A bstract A search for the pair production of the lightest supersymmetric partner of the top quark, the top squark ( $$ {\overset{\sim }{\textrm{t}}}_1 $$ t ~ 1 ), is presented. The search targets the four-body decay of the $$ {\overset{\sim }{\textrm{t}}}_1 $$ t ~ 1 , which is preferred when the mass difference between the top squark and the lightest supersymmetric particle is smaller than the mass of the W boson. This decay mode consists of a bottom quark, two other fermions, and the lightest neutralino ( $$ {\overset{\sim }{\chi}}_1^0 $$ χ ~ 1 0 ), which is assumed to be the lightest supersymmetric particle. The data correspond to an integrated luminosity of 138 fb − 1 of proton-proton collisions at a center-of-mass energy of 13 TeV collected by the CMS experiment at the CERN LHC. Events are selected using the presence of a high-momentum jet, an electron or muon with low transverse momentum, and a significant missing transverse momentum. The signal is selected based on a multivariate approach that is optimized for the difference between m ( $$ {\overset{\sim }{\textrm{t}}}_1 $$ t ~ 1 ) and m ( $$ {\overset{\sim }{\chi}}_1^0 $$ χ ~ 1 0 ). The contribution from leading background processes is estimated from data. No significant excess is observed above the expectation from standard model processes. The results of this search exclude top squarks at 95% confidence level for masses up to 480 and 700 GeV for m ( $$ {\overset{\sim }{\textrm{t}}}_1 $$ t ~ 1 ) − m ( $$ {\overset{\sim }{\chi}}_1^0 $$ χ ~ 1 0 ) = 10 and 80 GeV, respectively.
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- NSF Public Access
- Search Results
- Combined searches for the production of supersymmetric top quark partners in proton–proton collisions at $$\sqrt{s} = 13\,\text {Te}\text {V} $$
Title:
Combined searches for the production of supersymmetric top quark partners in proton–proton collisions at $$\sqrt{s} = 13\,\text {Te}\text {V} $$
Abstract A combination of searches for top squark pair production using proton–proton collision data at a center-of-mass energy of 13 $$\,\text {Te}\text {V}$$ Te at the CERN LHC, corresponding to an integrated luminosity of 137 $$\,\text {fb}^{-1}$$ fb - 1 collected by the CMS experiment, is presented. Signatures with at least 2 jets and large missing transverse momentum are categorized into events with 0, 1, or 2 leptons. New results for regions of parameter space where the kinematical properties of top squark pair production and top quark pair production are very similar are presented. Depending on the model, the combined result excludes a top squark mass up to 1325 $$\,\text {Ge}\text {V}$$ Ge for a massless neutralino, and a neutralino mass up to 700 $$\,\text {Ge}\text {V}$$ Ge for a top squark mass of 1150 $$\,\text {Ge}\text {V}$$ Ge . Top squarks with masses from 145 to 295 $$\,\text {Ge}\text {V}$$ Ge , for neutralino masses from 0 to 100 $$\,\text {Ge}\text {V}$$ Ge , with a mass difference between the top squark and the neutralino in a window of 30 $$\,\text {Ge}\text {V}$$ Ge around the mass of the top quark, are excluded for the first time with CMS data. The results of theses searches are also interpreted in an alternative signal model of dark matter production via a spin-0 mediator in association with a top quark pair. Upper limits are set on the cross section for mediator particle masses of up to 420 $$\,\text {Ge}\text {V}$$ Ge .
