18px; margin-top:0px;">Similar Records in DOE PAGES and OSTI.GOV collections:</p> <aside> <ul class="item-list" itemscope itemtype="http://schema.org/ItemList" style="padding-left:0; list-style-type: none;"> <li> <div class="article item document" itemprop="itemListElement" itemscope itemtype="http://schema.org/WebPage"><meta itemprop="position" content="1" /><div class="item-info"> <h2 class="title" itemprop="name headline"><a href="/pages/biblio/1905125-gluon-versus-photon-production-diphoton-resonance" itemprop="url">Gluon versus photon production of a 750 GeV diphoton resonance</a></h2> <div class="metadata"> <small class="text-muted" style="text-transform:uppercase;display:block;line-height:2.5em;">Journal Article</small><span class="authors"> <span class="author">Csáki, Csaba</span> ; <span class="author">Hubisz, Jay</span> ; <span class="author">Lombardo, Salvator</span> ; <span class="author">...</span> <span class="text-muted pubdata"> - Physical Review. D.</span> </span> </div> <div class="abstract">We report the production mechanism of a 750 GeV diphoton resonance, either via gluon or photon fusion, can be probed by studying kinematic observables in the diphoton events. We perform a detector study of the two production modes of a hypothetical scalar or tensor diphoton resonance in order to characterize the features of the two scenarios. The nature of the resonance production can be determined from the jet multiplicity, the jet and diphoton rapidities, the rate of central pseudorapidity gaps, or the possible detection of forward protons from elastic photoproduction for events in the signal region. Kinematic distributions for both<a href='#' onclick='$(this).hide().next().show().next().show();return false;' style='margin-left:10px;'>more »</a><span style='display:none;'> signals and expected irreducible diphoton background events are provided for comparison along with a study of observables useful for distinguishing the two scenarios at an integrated luminosity of 20 fb<sup>-1</sup>. We find that decay photons from a 750 GeV scalar resonance have a preference for acceptance in the central detector barrel, while background events are more likely to give accepted photons in the detector end caps. This disfavors the interpretation of the large number of excess events found by the Run-2 CMS diphoton search with one photon detected in the end cap as a wide spin-0 resonance signal. However, one expects more end cap photons in the case of spin-2 resonance.</span><a href='#' onclick='$(this).hide().prev().hide().prev().show();return false;' style='margin-left:10px;display:none;'>« less</a></div><div class="metadata-links small clearfix text-muted" style="margin-top:15px;"> <span class="fa fa-book text-muted" aria-hidden="true"></span> Cited by 33<div class="pure-menu pure-menu-horizontal pull-right" style="width:unset;"> <ul class="pure-menu-list"> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc doi-link " href="https://doi.org/10.1103/physrevd.93.095020" target="_blank" rel="noopener" title="Link to document DOI" data-ostiid="1905125" data-product-type="Journal Article" data-product-subtype="AM" >https://doi.org/10.1103/physrevd.93.095020</a></span></li> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc fulltext-link " href="/pages/servlets/purl/1905125" title="Link to document media" target="_blank" rel="noopener" data-ostiid="1905125" data-product-type="Journal Article" data-product-subtype="AM" >Full Text Available</a></span></li> </ul> </div> </div> </div> <div class="clearfix"></div> </div> </li> <li> <div class="article item document" itemprop="itemListElement" itemscope itemtype="http://schema.org/WebPage"><meta itemprop="position" content="2" /><div class="item-info"> <h2 class="title" itemprop="name headline"><a href="/pages/biblio/1602010-isolating-top-contributions-production-diphoton-excess" itemprop="url">Isolating top contributions in the production of the 750 GeV diphoton excess</a></h2> <div class="metadata"> <small class="text-muted" style="text-transform:uppercase;display:block;line-height:2.5em;">Journal Article</small><span class="authors"> <span class="author">Zhang, Hao</span> <span class="text-muted pubdata"> - Physical Review D</span> </span> </div> <div class="abstract">Recently, both ATLAS and CMS collaborations report an excess at 750GeV in the diphoton invariant mass spectrum at 13TeV LHC. If it is a new scalar produced via loop induced gluon-gluon fusion process, it is important to know what is the particle in the loop. In this work, we investigate the possibility of determine the fraction of the contribution from the standard model top-quark in the loop.