Berndt Müller
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Berndt Müller has a total of 204 co-authors. Here are the top co-authors by number of shared publications:
- Walter Greiner
Johann Wolfgang Goethe-Universität Frankfurt
18 shared publications - Xiaojun Yao
University of Washington
18 shared publications - Jonathan Pettitt
University of Aberdeen
15 shared publications - Andreas Schäfer
University of Regensburg
13 shared publications - Clemens Seidl
Universität Regensburg
12 shared publications - Bernadette Connolly
University of Aberdeen
9 shared publications
Latest Publications
- Open Access
- 12 October 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (10) , 137
Local thermalization of SU(2) lattice gauge fields on quantum computers
A bstract: We simulate the local thermalization dynamics for minimally truncated SU(2) pure gauge theory on linear plaquette chains with up to 151 plaquettes using IBM quantum computers. We study the time dependence of the entanglement spectrum, Rényi-2 entropy and anti-flatness on small subsystems. The quantum hardware results obtained after error mitigation agree with classical simulator results for chains consisting of up to 101 plaquettes. Our results demonstrate the feasibility of local thermalization studies for chaotic quantum systems, such as nonabelian lattice gauge theories, on current noisy quantum computing platforms.
- 12 October 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (10) , 137
Open AccessLocal thermalization of SU(2) lattice gauge fields on quantum computers
A bstract: We simulate the local thermalization dynamics for minimally truncated SU(2) pure gauge theory on linear plaquette chains with up to 151 plaquettes using IBM quantum computers. We study the time dependence of the entanglement spectrum, Rényi-2 entropy and anti-flatness on small subsystems. The quantum hardware results obtained after error mitigation agree with classical simulator results for chains consisting of up to 101 plaquettes. Our results demonstrate the feasibility of local thermalization studies for chaotic quantum systems, such as nonabelian lattice gauge theories, on current noisy quantum computing platforms.
- Open Access
- 5 October 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (7)
Minimally truncated SU(3) lattice gauge theory and string tension
We study SU(3) gauge theory on small lattices in the minimal (qutrit) electric field truncation retaining only the 1 , 3 , 3 ¯ representations for the link variables. Explicit expressions are given for the Kogut-Susskind Hamiltonian for the square plaquette chain and the two-dimensional honeycomb lattice. Our formalism can be easily extended to the minimally truncated general SU ( N c ) gauge theory. The addition of (static) quarks is discussed. We present results for the energy spectrum of the gauge field on these lattices by exact diagonalization of the Hamiltonian and analyze its statistical properties. We also compute the SU(3) string tension and discuss how it is modified by vacuum fluctuations. Finally, we calculate the potential energies of a static quark-antiquark pair and three static quarks and study their screening at finite temperature.
- 5 October 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (7)
Open AccessMinimally truncated SU(3) lattice gauge theory and string tension
We study SU(3) gauge theory on small lattices in the minimal (qutrit) electric field truncation retaining only the 1 , 3 , 3 ¯ representations for the link variables. Explicit expressions are given for the Kogut-Susskind Hamiltonian for the square plaquette chain and the two-dimensional honeycomb lattice. Our formalism can be easily extended to the minimally truncated general SU ( N c ) gauge theory. The addition of (static) quarks is discussed. We present results for the energy spectrum of the gauge field on these lattices by exact diagonalization of the Hamiltonian and analyze its statistical properties. We also compute the SU(3) string tension and discuss how it is modified by vacuum fluctuations. Finally, we calculate the potential energies of a static quark-antiquark pair and three static quarks and study their screening at finite temperature.
- Open Access
- 22 September 2026
- Published by Springer Nature
- p. 105-137
What Is the Quark-Gluon Plasma Made Of?
This article surveys our present understanding of the internal structure of the fully developed quark-gluon plasma at temperatures outside the crossover region. The theoretical part of the review covers perturbative and nonperturbative approaches to quark-gluon plasma structure, in particular, hard-thermal loop effective theory, lattice QCD and the functional renormalization group. The phenomenological part of the review scrutinizes the information that has been derived from bulk observables and hard probes in relativistic heavy ion collisions in terms of how it informs our knowledge about the structure of the quark-gluon plasma. The final section lists possible avenues for future progress.