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- NSF-PAR ID:
- 10330326
- Author(s) / Creator(s):
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C.; Nabili, S.; Palmer, C.; Seidel, M.; Skuja, A.; Wang, L.; Wong, K.; Abercrombie, D.; Andreassi, G.; Bi, R.; Brandt, S.; Busza, W.; Cali, I. A.; Chen, Y.; D’Alfonso, M.; Eysermans, J.; Freer, C.; Ceballos, G. Gomez; Goncharov, M.; Harris, P.; Hu, M.; Klute, M.; Kovalskyi, D.; Krupa, J.; Lee, Y.-J.; Maier, B.; Mironov, C.; Paus, C.; Rankin, D.; Roland, C.; Roland, G.; Shi, Z.; Stephans, G. S.; Wang, J.; Wang, Z.; Wyslouch, B.; Chatterjee, R. M.; Evans, A.; Hansen, P.; Hiltbrand, J.; Jain, Sh.; Krohn, M.; Kubota, Y.; Mans, J.; Revering, M.; Rusack, R.; Saradhy, R.; Schroeder, N.; Strobbe, N.; Wadud, M. A.; Bloom, K.; Bryson, M.; Chauhan, S.; Claes, D. R.; Fangmeier, C.; Finco, L.; Golf, F.; Joo, C.; Kravchenko, I.; Musich, M.; Reed, I.; Siado, J. E.; Snow, G. 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P.; Gandrakota, A.; Gershtein, Y.; Halkiadakis, E.; Hart, A.; Heindl, M.; Karacheban, O.; Laflotte, I.; Lath, A.; Montalvo, R.; Nash, K.; Osherson, M.; Salur, S.; Schnetzer, S.; Somalwar, S.; Stone, R.; Thayil, S. A.; Thomas, S.; Wang, H.; Acharya, H.; Delannoy, A. G.; Spanier, S.; Bouhali, O.; Dalchenko, M.; Delgado, A.; Eusebi, R.; Gilmore, J.; Huang, T.; Kamon, T.; Kim, H.; Luo, S.; Malhotra, S.; Mueller, R.; Overton, D.; Rathjens, D.; Safonov, A.; Akchurin, N.; Damgov, J.; Hegde, V.; Kunori, S.; Lamichhane, K.; Lee, S. W.; Mengke, T.; Muthumuni, S.; Peltola, T.; Volobouev, I.; Wang, Z.; Whitbeck, A.; Appelt, E.; Greene, S.; Gurrola, A.; Johns, W.; Melo, A.; Ni, H.; Padeken, K.; Romeo, F.; Sheldon, P.; Tuo, S.; Velkovska, J.; Arenton, M. W.; Cox, B.; Cummings, G.; Hakala, J.; Hirosky, R.; Joyce, M.; Ledovskoy, A.; Li, A.; Neu, C.; Tannenwald, B.; White, S.; Wolfe, E.; Poudyal, N.; Black, K.; Bose, T.; Buchanan, J.; Caillol, C.; Dasu, S.; De Bruyn, I.; Everaerts, P.; Fienga, F.; Galloni, C.; He, H.; Herndon, M.; Hervé, A.; Hussain, U.; Lanaro, A.; Loeliger, A.; Loveless, R.; Sreekala, J. Madhusudanan; Mallampalli, A.; Mohammadi, A.; Pinna, D.; Savin, A.; Shang, V.; Sharma, V.; Smith, W. H.; Teague, D.; Trembath-reichert, S.; Vetens, W. « less
- Date Published:
- Journal Name:
- The European Physical Journal C
- Volume:
- 81
- Issue:
- 11
- ISSN:
- 1434-6044
- Format(s):
- Medium: X
- Sponsoring Org:
- National Science Foundation
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Abstract The mass of the top quark is measured in 36.3
$$\,\text {fb}^{-1}$$ $$\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V} $$ $$171.77\pm 0.37\,\text {Ge}\hspace{-.08em}\text {V} $$ -
Aad, G. ; Abbott, B. ; Abbott, D. C. ; Abud, A. Abed ; Abeling, K. ; Abhayasinghe, D. K. ; Abidi, S. H. ; AbouZeid, O. S. ; Abraham, N. L. ; Abramowicz, H. ; et al ( , The European Physical Journal C)null (Ed.)Abstract A search for direct pair production of scalar partners of the top quark (top squarks or scalar third-generation up-type leptoquarks) in the all-hadronic $$t{\bar{t}}$$ t t ¯ plus missing transverse momentum final state is presented. The analysis of 139 $$\hbox {fb}^{-1}$$ fb - 1 of $${\sqrt{s}=13}$$ s = 13 TeV proton–proton collision data collected using the ATLAS detector at the LHC yields no significant excess over the Standard Model background expectation. To interpret the results, a supersymmetric model is used where the top squark decays via $${\tilde{t}} \rightarrow t^{(*)} {\tilde{\chi }}^0_1$$ t ~ → t ( ∗ ) χ ~ 1 0 , with $$t^{(*)}$$ t ( ∗ ) denoting an on-shell (off-shell) top quark and $${\tilde{\chi }}^0_1$$ χ ~ 1 0 the lightest neutralino. Three specific event selections are optimised for the following scenarios. In the scenario where $$m_{{\tilde{t}}}> m_t+m_{{\tilde{\chi }}^0_1}$$ m t ~ > m t + m χ ~ 1 0 , top squark masses are excluded in the range 400–1250 GeV for $${\tilde{\chi }}^0_1$$ χ ~ 1 0 masses below 200 GeV at 95% confidence level. In the situation where $$m_{{\tilde{t}}}\sim m_t+m_{{\tilde{\chi }}^0_1}$$ m t ~ ∼ m t + m χ ~ 1 0 , top squark masses in the range 300–630 GeV are excluded, while in the case where $$m_{{\tilde{t}}}< m_W+m_b+m_{{\tilde{\chi }}^0_1}$$ m t ~ < m W + m b + m χ ~ 1 0 (with $$m_{{\tilde{t}}}-m_{{\tilde{\chi }}^0_1}\ge 5$$ m t ~ - m χ ~ 1 0 ≥ 5 GeV), considered for the first time in an ATLAS all-hadronic search, top squark masses in the range 300–660 GeV are excluded. Limits are also set for scalar third-generation up-type leptoquarks, excluding leptoquarks with masses below 1240 GeV when considering only leptoquark decays into a top quark and a neutrino.more » « less
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Tumasyan, A. ; Adam, W. ; Andrejkovic, J. W. ; Bergauer, T. ; Chatterjee, S. ; Damanakis, K. ; Dragicevic, M. ; Escalante Del Valle, A. ; Hussain, P. S. ; Jeitler, M. ; et al ( , Journal of High Energy Physics)A bstract A search for pair production of the supersymmetric partner of the top quark, the top squark, in proton-proton collisions at $$ \sqrt{s} $$ s = 13 TeV is presented in final states containing at least one hadronically decaying tau lepton and large missing transverse momentum. This final state is highly sensitive to scenarios of supersymmetry in which the decay of the top squark to tau leptons is enhanced. The search uses a data sample corresponding to an integrated luminosity of 138 fb − 1 , which was recorded with the CMS detector during 2016–2018. No significant excess is observed with respect to the standard model predictions. Exclusion limits at 95% confidence level on the masses of the top squark and the lightest neutralino are presented under the assumptions of simplified models. The results probe top squark masses up to 1150 GeV for a nearly massless neutralino. This search covers a relatively less explored parameter space in the context of supersymmetry, and the exclusion limit is the most stringent to date for the model considered here.more » « less
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Cite: MLA FormatTumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Chatterjee, S., Dragicevic, M., Del Valle, A. Escalante, Frühwirth, R., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Mikulec, I., Paulitsch, P., Pitters, F. M., Schieck, J., Schöfbeck, R., Spanring, M., Templ, S., Waltenberger, W., Wulz, C.-E., Chekhovsky, V., Litomin, A., Makarenko, V., Darwish, M. R., De Wolf, E. A., Janssen, X., Kello, T., Lelek, A., Sfar, H. Rejeb, Mechelen, P. Van, Putte, S. Van, Van Remortel, N., Blekman, F., Bols, E. S., D’Hondt, J., De Clercq, J., Delcourt, M., El Faham, H., Lowette, S., Moortgat, S., Morton, A., Müller, D., Sahasransu, A. R., Tavernier, S., Doninck, W. Van, Mulders, P. Van, Beghin, D., Bilin, B., Clerbaux, B., De Lentdecker, G., Favart, L., Grebenyuk, A., Kalsi, A. K., Lee, K., Mahdavikhorrami, M., Makarenko, I., Moureaux, L., Pétré, L., Popov, A., Postiau, N., Starling, E., Thomas, L., Bemden, M. Vanden, Velde, C. Vander, Vanlaer, P., Vannerom, D., Wezenbeek, L., Cornelis, T., Dobur, D., Knolle, J., Lambrecht, L., Mestdach, G., Niedziela, M., Roskas, C., Samalan, A., Skovpen, K., Tytgat, M., Verbeke, W., Vermassen, B., Vit, M., Bethani, A., Bruno, G., Bury, F., Caputo, C., David, P., Delaere, C., Donertas, I. S., Giammanco, A., Jaffel, K., Jain, Sa., Lemaitre, V., Mondal, K., Prisciandaro, J., Taliercio, A., Teklishyn, M., Tran, T. T., Vischia, P., Wertz, S., Alves, G. A., Hensel, C., Moraes, A., Júnior, W. L., Pereira, M. Alves, Filho, M. Barroso, Malbouisson, H. Brandao, Carvalho, W., Chinellato, J., Da