</div><div class="metadata-links small clearfix text-muted" style="margin-top:15px;"> <div class="pure-menu pure-menu-horizontal pull-right" style="width:unset;"> <ul class="pure-menu-list"> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc doi-link " href="https://doi.org/10.1103/PhysRevD.93.114032" target="_blank" rel="noopener" title="Link to document DOI" data-ostiid="1602010" data-product-type="Journal Article" data-product-subtype="AM" >https://doi.org/10.1103/PhysRevD.93.114032</a></span></li> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc fulltext-link " href="/pages/servlets/purl/1602010" title="Link to document media" target="_blank" rel="noopener" data-ostiid="1602010" data-product-type="Journal Article" data-product-subtype="AM" >Full Text Available</a></span></li> </ul> </div> </div> </div> <div class="clearfix"></div> </div> </li> <li> <div class="article item document" itemprop="itemListElement" itemscope itemtype="http://schema.org/WebPage"><meta itemprop="position" content="3" /><div class="item-info"> <h2 class="title" itemprop="name headline"><a href="/biblio/1371554-from-diphoton-resonance-multilepton-excesses" itemprop="url">From the 750 GeV diphoton resonance to multilepton excesses</a></h2> <div class="metadata"> <small class="text-muted" style="text-transform:uppercase;display:block;line-height:2.5em;">Journal Article</small><span class="authors"> <span class="author">Bae, Kyu Jung</span> ; <span class="author">Chen, Chuan-Ren</span> ; <span class="author">Hamaguchi, Koichi</span> ; <span class="author">...</span> <span class="text-muted pubdata"> - Physical Review D</span> </span> </div> <div class="abstract">Weakly coupled models for the 750 GeV diphoton resonance often invoke new particles carrying both color and/or electric charges to mediate loop-induced couplings of the resonance to two gluons and two photons. The new colored particles may not be stable and could decay into final states containing standard model particles. We consider an electroweak doublet of vectorlike quarks (VLQs) carrying electric charges of 5/3 and 2/3, respectively, which mediate the loop-induced couplings of the 750 GeV resonance. If the VLQ has a mass at around 1 TeV, it naturally gives rise to the observed diphoton signal strength while all couplings<a href='#' onclick='$(this).hide().next().show().next().show();return false;' style='margin-left:10px;'>more »</a><span style='display:none;'> remain perturbative up to a high scale. At the same time, if the charge-5/3 VLQ decays into final states containing top quark and W boson, it would contribute to the multilepton excesses observed in both run 1 and run 2 data. It is also possible to incorporate a dark matter candidate in the decay final states to explain the observed relic density.</span><a href='#' onclick='$(this).hide().prev().hide().prev().show();return false;' style='margin-left:10px;display:none;'>« less</a></div><div class="metadata-links small clearfix text-muted" style="margin-top:15px;"> <div class="pure-menu pure-menu-horizontal pull-right" style="width:unset;"> <ul class="pure-menu-list"> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc doi-link " href="https://doi.org/10.1103/PhysRevD.94.015035" target="_blank" rel="noopener" title="Link to document DOI" data-ostiid="1371554" data-product-type="Journal Article" data-product-subtype="AC" >https://doi.org/10.1103/PhysRevD.94.015035</a></span></li> </ul> </div> </div> </div> <div class="clearfix"></div> </div> </li> <li> <div class="article item document" itemprop="itemListElement" itemscope itemtype="http://schema.org/WebPage"><meta itemprop="position" content="4" /><div class="item-info"> <h2 class="title" itemprop="name headline"><a href="/pages/biblio/1401006-string-consistency-heavy-exotics-gev-diphoton-excess-lhc" itemprop="url">String consistency, heavy exotics, and the 750 GeV diphoton excess at the LHC</a></h2> <div class="metadata"> <small class="text-muted" style="text-transform:uppercase;display:block;line-height:2.5em;">Journal Article</small><span class="authors"> <span class="author">Cvetič, Mirjam</span> ; <span class="author">Halverson, James</span> ; <span class="author">Langacker, Paul</span> <span class="text-muted pubdata"> - Fortschritte der Physik</span> </span> </div> <div class="abstract">String consistency conditions are stronger than anomaly cancellation and can require the addition of exotics in the visible sector. We study such exotics and demonstrate that they may account for the modest excess at 750 GeV in recent diphoton resonance searches performed by the ATLAS and CMS collaborations. In a previous analysis of type II MSSM D‐brane quivers we systematically added up to five exotics for the sake of satisfying string consistency conditions. Using this dataset, we demonstrate that 89780 of the 89964 quivers have exotics, 78155 of which include singlets that may couple to MSSM or exotic multiplets with<a href='#' onclick='$(this).hide().next().show().next().show();return false;' style='margin-left:10px;'>more »</a><span style='display:none;'> coupling structures governed by U (1) symmetries that are often anomalous. We demonstrate that certain sets of exotics are far preferred over others and study the structure of singlet couplings to heavy exotics carrying standard model