- 22 September 2026
- Published by Springer Nature
- p. 105-137
Open AccessWhat Is the Quark-Gluon Plasma Made Of?
This article surveys our present understanding of the internal structure of the fully developed quark-gluon plasma at temperatures outside the crossover region. The theoretical part of the review covers perturbative and nonperturbative approaches to quark-gluon plasma structure, in particular, hard-thermal loop effective theory, lattice QCD and the functional renormalization group. The phenomenological part of the review scrutinizes the information that has been derived from bulk observables and hard probes in relativistic heavy ion collisions in terms of how it informs our knowledge about the structure of the quark-gluon plasma. The final section lists possible avenues for future progress.
- Open Access
- 21 August 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (8) , 172
A new effective field theory for heavy quarks in the quark-gluon plasma
A bstract: An effective field theory framework is developed to study the interaction of heavy quarks in strongly coupled quark-gluon plasma (QGP). The latter is treated as a relativistic non-dissipative colorless fluid which can be studied using a derivatively coupled effective field theory based on previous work. Coupling this to heavy quarks provides a systematic way to obtain the interaction between the heavy quark and phonons, excitations of the fluid. In particular we calculate the quasiparticle width of heavy quark to phonon and phonon-heavy quark scattering in a thermal medium.
- 21 August 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (8) , 172
Open AccessA new effective field theory for heavy quarks in the quark-gluon plasma
A bstract: An effective field theory framework is developed to study the interaction of heavy quarks in strongly coupled quark-gluon plasma (QGP). The latter is treated as a relativistic non-dissipative colorless fluid which can be studied using a derivatively coupled effective field theory based on previous work. Coupling this to heavy quarks provides a systematic way to obtain the interaction between the heavy quark and phonons, excitations of the fluid. In particular we calculate the quasiparticle width of heavy quark to phonon and phonon-heavy quark scattering in a thermal medium.
- Open Access
- 11 June 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 136 (23) , 230403
Magic Barrier before Thermalization
We investigate the time dependence of antiflatness in the entanglement spectrum, a measure for nonstabilizerness and lower bound for nonlocal quantum magic resource, on a subsystem of a linear SU(2) plaquette chain during thermalization. Tracing the time evolution of a large number of initial states, we find that the antiflatness exhibits a barrierlike maximum during the time period when the entanglement entropy of the subsystem grows rapidly from the initial value to the microcanonical entropy. The location of the peak is strongly correlated with the time when the entanglement exhibits the strongest growth. This behavior is found for generic highly excited initial computational basis states and persists for coupling constants across the ergodic regime, revealing a universal structure of the entanglement spectrum during thermalization. We conclude that quantitative simulations of thermalization for non-Abelian gauge theories require quantum computing. We speculate that this property generalizes to other quantum chaotic systems, a conjecture supported by analogous behavior observed in real-time simulations of the mixed-field Ising model.
- 11 June 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 136 (23) , 230403
Open AccessMagic Barrier before Thermalization
We investigate the time dependence of antiflatness in the entanglement spectrum, a measure for nonstabilizerness and lower bound for nonlocal quantum magic resource, on a subsystem of a linear SU(2) plaquette chain during thermalization. Tracing the time evolution of a large number of initial states, we find that the antiflatness exhibits a barrierlike maximum during the time period when the entanglement entropy of the subsystem grows rapidly from the initial value to the microcanonical entropy. The location of the peak is strongly correlated with the time when the entanglement exhibits the strongest growth. This behavior is found for generic highly excited initial computational basis states and persists for coupling constants across the ergodic regime, revealing a universal structure of the entanglement spectrum during thermalization. We conclude that quantitative simulations of thermalization for non-Abelian gauge theories require quantum computing. We speculate that this property generalizes to other quantum chaotic systems, a conjecture supported by analogous behavior observed in real-time simulations of the mixed-field Ising model.
