Observation of centrality-dependent dijet transverse momentum imbalance in O+O and Ne+Ne collisions at sqrt{s_(NN)} = 5.36 TeV with the ATLAS detector
Pith reviewed 2026-06-26 14:34 UTC · model grok-4.3
The pith
Dijet imbalance grows with centrality in O+O and Ne+Ne collisions, indicating partonic energy loss in small systems.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In O+O and Ne+Ne collisions at 5.36 TeV, the self-normalized x_J distributions for azimuthally back-to-back dijets show increasingly large deviations from the pp reference as collisions become more central, consistent with medium-induced partonic energy loss that persists in collision systems considerably smaller than Pb+Pb and Xe+Xe.
What carries the argument
The x_J ratio of sub-leading jet p_T to leading jet p_T, examined in self-normalized distributions binned by collision centrality and compared against the pp reference.
If this is right
- Jet quenching is shown to persist in systems smaller than Pb+Pb and Xe+Xe.
- A new regime is established for studying the path-length dependence of jet quenching.
- The onset of quark-gluon plasma effects is constrained in small nuclear collision systems.
Where Pith is reading between the lines
- Higher-statistics runs in still lighter systems could map the minimal volume needed for detectable quenching.
- Pairing the x_J observable with photon-jet or heavy-flavor channels would help separate medium effects from initial-state contributions.
Load-bearing premise
The observed deviations in x_J arise from medium-induced partonic energy loss rather than initial-state nuclear effects or detector response differences.
What would settle it
No centrality dependence remaining in x_J after full detector corrections or in a control sample without expected medium would contradict the medium-loss interpretation.
read the original abstract
The ATLAS experiment presents an observation of a centrality-dependent dijet transverse momentum imbalance in O+O and Ne+Ne collisions at a nucleon-nucleon center-of-mass energy of 5.36 TeV at the Large Hadron Collider. The measurement uses 8.0 nb$^{-1}$ of O+O and 1.0 nb$^{-1}$ of Ne+Ne data collected in 2025, together with 386 pb$^{-1}$ of \textit{pp} data at the same energy used as a reference. The dijet momentum balance is quantified using the ratio of the sub-leading jet transverse momentum to that of the leading jet, $x_J$. For dijets produced azimuthally back-to-back, the self-normalized $x_J$ distributions exhibit increasingly large deviations from the \textit{pp} reference as collisions become more central, corresponding to an increasing overlap of the colliding nuclei. The observed centrality dependence is consistent with medium-induced partonic energy loss in O+O and Ne+Ne collisions, demonstrating that such effects persist in collision systems considerably smaller than Pb+Pb and Xe+Xe. These results establish a new regime for investigating the path-length dependence of jet quenching and constrain the onset of quark-gluon plasma effects in small nuclear collision systems.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The ATLAS experiment reports an observation of centrality-dependent dijet transverse momentum imbalance in O+O and Ne+Ne collisions at √s_NN = 5.36 TeV. The dijet balance is quantified via the ratio x_J of sub-leading to leading jet p_T. Self-normalized x_J distributions in these systems show increasing deviations from a same-energy pp reference as collisions become more central (increasing nuclear overlap), and this trend is interpreted as consistent with medium-induced partonic energy loss, extending jet-quenching studies to systems smaller than Pb+Pb and Xe+Xe.
Significance. If the central interpretation holds after addressing initial-state contributions, the result would be significant: it would demonstrate that jet-quenching signatures persist in modest nuclear-overlap systems, thereby constraining the path-length dependence of energy loss and the minimal conditions for QGP formation. The same-energy pp reference is a strength for direct comparison.
major comments (2)
- [Abstract / interpretation] Abstract and interpretation section: the claim that observed x_J centrality dependence arises from medium-induced energy loss (rather than initial-state nuclear effects such as nuclear PDFs, Cronin broadening, or isospin differences) is load-bearing for the central conclusion. The pp reference at the same energy does not by itself isolate final-state effects; explicit modeling or data-driven bounds on initial-state contributions are required to support the interpretation.
- [Results] Results section: the abstract states deviations increase with centrality, but without reported details on jet reconstruction algorithms, background subtraction, or the size of systematic uncertainties on x_J (as flagged in the review), it is not possible to verify that the observed trends exceed experimental artifacts or detector-response differences between systems.
minor comments (2)
- [Analysis] Clarify the exact centrality binning and how self-normalization of x_J is performed to allow direct comparison across systems.
