Georgios Bakas
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Research Interests
Georgios Bakas has a total of 1000 co-authors. Here are the top co-authors by number of shared publications:
- A. Buchot Perraguin
The University of Alabama
155 shared publications - A. Mestvirishvili
The University of Iowa
155 shared publications - A. R. Kanuganti
University of Tennessee
155 shared publications - A. Rose
169 Imperial College, London, U.K.
155 shared publications - A. Zabi
Laboratoire Leprince-Ringuet
155 shared publications - Alberto Belloni
University of Maryland, College Park, Maryland
155 shared publications
Latest Publications
- Open Access
- 15 October 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (10)
Erratum: Measurement of the Zγ production cross section and search for anomalous neutral triple gauge couplings in pp collisions at $ \sqrt{s}=13 $ TeV- 15 October 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (10)
Open AccessErratum: Measurement of the Zγ production cross section and search for anomalous neutral triple gauge couplings in pp collisions at $ \sqrt{s}=13 $ TeV - Open Access
- 22 September 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 137 (13) , 131801
Search for the Nonresonant Production of a Pair of Additional Higgs Bosons in the Type-X Two-Higgs-Doublet Model in Proton-Proton Collisions at s = 13 TeV
A search is presented for the production of two additional Higgs bosons from an off-shell boson, where both additional particles decay to τ lepton pairs. The search is performed with a data sample collected with the CMS detector from proton-proton collisions at the LHC at s = 13 TeV , corresponding to an integrated luminosity of 138 fb − 1 . No deviation from the standard model background is observed. Exclusion limits are set on the type-X two-Higgs-doublet model alignment scenario. These results exclude previously unexplored regions of parameter space and provide constraints complementary to those from earlier searches.
- 22 September 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 137 (13) , 131801
Open AccessSearch for the Nonresonant Production of a Pair of Additional Higgs Bosons in the Type-X Two-Higgs-Doublet Model in Proton-Proton Collisions at s = 13 TeV
A search is presented for the production of two additional Higgs bosons from an off-shell boson, where both additional particles decay to τ lepton pairs. The search is performed with a data sample collected with the CMS detector from proton-proton collisions at the LHC at s = 13 TeV , corresponding to an integrated luminosity of 138 fb − 1 . No deviation from the standard model background is observed. Exclusion limits are set on the type-X two-Higgs-doublet model alignment scenario. These results exclude previously unexplored regions of parameter space and provide constraints complementary to those from earlier searches.
- Open Access
- 16 September 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (9)
Erratum: Measurements of inclusive and differential cross sections for the Higgs boson production and decay to four-leptons in proton-proton collisions at $ \sqrt{s}=13 $ TeV- 16 September 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (9)
Open AccessErratum: Measurements of inclusive and differential cross sections for the Higgs boson production and decay to four-leptons in proton-proton collisions at $ \sqrt{s}=13 $ TeV - Open Access
- 14 September 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (9)
Erratum: Measurements of the Higgs boson production cross section in the four-lepton final state in proton-proton collisions at $ \sqrt{s}=13.6 $ TeV- 14 September 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (9)
Open AccessErratum: Measurements of the Higgs boson production cross section in the four-lepton final state in proton-proton collisions at $ \sqrt{s}=13.6 $ TeV - Open Access
- 6 August 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (8)
Measurement of the Zγ production cross section and search for anomalous neutral triple gauge couplings in pp collisions at $ \sqrt{s}=13 $ TeVA bstract: A measurement of the fiducial cross section of the associated production of a Z boson and a high- p T photon, where the Z decays to two neutrinos, and a search for anomalous triple gauge couplings are reported. The results are based on data collected by the CMS experiment at the LHC in proton-proton collisions at $$ \sqrt{s}=13 $$ TeV during 2016–2018, corresponding to an integrated luminosity of 138 fb − 1 . The fiducial Zγ cross section, where a photon with a p T greater than 225 GeV is produced in association with a Z, and the Z decays to a $$ \upnu \overline{\upnu} $$ pair $$ \left(\mathrm{Z}\left(\upnu \overline{\upnu}\right)\upgamma \right) $$ , is measured to be $$ {23.3}_{-1.3}^{+1.4} $$ fb, in agreement, within