charges. Typical possibilities include singlets that may decay to vector‐like quarks and/or vector‐like leptons and subsequently to two photons. We show that a narrow width diphoton excess can be accounted for while evading existing bounds if multiple exotics are added, with vector‐like leptons of mass GeV and vector‐like quarks with masses up to ≃ 3 TeV. However, a large width , as suggested by the ATLAS data, cannot be easily accommodated in this framework. Renormalization group equations with GUT‐scale boundary conditions show that these supersymmetric models are perturbative and stable. Type IIA compactifications on toroidal orbifolds allow for O (10) Yukawa couplings in the ultraviolet. We also discuss the possibility of accounting for the diphoton excess in a low string scale scenario via the decay of string axions.</span><a href='#' onclick='$(this).hide().prev().hide().prev().show();return false;' style='margin-left:10px;display:none;'>« less</a></div><div class="metadata-links small clearfix text-muted" style="margin-top:15px;"> <span class="fa fa-book text-muted" aria-hidden="true"></span> Cited by 3<div class="pure-menu pure-menu-horizontal pull-right" style="width:unset;"> <ul class="pure-menu-list"> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc doi-link " href="https://doi.org/10.1002/prop.201600080" target="_blank" rel="noopener" title="Link to document DOI" data-ostiid="1401006" data-product-type="Journal Article" data-product-subtype="PM" >https://doi.org/10.1002/prop.201600080</a></span></li> </ul> </div> </div> </div> <div class="clearfix"></div> </div> </li> <li> <div class="article item document" itemprop="itemListElement" itemscope itemtype="http://schema.org/WebPage"><meta itemprop="position" content="5" /><div class="item-info"> <h2 class="title" itemprop="name headline"><a href="/pages/biblio/1253728-how-resonance-continuum-interference-changes-gev-diphoton-excess-signal-enhancement-peak-shift" itemprop="url">How resonance-continuum interference changes 750 GeV diphoton excess: Signal enhancement and peak shift</a></h2> <div class="metadata"> <small class="text-muted" style="text-transform:uppercase;display:block;line-height:2.5em;">Journal Article</small><span class="authors"> <span class="author">Jung, Sunghoon</span> ; <span class="author">Song, Jeonghyeon</span> ; <span class="author">Yoon, Yeo Woong</span> <span class="text-muted pubdata"> - Journal of High Energy Physics (Online)</span> </span> </div> <div class="abstract">A hypothetical new scalar resonance, a candidate explanation for the recently observed 750 GeV diphoton excess at the LHC 13 TeV, necessarily interferes with the continuum background gg → γγ. The interference has two considerable effects: (1) enhancing or suppressing diphoton signal rate due to the imaginary-part interference and (2) distorting resonance shape due to the real-part interference. We study them based on the best-fit analysis of two benchmark models: two Higgs doublets with ~50 GeV width (exhibiting the imaginary-part interference effect) and a singlet scalar with 5 GeV width (exhibiting the real-part one), both extended with vector-like fermions. Furthermore,<a href='#' onclick='$(this).hide().next().show().next().show();return false;' style='margin-left:10px;'>more »</a><span style='display:none;'> we find that the resonance contribution can be enhanced by a factor of 2 (1.6) for 3 (6) fb signal rate, or the 68% CL allowed mass region is shifted by O (1) GeV. If the best-fit excess rate decreases in the future data, the interference effects will become more significant.</span><a href='#' onclick='$(this).hide().prev().hide().prev().show();return false;' style='margin-left:10px;display:none;'>« less</a></div><div class="metadata-links small clearfix text-muted" style="margin-top:15px;"> <span class="fa fa-book text-muted" aria-hidden="true"></span> Cited by 1<div class="pure-menu pure-menu-horizontal pull-right" style="width:unset;"> <ul class="pure-menu-list"> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc doi-link " href="https://doi.org/10.1007/JHEP05(2016)009" target="_blank" rel="noopener" title="Link to document DOI" data-ostiid="1253728" data-product-type="Journal Article" data-product-subtype="AM" >https://doi.org/10.1007/JHEP05(2016)009</a></span></li> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc fulltext-link " href="/pages/servlets/purl/1253728" title="Link to document media" target="_blank" rel="noopener" data-ostiid="1253728" data-product-type="Journal Article" data-product-subtype="AM" >Full Text Available</a></span></li> </ul> </div> </div> </div> <div class="clearfix"></div> </div> </li> </ul> </aside> </div> </section> </div> <div class="col-sm-3 order-sm-3"> <ul class="nav nav-stacked"> <li class="active"><a class="tab-nav disabled" data-tab="related" style="color: #636c72 !important; 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Title: Diphoton excess at 750 GeV: gluon–gluon fusion or quark–antiquark annihilation?