- Open Access
- 23 April 2026
- Published by Oxford University Press (OUP) in Nucleic Acids Research
- Vol. 54 (8)
Cap-adjacent 2′- O -ribose methylation of RNA in C. elegans is required for postembryonic growth and germline development in the presence of the decapping exonuclease EOL-1
Cap-adjacent 2′-O-ribose methylation (cOMe) of the first two transcribed nucleotides of RNA polymerase II transcripts is a conserved feature in many eukaryotes. In mammals, these modifications are key to a transcript surveillance system that regulates the interferon response, but the broader functions of cOMe remain poorly understood. To understand the role of cOMe in Caenorhabditis elegans, we functionally characterized the methyltransferases (CMTR-1 and CMTR-2) responsible for installing these modifications. These enzymes have distinct expression patterns, protein interaction partners, and loss-of-function phenotypes. Loss of CMTR-1 causes dramatic reductions in cOMe, impaired growth, and sterility. In contrast, animals lacking CMTR-2 are superficially wild-type, though CMTR-2 loss enhances the severity of the cmtr-1 mutant phenotype. Depletion of CMTR-1 causes downregulation of transcripts associated with germline sex determination and upregulation of those involved in the intracellular pathogen response (IPR). We show that the absence of the decapping exonuclease, EOL-1, an IPR component, completely suppresses the sterility and growth defects caused by CMTR-1 loss, and reverses the associated steady-state transcript changes. Our work shows the physiological relevance of cOMe in protecting transcripts from decapping exonucleases, raising the possibility that cOMe plays a role in RNA-mediated immune surveillance beyond the vertebrates.
- 23 April 2026
- Published by Oxford University Press (OUP) in Nucleic Acids Research
- Vol. 54 (8)
Open AccessCap-adjacent 2′- O -ribose methylation of RNA in C. elegans is required for postembryonic growth and germline development in the presence of the decapping exonuclease EOL-1
Cap-adjacent 2′-O-ribose methylation (cOMe) of the first two transcribed nucleotides of RNA polymerase II transcripts is a conserved feature in many eukaryotes. In mammals, these modifications are key to a transcript surveillance system that regulates the interferon response, but the broader functions of cOMe remain poorly understood. To understand the role of cOMe in Caenorhabditis elegans, we functionally characterized the methyltransferases (CMTR-1 and CMTR-2) responsible for installing these modifications. These enzymes have distinct expression patterns, protein interaction partners, and loss-of-function phenotypes. Loss of CMTR-1 causes dramatic reductions in cOMe, impaired growth, and sterility. In contrast, animals lacking CMTR-2 are superficially wild-type, though CMTR-2 loss enhances the severity of the cmtr-1 mutant phenotype. Depletion of CMTR-1 causes downregulation of transcripts associated with germline sex determination and upregulation of those involved in the intracellular pathogen response (IPR). We show that the absence of the decapping exonuclease, EOL-1, an IPR component, completely suppresses the sterility and growth defects caused by CMTR-1 loss, and reverses the associated steady-state transcript changes. Our work shows the physiological relevance of cOMe in protecting transcripts from decapping exonucleases, raising the possibility that cOMe plays a role in RNA-mediated immune surveillance beyond the vertebrates.
- 6 February 2026
- Published by Elsevier in Journal of Subatomic Particles and Cosmology
- Vol. 5
Local spin polarization by color-field correlators and momentum anisotropy
- 6 February 2026
- Published by Elsevier in Journal of Subatomic Particles and Cosmology
- Vol. 5
Local spin polarization by color-field correlators and momentum anisotropy
- Open Access
Minimally Truncated SU(3) Lattice Gauge Theory and String Tension
We study SU(3) gauge theory on small lattices in the minimal (qutrit) electric field truncation retaining only the ${\bf 1}, {\bf 3}, {\bf \overline{3}}$ representations for the link variables. Explicit expressions are given for the Kogut-Susskind Hamiltonian for the square plaquette chain and the two-dimensional honeycomb lattice. Our formalism can be easily extended to the minimally truncated general SU($N_c$) gauge theory. The addition of (static) quarks is discussed. We present results for the energy spectrum of the gauge field on these lattices by exact diagonalization of the Hamiltonian and analyze its statistical properties. We also compute the SU(3) string tension and discuss how it is modified by vacuum fluctuations. Finally, we calculate the potential energies of a static quark-antiquark pair and three static quarks and study their screening at finite temperature.Open AccessMinimally Truncated SU(3) Lattice Gauge Theory and String Tension
