## In each analysis pool, these plots contributed:

### Analysis Pool:ATLAS_7_LMDY

ATLAS_2014_I1288706/ATLAS_2014_I1288706_d02-x01-y01 :

### Analysis Pool:CMS_7_Zjj

CMS_2013_I1256943/CMS_2013_I1256943_d07-x01-y01 :

### Analysis Pool:ATLAS_7_GAMMA

ATLAS_2012_I1199269/ATLAS_2012_I1199269_d02-x01-y01 :

### Analysis Pool:CMS_7_Wjj

CMS_2014_I1303894/CMS_2014_I1303894_d12-x01-y01 :

### Analysis Pool:CMS_7_GAMMA

CMS_2014_I1266056/CMS_2014_I1266056_d01-x01-y01 :

### Analysis Pool:ATLAS_7_W_GAMMA_MU

ATLAS_2013_I1217863_W_MU/ATLAS_2013_I1217863_W_MU_d07-x01-y03 :

### Analysis Pool:ATLAS_7_Zjj_MU

ATLAS_2014_I1306294_MU/ATLAS_2014_I1306294_MU_d03-x01-y01 :

### Analysis Pool:ATLAS_7_Z_GAMMA

ATLAS_2013_I1217863_Z/ATLAS_2013_I1217863_Z_d11-x01-y01 :

### Analysis Pool:ATLAS_7_W_GAMMA_EL

ATLAS_2013_I1217863_W_EL/ATLAS_2013_I1217863_W_EL_d07-x01-y02 :

### Analysis Pool:ATLAS_7_ZZ

ATLAS_2012_I1203852/ATLAS_2012_I1203852_d01-x01-y02 :

### Analysis Pool:ATLAS_7_Wjj_MU

ATLAS_2014_I1319490_MU/ATLAS_2014_I1319490_MU_d21-x01-y03 :

### Analysis Pool:ATLAS_7_Wjj_EL

ATLAS_2014_I1319490_EL/ATLAS_2014_I1319490_EL_d21-x01-y02 :

### Analysis Pool:ATLAS_7_Zjj_EL

ATLAS_2014_I1306294_EL/ATLAS_2014_I1306294_EL_d23-x01-y01 :

### Analysis Pool:ATLAS_7_WW

ATLAS_2013_I1190187/ATLAS_2013_I1190187_d01-x01-y03 :

### Analysis Pool:ATLAS_7_Wjj

ATLAS_2015_I1345452/ATLAS_2015_I1345452_d13-x01-y02:

### Pseudo-top-antitop cross sections (ATLAS_2015_I1345452)

Inspire | HepData | arXiv:1502.05923 [hep-ex]

Various differential cross-sections are measured in top-quark pair ($t\bar{t}$) events produced in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=7$ TeV at the LHC with the ATLAS detector. These differential cross-sections are presented in a data set corresponding to an integrated luminosity of 4.6 fb$^{-1}$. The differential cross-sections are presented in terms of kinematic variables of a top-quark proxy referred to as the pseudo-top-quark whose dependence on theoretical models is minimal. The pseudo-top-quark can be defined in terms of either reconstructed detector objects or stable particles in an analogous way. The measurements are performed on $t\bar{t}$ events in the lepton+jets channel, requiring exactly one charged lepton and at least four jets with at least two of them tagged as originating from a $b$-quark. The hadronic and leptonic pseudo-top-quarks are defined via the leptonic or hadronic decay mode of the W boson produced by the top-quark decay in events with a single charged lepton. The cross-section is measured as a function of the transverse momentum and rapidity of both the hadronic and leptonic pseudo-top-quark as well as the transverse momentum, rapidity and invariant mass of the pseudo-top-quark pair system. The measurements are corrected for detector effects and are presented within a kinematic range that closely matches the detector acceptance.