uncertainties, with the standard model prediction. The differential cross section as a function of the photon p T has been measured and compared with standard model predictions computed at next-to-leading and at next-to-next-to-leading order in perturbative quantum chromodynamics. Constraints have been placed on the presence of anomalous couplings that affect the ZZγ and Zγγ vertex using the p T spectrum of the photons. The observed 95% confidence level intervals for CP -conserving $$ {h}_3^{\upgamma} $$ and $$ {h}_4^{\upgamma} $$ are determined to be ( − 3.4, 3.5) × 10 − 4 and ( − 6.8, 6.8) × 10 − 7 , and for $$ {h}_3^{\mathrm{Z}} $$ and $$ {h}_4^{\mathrm{Z}} $$ they are ( − 2.2, 2.2) × 10 − 4 and ( − 4.1, 4.2) × 10 − 7 , respectively. These are the strictest limits to date on $$ {h}_3^{\upgamma} $$ , $$ {h}_3^{\mathrm{Z}} $$ and $$ {h}_4^{\mathrm{Z}} $$ .- 6 August 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (8)
Open AccessMeasurement of the Zγ production cross section and search for anomalous neutral triple gauge couplings in pp collisions at $ \sqrt{s}=13 $ TeVA bstract: A measurement of the fiducial cross section of the associated production of a Z boson and a high- p T photon, where the Z decays to two neutrinos, and a search for anomalous triple gauge couplings are reported. The results are based on data collected by the CMS experiment at the LHC in proton-proton collisions at $$ \sqrt{s}=13 $$ TeV during 2016–2018, corresponding to an integrated luminosity of 138 fb − 1 . The fiducial Zγ cross section, where a photon with a p T greater than 225 GeV is produced in association with a Z, and the Z decays to a $$ \upnu \overline{\upnu} $$ pair $$ \left(\mathrm{Z}\left(\upnu \overline{\upnu}\right)\upgamma \right) $$ , is measured to be $$ {23.3}_{-1.3}^{+1.4} $$ fb, in agreement, within uncertainties, with the standard model prediction. The differential cross section as a function of the photon p T has been measured and compared with standard model predictions computed at next-to-leading and at next-to-next-to-leading order in perturbative quantum chromodynamics. Constraints have been placed on the presence of anomalous couplings that affect the ZZγ and Zγγ vertex using the p T spectrum of the photons. The observed 95% confidence level intervals for CP -conserving $$ {h}_3^{\upgamma} $$ and $$ {h}_4^{\upgamma} $$ are determined to be ( − 3.4, 3.5) × 10 − 4 and ( − 6.8, 6.8) × 10 − 7 , and for $$ {h}_3^{\mathrm{Z}} $$ and $$ {h}_4^{\mathrm{Z}} $$ they are ( − 2.2, 2.2) × 10 − 4 and ( − 4.1, 4.2) × 10 − 7 , respectively. These are the strictest limits to date on $$ {h}_3^{\upgamma} $$ , $$ {h}_3^{\mathrm{Z}} $$ and $$ {h}_4^{\mathrm{Z}} $$ . - Open Access
- 1 July 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (7)
Search for a new neutral gauge boson produced in association with one or two b jets and decaying into a pair of muons in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: A search for a new neutral gauge boson, Z ′ , produced in association with one or two jets, including at least one b jet, and decaying into a pair of muons is presented. The analysis uses proton-proton collision data collected with the CMS detector at $$ \sqrt{s}=13 $$ TeV, corresponding to an integrated luminosity of 138 fb − 1 . No significant deviation from background expectations is observed. Upper limits at 95% confidence level on the product of cross section, branching fraction to dimuons, acceptance, and efficiency, from 0.2 to 2 fb, are set for Z ′ boson masses between 125 and 350 GeV. Process-dependent products of acceptance and efficiency, and model-independent limits on the signal yield are provided. These are the only results to date in the 125–200 GeV mass range and the most stringent for b quark fusion production modes in the 200–350 GeV range, complementing inclusive Z ′ boson searches.- 1 July 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (7)
Open AccessSearch for a new neutral gauge boson produced in association with one or two b jets and decaying into a pair of muons in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: A search for a new neutral gauge boson, Z ′ , produced in association with one or two jets, including at least one b jet, and decaying into a pair of muons is presented. The analysis uses proton-proton collision data collected with the CMS detector at $$ \sqrt{s}=13 $$ TeV, corresponding to an integrated luminosity of 138 fb − 1 . No significant deviation from background expectations is observed. Upper limits at 95% confidence level on the product of cross section, branching fraction to dimuons, acceptance, and efficiency, from 0.2 to 2 fb, are set for Z ′ boson masses between 125 and 350 GeV. Process-dependent products of acceptance and efficiency, and model-independent limits on the signal yield are provided. These are the only results to date in the 125–200 GeV mass range and the most stringent for b quark fusion production modes in the 200–350 GeV range, complementing inclusive Z ′ boson searches. - Open Access