Costa, E. M., Da Silveira, G. G., De Jesus Damiao, D., De Souza, S. Fonseca, Figueiredo, D. Matos, Herrera, C. Mora, Amarilo, K. Mota, Mundim, L., Nogima, H., Teles, P. Rebello, Santoro, A., Do Amaral, S. M., Sznajder, A., Thiel, M., Da Silva De Araujo, F. Torres, Pereira, A. Vilela, Bernardes, C. A., Calligaris, L., Tomei, T. R., Gregores, E. M., Lemos, D. S., Mercadante, P. G., Novaes, S. F., Padula, Sandra S., Aleksandrov, A., Antchev, G., Hadjiiska, R., Iaydjiev, P., Misheva, M., Rodozov, M., Shopova, M., Sultanov, G., Dimitrov, A., Ivanov, T., Litov, L., Pavlov, B., Petkov, P., Petrov, A., Cheng, T., Guo, Q., Javaid, T., Mittal, M., Wang, H., Yuan, L., Ahmad, M., Bauer, G., Dozen, C., Hu, Z., Martins, J., Wang, Y., Yi, K., Chapon, E., Chen, G. M., Chen, H. S., Chen, M., Iemmi, F., Kapoor, A., Leggat, D., Liao, H., LIU, Z.-A., Milosevic, V., Monti, F., Sharma, R., Tao, J., Thomas-wilsker, J., Wang, J., Zhang, H., Zhang, S., Zhao, J., Agapitos, A., An, Y., Ban, Y., Chen, C., Levin, A., Li, Q., Lyu, X., Mao, Y., Qian, S. J., Wang, D., Wang, Q., Xiao, J., Lu, M., You, Z., Gao, X., Okawa, H., Lin, Z., Xiao, M., Avila, C., Cabrera, A., Florez, C., Fraga, J., Sarkar, A., Delgado, M. A., Guisao, J. Mejia, Ramirez, F., Alvarez, J. D., González, C. 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Cite: APA FormatTumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Chatterjee, S., Dragicevic, M., Del Valle, A. Escalante, Frühwirth, R., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Mikulec, I., Paulitsch, P., Pitters, F. M., Schieck, J., Schöfbeck, R., Spanring, M., Templ, S., Waltenberger, W., Wulz, C.-E., Chekhovsky, V., Litomin, A., Makarenko, V., Darwish, M. R., De Wolf, E. A., Janssen, X., Kello, T., Lelek, A., Sfar, H. Rejeb, Mechelen, P. Van, Putte, S. Van, Van Remortel, N., Blekman, F., Bols, E. S., D’Hondt, J., De Clercq, J., Delcourt, M., El Faham, H., Lowette, S., Moortgat, S., Morton, A., Müller, D., Sahasransu, A. R., Tavernier, S., Doninck, W. Van, Mulders, P. Van, Beghin, D., Bilin, B., Clerbaux, B., De Lentdecker, G., Favart, L., Grebenyuk, A., Kalsi, A. K., Lee, K., Mahdavikhorrami, M., Makarenko, I., Moureaux, L., Pétré, L., Popov, A., Postiau, N., Starling, E., Thomas, L., Bemden, M. Vanden, Velde, C. 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- Chicago
Cite: Chicago FormatTumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Chatterjee, S., Dragicevic, M., Del Valle, A. Escalante, Frühwirth, R., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Mikulec, I., Paulitsch, P., Pitters, F. M., Schieck, J., Schöfbeck, R., Spanring, M., Templ, S., Waltenberger, W., Wulz, C.-E., Chekhovsky, V., Litomin, A., Makarenko, V., Darwish, M. R., De Wolf, E. A., Janssen, X., Kello, T., Lelek, A., Sfar, H. Rejeb, Mechelen, P. Van, Putte, S. Van, Van Remortel, N., Blekman, F., Bols, E. S., D’Hondt, J., De Clercq, J., Delcourt, M., El Faham, H., Lowette, S., Moortgat, S., Morton, A., Müller, D., Sahasransu, A. R., Tavernier, S., Doninck, W. Van, Mulders, P. Van, Beghin, D., Bilin, B., Clerbaux, B., De Lentdecker, G., Favart, L., Grebenyuk, A., Kalsi, A. K., Lee, K., Mahdavikhorrami, M., Makarenko, I., Moureaux, L., Pétré, L., Popov, A., Postiau, N., Starling, E., Thomas, L., Bemden, M. Vanden, Velde, C. 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W., Cox, B., Cummings, G., Hakala, J., Hirosky, R., Joyce, M., Ledovskoy, A., Li, A., Neu, C., Tannenwald, B., White, S., Wolfe, E., Poudyal, N., Black, K., Bose, T., Buchanan, J., Caillol, C., Dasu, S., De Bruyn, I., Everaerts, P., Fienga, F., Galloni, C., He, H., Herndon, M., Hervé, A., Hussain, U., Lanaro, A., Loeliger, A., Loveless, R., Sreekala, J. Madhusudanan, Mallampalli, A., Mohammadi, A., Pinna, D., Savin, A., Shang, V., Sharma, V., Smith, W. H., Teague, D., Trembath-reichert, S., and Vetens, W. "Combined searches for the production of supersymmetric top quark partners in proton–proton collisions at $$\sqrt{s} = 13\,\text {Te}\text {V} $$". The European Physical Journal C 81 (11). Country unknown/Code not available. https://doi.org/10.1140/epjc/s10052-021-09721-5. https://par.nsf.gov/biblio/10330326.
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Cite: BibTeX Format@article{osti_10330326,
place = {Country unknown/Code not available}, title = {Combined searches for the production of supersymmetric top quark partners in proton–proton collisions at $$\sqrt{s} = 13\,\text {Te}\text {V} $$}, url = {https://par.nsf.gov/biblio/10330326}, DOI = {10.1140/epjc/s10052-021-09721-5}, abstractNote = {Abstract A combination of searches for top squark pair production using proton–proton collision data at a center-of-mass energy of 13 $$\,\text {Te}\text {V}$$ Te at the CERN LHC, corresponding to an integrated luminosity of 137 $$\,\text {fb}^{-1}$$ fb - 1 collected by the CMS experiment, is presented. Signatures with at least 2 jets and large missing transverse momentum are categorized into events with 0, 1, or 2 leptons. New results for regions of parameter space where the kinematical properties of top squark pair production and top quark pair production are very similar are presented. Depending on the model, the combined result excludes a top squark mass up to 1325 $$\,\text {Ge}\text {V}$$ Ge for a massless neutralino, and a neutralino mass up to 700 $$\,\text {Ge}\text {V}$$ Ge for a top squark mass of 1150 $$\,\text {Ge}\text {V}$$ Ge . Top squarks with masses from 145 to 295 $$\,\text {Ge}\text {V}$$ Ge , for neutralino masses from 0 to 100 $$\,\text {Ge}\text {V}$$ Ge , with a mass difference between the top squark and the neutralino in a window of 30 $$\,\text {Ge}\text {V}$$ Ge around the mass of the top quark, are excluded for the first time with CMS data. The results of theses searches are also interpreted in an alternative signal model of dark matter production via a spin-0 mediator in association with a top quark pair. Upper limits are set on the cross section for mediator particle masses of up to 420 $$\,\text {Ge}\text {V}$$ Ge .}, journal = {The European Physical Journal C}, volume = {81}, number = {11}, author = {Tumasyan, A. and Adam, W. and Andrejkovic, J. W. and Bergauer, T. and Chatterjee, S. and Dragicevic, M. and Del Valle, A. Escalante and Frühwirth, R. and Jeitler, M. and Krammer, N. and Lechner, L. and Liko, D. and Mikulec, I. and Paulitsch, P. and Pitters, F. M. and Schieck, J. and Schöfbeck, R. and Spanring, M. and Templ, S. and Waltenberger, W. and Wulz, C.-E. and Chekhovsky, V. and Litomin, A. and Makarenko, V. and Darwish, M. R. and De Wolf, E. A. and Janssen, X. and Kello, T. and Lelek, A. and Sfar, H. Rejeb and Mechelen, P. Van and Putte, S. Van and Van Remortel, N. and Blekman, F. and Bols, E. S. and D’Hondt, J. and De Clercq, J. and Delcourt, M. and El Faham, H. and Lowette, S. and Moortgat, S. and Morton, A. and Müller, D. and Sahasransu, A. 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