### W + jets (ATLAS_2014_I1319490_EL)

Inspire | HepData | Eur.Phys.J. C75 (2015) 82 | doi:10.1140/epjc/s10052-015-3262-7 | arXiv:1409.8639 [hep-ex]

Measurements of cross sections for the production of a $W$ boson in association with jets in proton–proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS experiment at the Large Hadron Collider. With an integrated luminosity of 4.6 $\text{fb}^{−1}$, this data set allows for an exploration of a large kinematic range, including jet production up to a transverse momentum of 1 TeV and multiplicities up to seven associated jets. The production cross sections for W bosons are measured in both the electron and muon decay channels. Differential cross sections for many observables are also presented including measurements of the jet observables such as the rapidities and the transverse momenta as well as measurements of event observables such as the scalar sums of the transverse momenta of the jets. The default routine will pick up the electron decay channel of the $W$ boson and compare it to the combined (muon and electron channel) data. Individual channels (for data) are available as well, use ATLAS_2014_I1312627_EL and ATLAS_2014_I1312627_MU to specify the decay channel directly.

### W + jets (ATLAS_2014_I1319490_MU)

Inspire | HepData | Eur.Phys.J. C75 (2015) 82 | doi:10.1140/epjc/s10052-015-3262-7 | arXiv:1409.8639 [hep-ex]

Measurements of cross sections for the production of a $W$ boson in association with jets in proton–proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS experiment at the Large Hadron Collider. With an integrated luminosity of 4.6 $\text{fb}^{−1}$, this data set allows for an exploration of a large kinematic range, including jet production up to a transverse momentum of 1 TeV and multiplicities up to seven associated jets. The production cross sections for W bosons are measured in both the electron and muon decay channels. Differential cross sections for many observables are also presented including measurements of the jet observables such as the rapidities and the transverse momenta as well as measurements of event observables such as the scalar sums of the transverse momenta of the jets. The default routine will pick up the electron decay channel of the $W$ boson and compare it to the combined (muon and electron channel) data. Individual channels (for data) are available as well, use ATLAS_2014_I1312627_EL and ATLAS_2014_I1312627_MU to specify the decay channel directly.

### Measurement of Z boson in association with b-jets at 7 TeV in ATLAS (muon channel) (ATLAS_2014_I1306294_MU)

Inspire | HepData | arXiv:1407.3643 [hep-ex] | JHEP 1410 (2014) 141

Measurements of differential production cross-sections of a $Z$ boson in association with $b$-jets in $pp$ collisions at $\sqrt{s}=7$ TeV are reported. The data analysed correspond to an integrated luminosity of 4.6 fb$^{-1}$ recorded with the ATLAS detector at the Large Hadron Collider. Particle-level cross-sections are determined for events with a $Z$ boson decaying into an electron or muon pair, and containing $b$-jets. For events with at least one $b$-jet, the cross-section is presented as a function of the $Z$ boson transverse momentum and rapidity, together with the inclusive $b$-jet cross-section as a function of $b$-jet transverse momentum, rapidity and angular separations between the $b$-jet and the $Z$ boson. For events with at least two $b$-jets, the cross-section is determined as a function of the invariant mass and angular separation of the two highest transverse momentum $b$-jets, and as a function of the $Z$ boson transverse momentum and rapidity. Results are compared to leading-order and next-to-leading-order perturbative QCD calculations. This Rivet module implements the event selection for Z decaying into muons. If you want to use electronic events, please refer to ATLAS\_2014\_I1306294\_EL

### Measurement of Z boson in association with b-jets at 7 TeV in ATLAS, (electron channel) (ATLAS_2014_I1306294_EL)

Inspire | HepData | arXiv:1407.3643 [hep-ex] | JHEP 1410 (2014) 141

Measurements of differential production cross-sections of a $Z$ boson in association with $b$-jets in $pp$ collisions at $\sqrt{s}=7$ TeV are reported. The data analysed correspond to an integrated luminosity of 4.6 fb$^{-1}$ recorded with the ATLAS detector at the Large Hadron Collider. Particle-level cross-sections are determined for events with a $Z$ boson decaying into an electron or muon pair, and containing $b$-jets. For events with at least one $b$-jet, the cross-section is presented as a function of the $Z$ boson transverse momentum and rapidity, together with the inclusive $b$-jet cross-section as a function of $b$-jet transverse momentum, rapidity and angular separations between the $b$-jet and the $Z$ boson. For events with at least two $b$-jets, the cross-section is determined as a function of the invariant mass and angular separation of the two highest transverse momentum $b$-jets, and as a function of the $Z$ boson transverse momentum and rapidity. Results are compared to leading-order and next-to-leading-order perturbative QCD calculations. This Rivet module implements the event selection for Z decaying into electrons. If you want to use muonic events, please refer to ATLAS\_2014\_I1306294\_MU