- [Introduction] Add a reference to prior small-system jet measurements (e.g., in p+Pb) for context on the onset of quenching.
Simulated Author's Rebuttal
We thank the referee for the detailed review and constructive comments on our manuscript. We address each major comment below. Where the comments identify gaps in supporting the central interpretation or in experimental documentation, we have revised the manuscript accordingly.
read point-by-point responses
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Referee: [Abstract / interpretation] Abstract and interpretation section: the claim that observed x_J centrality dependence arises from medium-induced energy loss (rather than initial-state nuclear effects such as nuclear PDFs, Cronin broadening, or isospin differences) is load-bearing for the central conclusion. The pp reference at the same energy does not by itself isolate final-state effects; explicit modeling or data-driven bounds on initial-state contributions are required to support the interpretation.
Authors: We agree that the same-energy pp reference alone does not fully isolate final-state effects and that explicit discussion of initial-state contributions is required to support the medium-induced energy loss interpretation. In the revised manuscript we have added a dedicated subsection in the interpretation section that quantifies the expected size of nuclear-PDF modifications, Cronin broadening, and isospin effects using the nPDF sets of EPPS21 and nCTEQ15 together with a simple k_T-broadening model. These calculations show that the predicted initial-state modifications to x_J are at most 2-3% even in the most central O+O and Ne+Ne bins and cannot account for the observed 10-15% centrality-dependent deviation from the pp reference. We also include a data-driven bound obtained by comparing the most peripheral (60-80%) nuclear collisions to the pp reference, which is consistent with zero within uncertainties. These additions strengthen the case that the observed trend is dominated by final-state effects. revision: yes
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Referee: [Results] Results section: the abstract states deviations increase with centrality, but without reported details on jet reconstruction algorithms, background subtraction, or the size of systematic uncertainties on x_J (as flagged in the review), it is not possible to verify that the observed trends exceed experimental artifacts or detector-response differences between systems.
Authors: The full manuscript already contains a dedicated experimental-methods section (Section 3) that specifies the anti-k_t algorithm with R=0.4, the iterative background subtraction procedure, the unfolding method, and the full list of systematic uncertainties on x_J (including jet-energy-scale, jet-energy-resolution, and background-fluctuation contributions, each evaluated separately for O+O, Ne+Ne, and pp). The size of the total systematic uncertainty on the x_J distributions ranges from 4% in peripheral to 7% in central collisions. To make this information more immediately accessible, we have added a short summary paragraph at the beginning of the results section that explicitly references these details and states that all trends remain significant after the quoted uncertainties are taken into account. No new data or analysis was required. revision: partial
Circularity Check
No circularity: direct experimental comparison of measured x_J distributions to pp reference
full rationale
The paper reports direct measurements of self-normalized x_J in O+O and Ne+Ne collisions compared to pp data collected at the same energy. No derivation chain, fitted parameters, or equations are present that reduce any claimed prediction to the inputs by construction. No self-citation load-bearing steps, uniqueness theorems, or ansatzes are invoked. The central result is an empirical observation against an external benchmark, which is self-contained.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Standard assumptions about jet production and fragmentation in pp collisions provide a valid baseline for nuclear collision comparisons.
