{"work":{"id":"bf7f3f64-80c5-4847-8cb1-3a6dbe2cdf14","openalex_id":null,"doi":"10.1140/epjc/","arxiv_id":null,"raw_key":null,"title":"Scattering of massless scalar field by charged dila- tonic black holes.The European Physical Journal C, 80:654, 2020","authors":null,"authors_text":"Yang Huang and Hongsheng Zhang","year":2020,"venue":null,"abstract":null,"external_url":"https://doi.org/10.1140/epjc/","cited_by_count":null,"metadata_source":"doi_reference","metadata_fetched_at":"2026-06-29T11:13:20.354941+00:00","pith_arxiv_id":null,"created_at":"2026-05-08T22:44:21.612348+00:00","updated_at":"2026-06-29T11:13:20.354941+00:00","title_quality_ok":true,"display_title":"Albouy, et al., Eur","render_title":"Albouy, et al., Eur"},"hub":{"state":{"work_id":"bf7f3f64-80c5-4847-8cb1-3a6dbe2cdf14","tier":"hub","tier_reason":"10+ Pith inbound or 1,000+ external citations","pith_inbound_count":91,"external_cited_by_count":null,"distinct_field_count":14,"first_pith_cited_at":"2019-06-25T05:16:00+00:00","last_pith_cited_at":"2026-06-26T17:13:23+00:00","author_build_status":"not_needed","summary_status":"needed","contexts_status":"needed","graph_status":"needed","ask_index_status":"not_needed","reader_status":"not_needed","recognition_status":"not_needed","updated_at":"2026-06-29T13:38:55.776341+00:00","tier_text":"hub"},"tier":"hub","role_counts":[{"context_role":"background","n":25},{"context_role":"method","n":2},{"context_role":"dataset","n":1}],"polarity_counts":[{"context_polarity":"background","n":24},{"context_polarity":"use_method","n":2},{"context_polarity":"unclear","n":1},{"context_polarity":"use_dataset","n":1}],"runs":{"context_extract":{"job_type":"context_extract","status":"succeeded","result":{"enqueued_papers":25},"error":null,"updated_at":"2026-06-28T00:07:04.363898+00:00"},"graph_features":{"job_type":"graph_features","status":"succeeded","result":{"co_cited":[{"title":"Masset, R","work_id":"238df2e4-a3e5-46f3-860e-3ae2b0094b97","shared_citers":26},{"title":"Feng, F.F","work_id":"aa5a5821-cbcf-44c7-b743-a852432392bd","shared_citers":23},{"title":"Physical Review Letters 85(10), 2200–2203 (2000)","work_id":"4deaf489-c81b-4322-bb0a-41188b0ad4db","shared_citers":13},{"title":"Navas, et al., Review of particle physics, Phys","work_id":"6e4dcae4-4b24-43e5-bee3-2fc9806bc8b5","shared_citers":10},{"title":"Strassler, K.M","work_id":"f5512874-0e46-48e3-86b0-58f135f8e424","shared_citers":8},{"title":"Exploring cosmic origins with CORE: B-mode component separation","work_id":"dacf65ad-e19b-4a01-96f6-621ad3f94b3a","shared_citers":7},{"title":"Pastore, S","work_id":"452a5ae5-edd9-4748-acb9-24dae2cec95e","shared_citers":6},{"title":"Wakamatsu, Is the Aharonov-Bohm phase shift for a non-closed path a measurable quantity?, The European Physical Journal Plus 139 (2) (2024) 1–19","work_id":"d0015eb1-1edd-4748-b41d-ab43566e7d68","shared_citers":6},{"title":"Cacciari, G.P","work_id":"babc8d5a-44b4-4b79-be2c-3c121a5bcd74","shared_citers":5},{"title":"Proceedings of Science 476, 1002 (2025) https://doi.org/10.22323/1","work_id":"6ce1e591-d365-4d46-a217-d28b53379aca","shared_citers":5},{"title":"The Astrophysical Journal879(2), 82 (2019) https://doi.org/10.3847/1538-4357/ ab22b8","work_id":"bc2eecb8-e63a-44fb-bdbc-a4f9fa7e075f","shared_citers":5},{"title":"Aaij, et