### Measurement of the low-mass Drell-Yan differential cross section at 7 TeV (ATLAS_2014_I1288706)

Inspire | HepData | JHEP06(2014)112 | doi:10.1007/JHEP06(2014)112 | arXiv:1404.1212 [hep-ex]

Measurements of the differential cross section for the process $Z/\gamma^\ast \rightarrow l$ $(l = e, \mu)$ as a function of dilepton invariant mass in pp collisions at $\sqrt{s} = 7$ TeV. The measurement is performed in the $e$ and $\mu$ channels for invariant masses between 26 GeV and 66 GeV in the fiducial region $p_\text{T}^\text{leading} > 15$ GeV, $p_\text{T}^\text{subleading} > 12$ GeV, $|\eta| < 2.4$ using an integrated luminosity of 1.6 $\text{fb}^{-1}$. The analysis is extended to invariant masses as low as 12 GeV in the muon channel within a fiducal region of $p_\text{T}^\text{leading} > 9$ GeV, $p_\text{T}^\text{subleading} > 6$ GeV, $|\eta| < 2.4$ with 35 $\text{pb}^{-1}$.

### W + charm production at 7 TeV (ATLAS_2014_I1282447)

Inspire | HepData | JHEP 1405 (2014) 068 | doi:10.1007/JHEP05(2014)068 | arXiv:1402.6263 [hep-ex]

This routine implements the measurement of $W$ boson production in association with a single charm quark with $4.6 \text{fb}^{-1}$ of $pp$ collision data at $\sqrt{s} = 7$ TeV collected with the ATLAS detector at the Large Hadron Collider. Results are quoted for the $W$ boson production decaying into either an electron or muon and the charm quark being identified as any charmed hadron above 5 GeV inside $\Delta R = 0.4$ of a jet with more than 25 GeV. Alternatively the presence of the charm quark is indicated by the presence of a $D$ or a $D^*$ meson with a $p_\text{T}$ above 8 GeV. The cross sections are quoted for the number of opposite sign minus same sign events, where the signs under consideration are the charge of the $W$ boson and the charmed hadrons tagging the event. Given are the integrated and differential cross sections as a function of the pseudorapidity of the lepton from the $W$-boson decay are measured. Additionally, the cross-section ratios $\sigma(W^+ + bar{c}) / \sigma(W^- + c)$ as well as the $p_\text{T}$ dependent cross sections of the $D$/$D^*$ mesons normalized to the $W$ inclusive cross sections are published. The measured data is unfolded to the Born level. One should therefore take care to run on samples without QED radiation off of the electrons. IMPORTANT NOTICE --- For the MC predictions in the paper, the branching fractions to $D$ and $D^*$ mesons have been adapted to be 0.2256 ($D$) and 0.2287 ($D^*$) (LEP/HERA combination). Some suggestion on how to do post-processing -- in case separate samples for $W^+ + c$ and $W^- + c$ and inclusive $W$ are used -- are included in the cc-file. This post-processing is needed to properly display the histograms for the cross section ratio plots $\sigma(W^+ + bar{c}) / \sigma(W^- + c)$ as well as for the cross section ratios of $W + D^{(*)}$ production over inclusive $W$ production ($\sigma(W^{+/-} D^{(*)}) / \sigma(W^{+/-})$) as a function of the $D^{(*)}$ meson transverse momentum.