We study SU(3) gauge theory on small lattices in the minimal (qutrit) electric field truncation retaining only the ${\bf 1}, {\bf 3}, {\bf \overline{3}}$ representations for the link variables. Explicit expressions are given for the Kogut-Susskind Hamiltonian for the square plaquette chain and the two-dimensional honeycomb lattice. Our formalism can be easily extended to the minimally truncated general SU($N_c$) gauge theory. The addition of (static) quarks is discussed. We present results for the energy spectrum of the gauge field on these lattices by exact diagonalization of the Hamiltonian and analyze its statistical properties. We also compute the SU(3) string tension and discuss how it is modified by vacuum fluctuations. Finally, we calculate the potential energies of a static quark-antiquark pair and three static quarks and study their screening at finite temperature. - Open Access
- 12 January 2026
- Published by American Physical Society (APS) in Physical Review C
- Vol. 113 (1)
Quark flavor equilibration of the quark-gluon plasma
The early stage of a heavy-ion collision is marked by rapid entropy production and the transition from a gluon saturated initial condition to a plasma of quarks and gluons that evolves hydrodynamically. However, during the early times of the hydrodynamic evolution, the chemical composition of the QCD medium is still largely unknown. We present a study of quark chemical equilibration in the (Q)GP using a novel model of viscous hydrodynamic evolution in partial chemical equilibrium. Motivated by the success of gluon saturated initial condition models, we initialize the QCD medium as a completely gluon dominated state. Local quark production during the hydrodynamic phase is then simulated through the evolution of time-dependent fugacities for each independent quark flavor, with the timescales set as free parameters to compare different rates of equilibration. We present the results of complete heavy-ion collision simulations using this partial chemical equilibrium model, and show the effects on hadronic and electromagnetic observables. In particular, we show that the development of flow is sensitive to the equilibration timescale, providing an empirical way to probe the chemical equilibration of the QCD medium.
- 12 January 2026
- Published by American Physical Society (APS) in Physical Review C
- Vol. 113 (1)
Open AccessQuark flavor equilibration of the quark-gluon plasma
The early stage of a heavy-ion collision is marked by rapid entropy production and the transition from a gluon saturated initial condition to a plasma of quarks and gluons that evolves hydrodynamically. However, during the early times of the hydrodynamic evolution, the chemical composition of the QCD medium is still largely unknown. We present a study of quark chemical equilibration in the (Q)GP using a novel model of viscous hydrodynamic evolution in partial chemical equilibrium. Motivated by the success of gluon saturated initial condition models, we initialize the QCD medium as a completely gluon dominated state. Local quark production during the hydrodynamic phase is then simulated through the evolution of time-dependent fugacities for each independent quark flavor, with the timescales set as free parameters to compare different rates of equilibration. We present the results of complete heavy-ion collision simulations using this partial chemical equilibrium model, and show the effects on hadronic and electromagnetic observables. In particular, we show that the development of flow is sensitive to the equilibration timescale, providing an empirical way to probe the chemical equilibration of the QCD medium.
- Open Access
- 22 October 2025
- Vol. 2025
The protein-protein interaction between two spliced leader trans -splicing factors is mediated by two interlinked α-helical domains.
SNA-1 and SNA-2 proteins are involved in spliced leader trans -splicing in Caenorhabditis elegans . They are components of the SL1 snRNP that donates the spliced leader 1 RNA which replaces the 5' end of most pre-mRNAs. SNA-1 and SNA-2 bind to each other, but the nature of their interaction is unclear. AlphaFold-Multimer predicts that the central region of SNA-1 and the C-terminal region of SNA-2 , each consisting of 3 α-helices, interlink to bring about the interaction between these proteins. Using yeast 2-hybrid assays we demonstrate that these regions are required and sufficient for this unusual mode of interaction between two proteins.
- 22 October 2025
- Vol. 2025
Open AccessThe protein-protein interaction between two spliced leader trans -splicing factors is mediated by two interlinked α-helical domains.
SNA-1 and SNA-2 proteins are involved in spliced leader trans -splicing in Caenorhabditis elegans . They are components of the SL1 snRNP that donates the spliced leader 1 RNA which replaces the 5' end of most pre-mRNAs. SNA-1 and SNA-2 bind to each other, but the nature of their interaction is unclear. AlphaFold-Multimer predicts that the central region of SNA-1 and the C-terminal region of SNA-2 , each consisting of 3 α-helices, interlink to bring about the interaction between these proteins. Using yeast 2-hybrid assays we demonstrate that these regions are required and sufficient for this unusual mode of interaction between two proteins.