al., Observation of a J/ψΛResonance Consistent with a Strange Pentaquark Candidate in B-→J/ψΛp¯Decays, Phys","work_id":"e8e48350-e8bc-46dc-b2db-27f689c5d1ae","shared_citers":4},{"title":"Barabash, et al., Phys","work_id":"10db733b-80f5-4873-a6d9-0e6b2043c8a5","shared_citers":4},{"title":"DESI 2024 VI: Cosmological Constraints from the Measurements of Baryon Acoustic Oscillations","work_id":"abaeab8e-c412-45ac-813e-f53689657023","shared_citers":4},{"title":"G., et al., 1998, @doi [AJ] 10.1086/300499 , http://adsabs.harvard.edu/abs/1998AJ....116.1009R 116","work_id":"f4711f38-d7d5-454b-a88b-02642c09bbd4","shared_citers":4},{"title":"K.-W., & Li, T","work_id":"32ff0a4d-a56d-4db2-a8d6-5ad8ca0dcec8","shared_citers":4},{"title":"Navas et al","work_id":"d56cdc88-8206-4cdb-a0f3-8e0c5fa5b969","shared_citers":4},{"title":"2013.11.081","work_id":"0a83db82-fe3b-4808-a34b-5e77806a6080","shared_citers":3},{"title":"Aaij, et al., Evidence of aJ/ψΛstructure and observation of excitedΞ− states in theΞ− b →J/ψΛK− decay, Sci","work_id":"9ef4d84e-12d4-4b90-a919-8dd65b6d5c22","shared_citers":3},{"title":"Aaij, et al., Observation of a narrow pentaquark state, Pc(4312)+, and of two-peak structure of theP c(4450)+, Phys","work_id":"ad98d413-58ae-43ad-80f9-2ad3d318698d","shared_citers":3},{"title":"Aaij, et al., Observation ofJ/ψpResonances Con- sistent with Pentaquark States inΛ 0 b →J/ψK − pDe- cays, Phys","work_id":"4ecbc9ca-2dbb-419b-bee3-e43ffee9048a","shared_citers":3},{"title":"Abbott, R","work_id":"ec2ceb71-84c6-42f9-8595-7d02bd369ca8","shared_citers":3},{"title":"An up- dated review of the new hadron states","work_id":"d36b538d-17d3-4a08-9af2-c7bcfed9ff13","shared_citers":3},{"title":"Beraudo, J.-P","work_id":"726c17f7-492c-49ae-b786-c01bec298700","shared_citers":3}],"time_series":[{"n":1,"year":2019},{"n":1,"year":2022},{"n":17,"year":2025},{"n":59,"year":2026}],"dependency_candidates":[{"n":1,"role":"method","polarity":"use_method","paper_title":"Multiplicative matching of neutral current deep-inelastic scattering processes at next-to-leading order in PYTHIA 8","primary_cat":"hep-ph","context_text":"is to compare the distributions of the DIS quantitiesx,y,Q 2 andW 2. We use a fixed value for the electromagnetic cou- pling with 1/α=137.036. We derive the electroweak pa- rameters from the input ofα(M Z), electroweak mixing an- gle sin2 θW =0.2312, and theZ-boson massM Z =91.1876 GeV . We use the PDF setNNPDF31_nlo_as_0118_luxqed [51] provided by the LHAPDF library [52]. The running of the strong coupling is handled by the PDF set. Setting up the event generation with beam energies cor- responding to the HERA experiments, 27.5 GeV for the elec- tron and 920 GeV for the proton, we generate events with the three generators at process level; without parton show- ers, beam remnants or hadronization. To focus solely on the higher-order effects, all partons","citing_arxiv_id":"2605.00502"},{"n":1,"role":"dataset","polarity":"use_dataset","paper_title":"Mesonic modes in confining model at finite temperature","primary_cat":"hep-ph","context_text":"extreme conditions from chiral quark models with nonlocal separable inter- actions. Symmetry13(1), 121 (2021). https://doi.org/10.3390/sym13010121. arXiv:2101.09574 [hep-ph] [33] C. Chen, F. Gao, S.x. Qin, Screening masses of positive- and negative-parity hadron ground states, including those with strangeness. Phys. Rev. D112(1), 014022 (2025). https://doi.org/10.1103/527r-mtxb. arXiv:2412.15045 [hep-ph] 15 [34] M. Cheng, et al., Meson screening masses from lattice qcd with two light and the strange quark. Eur. Phys. J. C71, 1564 (2011). https://doi.org/10.1140/epjc/ s10052-011-1564-y. arXiv:1010.1216 [hep-lat] [35] A. Bazavov, et al., The chiral transition andu(1) a symmetry restoration from lattice qcd using domain wall fermions. Phys. Rev. D86, 094503 (2012).","citing_arxiv_id":"2604.06275"},{"n":1,"role":"method","polarity":"use_method","paper_title":"Measure charge transport in high-energy nuclear collisions with an energy scan of isobaric collisions","primary_cat":"nucl-ex","context_text":"itively and negatively charged particles, respectively. Sinceπ,K, andpdominate the charged hadron yields, Qmay also be written as Q= (N π+ +N K+ +N p)−(N π− +N K− +N ¯p).(2) arXiv:2604.02825v1 [nucl-ex] 3 Apr 2026 2 Because pions dominate the charged multiplicity and Nπ+ ≈N π− with large absolute values, extractingQ with high precision is challenging. A recent proposal [18] demonstrated that the charge difference (∆Q) between two isobar systems-nuclei with identical mass numberAbut different atomic number Z-can be determined precisely using a double-ratio method. Defining ∆Q=Q Iso1 −Q Iso2,(3) and exploiting the near equality of particle multiplic- ities in the two systems, the charge difference can be approximated as","citing_arxiv_id":"2604.02825"}]},"error":null,"updated_at":"2026-06-28T00:06:44.851296+00:00"},"identity_refresh":{"job_type":"identity_refresh","status":"succeeded","result":{"items":[{"title":"Qwen3 Technical Report","outcome":"unchanged","work_id":"25a4e30c-1232-48e7-9925-02fa12ba7c9e","resolver":"local_arxiv","confidence":0.98,"old_work_id":"25a4e30c-1232-48e7-9925-02fa12ba7c9e"}],"counts":{"fixed":0,"merged":0,"unchanged":1,"quarantined":0,"needs_external_resolution":0},"errors":[],"attempted":1},"error":null,"updated_at":"2026-06-28T00:06:58.722912+00:00"},"summary_claims":{"job_type":"summary_claims","status":"succeeded","result":{"title":"Albouy, et al., Eur","claims":[{"claim_text":"nonsupersymmetric heterotic string models. Phys. Rev. D108(8), 086007 (2023) https://doi.org/10.1103/PhysRevD.108.086007 arXiv:2306.16878 [hep-th] [28] Saxena, V.: A T-duality of non-supersymmetric heterotic strings and an impli- cation for Topological Modular Forms. JHEP 09, 056 (2024) https://doi.org/ 10.1007/JHEP09(2024)056 arXiv:2405.19409 [hep-th] [29] Basaad, E., Detraux, L.A., Avalos, A.R.D., Faraggi, A.E., Percival, B.: Vac- uum energy in non-supersymmetric quasi-realistic heterotic-stri","claim_type":"background","confidence":0.9,"evidence_strength":"citation_context"},{"claim_text":"itively and negatively charged particles, respectively. Sinceπ,K, andpdominate the charged hadron yields, Qmay also be written as Q= (N π+ +N K+ +N p)−(N π− +N K− +N ¯p).