### Inclusive isolated prompt photon analysis with 2011 LHC data (ATLAS_2013_I1263495)

Inspire | HepData | arXiv:1311.1440 [hep-ex] | Phys.Rev. D89 (2014) 052004

A measurement of the cross section for the production of isolated prompt photons in pp collisions at a center-of-mass energy $sqrt{s} = 7$ TeV is presented. The results are based on an integrated luminosity of 4.6 fb$^{-1}$ collected with the ATLAS detector at the LHC. The cross section is measured as a function of photon pseudorapidity $\eta^\gamma$ and transverse energy $E_T^\gamma$ in the kinematic range $100 < E_T^\gamma < 1000$ GeV and in the regions $|\eta^\gamma| < 1.37$ and $1.52 < |\eta^\gamma| < 2.37$. The results are compared to leading-order parton-shower Monte Carlo models and next-to-leading order perturbative QCD calculations. Next to-leading-order perturbative QCD calculations agree well with the measured cross sections as a function of $E_T^\gamma$ and $\eta^\gamma$.

### Photon + jets (ATLAS_2013_I1244522)

Inspire | HepData | Nucl.Phys. B875 (2013) 483-535 | doi:10.1016/j.nuclphysb.2013.07.025 | arXiv:1307.6795 [hep-ex]

Measurements of isolated photon plus jet production in $pp$ collisions at a centre-of-mass energy of 7 TeV with the ATLAS detector at the LHC using an integrated luminosity of $37 \text{pb}^{-1}$. Differential cross sections are presented as functions of photon transverse energy, jet transverse momentum and jet rapidity. In addition, the differential cross sections as functions of the difference between the azimuthal angles of the photon and the jet, the photon-jet invariant mass as well as the scattering angle in the photon-jet centre-of-mass frame have been measured.

### $Z +$ jets in $pp$ at 7 TeV (electron channel) (ATLAS_2013_I1230812_EL)

Inspire | HepData | arXiv:1304.7098 [hep-ex] | J. High Energy Phys. 07 (2013) 032

Measurements of the production of jets of particles in association with a Z boson in pp collisions at $\sqrt{s}$ = 7 TeV are presented, using data corresponding to an integrated luminosity of 4.6/fb collected by the ATLAS experiment at the Large Hadron Collider. Inclusive and differential jet cross sections in Z events, with Z decaying into electron or muon pairs, are measured for jets with transverse momentum $p_T > 30$ GeV and rapidity $|y| < 4.4$. This Rivet module implements the event selection for Z decaying into electrons and uses the data measured explicitly in this channel (not the combined results shown in the paper plots). If you want to use muonic events, please refer to ATLAS\_2013\_I1230812\_MU.

### $Z +$ jets in $pp$ at 7 TeV (muon channel) (ATLAS_2013_I1230812_MU)

Inspire | HepData | arXiv:1304.7098 [hep-ex] | J. High Energy Phys. 07 (2013) 032

Measurements of the production of jets of particles in association with a Z boson in pp collisions at $\sqrt{s}$ = 7 TeV are presented, using data corresponding to an integrated luminosity of 4.6/fb collected by the ATLAS experiment at the Large Hadron Collider. Inclusive and differential jet cross sections in Z events, with Z decaying into electron or muon pairs, are measured for jets with transverse momentum $p_T > 30$ GeV and rapidity $|y| < 4.4$. This Rivet module implements the event selection for Z decaying into muons and uses the data measured explicitly in this channel (not the combined results shown in the paper plots). If you want to use electronic events, please refer to ATLAS\_2013\_I1230812\_EL.

### W + b production at 7 TeV (ATLAS_2013_I1219109_MU)

Inspire | HepData | JHEP 1306 (2013) 084 | doi:10.1007/JHEP06(2013)084 | arXiv:1302.2929 [hep-ex]

Measurements of the W+b-jets ($W+b+X$ and $W+b\bar{b}+X$) production cross-section in proton-proton collisions at a centre-of-mass energy of 7 TeV at the LHC. These results are based on data corresponding to an integrated luminosity of 4.6 $fb^{−1}$, collected with the ATLAS detector. Cross-sections are presented as a function of jet multiplicity and of the transverse momentum of the leading b-jet for both the combined muon and electron decay modes of the W boson. The default routine will consider the electron decay channel of the W boson. Use ATLAS_2013_I1219109_EL and ATLAS_2013_I1219109_MU to specify the decay channel directly.