- 15 May 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (5)
Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the γγττ final state in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: The results of a search for the production of two scalar bosons in final states with two photons and two tau leptons are presented. The search considers both nonresonant production of a Higgs boson pair, HH, and resonant production via a new boson X which decays either to HH or to H and a new scalar Y. The analysis uses up to 138 fb − 1 of proton-proton collision data, recorded between 2016 and 2018 by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV. No evidence for signal is found in the data. For the nonresonant production, the observed (expected) upper limit at 95% confidence level (CL) on the HH production cross section is set at 930 (740) fb, corresponding to 33 (26) times the standard model prediction. At 95% CL, HH production is observed (expected) to be excluded for values of κ λ outside the range between −12 (−9.4) and 17 (15). Observed (expected) upper limits at 95% CL for the X → HH cross section are found to be within 160 to 2200 (200 to 1800) fb, depending on the mass of X. In the X → Y(ττ)H(γγ) search, the observed (expected) upper limits on the product of the production cross section and decay branching fractions vary between 0.059–1.2 fb (0.087–0.68 fb). For the X → Y(γγ)H(ττ) search the observed (expected) upper limits on the product of the production cross section and Y → γγ branching fraction vary between 0.69–15 fb (0.73–8.3 fb) in the low Y mass search, tightening constraints on the next-to-minimal supersymmetric standard model, and between 0.64–10 fb (0.70–7.6 fb) in the high Y mass search.
- 15 May 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (5)
Open AccessSearch for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the γγττ final state in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: The results of a search for the production of two scalar bosons in final states with two photons and two tau leptons are presented. The search considers both nonresonant production of a Higgs boson pair, HH, and resonant production via a new boson X which decays either to HH or to H and a new scalar Y. The analysis uses up to 138 fb − 1 of proton-proton collision data, recorded between 2016 and 2018 by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV. No evidence for signal is found in the data. For the nonresonant production, the observed (expected) upper limit at 95% confidence level (CL) on the HH production cross section is set at 930 (740) fb, corresponding to 33 (26) times the standard model prediction. At 95% CL, HH production is observed (expected) to be excluded for values of κ λ outside the range between −12 (−9.4) and 17 (15). Observed (expected) upper limits at 95% CL for the X → HH cross section are found to be within 160 to 2200 (200 to 1800) fb, depending on the mass of X. In the X → Y(ττ)H(γγ) search, the observed (expected) upper limits on the product of the production cross section and decay branching fractions vary between 0.059–1.2 fb (0.087–0.68 fb). For the X → Y(γγ)H(ττ) search the observed (expected) upper limits on the product of the production cross section and Y → γγ branching fraction vary between 0.69–15 fb (0.73–8.3 fb) in the low Y mass search, tightening constraints on the next-to-minimal supersymmetric standard model, and between 0.64–10 fb (0.70–7.6 fb) in the high Y mass search.
- Open Access
- 5 May 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 136 (18) , 181801
First Evidence for Mixing-Induced C P Violation in B s 0 → J / ψ ϕ ( 1020 ) Decays in p p Collisions at s = 13 TeV
A novel machine-learning-based flavor-tagging algorithm combining same-side and opposite-side tagging is used to obtain the equivalent of 27 500 tagged B s 0 → J / ψ ϕ ( 1020 ) decays from p p collisions at s = 13 TeV , collected by the CMS experiment and corresponding to an integrated luminosity of 96.5 fb − 1 . A time- and flavor-dependent angular analysis of the μ + μ − K + K − final state, consistent with a ϕ ( 1020 ) → K + K − decay, is used to measure parameters of the B s 0 − B ¯ s 0 system. The weak phase is measured to be ϕ s = − 73 ± 22 ( stat ) ± 10 ( syst ) mrad , which, combined with the s = 8 TeV CMS result, gives ϕ s = − 75 ± 23 mrad . This value differs from zero by 3.2 standard deviations, providing the first evidence for mixing-induced C P violation in B s 0 → J / ψ ϕ ( 1020 ) decays. All measured physics parameters are found to agree with standard model predictions where available.