(2) arXiv:2604.02825v1 [nucl-ex] 3 Apr 2026 2 Because pions dominate the charged multiplicity and Nπ+ ≈N π− with large absolute values, extractingQ with high precision is challenging. A recent proposal [18] demonstrated that the charge difference (∆Q) between two isobar systems-nuclei with identical mass numberAbut different ato","claim_type":"method","confidence":0.9,"evidence_strength":"citation_context"},{"claim_text":"is to compare the distributions of the DIS quantitiesx,y,Q 2 andW 2. We use a fixed value for the electromagnetic cou- pling with 1/α=137.036. We derive the electroweak pa- rameters from the input ofα(M Z), electroweak mixing an- gle sin2 θW =0.2312, and theZ-boson massM Z =91.1876 GeV . We use the PDF setNNPDF31_nlo_as_0118_luxqed [51] provided by the LHAPDF library [52]. The running of the strong coupling is handled by the PDF set. Setting up the event generation with beam energies cor- respon","claim_type":"method","confidence":0.9,"evidence_strength":"citation_context"},{"claim_text":"\"Toward the classification of the realistic free fermionic models\". In: Int. J. Mod. Phys. A14 (1999), pp. 1663-1702.doi:10.1142/S0217751X99000841. [80] K. Christodoulides, A. E. Faraggi, and J. Rizos. \"Top quark mass in exophobic Pati-Salam heterotic string model\". In:Physics Letters B702.1 (2011), pp. 81-89. issn: 0370-2693.doi:https://doi.org/10.1016/j.physletb.2011.06.051. [81] J. Rizos. \"Top quark mass coupling and classification of weakly-coupled heterotic superstring vacua\". In:Eur. Phys.","claim_type":"background","confidence":0.9,"evidence_strength":"citation_context"},{"claim_text":"Freedman and Antoine Van Proeyen.Supergravity. Cambridge, UK: Cam- bridge Univ. Press, May 2012.doi:10.1017/CBO9781139026833. [7] G. D. Kerlick. \"Cosmology and Particle Pair Production via Gravitational Spin Spin Interaction in the Einstein-Cartan-Sciama-Kibble Theory of Gravity\". In:Phys. Rev. D12 (1975), pp. 3004-3006.doi:10.1103/PhysRevD.12.3004. [8] Amir Hadi Ziaie et al. \"Einstein-Cartan gravitational collapse of a homogeneous Weyssenhoff fluid\". In:Eur. Phys. J. C74.11 (2014), p. 3154.doi:","claim_type":"background","confidence":0.9,"evidence_strength":"citation_context"},{"claim_text":"Observable SM prediction+m ν Experimental limits (g−2) e/2 Cs: 0.00115965218161(23) [146] Rb: 0.001159652180252(95) [147] 0.00115965218062(12) [145] (g−2) µ/2 0.00116592033(62) [148] 0.00116592059(22) [149] BR(µ→eγ) ≲O(10 −55) [150-152] <1.5·10 −13 [153] (<6·10 −14 [153, 154]) BR(µ→3e) ≲O(10 −55) [150, 155] <1.0·10 −12 [156] (Mu3e:<5·10 −16 [157]) BR(µ+N→e+N) ≲O(10 −54) [158] BRAu <7·10 −13 [159] (Mu2e:BR Al <2.87·10 −17 [160]) (COMET:BR Al <2·10 −17 [161]) BR(τ→eγ) ≲O(10 −49) [151] <3.3·10 −8 [","claim_type":"background","confidence":0.9,"evidence_strength":"citation_context"}],"why_cited":"Pith tracks Albouy, et al., Eur because it crossed a citation-hub threshold. Current citing contexts most often use it as background evidence (25 contexts).","role_counts":[{"n":25,"context_role":"background"},{"n":2,"context_role":"method"},{"n":1,"context_role":"dataset"}]},"error":null,"updated_at":"2026-06-28T00:06:44.755244+00:00"}},"summary":{"title":"Albouy, et al., Eur","claims":[{"claim_text":"nonsupersymmetric heterotic string models. Phys. Rev. D108(8), 086007 (2023) https://doi.org/10.1103/PhysRevD.108.086007 arXiv:2306.16878 [hep-th] [28] Saxena, V.: A T-duality of non-supersymmetric heterotic strings and an impli- cation for Topological Modular Forms. JHEP 09, 056 (2024) https://doi.org/ 10.1007/JHEP09(2024)056 arXiv:2405.19409 [hep-th] [29] Basaad, E., Detraux, L.A., Avalos, A.R.D., Faraggi, A.E., Percival, B.: Vac- uum energy in non-supersymmetric quasi-realistic heterotic-stri","claim_type":"background","confidence":0.9,"evidence_strength":"citation_context"},{"claim_text":"itively and negatively charged particles, respectively. Sinceπ,K, andpdominate the charged hadron yields, Qmay also be written as Q= (N π+ +N K+ +N p)−(N π− +N K− +N ¯p).