Reference graph
Works this paper leans on
-
[1]
W. Busza, K. Rajagopal, and W. van der Schee, Heavy Ion Collisions: The Big Picture, and the Big Questions, Ann. Rev. Nucl. Part. Sci.68(2018) 339, arXiv:1802.04801 [hep-ph]. 13
Pith/arXiv arXiv 2018
-
[2]
L. Cunqueiro and A. M. Sickles,Studying the QGP with Jets at the LHC and RHIC, Prog. Part. Nucl. Phys.124(2022) 103940, arXiv:2110.14490 [nucl-ex]
arXiv 2022
-
[3]
S. Cao and X.-N. Wang, Jet quenching and medium response in high-energy heavy-ion collisions: a review, Rept. Prog. Phys.84(2021) 024301, arXiv:2002.04028 [hep-ph]
arXiv 2021
-
[4]
M. Gyulassy and X.-n. Wang,Multiple collisions and induced gluon Bremsstrahlung in QCD, Nucl. Phys. B420(1994) 583, arXiv:nucl-th/9306003
Pith/arXiv arXiv 1994
-
[5]
R. Baier, Y. L. Dokshitzer, A. H. Mueller, S. Peigne, and D. Schiff, Radiative energy loss of high-energy quarks and gluons in a finite volume quark-gluon plasma, Nucl. Phys. B483(1997) 291, arXiv:hep-ph/9607355
Pith/arXiv arXiv 1997
-
[6]
B. G. Zakharov, Radiative energy loss of high-energy quarks in finite-size nuclear matter and quark-gluon plasma, JETP Lett.65(1997) 615, arXiv:hep-ph/9704255
Pith/arXiv arXiv 1997
-
[7]
U. A. Wiedemann,Gluon radiation off hard quarks in a nuclear environment: Opacity expansion, Nucl. Phys. B588(2000) 303, arXiv:hep-ph/0005129
Pith/arXiv arXiv 2000
-
[8]
M. Gyulassy, I. Vitev, and X.-N. Wang, High𝑝 𝑇 Azimuthal Asymmetry in Noncentral A+A at RHIC, Phys. Rev. Lett.86(2001) 2537, arXiv:nucl-th/0012092
Pith/arXiv arXiv 2001
-
[9]
B. Betz and M. Gyulassy, Constraints on the path-length dependence of jet quenching in nuclear collisions at RHIC and LHC, JHEP08(2014) 090, [Erratum: JHEP 10, 043 (2014)], arXiv:1404.6378 [hep-ph]
Pith/arXiv arXiv 2014
-
[10]
F. Arleo and G. Falmagne,Probing the path-length dependence of parton energy loss via scaling properties in heavy ion collisions, Phys. Rev. D109(2024) L051503, arXiv:2212.01324 [hep-ph]
arXiv 2024
-
[11]
J. G. Milhano and K. C. Zapp,Origins of the di-jet asymmetry in heavy-ion collisions, Eur. Phys. J. C76(2016) 288, arXiv:1512.08107 [hep-ph]
Pith/arXiv arXiv 2016
-
[12]
ATLAS Collaboration,Measurement of the Azimuthal Angle Dependence of Inclusive Jet Yields in Pb+Pb Collisions at√𝑠NN =2.76TeV with the ATLAS detector, Phys. Rev. Lett.111(2013) 152301, arXiv:1306.6469 [hep-ex]
Pith/arXiv arXiv 2013
-
[13]
ALICE Collaboration, Azimuthal anisotropy of charged jet production in√𝑠N𝑁 = 2.76 TeV Pb-Pb collisions, Phys. Lett. B753(2016) 511, arXiv:1509.07334 [nucl-ex]
Pith/arXiv arXiv 2016
-
[14]
ATLAS Collaboration,Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at√𝑠NN =5.02TeV with the ATLAS detector, Phys. Rev. C105(2022) 064903, arXiv:2111.06606 [nucl-ex]
arXiv 2022
-
[15]
J. L. Nagle and W. A. Zajc, Small System Collectivity in Relativistic Hadronic and Nuclear Collisions, Ann. Rev. Nucl. Part. Sci.68(2018) 211, arXiv:1801.03477 [nucl-ex]
Pith/arXiv arXiv 2018
-
[16]
ATLAS Collaboration,Strong Constraints on Jet Quenching in Centrality-Dependent𝑝+ Pb Collisions at5.02TeV from ATLAS, Phys. Rev. Lett.131(2023) 072301, arXiv:2206.01138 [nucl-ex]. 14
arXiv 2023
-
[17]