### W + b production at 7 TeV (ATLAS_2013_I1219109_EL)

Inspire | HepData | JHEP 1306 (2013) 084 | doi:10.1007/JHEP06(2013)084 | arXiv:1302.2929 [hep-ex]

Measurements of the W+b-jets ($W+b+X$ and $W+b\bar{b}+X$) production cross-section in proton-proton collisions at a centre-of-mass energy of 7 TeV at the LHC. These results are based on data corresponding to an integrated luminosity of 4.6 $fb^{−1}$, collected with the ATLAS detector. Cross-sections are presented as a function of jet multiplicity and of the transverse momentum of the leading b-jet for both the combined muon and electron decay modes of the W boson. The default routine will consider the electron decay channel of the W boson. Use ATLAS_2013_I1219109_EL and ATLAS_2013_I1219109_MU to specify the decay channel directly.

### W + gamma production at 7 TeV (ATLAS_2013_I1217863_W_MU)

Inspire | HepData | Phys.Rev. D87 (2013) 112003 | doi:10.1103/PhysRevD.87.112003 | arXiv:1302.1283 [hep-ex]

Measurements of the differential fiducial cross sections for the production of a W boson in association with a high-energy photon are measured using pp collisions at \sqrt{s}=7 TeV. The analysis uses a data sample with an integrated luminosity of 4.6 fb-1 collected by the ATLAS detector during the 2011 LHC data-taking period. Events are selected using leptonic decays of the W bosons with the requirement of an associated isolated photon. The default routine will consider the electron decay channel of the W boson. Use ATLAS_2013_I1217863_W_EL and ATLAS_2013_I1217863_W_MU to specify the decay channel directly.

### Z + gamma production at 7 TeV (ATLAS_2013_I1217863_Z)

Inspire | HepData | Phys.Rev. D87 (2013) 112003 | doi:10.1103/PhysRevD.87.112003 | arXiv:1302.1283 [hep-ex]

Measurements of the differential fiducial cross sections for the production of a Z boson in association with a high-energy photon are measured using pp collisions at \sqrt{s}=7 TeV. The analysis uses a data sample with an integrated luminosity of 4.6 fb-1 collected by the ATLAS detector during the 2011 LHC data-taking period. Events are selected using leptonic decays of the Z bosons with the requirement of an associated isolated photon. The default routine will consider the electron decay channel of the Z boson. Use ATLAS_2013_I1217863_Z_EL and ATLAS_2013_I1217863_Z_MU to specify the decay channel directly.

### W + gamma production at 7 TeV (ATLAS_2013_I1217863_W_EL)

Inspire | HepData | Phys.Rev. D87 (2013) 112003 | doi:10.1103/PhysRevD.87.112003 | arXiv:1302.1283 [hep-ex]

Measurements of the differential fiducial cross sections for the production of a W boson in association with a high-energy photon are measured using pp collisions at \sqrt{s}=7 TeV. The analysis uses a data sample with an integrated luminosity of 4.6 fb-1 collected by the ATLAS detector during the 2011 LHC data-taking period. Events are selected using leptonic decays of the W bosons with the requirement of an associated isolated photon. The default routine will consider the electron decay channel of the W boson. Use ATLAS_2013_I1217863_W_EL and ATLAS_2013_I1217863_W_MU to specify the decay channel directly.

### Measurement of the $W^+ W^-$ production cross-section at 7 TeV (ATLAS_2013_I1190187)

Inspire | HepData | arXiv:1210.2979 [hep-ex]

Measurement of the fiducial cross section for $W^+ W^-$ production in proton proton collisions at a centre-of mass energy of 7 TeV, is presented, using data corresponding to an integrated luminosity of 4.6/fb collected by the ATLAS experiment at the Large Hadron Collider. The cross section is measured in the leptonic decay channels, using electron+MET and muon+MET $W$ decays. $W \to \tau$ processes with the tau decaying into electron + MET or muon + MET are also included in the measurement. The fiducial region contains dressed leptons in restricted $p_T$ and $\eta$ ranges. The selection has specific requirements for each production channel. A measurement of the normalized fiducial cross section as a function of the leading lepton transverse momentum is also presented.