(2) arXiv:2604.02825v1 [nucl-ex] 3 Apr 2026 2 Because pions dominate the charged multiplicity and Nπ+ ≈N π− with large absolute values, extractingQ with high precision is challenging. A recent proposal [18] demonstrated that the charge difference (∆Q) between two isobar systems-nuclei with identical mass numberAbut different ato","claim_type":"method","confidence":0.9,"evidence_strength":"citation_context"},{"claim_text":"is to compare the distributions of the DIS quantitiesx,y,Q 2 andW 2. We use a fixed value for the electromagnetic cou- pling with 1/α=137.036. We derive the electroweak pa- rameters from the input ofα(M Z), electroweak mixing an- gle sin2 θW =0.2312, and theZ-boson massM Z =91.1876 GeV . We use the PDF setNNPDF31_nlo_as_0118_luxqed [51] provided by the LHAPDF library [52]. The running of the strong coupling is handled by the PDF set. Setting up the event generation with beam energies cor- respon","claim_type":"method","confidence":0.9,"evidence_strength":"citation_context"},{"claim_text":"\"Toward the classification of the realistic free fermionic models\". In: Int. J. Mod. Phys. A14 (1999), pp. 1663-1702.doi:10.1142/S0217751X99000841. [80] K. Christodoulides, A. E. Faraggi, and J. Rizos. \"Top quark mass in exophobic Pati-Salam heterotic string model\". In:Physics Letters B702.1 (2011), pp. 81-89. issn: 0370-2693.doi:https://doi.org/10.1016/j.physletb.2011.06.051. [81] J. Rizos. \"Top quark mass coupling and classification of weakly-coupled heterotic superstring vacua\". In:Eur. Phys.","claim_type":"background","confidence":0.9,"evidence_strength":"citation_context"},{"claim_text":"Freedman and Antoine Van Proeyen.Supergravity. Cambridge, UK: Cam- bridge Univ. Press, May 2012.doi:10.1017/CBO9781139026833. [7] G. D. Kerlick. \"Cosmology and Particle Pair Production via Gravitational Spin Spin Interaction in the Einstein-Cartan-Sciama-Kibble Theory of Gravity\". In:Phys. Rev. D12 (1975), pp. 3004-3006.doi:10.1103/PhysRevD.12.3004. [8] Amir Hadi Ziaie et al. \"Einstein-Cartan gravitational collapse of a homogeneous Weyssenhoff fluid\". In:Eur. Phys. J. C74.11 (2014), p. 3154.doi:","claim_type":"background","confidence":0.9,"evidence_strength":"citation_context"},{"claim_text":"Observable SM prediction+m ν Experimental limits (g−2) e/2 Cs: 0.00115965218161(23) [146] Rb: 0.001159652180252(95) [147] 0.00115965218062(12) [145] (g−2) µ/2 0.00116592033(62) [148] 0.00116592059(22) [149] BR(µ→eγ) ≲O(10 −55) [150-152] <1.5·10 −13 [153] (<6·10 −14 [153, 154]) BR(µ→3e) ≲O(10 −55) [150, 155] <1.0·10 −12 [156] (Mu3e:<5·10 −16 [157]) BR(µ+N→e+N) ≲O(10 −54) [158] BRAu <7·10 −13 [159] (Mu2e:BR Al <2.87·10 −17 [160]) (COMET:BR Al <2·10 −17 [161]) BR(τ→eγ) ≲O(10 −49) [151] <3.3·10 −8 [","claim_type":"background","confidence":0.9,"evidence_strength":"citation_context"}],"why_cited":"Pith tracks Albouy, et al., Eur because it crossed a citation-hub threshold. Current citing contexts most often use it as background evidence (25 contexts).","role_counts":[{"n":25,"context_role":"background"},{"n":2,"context_role":"method"},{"n":1,"context_role":"dataset"}]},"graph":{"co_cited":[{"title":"Masset, R","work_id":"238df2e4-a3e5-46f3-860e-3ae2b0094b97","shared_citers":26},{"title":"Feng, F.F","work_id":"aa5a5821-cbcf-44c7-b743-a852432392bd","shared_citers":23},{"title":"Physical Review Letters 85(10), 2200–2203 (2000)","work_id":"4deaf489-c81b-4322-bb0a-41188b0ad4db","shared_citers":13},{"title":"Navas, et al., Review of particle physics, Phys","work_id":"6e4dcae4-4b24-43e5-bee3-2fc9806bc8b5","shared_citers":10},{"title":"Strassler, K.M","work_id":"f5512874-0e46-48e3-86b0-58f135f8e424","shared_citers":8},{"title":"Exploring cosmic origins with CORE: B-mode component separation","work_id":"dacf65ad-e19b-4a01-96f6-621ad3f94b3a","shared_citers":7},{"title":"Pastore, S","work_id":"452a5ae5-edd9-4748-acb9-24dae2cec95e","shared_citers":6},{"title":"Wakamatsu, Is the Aharonov-Bohm phase shift for a non-closed path a measurable quantity?, The European Physical Journal Plus 139 (2) (2024) 1–19","work_id":"d0015eb1-1edd-4748-b41d-ab43566e7d68","shared_citers":6},{"title":"Cacciari, G.P","work_id":"babc8d5a-44b4-4b79-be2c-3c121a5bcd74","shared_citers":5},{"title":"Proceedings of Science 476, 1002 (2025) https://doi.org/10.22323/1","work_id":"6ce1e591-d365-4d46-a217-d28b53379aca","shared_citers":5},{"title":"The Astrophysical Journal879(2), 82 (2019) https://doi.org/10.3847/1538-4357/ ab22b8","work_id":"bc2eecb8-e63a-44fb-bdbc-a4f9fa7e075f","shared_citers":5},{"title":"Aaij, et al., Observation of a J/ψΛResonance Consistent with a Strange Pentaquark Candidate in B-→J/ψΛp¯Decays, Phys","work_id":"e8e48350-e8bc-46dc-b2db-27f689c5d1ae","shared_citers":4},{"title":"Barabash, et al., Phys","work_id":"10db733b-80f5-4873-a6d9-0e6b2043c8a5","shared_citers":4},{"title":"DESI 2024 VI: Cosmological Constraints from the Measurements of Baryon Acoustic Oscillations","work_id":"abaeab8e-c412-45ac-813e-f53689657023","shared_citers":4},{"title":"G., et al., 1998, @doi [AJ] 10.1086/300499 , http://adsabs.harvard.edu/abs/1998AJ....116.1009R 116","work_id":"f4711f38-d7d5-454b-a88b-02642c09bbd4","shared_citers":4},{"title":"K.-W., & Li, T","work_id":"32ff0a4d-a56d-4db2-a8d6-5ad8ca0dcec8","shared_citers":4},{"title":"Navas et al","work_id":"d56cdc88-8206-4cdb-a0f3-8e0c5fa5b969","shared_citers":4},{"title":"2013.11.081","work_id":"0a83db82-fe3b-4808-a34b-5e77806a6080","shared_citers":3},{"title":"Aaij, et al., Evidence of aJ/ψΛstructure and observation of excitedΞ− states in theΞ− b →J/ψΛK− decay, Sci","work_id":"9ef4d84e-12d4-4b90-a919-8dd65b6d5c22","shared_citers":3},{"title":"Aaij, et al., Observation of a narrow pentaquark state, Pc(4312)+, and of two-peak structure of theP c(4450)+, Phys","work_id":"ad98d413-58ae-43ad-80f9-2ad3d318698d","shared_citers":3},{"title":"Aaij, et al., Observation ofJ/ψpResonances Con- sistent with Pentaquark States inΛ 0 b →J/ψK − pDe- cays, Phys","work_id":"4ecbc9ca-2dbb-419b-bee3-e43ffee9048a","shared_citers":3},{"title":"Abbott, R","work_id":"ec2ceb71-84c6-42f9-8595-7d02bd369ca8","shared_citers":3},{"title":"An up- dated review of the new hadron states","work_id":"d36b538d-17d3-4a08-9af2-c7bcfed9ff13","shared_citers":3},{"title":"Beraudo, J.-P","work_id":"726c17f7-492c-49ae-b786-c01bec298700","shared_citers":3}],"time_series":[{"n":1,"year":2019},{"n":1,"year":2022},{"n":17,"year":2025},{"n":59,"year":2026}],"dependency_candidates":[{"n":1,"role":"method","polarity":"use_method","paper_title":"Multiplicative matching of neutral current deep-inelastic scattering processes at next-to-leading order in PYTHIA 8","primary_cat":"hep-ph","context_text":"is to compare the distributions of the DIS quantitiesx,y,Q 2 andW 2. We use a fixed value for the electromagnetic cou- pling with 1/α=137.036. We derive the electroweak pa- rameters from the input ofα(M Z), electroweak mixing an- gle sin2 θW =0.2312, and theZ-boson massM Z =91.1876 GeV . We use the PDF setNNPDF31_nlo_as_0118_luxqed [51] provided by the LHAPDF library [52]. The running of the strong coupling is handled by the PDF set. Setting up the event generation with beam energies cor- responding to the HERA experiments, 27.5 GeV for the elec- tron and 920 GeV for the proton, we generate events with the three generators at process level; without parton show- ers, beam remnants or hadronization. To focus solely on the higher-order effects, all partons","citing_arxiv_id":"2605.00502"},{"n":1,"role":"dataset","polarity":"use_dataset","paper_title":"Mesonic modes in confining model at finite temperature","primary_cat":"hep-ph","context_text":"extreme conditions from chiral quark models with nonlocal separable inter- actions. Symmetry13(1), 121 (2021). https://doi.org/10.3390/sym13010121. arXiv:2101.09574 [hep-ph] [33] C. Chen, F. Gao, S.x. Qin, Screening masses of positive- and negative-parity hadron ground states, including those with strangeness. Phys. Rev. D112(1), 014022 (2025). https://doi.org/10.1103/527r-mtxb. arXiv:2412.15045 [hep-ph] 15 [34] M. Cheng, et al., Meson screening masses from lattice qcd with two light and the strange quark. Eur. Phys. J. C71, 1564 (2011). https://doi.org/10.1140/epjc/ s10052-011-1564-y. arXiv:1010.1216 [hep-lat] [35] A. Bazavov, et al., The chiral transition andu(1) a symmetry restoration from lattice qcd using domain wall fermions. Phys. Rev. D86, 094503 (2012).","citing_arxiv_id":"2604.06275"},{"n":1,"role":"method","polarity":"use_method","paper_title":"Measure charge transport in high-energy nuclear collisions with an energy scan of isobaric collisions","primary_cat":"nucl-ex","context_text":"itively and negatively charged particles, respectively. Sinceπ,K, andpdominate the charged hadron yields, Qmay also be written as Q= (N π+ +N K+ +N p)−(N π− +N K− +N ¯p).(2) arXiv:2604.02825v1 [nucl-ex] 3 Apr 2026 2 Because pions dominate the charged multiplicity and Nπ+ ≈N π− with large absolute values, extractingQ with high precision is challenging. A recent proposal [18] demonstrated that the charge difference (∆Q) between two isobar systems-nuclei with identical mass numberAbut different atomic number Z-can be determined precisely using a double-ratio method. Defining ∆Q=Q Iso1 −Q Iso2,(3) and exploiting the near equality of particle multiplic- ities in the two systems, the charge difference can be approximated as","citing_arxiv_id":"2604.02825"}]},"authors":[]}}