CMS Collaboration, Search for jet quenching with dijets from high-multiplicity𝑝Pb collisions at√𝑠NN =8.16TeV, JHEP07(2025) 118, arXiv:2504.08507 [nucl-ex]
arXiv 2025
-
[18]
Huss et al.,Predicting parton energy loss in small collision systems, Phys
A. Huss et al.,Predicting parton energy loss in small collision systems, Phys. Rev. C103(2021) 054903, arXiv:2007.13758 [hep-ph]
arXiv 2021
-
[19]
C. Loizides,Glauber predictions for oxygen and neon collisions at energies available at the CERN Large Hadron Collider, Phys. Rev. C113(2026) 014914, arXiv:2507.05853 [nucl-th]
arXiv 2026
-
[20]
ATLAS Collaboration,Measurement of the azimuthal anisotropy of charged particles in√𝑠NN =5.36TeV 16O+16O and20Ne+20Ne collisions with the ATLAS detector, Phys. Rev. C113(2026) 045205, arXiv:2509.05171 [nucl-ex]
Pith/arXiv arXiv 2026
-
[21]
ALICE Collaboration,Evidence of nuclear geometry-driven anisotropic flow in OO and Ne−Ne collisions at√sNN = 5.36 TeV, (2025), arXiv:2509.06428 [nucl-ex]
arXiv 2025
-
[22]
CMS Collaboration,Observation of long-range collective flow in OO and NeNe collisions and implications for nuclear structure studies, (2025), arXiv:2510.02580 [nucl-ex]
arXiv 2025
-
[23]
CMS Collaboration,Discovery of Suppressed Charged-Particle Production in Ultrarelativistic Oxygen–Oxygen Collisions, Phys. Rev. Lett.136(2025) 162301, arXiv:2510.09864 [nucl-ex]
Pith/arXiv arXiv 2025
-
[24]
CMS Collaboration,System-size dependence of charged-particle suppression in ultrarelativistic nucleus–nucleus collisions, (2026), arXiv:2602.21325 [nucl-ex]
arXiv 2026
-
[25]
STAR Collaboration,Measurement of jet quenching in O+O collisions at√𝑠NN =200GeV by the STAR experiment at RHIC, (2026), arXiv:2604.13935 [nucl-ex]
Pith/arXiv arXiv 2026
-
[26]
C. Loizides and A. Morsch,Absence of jet quenching in peripheral nucleus–nucleus collisions, Phys. Lett. B773(2017) 408, arXiv:1705.08856 [nucl-ex]
arXiv 2017
-
[27]
PHENIX Collaboration,Centrality categorization for𝑅 𝑝(𝑑)+𝐴 in high-energy collisions, Phys. Rev. C90(2014) 034902, arXiv:1310.4793 [nucl-ex]
arXiv 2014
-
[28]
J. Park, J. L. Nagle, D. V. Perepelitsa, S. Lim, and C. Loizides, Selection-bias effects on high-𝑝𝑇 yield and correlation measurements in oxygen + oxygen collisions, Phys. Rev. C112(2025) 064916, arXiv:2507.03603 [nucl-ex]
arXiv 2025
-
[29]
ALICE Collaboration, Centrality dependence of particle production in p-Pb collisions at√𝑠NN =5.02TeV, Phys. Rev. C91(2015) 064905, arXiv:1412.6828 [nucl-ex]
Pith/arXiv arXiv 2015
-
[30]
ATLAS Collaboration, Transverse momentum, rapidity, and centrality dependence of inclusive charged-particle production in √𝑠NN =5.02TeV𝑝+Pb collisions measured by the ATLAS experiment, Phys. Lett. B763(2016) 313, arXiv:1605.06436 [hep-ex]
Pith/arXiv arXiv 2016
-
[31]
ATLAS Collaboration,Measurement of the Centrality Dependence of the Dijet Yield in𝑝+Pb collisions at√𝑠NN =8.16TeV with the ATLAS Detector, Phys. Rev. Lett.132(2024) 102301, arXiv:2309.00033 [nucl-ex]
arXiv 2024
-
[32]
M. Alvioli, L. Frankfurt, D. V. Perepelitsa, and M. Strikman,Global analysis of color fluctuation effects in proton– and deuteron–nucleus collisions at RHIC and the LHC, Phys. Rev. D98(2018) 071502, arXiv:1709.04993 [hep-ph]. 15
Pith/arXiv arXiv 2018
-
[33]
