We investigate the sensitivity of the 14 TeV LHC to pair-produced top partners (T) decaying into the Standard Model top quark (t) plus either a gluon (g) or a photon (γ). The decays T → tg and T → tγ can be dominant when the mixing between the top partner and top quark are negligible. In this case, the conventional decays T → bW , T → tZ, and T → th are highly suppressed and can be neglected. We take a model-independent approach using effective operators for the T -t-g and T -t-γ interactions, considering both spin- $$ \frac{1}{2} $$ and spin- $$ \frac{3}{2} $$ top partners. We perform a semi-realistic simulation with boosted top quark tagging and an appropriate implementation of a jet-faking-photon rate. Despite a simple dimensional analysis indicating that the branching ratios BR(T → tγ) ≪ BR(T → tg) due to the electric-magnetic coupling being much smaller than the strong force coupling, our study shows that the LHC sensitivity to $$ T\overline{T}\to t\overline{t}\gamma g $$ is more significant than the sensitivity to $$ T\overline{T}\to t\overline{t} gg $$ . This is due to much smaller backgrounds attributed to the isolated high-p T photon. We find that with these decay channels and 3 ab−1 of data, the LHC is sensitive to top partner masses m T ≲ 1.4-1.8 TeV for spin- $$ \frac{1}{2} $$ and spin- $$ \frac{3}{2} $$ top partners, respectively.
{ "license": [ { "url": "https://creativecommons.org/licenses/by/3.0", "license": "CC-BY-3.0" } ], "copyright": [ { "material": "Article", "holder": "The Author(s)", "year": "2019" } ], "control_number": "45062", "_oai": { "updated": "2019-01-19T21:30:29Z", "id": "oai:repo.scoap3.org:45062", "sets": [ "JHEP" ] }, "authors": [ { "affiliations": [ { "country": "USA", "value": "Department of Physics and Astronomy, University of Kansas, Lawrence, KS, 66045, U.S.A.", "organization": "University of Kansas" }, { "country": "Saudi Arabia", "value": "Department of Physics, Jazan University, Jazan, 45142, Saudi Arabia", "organization": "Jazan University" } ], "surname": "Alhazmi", "email": "haider@ku.edu", "full_name": "Alhazmi, Haider", "given_names": "Haider" }, { "affiliations": [ { "country": "USA", "value": "Department of Physics and Astronomy, University of Kansas, Lawrence, KS, 66045, U.S.A.", "organization": "University of Kansas" } ], "surname": "Kim", "email": "jeonghan.kim@ku.edu", "full_name": "Kim, Jeong", "given_names": "Jeong" }, { "affiliations": [ { "country": "USA", "value": "Department of Physics and Astronomy, University of Kansas, Lawrence, KS, 66045, U.S.A.", "organization": "University of Kansas" } ], "surname": "Kong", "email": "kckong@ku.edu", "full_name": "Kong, Kyoungchul", "given_names": "Kyoungchul" }, { "affiliations": [ { "country": "USA", "value": "Department of Physics and Astronomy, University of Kansas, Lawrence, KS, 66045, U.S.A.", "organization": "University of Kansas" } ], "surname": "Lewis", "email": "ian.lewis@ku.edu", "full_name": "Lewis, Ian", "given_names": "Ian" } ], "_files": [ { "checksum": "md5:b91ba20fb144380cc8738227b06bb93b", "filetype": "xml", "bucket": "1f4904ab-d315-456d-aadd-3429504f54e1", "version_id": "c811907c-2524-4957-a0db-d3caf3c3036e", "key": "10.1007/JHEP01(2019)139.xml", "size": 16736 }, { "checksum": "md5:99823b1277a5e00e0187ab8b18f692b2", "filetype": "pdf/a", "bucket": "1f4904ab-d315-456d-aadd-3429504f54e1", "version_id": "24ede761-c0a4-4a01-a2c6-99e1e7d8ce58", "key": "10.1007/JHEP01(2019)139_a.pdf", "size": 1828598 } ], "record_creation_date": "2019-01-19T22:30:26.206511", "titles": [ { "source": "Springer", "title": "Shedding light on top partner at the LHC" } ], "collections": [ { "primary": "Journal of High Energy Physics" } ], "dois": [ { "value": "10.1007/JHEP01(2019)139" } ], "publication_info": [ { "page_end": "30", "journal_title": "Journal of High Energy Physics", "material": "article", "journal_volume": "2019", "year": 2019, "page_start": "1", "journal_issue": "1" } ], "$schema": "http://repo.scoap3.org/schemas/hep.json", "abstracts": [ { "source": "Springer", "value": "We investigate the sensitivity of the 14 TeV LHC to pair-produced top partners (T) decaying into the Standard Model top quark (t) plus either a gluon (g) or a photon (\u03b3). The decays T \u2192 tg and T \u2192 t\u03b3 can be dominant when the mixing between the top partner and top quark are negligible. In this case, the conventional decays T \u2192 bW , T \u2192 tZ, and T \u2192 th are highly suppressed and can be neglected. We take a model-independent approach using effective operators for the T -t-g and T -t-\u03b3 interactions, considering both spin- <math> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </math> $$ \\frac{1}{2} $$ and spin- <math> <mfrac> <mn>3</mn> <mn>2</mn> </mfrac> </math> $$ \\frac{3}{2} $$ top partners. We perform a semi-realistic simulation with boosted top quark tagging and an appropriate implementation of a jet-faking-photon rate. Despite a simple dimensional analysis indicating that the branching ratios BR(T \u2192 t\u03b3) \u226a BR(T \u2192 tg) due to the electric-magnetic coupling being much smaller than the strong force coupling, our study shows that the LHC sensitivity to <math> <mi>T</mi> <mover> <mi>T</mi> <mo>\u00af</mo> </mover> <mo>\u2192</mo> <mi>t</mi> <mover> <mi>t</mi> <mo>\u00af</mo> </mover> <mi>\u03b3</mi> <mi>g</mi> </math> $$ T\\overline{T}\\to t\\overline{t}\\gamma g $$ is more significant than the sensitivity to <math> <mi>T</mi> <mover> <mi>T</mi> <mo>\u00af</mo> </mover> <mo>\u2192</mo> <mi>t</mi> <mover> <mi>t</mi> <mo>\u00af</mo> </mover> <mi>gg</mi> </math> $$ T\\overline{T}\\to t\\overline{t} gg $$ . This is due to much smaller backgrounds attributed to the isolated high-p T photon. We find that with these decay channels and 3 ab\u22121 of data, the LHC is sensitive to top partner masses m T \u2272 1.4-1.8 TeV for spin- <math> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </math> $$ \\frac{1}{2} $$ and spin- <math> <mfrac> <mn>3</mn> <mn>2</mn> </mfrac> </math> $$ \\frac{3}{2} $$ top partners, respectively." } ], "imprints": [ { "date": "2019-01-16", "publisher": "Springer" } ], "acquisition_source": { "date": "2019-01-19T22:30:26.206471", "source": "Springer", "method": "Springer", "submission_number": "635b1bde1c3111e9bf0c02163e01809a" } }