### Measurement of the $ZZ(*)$ production cross-section in $pp$ collisions at 7 TeV with ATLAS (ATLAS_2012_I1203852)

Inspire | HepData | arXiv:1211.6096 [hep-ex]

Measurement of the fiducial cross section for $ZZ(*)$ production in proton proton collisions at a centre-of mass energy of 7 TeV, is presented, using data corresponding to an integrated luminosity of 4.6/fb collected by the ATLAS experiment at the Large Hadron Collider. The cross-section is measured using processes with two $Z$ bosons decaying to electrons or muons or with one $Z$ boson decaying to electrons or muons and a second $Z$ boson decaying to neutrinos. The fiducial region contains dressed leptons in restricted $p_T$ and $\eta$ ranges. The selection has specific requirements for both production processes. A measurement of the normalized fiducial cross-section as a function of $ZZ$ invariant mass, leading $Z$ $p_T$ and angle of two leptons coming from the leading $Z$ is also presented for both signal processes.

### Inclusive diphoton $+ X$ events at $\sqrt{s} = 7$ TeV (ATLAS_2012_I1199269)

Inspire | HepData | arXiv:1211.1913 [hep-ex] | JHEP 1301 (2013) 086

The ATLAS experiment at the LHC has measured the production cross section of events with two isolated photons in the final state, in proton-proton collisions at $\sqrt{s} = 7$ TeV. The full data set collected in 2011, corresponding to an integrated luminosity of 4.9 fb$^{-1}$, is used. The amount of background, from hadronic jets and isolated electrons, is estimated with data-driven techniques and subtracted. The total cross section, for two isolated photons with transverse energies above 25 GeV and 22 GeV respectively, in the acceptance of the electromagnetic calorimeter ($|\eta|<1.37$ and $1.52<|\eta|<2.37$) and with an angular separation $\Delta R>0.4$, is $44.0^{+3.2}_{-4.2}$ pb. The differential cross sections as a function of the di-photon invariant mass, transverse momentum, azimuthal separation, and cosine of the polar angle of the largest transverse energy photon in the Collins--Soper di-photon rest frame are also measured. The results are compared to the prediction of leading-order parton-shower and next-to-leading-order and next-to-next-to-leading-order parton-level generators.

### Isolated prompt photon + jet cross-section (ATLAS_2012_I1093738)

Inspire | HepData | arXiv:1203.3161 [hep-ex]

A measurement of the production cross section for isolated photons in association with jets in $pp$ collisions at $\sqrt{s} = 7$ TeV. Photons with $|\eta|<1.37$ and $E_T>25$ GeV and jets with $|y|<4.4$ and $p_T>20$ GeV are selected. The differential cross section as a function of the photon transverse energy is measured, for three leading jet rapidity configurations, separately for the cases where the photon and jet rapidities have the same or the opposite sign. The measurement uses 37 pb$^{-1}$ of integrated luminosity collected with the ATLAS detector.

### Measurement of electron and muon differential cross-section from heavy-flavour decays (ATLAS_2011_I926145)

Inspire | HepData | CERN-PH-EP-2011-108 | arXiv:1109.0525 [hep-ex]

Measurement of inclusive electron and muon cross sections for $7 < p_\perp <26$ GeV in $|\eta| <2.0$, excluding $1.37<|\eta|<1.52$, and muon cross section for $4 < p_\perp < 100$ GeV in $|\eta| <2.50$. The $W/Z/\gamma^*$ component must be subtracted to leave the heavy flavour contribution.

### Jet multiplicity and differential cross-sections of $Z$+jets events in $pp$ at $\sqrt{s} = 7$ TeV (CMS_2015_I1310737)

Inspire | HepData | Phys.Rev. D91 (2015) 052008 | http://dx.doi.org/10.1103/PhysRevD.91.052008 | http://arxiv.org/abs/arXiv:1408.3104 | http://inspirehep.net/record/1310737

Measurements of differential cross sections are presented for the production of a Z boson and at least one hadronic jet in proton-proton collisions at $\sqrt{s}=7$ TeV, recorded by the CMS detector, using a data sample corresponding to an integrated luminosity of 4.9 $\text{fb}^{-1}$. The jet multiplicity distribution is measured for up to six jets. The differential cross sections are measured as a function of jet transverse momentum and pseudorapidity for the four highest transverse momentum jets. The distribution of the scalar sum of jet transverse momenta is also measured as a function of the jet multiplicity. The measurements are compared with theoretical predictions at leading and next-to-leading order in perturbative QCD. Cuts: First two leading electrons or muons with $p_T > 20$ GeV and $|\eta| < 2.4$ Dilepton invariant mass in the [71,111] GeV range Jets $p_T > 30$ GeV and $|\eta| < 2.4$ $\Delta{R}($lepton,jet$) > 0.5$