- 5 May 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 136 (18) , 181801
Open AccessFirst Evidence for Mixing-Induced C P Violation in B s 0 → J / ψ ϕ ( 1020 ) Decays in p p Collisions at s = 13 TeV
A novel machine-learning-based flavor-tagging algorithm combining same-side and opposite-side tagging is used to obtain the equivalent of 27 500 tagged B s 0 → J / ψ ϕ ( 1020 ) decays from p p collisions at s = 13 TeV , collected by the CMS experiment and corresponding to an integrated luminosity of 96.5 fb − 1 . A time- and flavor-dependent angular analysis of the μ + μ − K + K − final state, consistent with a ϕ ( 1020 ) → K + K − decay, is used to measure parameters of the B s 0 − B ¯ s 0 system. The weak phase is measured to be ϕ s = − 73 ± 22 ( stat ) ± 10 ( syst ) mrad , which, combined with the s = 8 TeV CMS result, gives ϕ s = − 75 ± 23 mrad . This value differs from zero by 3.2 standard deviations, providing the first evidence for mixing-induced C P violation in B s 0 → J / ψ ϕ ( 1020 ) decays. All measured physics parameters are found to agree with standard model predictions where available.
- Open Access
- 17 April 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (4)
Jet fragmentation function and groomed substructure of bottom quark jets in proton-proton collisions at 5.02 TeV
A bstract: A measurement of the substructure of bottom quark jets (b jets) in proton-proton (pp) collisions is presented. The measurement uses data collected in pp collisions at $$ \sqrt{s}=5.02 $$ TeV, with a low number of simultaneous interactions per bunch crossing, recorded by the CMS experiment in 2017, corresponding to an integrated luminosity of 301 pb − 1 . An algorithm to identify and cluster the charged decay daughters of b hadrons is developed for this analysis, which facilitates the exposure of the gluon radiation pattern of b jets using iterative Cambridge-Aachen declustering. The soft-drop-groomed jet radius, R g , and momentum balance, z g , of b quark jets are presented. These observables can be used to test perturbative quantum chromodynamics predictions that account for mass effects. Because the b hadron is partially reconstructed from its charged decay daughters, only charged particles are used for the jet substructure studies. In addition, a jet fragmentation function, z b,ch , is measured, which is defined as the distribution of the ratio of the transverse momentum ( p T ) of the partially reconstructed b hadron with respect to the charged-particle component of the jet p T . The substructure variable distributions are unfolded to the charged-particle level. The b jet substructure is compared to the substructure of jets in an inclusive jet sample that is dominated by light-quark and gluon jets in order to assess the role of the b quark mass. A strong suppression of emissions at small R g values is observed for b jets when compared to inclusive jets, consistent with the dead-cone effect. The measurement is also compared with theoretical predictions from Monte Carlo event generators. This is the first substructure measurement of b jets that clusters together the b hadron decay daughters independent of the b hadron species and decay channel.- 17 April 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (4)
Open AccessJet fragmentation function and groomed substructure of bottom quark jets in proton-proton collisions at 5.02 TeV
A bstract: A measurement of the substructure of bottom quark jets (b jets) in proton-proton (pp) collisions is presented. The measurement uses data collected in pp collisions at $$ \sqrt{s}=5.02 $$ TeV, with a low number of simultaneous interactions per bunch crossing, recorded by the CMS experiment in 2017, corresponding to an integrated luminosity of 301 pb − 1 . An algorithm to identify and cluster the charged decay daughters of b hadrons is developed for this analysis, which facilitates the exposure of the gluon radiation pattern of b jets using iterative Cambridge-Aachen declustering. The soft-drop-groomed jet radius, R g , and momentum balance, z g , of b quark jets are presented. These observables can be used to test perturbative quantum chromodynamics predictions that account for mass effects. Because the b hadron is partially reconstructed from its charged decay daughters, only charged particles are used for the jet substructure studies. In addition, a jet fragmentation function, z b,ch , is measured, which is defined as the distribution of the ratio of the transverse momentum ( p T ) of the partially reconstructed b hadron with respect to the charged-particle component of the jet p