Abstract

Citation Formats

Figures / Tables:

Supersoft SUSY models and the 750 GeV diphoton excess, beyond effective operators journal, July 2016

750 GeV diphoton excess explained by a resonant sneutrino in R -parity violating supersymmetry journal, June 2016

Distinguishing b -quark and gluon jets with a tagged b hadron journal, March 2016

Interpretation of the diphoton excess at CMS and ATLAS journal, March 2016

Singlet scalar resonances and the diphoton excess journal, April 2016

Identifying the colour of TeV-scale resonances journal, January 2012

Effective interpretations of a diphoton excess journal, April 2016

FastJet user manual: (for version 3.0.2) journal, March 2012

Vector leptoquarks and the 750 GeV diphoton resonance at the LHC journal, June 2016

Diphoton resonance at 750 GeV in the broken R -symmetric MSSM journal, August 2016

Symmetries behind the 750 GeV diphoton excess journal, June 2016

Can the new resonance at LHC be a CP-odd Higgs boson? journal, June 2016

Knocking on new physics’ door with a scalar resonance journal, March 2016

Implication of the 750 GeV diphoton resonance on two-Higgs-doublet model and its extensions with Higgs field journal, March 2016

The LHC diphoton resonance and dark matter journal, April 2016

Transverse-momentum resummation: Higgs boson production at the Tevatron and the LHC journal, November 2011

String consistency, heavy exotics, and the 750 GeV diphoton excess at the LHC: String consistency, heavy exotics, and the 750 GeV diphoton excess journal, August 2016

LHC diphoton resonance at $$750\,\text {GeV}$$ 750 GeV as an indication of $$SU(3)_L\times U(1)_X$$ S U ( 3 ) L × U ( 1 ) X electroweak symmetry journal, July 2016

A resonance without resonance: Scrutinizing the diphoton excess at 750 GeV journal, April 2016

A pseudoscalar decaying to photon pairs in the early LHC Run 2 data journal, March 2016

The diphoton resonance as a gravity mediator of dark matter journal, April 2016

Goldstones in diphotons journal, April 2016

The 750 GeV diphoton excess as a first light on supersymmetry breaking journal, August 2016

750 GeV diphoton resonance, 125 GeV Higgs and muon g− 2 anomaly in deflected anomaly mediation SUSY breaking scenarios journal, August 2016

Back-to-back jets in QCD journal, December 1981

Simple U ( 1 ) gauge theory explanation of the diphoton excess journal, March 2016

Status and prospects of the two-Higgs-doublet S U ( 6 ) / S p ( 6 ) little-Higgs model and the alignment limit journal, July 2016