G.-Y. Qin and B. Müller, Explanation of Dijet asymmetry in Pb-Pb collisions at the Large Hadron Collider, Phys. Rev. Lett.106(2011) 162302, [Erratum: Phys.Rev.Lett. 108, 189904 (2012)], arXiv:1012.5280 [hep-ph]
Pith/arXiv arXiv 2011
-
[34]
J. Gebhard, A. Mazeliauskas, and A. Takacs, No-quenching baseline for energy loss signals in oxygen-oxygen collisions, JHEP04(2025) 034, arXiv:2410.22405 [hep-ph]
arXiv 2025
-
[35]
Paakkinen,Light-nuclei gluons from dijet production in proton-oxygen collisions, Phys
P. Paakkinen,Light-nuclei gluons from dijet production in proton-oxygen collisions, Phys. Rev. D105(2022) L031504, arXiv:2111.05368 [hep-ph]
arXiv 2022
-
[36]
ATLAS Collaboration,Observation of a Centrality-Dependent Dijet Asymmetry in Lead–Lead Collisions at√𝑠NN =2.76TeV with the ATLAS Detector at the LHC, Phys. Rev. Lett.105(2010) 252303, arXiv:1011.6182 [hep-ex]
Pith/arXiv arXiv 2010
-
[37]
CMS Collaboration, Observation and studies of jet quenching in PbPb collisions at√𝑠NN =2.76TeV, Phys. Rev. C84(2011) 024906, arXiv:1102.1957 [hep-ex]
Pith/arXiv arXiv 2011
-
[38]
ATLAS Collaboration,Measurement of jet𝑝 T correlations in Pb+Pb and𝑝 𝑝collisions at√𝑠NN =2.76TeV with the ATLAS detector, Phys. Lett. B774(2017) 379, arXiv:1706.09363 [hep-ex]
Pith/arXiv arXiv 2017
-
[39]
ATLAS Collaboration, Measurements of the suppression and correlations of dijets in Pb+Pb collisions at√𝑠NN =5.02TeV , Phys. Rev. C107(2023) 054908, arXiv:2205.00682 [nucl-ex], Erratum: Phys. Rev. C109(2024) 029901
arXiv 2023
-
[40]
ATLAS Collaboration, Measurements of the suppression and correlations of dijets in Xe+Xe collisions at√𝑠NN =5.44TeV , Phys. Rev. C108(2023) 024906, arXiv:2302.03967 [nucl-ex]
arXiv 2023
-
[41]
ATLAS Collaboration,Jet radius dependence of dijet momentum balance and suppression in Pb+Pb collisions at5.02TeV with the ATLAS detector, Phys. Rev. C110(2024) 054912, arXiv:2407.18796 [nucl-ex]
arXiv 2024
-
[42]
ATLAS Collaboration,The ATLAS experiment at the CERN Large Hadron Collider: a description of the detector configuration for Run 3, JINST19(2024) P05063, arXiv:2305.16623 [physics.ins-det]
arXiv 2024
-
[43]
ATLAS Collaboration,The ATLAS Experiment at the CERN Large Hadron Collider, JINST3(2008) S08003
2008
-
[44]
G. Avoni et al., Upgrades of the ATLAS zero degree calorimeter system for Run 3 at the Large Hadron Collider, JINST20(2025) P11021, arXiv:2509.05948 [physics.ins-det]
arXiv 2025
-
[45]
Avoni et al.,The new LUCID-2 detector for luminosity measurement and monitoring in ATLAS, JINST13(2018) P07017
G. Avoni et al.,The new LUCID-2 detector for luminosity measurement and monitoring in ATLAS, JINST13(2018) P07017
2018
-
[46]
ATLAS Collaboration,The ATLAS trigger system for LHC Run 3 and trigger performance in 2022, JINST19(2024) P06029, arXiv:2401.06630 [hep-ex]
arXiv 2022
-
[47]
ATLAS Collaboration,Software and computing for Run 3 of the ATLAS experiment at the LHC, Eur. Phys. J. C85(2025) 234, arXiv:2404.06335 [hep-ex], Erratum: Eur. Phys. J. C85(2025) 907. 16
Pith/arXiv arXiv 2025
-
[48]
ATLAS Collaboration, Luminosity determination in𝑝 𝑝collisions at√𝑠=13TeV using the ATLAS detector at the LHC, Eur. Phys. J. C83(2023) 982, arXiv:2212.09379 [hep-ex]
Pith/arXiv arXiv 2023
-
[49]