T . The substructure variable distributions are unfolded to the charged-particle level. The b jet substructure is compared to the substructure of jets in an inclusive jet sample that is dominated by light-quark and gluon jets in order to assess the role of the b quark mass. A strong suppression of emissions at small R g values is observed for b jets when compared to inclusive jets, consistent with the dead-cone effect. The measurement is also compared with theoretical predictions from Monte Carlo event generators. This is the first substructure measurement of b jets that clusters together the b hadron decay daughters independent of the b hadron species and decay channel. - Open Access
- 16 April 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (4)
Search for light pseudoscalar boson pairs produced from Higgs boson decays using the 4τ and 2μ2τ final states in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: A search for a pair of light pseudoscalar bosons (a 1 ) produced in the decay of the 125 GeV Higgs boson is presented. The analysis examines decay modes where one a 1 decays into a pair of tau leptons and the other decays into either another pair of tau leptons or a pair of muons. The a 1 boson mass probed in this study ranges from 4 to 15 GeV. The data sample was recorded by the CMS experiment in proton-proton collisions at a center-of-mass energy of 13 TeV and corresponds to an integrated luminosity of 138 fb − 1 . No excess above standard model (SM) expectations is observed. The study combines the 4τ and 2μ2τ channels to set upper limits at 95% confidence level (CL) on the product of the Higgs boson production cross section and the branching fraction to the 4τ final state, relative to the Higgs boson production cross section predicted by the SM. In this interpretation, the a 1 boson is assumed to have Yukawa-like couplings to fermions, with coupling strengths proportional to the respective fermion masses. The observed (expected) upper limits range between 0.007 (0.011) and 0.079 (0.066) across the mass range considered. The results are also interpreted in the context of models with two Higgs doublets and an additional complex singlet field (2HD+S). The tightest constraints are obtained for the Type III 2HD+S model. In this case, assuming the Higgs boson production cross section equals the SM prediction, values of the branching ratio for the Higgs boson decay into a pair of a 1 bosons exceeding 16% are excluded at 95% CL for a 1 boson masses between 5 and 15 GeV and tan β > 2, with the exception of scenarios in which the a 1 boson mixes with charm or bottom quark-antiquark bound states.
- 16 April 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (4)
Open AccessSearch for light pseudoscalar boson pairs produced from Higgs boson decays using the 4τ and 2μ2τ final states in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: A search for a pair of light pseudoscalar bosons (a 1 ) produced in the decay of the 125 GeV Higgs boson is presented. The analysis examines decay modes where one a 1 decays into a pair of tau leptons and the other decays into either another pair of tau leptons or a pair of muons. The a 1 boson mass probed in this study ranges from 4 to 15 GeV. The data sample was recorded by the CMS experiment in proton-proton collisions at a center-of-mass energy of 13 TeV and corresponds to an integrated luminosity of 138 fb − 1 . No excess above standard model (SM) expectations is observed. The study combines the 4τ and 2μ2τ channels to set upper limits at 95% confidence level (CL) on the product of the Higgs boson production cross section and the branching fraction to the 4τ final state, relative to the Higgs boson production cross section predicted by the SM. In this interpretation, the a 1 boson is assumed to have Yukawa-like couplings to fermions, with coupling strengths proportional to the respective fermion masses. The observed (expected) upper limits range between 0.007 (0.011) and 0.079 (0.066) across the mass range considered. The results are also interpreted in the context of models with two Higgs doublets and an additional complex singlet field (2HD+S). The tightest constraints are obtained for the Type III 2HD+S model. In this case, assuming the Higgs boson production cross section equals the SM prediction, values of the branching ratio for the Higgs boson decay into a pair of a 1 bosons exceeding 16% are excluded at 95% CL for a 1 boson masses between 5 and 15 GeV and tan β > 2, with the exception of scenarios in which the a 1 boson mixes with charm or bottom quark-antiquark bound states.