LHC diphoton resonance from gauge symmetry journal, June 2016

Higgs stability and the 750 GeV diphoton excess journal, April 2016

Electroweak vacuum stability and diphoton excess at 750 GeV journal, July 2016

LHC probes the hidden sector journal, September 2013

New vector bosons and the diphoton excess journal, August 2016

Di-photon excess illuminates dark matter journal, March 2016

Back-to-back jets: Fourier transform from b to kT journal, April 1982

750 GeV Diphoton Excess from the Goldstino Superpartner journal, April 2016

Model-independent combination of diphoton constraints at 750 GeV journal, May 2016

Hard scattering factorization from effective field theory journal, July 2002

Footprints of New Strong Dynamics via Anomaly and the 750 GeV Diphoton journal, April 2016

Supersoft SUSY models and the 750 GeV diphoton excess, beyond effective operators
journal, July 2016

750 GeV diphoton excess explained by a resonant sneutrino in $R$ -parity violating supersymmetry
journal, June 2016

Distinguishing $b$ -quark and gluon jets with a tagged $b$ hadron
journal, March 2016

Interpretation of the diphoton excess at CMS and ATLAS
journal, March 2016

Singlet scalar resonances and the diphoton excess
journal, April 2016

Identifying the colour of TeV-scale resonances
journal, January 2012

Effective interpretations of a diphoton excess
journal, April 2016

FastJet user manual: (for version 3.0.2)
journal, March 2012

Vector leptoquarks and the 750 GeV diphoton resonance at the LHC
journal, June 2016

Diphoton resonance at 750 GeV in the broken $R$ -symmetric MSSM
journal, August 2016

Symmetries behind the 750 GeV diphoton excess
journal, June 2016

Can the new resonance at LHC be a CP-odd Higgs boson?
journal, June 2016

Knocking on new physics’ door with a scalar resonance
journal, March 2016

Implication of the 750 GeV diphoton resonance on two-Higgs-doublet model and its extensions with Higgs field
journal, March 2016

The LHC diphoton resonance and dark matter
journal, April 2016

Transverse-momentum resummation: Higgs boson production at the Tevatron and the LHC
journal, November 2011

String consistency, heavy exotics, and the 750 GeV diphoton excess at the LHC: String consistency, heavy exotics, and the 750 GeV diphoton excess
journal, August 2016

LHC diphoton resonance at $$750\,\text {GeV}$$ 750 GeV as an indication of $$SU(3)_L\times U(1)_X$$ S U ( 3 ) L × U ( 1 ) X electroweak symmetry
journal, July 2016

A resonance without resonance: Scrutinizing the diphoton excess at 750 GeV
journal, April 2016

A pseudoscalar decaying to photon pairs in the early LHC Run 2 data
journal, March 2016

The diphoton resonance as a gravity mediator of dark matter
journal, April 2016

Goldstones in diphotons
journal, April 2016

The 750 GeV diphoton excess as a first light on supersymmetry breaking
journal, August 2016

750 GeV diphoton resonance, 125 GeV Higgs and muon g− 2 anomaly in deflected anomaly mediation SUSY breaking scenarios
journal, August 2016

Back-to-back jets in QCD
journal, December 1981

Simple $U (1)$ gauge theory explanation of the diphoton excess
journal, March 2016

Status and prospects of the two-Higgs-doublet $S U (6) / S p (6)$ little-Higgs model and the alignment limit
journal, July 2016

LHC diphoton resonance from gauge symmetry
journal, June 2016

Higgs stability and the 750 GeV diphoton excess
journal, April 2016

Electroweak vacuum stability and diphoton excess at 750 GeV
journal, July 2016

LHC probes the hidden sector
journal, September 2013

New vector bosons and the diphoton excess
journal, August 2016

Di-photon excess illuminates dark matter
journal, March 2016

Back-to-back jets: Fourier transform from b to kT
journal, April 1982

750 GeV Diphoton Excess from the Goldstino Superpartner
journal, April 2016

Model-independent combination of diphoton constraints at 750 GeV
journal, May 2016

Hard scattering factorization from effective field theory
journal, July 2002

Footprints of New Strong Dynamics via Anomaly and the 750 GeV Diphoton
journal, April 2016