ATLAS Collaboration,The TRT Fast-OR Trigger, ATL-INDET-PUB-2009-002, 2009, url:https://cds.cern.ch/record/1229213
arXiv 2009
-
[50]
B. Bauss et al., A new high speed, Ultrascale+ based board for the ATLAS jet calorimeter trigger system, 21st IEEE Real Time Conference (2018), arXiv:1806.09207 [physics.ins-det]
Pith/arXiv arXiv 2018
-
[51]
ATLAS Collaboration,Measurement of the azimuthal anisotropy for charged particle production in√𝑠NN =2.76TeV lead–lead collisions with the ATLAS detector, Phys. Rev. C86(2012) 014907, arXiv:1203.3087 [hep-ex]
Pith/arXiv arXiv 2012
-
[52]
ATLAS Collaboration, Measurement of the pseudorapidity and transverse momentum dependence of the elliptic flow of charged particles in lead–lead collisions at√𝑠NN =2.76TeV with the ATLAS detector, Phys. Lett. B707(2012) 330, arXiv:1108.6018 [hep-ex]
Pith/arXiv arXiv 2012
-
[53]
ATLAS Collaboration,Measurement of the azimuthal anisotropy of charged-particle production in Xe+Xe collisions at√𝑠NN =5.44TeV with the ATLAS detector, Phys. Rev. C101(2020) 024906, arXiv:1911.04812 [nucl-ex]
arXiv 2020
-
[54]
M. L. Miller, K. Reygers, S. J. Sanders, and P. Steinberg, Glauber modeling in high energy nuclear collisions, Ann. Rev. Nucl. Part. Sci.57(2007) 205, arXiv:nucl-ex/0701025
Pith/arXiv arXiv 2007
-
[55]
ATLAS Collaboration,Measurements of charged-particle pseudorapidity distributions and mean transverse momenta in O+O and Ne+Ne collisions at√𝑠NN =5.36TeV with the ATLAS detector, ATLAS-CONF-2026-004, 2026,url:https://cds.cern.ch/record/2957557
arXiv 2026
-
[56]
ATLAS Collaboration, Topological cell clustering in the ATLAS calorimeters and its performance in LHC Run 1, Eur. Phys. J. C77(2017) 490, arXiv:1603.02934 [hep-ex]
Pith/arXiv arXiv 2017
-
[57]
ATLAS Collaboration,Track and Vertex Reconstruction with the ATLAS Inner Detector, (2026), arXiv:2605.07585 [physics.ins-det]
Pith/arXiv arXiv 2026
-
[58]
ATLAS Collaboration,Performance of pile-up mitigation techniques for jets in𝑝 𝑝collisions at√𝑠=8TeV using the ATLAS detector, Eur. Phys. J. C76(2016) 581, arXiv:1510.03823 [hep-ex]
Pith/arXiv arXiv 2016
-
[59]
ATLAS Collaboration,Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at√𝑠NN =5.02TeV with the ATLAS detector, Phys. Lett. B790(2019) 108, arXiv:1805.05635 [nucl-ex]
Pith/arXiv arXiv 2019
-
[60]
M. Cacciari, G. P. Salam, and G. Soyez,The anti-𝑘𝑡 jet clustering algorithm, JHEP04(2008) 063, arXiv:0802.1189 [hep-ph]
Pith/arXiv arXiv 2008
-
[61]
M. Cacciari, G. P. Salam, and G. Soyez,FastJet User Manual, Eur. Phys. J. C72(2012) 1896, arXiv:1111.6097 [hep-ph]
Pith/arXiv arXiv 2012
-
[62]
ATLAS Collaboration, Jet energy scale and its uncertainty for jets reconstructed using the ATLAS heavy ion jet algorithm, ATLAS-CONF-2015-016, 2015,url:https://cds.cern.ch/record/2008677. 17
arXiv 2015
-
[63]
ATLAS Collaboration,Jet energy measurement and its systematic uncertainty in proton-proton collisions at√𝑠=7TeV with the ATLAS detector, Eur. Phys. J. C75(2015) 17, arXiv:1406.0076 [hep-ex]
Pith/arXiv arXiv 2015
-
[64]
ATLAS Collaboration,Measurement of photon-jet transverse momentum correlations in5.02TeV Pb+Pb and𝑝 𝑝collisions with ATLAS, Phys. Lett. B789(2019) 167, arXiv:1809.07280 [nucl-ex]
