MASS LIMITS for Excited ${{\boldsymbol q}}$ (${{\boldsymbol q}^{*}}$)

Limits for Excited ${{\boldsymbol q}}$ (${{\boldsymbol q}^{*}}$) from Single Production INSPIRE search

These limits are from ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\overline{\mathit q}}}$ , ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit q}^{*}}$ X, or ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}$ X and depend on transition magnetic couplings between ${{\mathit q}}$ and ${{\mathit q}^{*}}$. Assumptions about ${{\mathit q}^{*}}$ decay mode are given in the footnotes and comments.
VALUE (GeV) CL% DOCUMENT ID TECN  COMMENT
$\bf{>6000}$ 95 1
AABOUD
2017AK
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit g}}$
• • • We do not use the following data for averages, fits, limits, etc. • • •
$\text{none 600 - 5400}$ 95 2
KHACHATRYAN
2017W
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit g}}$
$\text{none 1100 - 2100}$ 95 3
AABOUD
2016
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}^{*}}{{\mathit X}}$ , ${{\mathit b}^{*}}$ $\rightarrow$ ${{\mathit b}}{{\mathit g}}$
$> 1500$ 95 4
AAD
2016AH
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}^{*}}{{\mathit X}}$ , ${{\mathit b}^{*}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$
$> 4400$ 95 5
AAD
2016AI
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit \gamma}}$
6
AAD
2016AV
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit W}}{{\mathit b}}$
$> 5200$ 95 7
AAD
2016S
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit g}}$
$> 1390$ 95 8
KHACHATRYAN
2016I
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}^{*}}{{\mathit X}}$ , ${{\mathit b}^{*}}$ $\rightarrow$ ${{\mathit t}}{{\mathit W}}$
$> 5000$ 95 9
KHACHATRYAN
2016K
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit g}}$
$\text{none 500 - 1600}$ 95 10
KHACHATRYAN
2016L
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit g}}$
$> 4060$ 95 11
AAD
2015V
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit g}}$
$> 3500$ 95 12
KHACHATRYAN
2015V
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit g}}$
$> 3500$ 95 13
AAD
2014A
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit \gamma}}$
$> 3200$ 95 14
KHACHATRYAN
2014
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit W}}$
$> 2900$ 95 15
KHACHATRYAN
2014
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit Z}}$
$\text{none 700 - 3500}$ 95 16
KHACHATRYAN
2014J
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit \gamma}}$
$> 2380$ 95 17
CHATRCHYAN
2013AJ
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit W}}$
$> 2150$ 95 18
CHATRCHYAN
2013AJ
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit q}^{*}}{{\mathit X}}$ , ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit q}}{{\mathit Z}}$
1  AABOUD 2017AK assume $\Lambda $ = ${\mathit m}_{{{\mathit q}^{*}}}$, ${{\mathit f}_{{s}}}$ = ${{\mathit f}}$ = ${{\mathit f}^{\,'}}$ = 1. The contact interactions are not included in ${{\mathit q}^{*}}$ production and decay amplitudes. Only the decay of ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit g}}{{\mathit u}}$ and ${{\mathit q}^{*}}$ $\rightarrow$ ${{\mathit g}}{{\mathit d}}$ is simulated as the benchmark signals in the analysis.
2  KHACHATRYAN 2017W assume $\Lambda $ = ${\mathit m}_{{{\mathit q}^{*}}}$, ${{\mathit f}_{{s}}}$ = ${{\mathit f}}$ = ${{\mathit f}^{\,'}}$ = 1. The contact interactions are not included in ${{\mathit q}^{*}}$ production and decay amplitudes.
3  AABOUD 2016 assume $\Lambda $ = ${\mathit m}_{{{\mathit b}^{*}}}$, ${{\mathit f}_{{s}}}$ = ${{\mathit f}}$ = ${{\mathit f}^{\,'}}$ = 1. The contact interactions are not included in the ${{\mathit b}^{*}}$ production and decay amplitudes.
4  AAD 2016AH search for ${{\mathit b}^{*}}$ decaying to ${{\mathit t}}{{\mathit W}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. ${{\mathit f}_{{g}}}$ = ${{\mathit f}_{{L}}}$ = ${{\mathit f}_{{R}}}$ = 1 are assumed. See their Fig. 12b for limits on $\sigma \cdot{}\mathit B$.
5  AAD 2016AI assume $\Lambda $ = ${\mathit m}_{{{\mathit q}^{*}}}$, ${{\mathit f}_{{s}}}$ = ${{\mathit f}}$ = ${{\mathit f}^{\,'}}$ = 1.
6  AAD 2016AV search for single production of vector-like quarks decaying to ${{\mathit W}}{{\mathit b}}$ in ${{\mathit p}}{{\mathit p}}$ collisions. See their Fig. 8 for the limits on couplings and mixings.
7  AAD 2016S assume $\Lambda $ = ${\mathit m}_{{{\mathit q}^{*}}}$, ${{\mathit f}_{{s}}}$ = ${{\mathit f}}$ = ${{\mathit f}^{\,'}}$ = 1. The contact interactions are not included in ${{\mathit q}^{*}}$ production and decay amplitudes.
8  KHACHATRYAN 2016I search for ${{\mathit b}^{*}}$ decaying to ${{\mathit t}}{{\mathit W}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. ${{\mathit \kappa}_{{L}}^{b}}$ = ${{\mathit g}_{{L}}}$ = 1, ${{\mathit \kappa}_{{R}}^{b}}$ = ${{\mathit g}_{{R}}}$ = 0 are assumed. See their Fig. 8 for limits on $\sigma \cdot{}\mathit B$.