### Differential cross-section of $W$ bosons + jets in $pp$ collisions at $\sqrt{s}=7$ TeV (CMS_2014_I1303894)

Inspire | HepData | Phys. Lett. B741 (2014) 12-37 | https://inspirehep.net/record/1303894 | http://arxiv.org/abs/1406.7533

A study of jet production in association with $W$ bosons has been performed, in events with the $W$ decaying to a muon. Jets are required to have $pT > 30$ GeV and $|eta| < 2.4$. Muons are required to have $pT > 25$ and $|eta| < 2.1$. Jets are only considered if they are separated from the muon by $\Delta{R} > 0.5$. Muons are dressed with photons in a cone of $0.1$ around the muon.

### Photon + jets triple differential cross-section (CMS_2014_I1266056)

Inspire | HepData | arXiv:1311.6141 [hep-ex]

A measurement of the triple differential cross section in photon+jets final states in $pp$ collisions at $\sqrt{s} = 7$ TeV. Photons with $|\eta|<2.5$ and $40$ GeV$<p_T<300$ GeV and jets with $|\eta|<2.5$ and $p_T>30$ GeV are selected. The measurement uses 2.14 fb$^{-1}$ of integrated luminosity collected with the CMS detector.

### Cross-section and angular correlations in $Z$ boson with $b$-hadrons events at $\sqrt{s} = 7$ TeV (CMS_2013_I1256943)

Inspire | HepData | 10.1007 / JHEP12(2013)039 | arXiv:1310.1349 | CERN-PH-EP-2013-153 | CMS-EWK-11-015

A study of proton-proton collisions in which two $b$-hadrons are produced in association with a $Z$ boson is reported. The collisions were recorded at a centre-of-mass energy of 7 TeV with the CMS detector at the LHC, for an integrated luminosity of 5.2/fb. The $b$-hadrons are identified by means of displaced secondary vertices, without the use of reconstructed jets, permitting the study of $b$-hadron pair production at small angular separation. Differential cross sections are presented as a function of the angular separation of the $b$-hadrons and the $Z$ boson. In addition, inclusive measurements are presented. For both the inclusive and differential studies,different ranges of $Z$ boson momentum are considered.

### CMS jet mass measurement in $W$ + jet events (CMS_2013_I1224539_WJET)

Inspire | HepData | arXiv:1303.4811

Measurements of the mass spectra of the jets in dijet and $W/Z$+jet events from proton--proton collisions at a centre-of-mass energy of 7 TeV using a data sample of integrated luminosity of 5 fb$^-1$. The jets are reconstructed using the both the anti-$k_T$ algorithm with $R=0.7$ (AK7) and the Cambridge-Aachen algorithm with $R=0.8$ (CA8) and $R=1.2$ (CA12) with several grooming techniques applied (ungroomed, filtered, pruned and trimmed). See the text of the paper for more details. For the dijet events the distributions are presented as a function of the mean Mass of the two leading jets in bins of the mean p_\perp of the two jets.

### CMS jet mass measurement in $Z$ + jet events (CMS_2013_I1224539_ZJET)

Inspire | HepData | arXiv:1303.4811

Measurements of the mass spectra of the jets in dijet and $W/Z$+jet events from proton--proton collisions at a centre-of-mass energy of 7 TeV using a data sample of integrated luminosity of 5 fb$^-1$. The jets are reconstructed using the both the anti-$k_T$ algorithm with $R=0.7$ (AK7) and the Cambridge-Aachen algorithm with $R=0.8$ (CA8) and $R=1.2$ (CA12) with several grooming techniques applied (ungroomed, filtered, pruned and trimmed). See the text of the paper for more details. For the dijet events the distributions are presented as a function of the mean Mass of the two leading jets in bins of the mean p_\perp of the two jets.

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