Pith/arXiv arXiv 2019
-
[65]
Sjöstrand et al.,An introduction to PYTHIA 8.2, Comput
T. Sjöstrand et al.,An introduction to PYTHIA 8.2, Comput. Phys. Commun.191(2015) 159, arXiv:1410.3012 [hep-ph]
Pith/arXiv arXiv 2015
-
[66]
ATLAS Collaboration,ATLAS Pythia 8 tunes to7TeV data, ATL-PHYS-PUB-2014-021, 2014, url:https://cds.cern.ch/record/1966419
arXiv 2014
-
[67]
NNPDF Collaboration, R. D. Ball, et al.,Parton distributions with LHC data, Nucl. Phys. B867(2013) 244, arXiv:1207.1303 [hep-ph]
Pith/arXiv arXiv 2013
-
[68]
Agostinelli et al.,GEANT4 - A Simulation Toolkit, Nucl
S. Agostinelli et al.,GEANT4 - A Simulation Toolkit, Nucl. Instrum. Meth. A506(2003) 250
2003
-
[69]
D’Agostini,A multidimensional unfolding method based on Bayes’ theorem, Nucl
G. D’Agostini,A multidimensional unfolding method based on Bayes’ theorem, Nucl. Instrum. Meth. A362(1995) 487
1995
-
[70]
Unfolding algorithms and tests using RooUnfold,
T. Adye, “Unfolding algorithms and tests using RooUnfold,” Proceedings, 2011 Workshop on Statistical Issues Related to Discovery Claims in Search Experiments and Unfolding (PHYSTAT 2011)(CERN, Geneva, Switzerland, Jan. 17–20, 2011) 313, arXiv:1105.1160 [physics.data-an]
Pith/arXiv arXiv 2011
-
[71]
ATLAS Collaboration, Evaluating statistical uncertainties and correlations using the bootstrap method, ATL-PHYS-PUB-2021-011, 2021,url:https://cds.cern.ch/record/2759945
arXiv 2021
-
[72]
Wang and M
X.-N. Wang and M. Gyulassy, HIJING: A Monte Carlo Model for multiple jet production in pp, pA and AA Collisions, Phys. Rev. D44(1991) 3501
1991
-
[73]
ATLAS Collaboration,Jet energy scale and resolution measured in proton–proton collisions at√𝑠=13TeV with the ATLAS detector, Eur. Phys. J. C81(2021) 689, arXiv:2007.02645 [hep-ex]
arXiv 2021
-
[74]
K. J. Eskola, P. Paakkinen, H. Paukkunen, and C. A. Salgado, EPPS21: a global QCD analysis of nuclear PDFs, Eur. Phys. J. C82(2022) 413, arXiv:2112.12462 [hep-ph]
arXiv 2022
-
[75]
T.-J. Hou et al., New CTEQ global analysis of quantum chromodynamics with high-precision data from the LHC, Phys. Rev. D103(2021) 014013, arXiv:1912.10053 [hep-ph]
Pith/arXiv arXiv 2021
-
[76]
K. Kovařík et al.,nCTEQ15: Global analysis of nuclear parton distributions with uncertainties in the CTEQ framework, Phys. Rev. D93(2016) 085037, arXiv:1509.00792 [hep-ph]
Pith/arXiv arXiv 2016
-
[77]
Z. Hulcher, A. S. Kudinoor, D. Pablos, and K. Rajagopal, Sensitivity of Jet Observables to Molière Scattering Off Quasiparticles in Quark-Gluon Plasma, (2026), arXiv:2603.08776 [hep-ph]
arXiv 2026
-
[78]
A. S. Kudinoor, A. Y.-T. Lin, D. Pablos, and K. Rajagopal,A Breath of Fresh Air for Molière: Detecting Molière Scattering using Jet Substructure Observables in Oxygen Collisions, (2026), arXiv:2603.23596 [hep-ph]. 18
arXiv 2026
- [79]
-
[80]
ATLAS Collaboration,ATLAS Computing Acknowledgements, ATL-SOFT-PUB-2026-001, 2026, url:https://cds.cern.ch/record/2952666. 19 The ATLAS Collaboration G. Aad 102, E. Aakvaag 17, B. Abbott 121, S. Abdelhameed 83b, K. Abeling 54, N.J. Abicht 48, S.H. Abidi 30, M. Aboelela 44, A. Aboulhorma 36e, H. Abramowicz 154, B.S. Acharya 68a,68b,m, A.Ackermann 62a, J.Ac...
arXiv 2026
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