Search for pair production of heavy particles decaying to a top quark and a gluon in the lepton+jets final state in proton–proton collisions at $$\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V} $$

A search is presented for the pair production of new heavy resonances, each decaying into a top quark (t) or antiquark and a gluon (g). The analysis uses data recorded with the CMS detector from proton-proton collisions at a center-of-mass energy of 13 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mspace></mml:mspace> <mml:mtext>Te</mml:mtext> <mml:mspace></mml:mspace> <mml:mtext>V</mml:mtext></mml:mrow> </mml:math> at the LHC, corresponding to an integrated luminosity of 138 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mspace></mml:mspace> <mml:msup><mml:mtext>fb</mml:mtext> <mml:mrow><mml:mo>-</mml:mo> <mml:mn>1</mml:mn></mml:mrow> </mml:msup> </mml:mrow> </mml:math> . Events with one muon or electron, multiple jets, and missing transverse momentum are selected. After using a deep neural network to enrich the data sample with signal-like events, distributions in the scalar sum of the transverse momenta of all reconstructed objects are analyzed in the search for a signal. No significant deviations from the standard model prediction are found. Upper limits at 95% confidence level are set on the product of cross section and branching fraction squared for the pair production of excited top quarks in the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow><mml:mmultiscripts><mml:mtext>t</mml:mtext> <mml:mrow></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> <mml:mo>→</mml:mo> <mml:mtext>tg</mml:mtext></mml:mrow> </mml:math> decay channel. The upper limits range from 120 to 0.8 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mspace></mml:mspace> <mml:mtext>fb</mml:mtext></mml:mrow> </mml:math> for a <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>t</mml:mtext> <mml:mrow></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> with spin-1/2 and from 15 to 1.0 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mspace></mml:mspace> <mml:mtext>fb</mml:mtext></mml:mrow> </mml:math> for a <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>t</mml:mtext> <mml:mrow></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> with spin-3/2. These correspond to mass exclusion limits up to 1050 and 1700 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mspace></mml:mspace> <mml:mtext>Ge</mml:mtext> <mml:mspace></mml:mspace> <mml:mtext>V</mml:mtext></mml:mrow> </mml:math> for spin-1/2 and spin-3/2 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>t</mml:mtext> <mml:mrow></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> particles, respectively. These are the most stringent limits to date on the existence of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow><mml:mmultiscripts><mml:mtext>t</mml:mtext> <mml:mrow></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> <mml:mo>→</mml:mo> <mml:mtext>tg</mml:mtext></mml:mrow> </mml:math> resonances.

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Journal
The European Physical Journal C
Published
2025-03-25
DOI
https://doi.org/10.1140/epjc/s10052-024-13729-y
Citations
1
Primary Topic
Particle physics theoretical and experimental studies
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article
Field-Weighted Citation Impact
1.87

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article

Search for pair production of heavy particles decaying to a top quark and a gluon in the lepton+jets final state in proton–proton collisions at $$\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V} $$

A. Santoro, T. Reis, B. Kailasapathy, M. A. Ciocci et al.
1 citations
The European Physical Journal C
Particle physics theoretical and experimental studies
1.87
article

Search for pair production of heavy particles decaying to a top quark and a gluon in the lepton+jets final state in proton–proton collisions at $$\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V} $$

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Mudholkar, Dongyub Lee, Jyothsna Rani Komaragiri, Nikhilesh Venkatasubramanian, L. A. T. Bauerdick, Jose Monroy, K. Kaadze, Y. Yao, G. S. F. Stephans, Paul Krueper
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Abstract

A search is presented for the pair production of new heavy resonances, each decaying into a top quark (t) or antiquark and a gluon (g). The analysis uses data recorded with the CMS detector from proton-proton collisions at a center-of-mass energy of 13 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mspace></mml:mspace> <mml:mtext>Te</mml:mtext> <mml:mspace></mml:mspace> <mml:mtext>V</mml:mtext></mml:mrow> </mml:math> at the LHC, corresponding to an integrated luminosity of 138 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mspace></mml:mspace> <mml:msup><mml:mtext>fb</mml:mtext> <mml:mrow><mml:mo>-</mml:mo> <mml:mn>1</mml:mn></mml:mrow> </mml:msup> </mml:mrow> </mml:math> . Events with one muon or electron, multiple jets, and missing transverse momentum are selected. After using a deep neural network to enrich the data sample with signal-like events, distributions in the scalar sum of the transverse momenta of all reconstructed objects are analyzed in the search for a signal. No significant deviations from the standard model prediction are found. Upper limits at 95% confidence level are set on the product of cross section and branching fraction squared for the pair production of excited top quarks in the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow><mml:mmultiscripts><mml:mtext>t</mml:mtext> <mml:mrow></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> <mml:mo>→</mml:mo> <mml:mtext>tg</mml:mtext></mml:mrow> </mml:math> decay channel. The upper limits range from 120 to 0.8 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mspace></mml:mspace> <mml:mtext>fb</mml:mtext></mml:mrow> </mml:math> for a <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>t</mml:mtext> <mml:mrow></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> with spin-1/2 and from 15 to 1.0 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mspace></mml:mspace> <mml:mtext>fb</mml:mtext></mml:mrow> </mml:math> for a <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>t</mml:mtext> <mml:mrow></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> with spin-3/2. These correspond to mass exclusion limits up to 1050 and 1700 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mspace></mml:mspace> <mml:mtext>Ge</mml:mtext> <mml:mspace></mml:mspace> <mml:mtext>V</mml:mtext></mml:mrow> </mml:math> for spin-1/2 and spin-3/2 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mtext>t</mml:mtext> <mml:mrow></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> </mml:math> particles, respectively. These are the most stringent limits to date on the existence of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow><mml:mmultiscripts><mml:mtext>t</mml:mtext> <mml:mrow></mml:mrow> <mml:mrow><mml:mrow></mml:mrow> <mml:mo>∗</mml:mo></mml:mrow> </mml:mmultiscripts> <mml:mo>→</mml:mo> <mml:mtext>tg</mml:mtext></mml:mrow> </mml:math> resonances.

The European Physical Journal CVol. 85(3)
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