${{\mathit b}^{\,'}}(-1$/3) mass limits from single production in ${{\mathit p}}{{\overline{\mathit p}}}$ and ${{\mathit p}}{{\mathit p}}$ collisions

INSPIRE   PDGID:
Q008BPS
VALUE (GeV) CL% DOCUMENT ID TECN  COMMENT
$\bf{> 3000}$ 95 1
TUMASYAN
2022O
 CMS ${{\mathit g}}$ ${{\mathit b}}$ $\rightarrow$ ${{\mathit b}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$ , B( ${{\mathit b}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$ )=1
$\bf{> 693}$ 95 2
ABAZOV
2011F
 D0 ${{\mathit q}}$ ${{\mathit u}}$ $\rightarrow$ ${{\mathit q}^{\,'}}{{\mathit b}^{\,'}}$ $\rightarrow$ ${{\mathit q}^{\,'}}$ ( ${{\mathit W}}{{\mathit u}}$ ) ${{\widetilde{\mathit \kappa}}}_{ {{\mathit u}} {{\mathit b}^{\,'}} }$=1, B( ${{\mathit b}^{\,'}}$ $\rightarrow$ ${{\mathit W}}{{\mathit u}}$ )=1
$\bf{> 430}$ 95 2
ABAZOV
2011F
 D0 ${{\mathit q}}$ ${{\mathit d}}$ $\rightarrow$ ${{\mathit q}}{{\mathit b}^{\,'}}$ $\rightarrow$ ${{\mathit q}}$ ( ${{\mathit Z}}{{\mathit d}}$ ) ${{\widetilde{\mathit \kappa}}}_{ {{\mathit d}} {{\mathit b}^{\,'}} }=\sqrt {2 }$, B( ${{\mathit b}^{\,'}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit d}}$ )=1
• • We do not use the following data for averages, fits, limits, etc. • •
$>2600$ 95 3
SIRUNYAN
2021AG
 CMS ${{\mathit g}}$ ${{\mathit b}}$ $\rightarrow$ ${{\mathit b}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$ , B( ${{\mathit b}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$ )=1
4
SIRUNYAN
2019AI
 CMS ${{\mathit b}}$ ${{\mathit Z}}$ $/$ ${{\mathit t}}$ ${{\mathit W}}$ $\rightarrow$ ${{\mathit b}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$
$>1500$ 95 5
AAD
2016AH
 ATLS ${{\mathit g}}$ ${{\mathit b}}$ $\rightarrow$ ${{\mathit b}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$ , B( ${{\mathit b}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$ )=1
$> 1390$ 95 6
KHACHATRYA..
2016I
 CMS ${{\mathit g}}$ ${{\mathit b}}$ $\rightarrow$ ${{\mathit b}_{{{L}}}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$ , B( ${{\mathit b}_{{{L}}}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$ )=1
$> 1430$ 95 7
KHACHATRYA..
2016I
 CMS ${{\mathit g}}$ ${{\mathit b}}$ $\rightarrow$ ${{\mathit b}_{{{R}}}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$ , B( ${{\mathit b}_{{{R}}}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$ )=1
$> 1530$ 95 8
KHACHATRYA..
2016I
 CMS ${{\mathit g}}$ ${{\mathit b}}$ $\rightarrow$ ${{\mathit b}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$ , B( ${{\mathit b}^{\,'}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$ )=1
1  TUMASYAN 2022O based on 138 fb${}^{-1}$ of data in ${{\mathit p}}{{\mathit p}}$ collisions at 13 TeV. No significant excess over SM expectation is found in the search for a left-handed ${{\mathit b}^{\,'}}$ assuming 100$\%$ decay to ${{\mathit t}}{{\mathit W}}$ using a ${{\mathit t}}$-tagged jet and a lepton from ${{\mathit W}}$. The model assumes that the ${{\mathit b}^{\,'}}$ has the excited quark couplings. The bound is from a statistical combination with an earlier analysis by SIRUNYAN 2021AG. The 95$\%$ CL bounds are also set as 3.0, 3.0, and 3.2 TeV, respectively, for left-handed, right-handed, and vector-like couplings.