9  KHACHATRYAN 2016K assume ${{\mathit \Lambda}}$ = ${\mathit m}_{{{\mathit q}^{*}}}$, ${{\mathit f}_{{s}}}$ = ${{\mathit f}}$ = ${{\mathit f}^{\,'}}$= 1. The contact interactions are not included in ${{\mathit q}^{*}}$ production and decay amplitudes.
10  KHACHATRYAN 2016L search for resonances decaying to dijets in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV using the data scouting technique which increases the sensitivity to the low mass resonances.
11  AAD 2015V assume ${{\mathit \Lambda}}$ = ${\mathit m}_{{{\mathit q}^{*}}}$, ${{\mathit f}_{{s}}}$ = ${{\mathit f}}$ = ${{\mathit f}^{\,'}}$ = 1. The contact interactions are not included in ${{\mathit q}^{*}}$ production and decay amplitudes.
12  KHACHATRYAN 2015V assume ${{\mathit \Lambda}}$ = ${\mathit m}_{{{\mathit q}^{*}}}$, ${{\mathit f}_{{s}}}$ = ${{\mathit f}}$ = ${{\mathit f}^{\,'}}$ = 1. The contact interactions are not included in ${{\mathit q}^{*}}$ production and decay amplitudes.
13  AAD 2014A assume ${{\mathit \Lambda}}$ = ${\mathit m}_{{{\mathit q}^{*}}}$, ${{\mathit f}_{{s}}}$ = ${{\mathit f}}$ = ${{\mathit f}^{\,'}}$ = 1.
14  KHACHATRYAN 2014 use the hadronic decay of ${{\mathit W}}$, assuming ${{\mathit \Lambda}}$ = ${\mathit m}_{{{\mathit q}^{*}}}$, ${{\mathit f}_{{s}}}={{\mathit f}}={{\mathit f}^{\,'}}$ = 1.
15  KHACHATRYAN 2014 use the hadronic decay of ${{\mathit Z}}$, assuming ${{\mathit \Lambda}}$ = ${\mathit m}_{{{\mathit q}^{*}}}$, ${{\mathit f}_{{s}}}={{\mathit f}}={{\mathit f}^{\,'}}$ = 1.
16  KHACHATRYAN 2014J assume ${{\mathit f}_{{s}}}$ = ${{\mathit f}}$ = ${{\mathit f}^{\,'}}$ = ${{\mathit \Lambda}}$ $/$ ${\mathit m}_{{{\mathit q}^{*}}}$.
17  CHATRCHYAN 2013AJ use the hadronic decay of ${{\mathit W}}$.
18  CHATRCHYAN 2013AJ use the hadronic decay of ${{\mathit Z}}$.
  References:
AABOUD 2017AK
PR D96 052004 Search for New Phenomena in Dijet Events using 37 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ Collision Data Collected at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
KHACHATRYAN 2017W
PL B769 520 Search for Dijet Resonances in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV and Constraints on Dark Matter and other Models
AABOUD 2016
PL B759 229 Search for Resonances in the Mass Distribution of Jet Pairs with One or Two Jets Identified as ${\mathit {\mathit b}}$-Jets in Proton-proton Collisions at $\sqrt {s }$ =13 TeV with the ATLAS Detector
AAD 2016S
PL B754 302 Search for New Phenomena in Dijet Mass and Angular Distributions from ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
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
AAD 2016AV
EPJ C76 442 Search for Single Production of Vector-like Quarks Decaying into ${{\mathit W}}{\mathit {\mathit b}}$ in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
AAD 2016AI
JHEP 1603 041 Search for New Phenomena with Photon $+$ Jet Events in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
KHACHATRYAN 2016K
PRL 116 071801 Search for Narrow Resonances Decaying to Dijets in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
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
KHACHATRYAN 2016L
PRL 117 031802 Search for Narrow Resonances in Dijet Final States at $\sqrt {s }$ = 8 TeV with the Novel CMS Technique of Data Scouting
AAD 2015V
PR D91 052007 Search for New Phenomena in the Dijet Mass Distribution using ${{\mathit p}}{{\mathit p}}$ Collision Data at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
KHACHATRYAN 2015V
PR D91 052009 Search for Resonances and Quantum Black Holes using Dijet Mass Spectra in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
AAD 2014A
PL B728 562 Search for New Phenomena in Photon + Jet Events Collected in Proton$−$Proton Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
KHACHATRYAN 2014
JHEP 1408 173 Search for Massive Resonances in Dijet Systems Containing Jets Tagged as ${{\mathit W}}$ or ${{\mathit Z}}$ Boson Decays in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV
KHACHATRYAN 2014J
PL B738 274 Search for Excited Quarks in the ${{\mathit \gamma}}$ + Jet Final State in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
CHATRCHYAN 2013AJ
PL B723 280 Search for Heavy Resonances in the ${{\mathit W}}/{{\mathit Z}}$-Tagged Dijet Mass Spectrum in ${{\mathit p}}{{\mathit p}}$ Collisions at 7 TeV
KHACHATRYAN 2014S
PL B739 23 Measurement of the ${\mathit {\mathit t}}{\mathit {\overline{\mathit t}}}$ Production Cross Section in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV in Dilepton Final States Containing one ${{\mathit \tau}}$ Lepton
AABOUD 2016AG
EPJ C76 670 Measurement of the ${\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ Dijet Cross Section in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV with the ATLAS Detector