Strongly interacting matter in extreme magnetic fields

  • Prabal Adhikari
  • , Martin Ammon
  • , Sidney S. Avancini
  • , Alejandro Ayala*
  • , Aritra Bandyopadhyay
  • , David Blaschke
  • , Fabio L. Braghin
  • , Pavel Buividovich
  • , Rafael P. Cardoso
  • , Casey Cartwright
  • , Jorge David Castaño-Yepes
  • , Maxim N. Chernodub
  • , Máximo Coppola
  • , Mayusree Das
  • , Mariana Dutra
  • , Gergely Endrődi
  • , Jianjun Fang
  • , Ricardo L.S. Farias
  • , Eduardo S. Fraga
  • , Arthur Frazon
  • Kenji Fukushima, Juan D. García-Muñoz, Eduardo Garnacho-Velasco, Daniel Gomez Dumm, Sebastian Grieninger, Francesca Gulminelli, Juan Hernandez, Chowdhury Aminul Islam, Matthias Kaminski, Andrey Kotov, Gastão Krein, Jing Li, Pok Man Lo, Marcelo Loewe, Odilon Lourenço, Gergely Markó, Kau D. Marquez, Ana Mizher, Banibrata Mukhopadhyay, Enrique Muñoz, Santiago Noguera, Rodrigo M. Nunes, Helena Pais, Letícia F. Palhares, Constança Providência, Alfredo Raya, Tulio Restrepo, Juan Cristóbal Rojas, Norberto N. Scoccola, Luigi Scurto, Armen Sedrakian, Dominik Smith, William Rafael Tavares, Maria E. Tejeda-Yeomans, Varese S. Timóteo, Laura Tolos, Cristian Villavicencio, Fridolin Weber, Shigehiro Yasui, Renato Zamora, Zenia Zuraiq
*Corresponding author for this work

Research output: Contribution to journalReview articlepeer-review

Abstract

Magnetic fields are ubiquitous across different physical systems of current interest; from the early Universe, compact astrophysical objects, and heavy-ion collisions to condensed matter systems. A proper treatment of the effects produced by magnetic fields during the dynamical evolution of these systems can help to understand observables that otherwise show puzzling behavior. Furthermore, when these fields are comparable to or stronger than ΛQCD, they serve as excellent probes to help elucidate the physics of strongly interacting matter under extreme conditions of temperature and density. This work provides a detailed report that contains in-depth analysis and expert insights into the specific topic of the effects of strong magnetic fields on QED and QCD systems. In this sense, the report is intended as a white paper contribution to the field. The subjects developed include the modification of meson static properties such as masses and form factors, the chiral magnetic effect, the description of anomalous transport coefficients, superconductivity in extreme magnetic fields, the properties of neutron stars, the evolution of heavy-ion collisions, as well as effects on the QCD phase diagram. We describe recent theory and phenomenological developments using effective models as well as LQCD methods. The work was motivated by presentations and discussions during the “Workshop on Strongly Interacting Matter in Strong Electromagnetic Fields” that took place in the European Centre for Theoretical Studies in Nuclear Physics and Related Areas (ECT*) in the city of Trento, Italy, September 25–29, 2023.

Original languageEnglish
Article number104199
JournalProgress in Particle and Nuclear Physics
Volume146
Issue numberPart 1
Early online date12 Sept 2025
DOIs
Publication statusPublished - Jan 2026

Bibliographical note

Publisher Copyright:
© 2025 The Authors

Funding

This work has been supported by STRONG-2020 “The strong interaction at the frontier of knowledge: fundamental research and applications” which received funding from the European Union's Horizon 2020 research and innovation programme under grant agreement No 824093. M.K. was supported, in part, by the U.S. Department of Energy grant DE-SC0012447. The material presented in this article is based in part upon work done while C.C. was supported by the U.S. Department of Energy, Office of Science, Office of Workforce Development for Teachers and Scientists, Office of Science Graduate Student Research (SCGSR) program. The SCGSR program is administered by the Oak Ridge Institute for Science and Education (ORISE) for the DOE. ORISE is managed by ORAU under contract number DE-SC0014664. All opinions expressed in this paper are the author's and do not necessarily reflect the policies and views of DOE, ORAU, or ORISE. CC is currently supported in part by the Netherlands Organisation for Scientific Research (NWO) under the VICI grant VI.C.202.104. S.G. was supported in part by the Office of Science, Office of Nuclear Physics, U.S. Department of Energy under Contract No. DE- FG88ER40388 and in part by a Feodor Lynen Research fellowship of the Alexander von Humboldt foundation and is also supported by the U.S. Department of Energy grant DE-FG02-97ER (UW Nuclear Theory). Part of the material presented in this work is based upon work done while S.G. was supported by the Fulbright Visiting Scholar Program which is sponsored by the US Department of State and the German-American Fulbright Commission and the DAAD. J.H. is supported by FWO-Vlaanderen through a Junior Postdoctoral Fellowship. Research by J.H. is also supported by FWO-Vlaanderen project G012222N, and by Vrije Universiteit Brussel through the Strategic Research Program High-Energy Physics. A.M. was financed, in part, by the São Paulo Research Foundation (FAPESP), Brasil, Process Number 2023/08826-7. The work of G.E. E.G.V. and G.M. was funded by the DFG (Collaborative Research Center CRC-TR 211 “Strong-interaction matter under extreme conditions” - project number 315477589 - TRR 211). G.E. acknowledges support by the Hungarian National Research, Development and Innovation Office (Research Grant Hungary). E.G.V. acknowledges support by the Helmholtz Graduate School for Hadron and Ion Research (HGS-HIRe for FAIR). The work of P.B. was funded in part by the UK STFC Consolidated Grant ST/T000988/1. This work was partially supported by Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq), 312032/2023-4 (R.L.S.F.); Fundação de Amparo à Pesquisa do Estado do Rio Grande do Sul (FAPERGS), Grants Nos. 19/2551- 0000690-0 and 19/2551-0001948-3 (R.L.S.F.); The work is also part of the project Instituto Nacional de Ciência e Tecnologia- Física Nuclear e Aplicações (INCT - FNA), Grant No. 464898/2014-5, by Fundação Carlos Chagas Filho de Amparo à Pesquisa do Estado do Rio de Janeiro (FAPERJ) under Grant No. SEI-260003/019544/2022 (W.R.T) and Grant No. SEI-260003/019683/2022 (T.R.). This study was financed in part by the Coordenação de Aperfeiçoamento de Pessoal de Nível Superior - Brasil (CAPES) – Finance Code 001 (R.M.N.) and Grant no. 88887.826087/2023-00 (R.P.C). A.B. acknowledges the support from the Alexander von Humboldt foundation. C.V. acknowledge financial support from ANID/FONDECYT under Grant No. 1250206. P.M.L. acknowledges partial support from the Polish National Science Center (NCN) under the Opus grant no. 2022/45/B/ST2/01527. The work of G.K. is a part of the project INCT-FNA proc. No. 464898/2014-5. G.K. is also supported by Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) under Grant No. 309262/2019-4 and by Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP) under Grant No. 2018/25225-9. The work of V.S.T. is also supported by Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) under Grant No. 305004/2022-0 and by Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP) under Grant No. 2019/10889-1. The work of A.A. was supported by UNAM-PAPIIT grant number IG100322 and by Consejo Nacional de Humanidades, Ciencia y Tecnología grant number CF-2023-G-433 and also acknowledges support from the PASPA program pf the Dirección de Asuntos del Personal Académico (DGAPA) of the Universidad Nacional Autónoma de México (UNAM) for a sabbatical stay duringh which this work was completed. The work of L.T. is supported under contract No. PID2022-139427NB-I00 financed by the Spanish MCIN/AEI/10.13039/501100011033/FEDER, UE; by the Generalitat de Catalunya under contract 2021 SGR 00171; by Generalitat Valenciana under contract PROMETEO/2020/023; from the project CEX2020-001058-M (Unidad de Excelencia “María de Maeztu”); from the European Union Horizon 2020 research and innovation programme under the program H2020-INFRAIA-2018-1, grant agreement No. 824093 of the STRONG-2020 project; and from the CRC-TR 211 ’Strong-interaction matter under extreme conditions’- project Nr. 315477589 - TRR 211. A.S. is supported by Deutsche Forschungsgemeinschaft (DFG) Grant No. SE 1836/5-3 and the Polish National Science Center (NCN) Grant No. 2023/51/B/ST9/02798. K.D.M. thanks the financial support from the São Paulo State Research Foundation (FAPESP), under Grant No. 2024/01623-6. The work of M.C. D.G.D. and N.N.S. has been partially funded by CONICET (Argentina) under Grant No. PIP 2022 GI-11220210100150CO, by ANPCyT (Argentina) under Grant No. PICT20-01847. The work of D.G.D. has also been funded by the National University of La Plata (Argentina), Project No. X824. S.N. acknowledges support by Ministerio de Ciencia e Innovación and Agencia Estatal de Investigación (Spain), and European Regional Development Fund Grant No. PID2019-105439GB-C21, by EU Horizon 2020 Grant No. 824093 (STRONG-2020), and by Conselleria de Innovación, Universidades, Ciencia y Sociedad Digital, Generalitat Valenciana, GVA PROMETEO/2021/083. The work was also partially supported by national funds from FCT (Fundação para a Ciência e a Tecnologia, I.P, Portugal) under projects UIDB/04564/2020 and UIDP/04564/2020, with DOI identifiers 10.54499/UIDB/04564/2020 and 10.54499/UIDP/04564/2020, respectively, and the project 2022.06460.PTDC with the associated DOI identifier 10.54499/2022.06460.PTDC. H.P. acknowledges the grant 2022.03966.CEECIND (FCT, Portugal) with DOI identifier 10.54499/2022.03966.CEECIND/CP1714/CT0004. L.S. acknowledges the PhD grant 2021.08779.BD (FCT, Portugal) with DOI identifier 10.54499/2021.08779.BD. P.A. is supported by the U.S. Department of Energy, Office of Science, Office of Nuclear Physics and Quantum Horizons Program under Award Number DE-SC0024385. P.A. also acknowledges the hospitality of the Kavli Institute for Theoretical Physics, Santa Barbara, through which the research was supported in part by the National Science Foundation under Grant No. NSF PHY-1748958. M.E.T-Y acknowledges support by Consejo Nacional de Humanidades, Ciencia y Tecnologia grant number A1-S-7655. The work of O.L. is a part of the project INCT-FNA proc. No. 464898/2014-5. It was also supported by Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) under Grants No. 307255/2023-9 and 401565/2023-8 (Universal) and by Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP) under Grant No. 2022/03575-3 (BPE). O.L. and M.D. also thank support from the Thematic Project No. 2024/17816-8 (FAPESP). The work of M.D. is a part of the project INCT-FNA proc. No. 464898/2014-5. It is also supported by Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) under Grant No. 308528/2021-2 and No. 401565/2023-8 (Universal). This study was also financed in part by the Coordenação de Aperfeiçoamento de Pessoal de Nível Superior - Brazil (CAPES) - Finance Code 001 - Project number 88887.687718/2022-0. F.L.B. is a member of INCT-FNA, 464898/2014-5 and he acknowledges partial support also from CNPq-312750/2021-8 and CNPq-407162/2023-2. The work of M.N.C. was funded by the EU's NextGenerationEU instrument through the National Recovery and Resilience Plan of Romania- Pillar III-C9-I8, managed by the Ministry of Research, Innovation and Digitization, within the project entitled “Facets of Rotating Quark-Gluon Plasma” (FORQ), contract no. 760079/23.05.2023 code CF 103/15.11.2022. D.B. received support from the Polish National Science Center (NCN) under Grant No. 2021/43/P/ST2/03319. V.S.T. was supported by FAPESP (grant2019/10889-1) and CNPq (grant 305004/2022-0). S.S.A. acknowledges partial support from CNPq-308963/2023-7 and INCT-FNA. B.M. acknowledges a project funded by SERB, India, with Ref. No. CRG/2022/003460, for partial support towards this research. M.D. acknowledges the Prime Minister's Research Fellows (PMRF) scheme, with Ref. No. TF/PMRF-22-5442.03. Z.Z. acknowledges the Prime Minister's Research Fellows (PMRF) scheme, with Ref. No. TF/PMRF-22-7307, for providing fellowship. E.M. thanks finantial support from ANID Fondecyt Project No. 1230440. M.L. and R.Z. acknowledge support from ANID/CONICYT FONDECYT regular (Chile) under grants numbers 1220035 and 1241436. This work has been supported by STRONG-2020 “The strong interaction at the frontier of knowledge: fundamental research and applications” which received funding from the European Union’s Horizon 2020 research and innovation programme under grant agreement No 824093 . M.K. was supported, in part, by the U.S. Department of Energy grant DE-SC0012447 . The material presented in this article is based in part upon work done while C.C. was supported by the U.S. Department of Energy, Office of Science, Office of Workforce Development for Teachers and Scientists, Office of Science Graduate Student Research (SCGSR) program . The SCGSR program is administered by the Oak Ridge Institute for Science and Education (ORISE) for the DOE. ORISE is managed by ORAU under contract number DE-SC0014664. All opinions expressed in this paper are the author’s and do not necessarily reflect the policies and views of DOE, ORAU, or ORISE. CC is currently supported in part by the Netherlands Organisation for Scientific Research (NWO) under the VICI grant VI.C.202.104 . S.G. was supported in part by the Office of Science, Office of Nuclear Physics, U.S. Department of Energy under Contract No. DE- FG88ER40388 and in part by a Feodor Lynen Research fellowship of the Alexander von Humboldt foundation . Part of the material presented in this work is based upon work done while S.G. was supported by the Fulbright Visiting Scholar Program which is sponsored by the US Department of State and the German-American Fulbright Commission and the DAAD . J.H. is supported by FWO-Vlaanderen through a Junior Postdoctoral Fellowship. Research by J.H. is also supported by FWO-Vlaanderen project G012222N , and by Vrije Universiteit Brussel through the Strategic Research Program High-Energy Physics. A.M. was financed, in part, by the São Paulo Research Foundation (FAPESP), Brasil , Process Number 2023/08826-7 . The work of G.E., E.G.V. and G.M. was funded by the DFG (Collaborative Research Center CRC-TR 211 “Strong-interaction matter under extreme conditions” - project number 315477589 - TRR 211). G.E. acknowledges support by the Hungarian National Research, Development and Innovation Office (Research Grant Hungary). E.G.V. acknowledges support by the Helmholtz Graduate School for Hadron and Ion Research (HGS-HIRe for FAIR) . The work of P.B. was funded in part by the UK STFC Consolidated Grant ST/T000988/1 . This work was partially supported by Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) , 312032/2023-4 (R.L.S.F.); Fundação de Amparo à Pesquisa do Estado do Rio Grande do Sul (FAPERGS) , Grants Nos. 19/2551- 0000690-0 and 19/2551-0001948-3 (R.L.S.F.); The work is also part of the project Instituto Nacional de Ciência e Tecnologia- Física Nuclear e Aplicações (INCT - FNA) , Grant No. 464898/2014-5 , by Fundação Carlos Chagas Filho de Amparo à Pesquisa do Estado do Rio de Janeiro (FAPERJ) under Grant No. SEI-260003/019544/2022 (W.R.T). This study was financed in part by the Coordenação de Aperfeiçoamento de Pessoal de Nível Superior - Brasil (CAPES) – Finance Code 001 (R.M.N.) and Grant no. 88887.826087/2023-00 (R.P.C). A.B. acknowledges the support from the Alexander von Humboldt foundation . C.V. acknowledge financial support from ANID/FONDECYT under Grant No. 1190192 . P.M.L. acknowledges partial support from the Polish National Science Center (NCN) under the Opus grant no. 2022/45/B/ST2/01527 . The work of G.K. is a part of the project INCT-FNA proc. No. 464898/2014-5. G.K. is also supported by Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) under Grant No. 309262/2019-4 and by Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP) under Grant No. 2018/25225-9 . The work of V.S.T. is also supported by Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) under Grant No. 305004/2022-0 and by Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP) under Grant No. 2019/10889-1 . The work of A.A. was supported by UNAM-PAPIIT grant number IG100322 and by Consejo Nacional de Humanidades , Ciencia Tecnología grant number CF-2023-G-433 . The work of L.T. is supported under contract No. PID2022-139427NB-I00 financed by the Spanish MCIN/AEI/10.13039/501100011033/FEDER, UE ; by the Generalitat de Catalunya under contract 2021 SGR 00171 ; by Generalitat Valenciana under contract PROMETEO/2020/023 ; from the project CEX2020-001058-M (Unidad de Excelencia “María de Maeztu”); from the European Union Horizon 2020 research and innovation programme under the program H2020-INFRAIA-2018-1, grant agreement No. 824093 of the STRONG-2020 project; and from the CRC-TR 211 ’Strong-interaction matter under extreme conditions’- project Nr. 315477589 - TRR 211. A.S. is supported by Deutsche Forschungsgemeinschaft (DFG) Grant No. SE 1836/5-3 and the Polish National Science Center (NCN) Grant No. 2023/51/B/ST9/02798 . K.D.M. thanks the financial support from the São Paulo State Research Foundation (FAPESP), under Grant No. 2024/01623-6 . The work of M.C., D.G.D. and N.N.S. has been partially funded by CONICET (Argentina) under Grant No. PIP 2022 GI-11220210100150CO , by ANPCyT (Argentina) under Grant No. PICT20-01847 . The work of D.G.D. has also been funded by the National University of La Plata (Argentina) , Project No. X824. S.N. acknowledges support by Ministerio de Ciencia e Innovación and Agencia Estatal de Investigación (Spain) , and European Regional Development Fund Grant No. PID2019-105439GB-C21 , by EU Horizon 2020 Grant No. 824093 (STRONG-2020), and by Conselleria de Innovación, Universidades, Ciencia y Sociedad Digital, Generalitat Valenciana , GVA PROMETEO/2021/083 . The work was also partially supported by national funds from FCT (Fundação para a Ciência e a Tecnologia, I.P, Portugal) under projects UIDB/04564/2020 and UIDP/04564/2020 , with DOI identifiers 10.54499/UIDB/04564/2020 and 10.54499/UIDP/04564/2020, respectively, and the project 2022.06460.PTDC with the associated DOI identifier 10.54499/2022.06460.PTDC. H.P. acknowledges the grant 2022.03966.CEECIND (FCT, Portugal) with DOI identifier 10.54499/2022.03966.CEECIND/CP1714/CT0004. L.S. acknowledges the PhD grant 2021.08779.BD (FCT, Portugal) with DOI identifier 10.54499/2021.08779.BD. P.A. is supported by the U.S. Department of Energy, Office of Science, Office of Nuclear Physics and Quantum Horizons Program under Award Number DE-SC0024385 . P.A. also acknowledges the hospitality of the Kavli Institute for Theoretical Physics, Santa Barbara, through which the research was supported in part by the National Science Foundation under Grant No. NSF PHY-1748958 . M.E.T-Y acknowledges support by Consejo Nacional de Humanidades, Ciencia Tecnologia grant number A1-S-7655 . The work of O.L. is a part of the project INCT-FNA proc. No. 464898/2014-5. It was also supported by Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) under Grants No. 307255/2023-9 and 401565/2023-8 (Universal) and by Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP) under Grant No. 2022/03575-3 (BPE). The work of M.D. is a part of the project INCT-FNA proc. No. 464898/2014-5. It is also supported by Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) under Grant No. 308528/2021-2 and No. 401565/2023-8 (Universal). This study was also financed in part by the Coordenação de Aperfeiçoamento de Pessoal de Nível Superior - Brazil (CAPES) - Finance Code 001 - Project number 88887.687718/2022-0 . F.L.B. is a member of INCT-FNA, 464898/2014-5 and he acknowledges partial support also from CNPq-312750/2021-8 and CNPq-407162/2023-2 . The work of M.N.C. was funded by the EU’s NextGenerationEU instrument through the National Recovery and Resilience Plan of Romania - Pillar III-C9-I8, managed by the Ministry of Research, Innovation and Digitization, within the project entitled “Facets of Rotating Quark-Gluon Plasma” (FORQ), contract no. 760079/23.05.2023 code CF 103/15.11.2022. D.B. received support from the Polish National Science Center (NCN) under Grant No. 2021/43/P/ST2/03319 . V.S.T. was supported by FAPESP (grant 2019/10889-1 ) and CNPq (grant 305004/2022-0 ).

FundersFunder number
Workforce Development for Teachers and Scientists
Helmholtz Graduate School for Hadron and Ion Research
Kavli Institute for Theoretical Physics, University of California, Santa Barbara
Narodowe Centrum Nauki
U.S. Department of State
Ministerul Cercetării, Inovării şi Digitalizării
Ciencia Tecnologia
Oak Ridge Institute for Science and Education
Ministerio de Ciencia e Innovación
Ciencia Tecnología
Deutscher Akademischer Austauschdienst
Vrije Universiteit Brussel
InCT
German-American Fulbright Program
Nemzeti Kutatási Fejlesztési és Innovációs Hivatal
Fund for Santa Barbara
Agencia Estatal de Investigación
Consejo Nacional de Humanidades
Office of Science Graduate Student Research Program
Office of Science
U.S. Department of EnergyDE-SC0012447
Consejo Nacional de Humanidades, Ciencias y Tecnologías2024/17816-8, 2022/03575-3, 307255/2023-9, CF-2023-G-433, 88887.687718/2022-0, 308528/2021-2, 401565/2023-8, A1-S-7655
Horizon 2020 Framework ProgrammeSTRONG-2020, 824093, 315477589, H2020-INFRAIA-2018-1
FORQ760079/23.05.2023, 2021/43/P/ST2/03319, CNPq-308963/2023-7
Fundação de Amparo à Pesquisa do Estado do Rio Grande do Sul19/2551-0001948-3, 19/2551- 0000690-0
NCN309262/2019-4, 2022/45/B/ST2/01527
Fundação de Amparo à Pesquisa do Estado de São Paulo2024/01623-6, 2023/08826-7, 2018/25225-9, 305004/2022-0, 2019/10889-1, 315477589 - TRR 211
Agencia Nacional de Investigación y Desarrollo1230440
Fundação para a Ciência e a TecnologiaUIDP/04564/2020, 2022.06460, 2021.08779, CEECIND/CP1714/CT0004, 2022.03966, UIDB/04564/2020
Generalitat ValencianaPROMETEO/2020/023, CEX2020-001058-M
Fonds Wetenschappelijk OnderzoekG012222N
National Recovery and Resilience Plan of RomaniaIII-C9-I8
Oak Ridge Associated UniversitiesDE-SC0014664
Comisión Nacional de Investigación Científica y Tecnológica1220035, 1241436
Alexander von Humboldt-StiftungDE-FG02-97ER
Universidad Nacional Autónoma de MéxicoMCIN/AEI/10.13039/501100011033/FEDER, IG100322, PID2022-139427NB-I00
Fondo Nacional de Desarrollo Científico y Tecnológico1250206, 1190192
Nederlandse Organisatie voor Wetenschappelijk OnderzoekVI.C.202.104
Instituto Nacional de Ciência e Tecnologia: Física Nuclear e AplicaçõesCNPq-407162/2023-2, CNPq-312750/2021-8
Agencia Nacional de Promoción Científica y TecnológicaPICT20-01847
Consejo Nacional de Investigaciones Científicas y TécnicasPIP 2022 GI-11220210100150CO
European Regional Development FundPID2019-105439GB-C21
Conselleria de Innovación, Universidades, Ciencia y Sociedad Digital, Generalitat ValencianaGVA PROMETEO/2021/083
National Science FoundationPHY-1748958
Fundação Carlos Chagas Filho de Amparo à Pesquisa do Estado do Rio de JaneiroSEI-260003/019683/2022, SEI-260003/019544/2022
Prime Minister's Research FellowsTF/PMRF-22-5442.03, TF/PMRF-22-7307
Nuclear PhysicsDE- FG88ER40388, DE-SC0024385
Deutsche Forschungsgemeinschaft2023/51/B/ST9/02798, SE 1836/5-3
Suomen Sairaanhoitajat ry464898/2014-5
Generalitat de Catalunya2021 SGR 00171
Coordenação de Aperfeiçoamento de Pessoal de Nível Superior88887.826087/2023-00
Conselho Nacional de Desenvolvimento Científico e Tecnológico312032/2023-4
Science and Technology Facilities CouncilST/T000988/1
Universidad Nacional de La PlataX824
Science and Engineering Research BoardCRG/2022/003460

    Keywords

    • Lattice quantum chromodynamics
    • Magnetic fields
    • Neutron stars
    • Quantum chromodynamics
    • Quantum electrodynamics

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