2  ABAZOV 2011F based on 5.4 fb${}^{-1}$ of data in ppbar collisions at 1.96 TeV. ABAZOV 2011F looked for single production of ${{\mathit b}^{\,'}}$ via the ${{\mathit W}}$ or ${{\mathit Z}}$ coupling to the first generation up or down quarks, respectively. Model independent cross section limits for the single production processes ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit b}^{\,'}}{{\mathit q}}$ $\rightarrow$ ${{\mathit W}}{{\mathit u}}{{\mathit q}}$ , and ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit b}^{\,'}}{{\mathit q}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit d}}{{\mathit q}}$ are given in Figs. 3 and 4, respectively, and the mass limits are obtained for the model of ATRE 2009 with degenerate bi-doublets of vector-like quarks.
3  SIRUNYAN 2021AG based on 137 fb${}^{-1}$ of data in ${{\mathit p}}{{\mathit p}}$ collisions at 13 TeV. No significant excess over SM expectation is found in the search for a left-handed ${{\mathit b}^{\,'}}$ assuming 100$\%$ decay to ${{\mathit t}}{{\mathit W}}$ using all hadronic final states, where ${{\mathit t}}$ and ${{\mathit W}}$ are tagged as single jets, respectively. The model assumes that the ${{\mathit b}^{\,'}}$ has the excited quark couplings. The 95$\%$ CL bounds are also set as 2.8 and 3.1 TeV, respectively, for the right-handed and vector-like couplings.
4  SIRUNYAN 2019AI based on 35.9 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ data at $\sqrt {s }$ = 13 TeV. Exclusion limits are set on the product of the production cross section and branching fraction for the ${{\mathit b}^{\,'}{(-1/3)}}{+}$ ${{\mathit b}}$ and ${{\mathit b}^{\,'}{(-1/3)}}{+}$ ${{\mathit t}}$ modes as a function of the vector-like quark mass in Figs. 7 and 8 and in Tab. 2 for relative vector-like quark widths between 1 and 30$\%$ for left- and right-handed vector-like quark couplings. No significant deviation from the SM prediction is observed.
5  AAD 2016AH based on 20.3 fb${}^{-1}$ of data in ${{\mathit p}}{{\mathit p}}$ collisions at 8 TeV. No significant excess over SM expectation is found in the search for a vector-like ${{\mathit b}^{\,'}}$ in the single-lepton and dilepton channels (${{\mathit \ell}}$ or ${{\mathit \ell}}{{\mathit \ell}}$ ) + 1,2,3 ${{\mathit j}}$ (${}\geq{}1{{\mathit b}}$). The model assumes that the ${{\mathit b}^{\,'}}$ has the excited quark couplings.
6  Based on 19.7 fb${}^{-1}$ of data in ${{\mathit p}}{{\mathit p}}$ collisions at 8 TeV. Limit on left-handed ${{\mathit b}^{\,'}}$ assuming 100$\%$ decay to ${{\mathit t}}{{\mathit W}}$ and using all-hadronic, lepton + jets, and dilepton final states.
7  Based on 19.7 fb${}^{-1}$ of data in ${{\mathit p}}{{\mathit p}}$ collisions at 8 TeV. Limit on right-handed ${{\mathit b}^{\,'}}$ assuming 100$\%$ decay to ${{\mathit t}}{{\mathit W}}$ and using all-hadronic, lepton + jets, and dilepton final states.
8  Based on 19.7 fb${}^{-1}$ of data in ${{\mathit p}}{{\mathit p}}$ collisions at 8 TeV. Limit on vector-like ${{\mathit b}^{\,'}}$ assuming 100$\%$ decay to ${{\mathit t}}{{\mathit W}}$ and using all-hadronic, lepton+jets, and dilepton final states.
References:
TUMASYAN 2022O
JHEP 2204 048 Search for a heavy resonance decaying into a top quark and a W boson in the lepton+jets final state at $ \sqrt{s} $ = 13 TeV
SIRUNYAN 2021AG
JHEP 2112 106 Search for a heavy resonance decaying to a top quark and a W boson at $ \sqrt{s} $ = 13 TeV in the fully hadronic final state
SIRUNYAN 2019AI
EPJ C79 90 Search for single production of vector-like quarks decaying to a top quark and a W boson in proton-proton collisions at $\sqrt{s} =$ 13 TeV
AAD 2016AH
JHEP 1602 110 Search for the Production of Single Vector-Like and Excited Quarks in the ${{\mathit W}}{\mathit {\mathit t}}$ Final State in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
KHACHATRYAN 2016I
JHEP 1601 166 Search for the Production of an Excited Bottom Quark Decaying to ${{\mathit t}}{{\mathit W}}$ in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
ABAZOV 2011F
PRL 106 081801 Search for Single Vectorlike Quarks in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV