| Nonminimal non-Abelian quantum vector fields in curved spacetime |
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| Quark-diquark models and baryonic fluctuations in QCD |
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| Quark-diquark string tension, excited baryonic resonances and thermal fluctuations |
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| Renormalization of vector fields with mass-like coupling in curved spacetime |
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| Baryonic susceptibilities, quark-diquark models, and quark-hadron duality at finite temperature |
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| Schwinger-Dyson equations and line integrals |
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| Fluctuations and correlations in thermal QCD |
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| Positive representations of complex distributions on groups |
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| Thermal correlators in the hadron resonance gas: A dual hagedorn distance |
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| Canonical bracket in quantum-classical hybrid systems |
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| Does the complex Langevin method give unbiased results? |
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| Heavy quark-antiquark free energy and thermodynamics of string-hadron avoided crossings |
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| Gibbs sampling of complex-valued distributions |
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| Heavy quark entropy shift: From the hadron resonance gas to power corrections |
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| Heavy QmQ free energy from hadronic states |
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| Formation spectra of charmed meson-nucleus systems using an antiproton beam |
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| Quark properties from the hadron resonance gas |
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| Compositeness of the strange, charm, and beauty odd parity Lambda states |
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| Polyakov loop spectroscopy in the confined phase of gluodynamics and QCD |
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| Quark-Hadron duality at finite temperature |
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| Leptonic CP violating effective action for Dirac and Majorana neutrinos |
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| Polyakov loop in various representations in the confined phase of QCD |
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| Excited hadrons, heavy quarks and qcd thermodynamics |
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| Odd-parity dynamically generated baryon resonances with beauty flavor |
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| Strangeness and charm in nuclear matter |
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| Heavy-quark spin symmetry for charmed and strange baryon resonances |
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| Charmed Mesons in Nuclei with Heavy-Quark Spin Symmetry |
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| Low-lying even parity meson resonances and spin-flavor symmetry revisited |
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| The perturbative scalar massless propagator in Schwarzschild spacetime |
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| Hidden charm N and Delta resonances with heavy-quark symmetry |
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| Odd parity bottom-flavored baryon resonances |
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| The hadron resonance gas model: Thermodynamics of QCD and Polyakov loop |
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| Polyakov loop and the hadron resonance gas model |
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| Charmed and strange baryon resonances with heavy-quark spin symmetry |
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| Statistical consistency of quantum-classical hybrids |
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| D- mesic atoms |
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| Derivative expansion of the heat kernel at finite temperature |
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| Odd-parity light baryon resonances |
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| Trace anomaly and dimension two gluon condensate above the phase transition |
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| Leading order one-loop CP and P violating effective action in the Standard Model |
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| Low-lying even-parity meson resonances and spin-flavor symmetry |
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| Correlations between perturbation theory and power corrections in QCD at zero and finite temperature |
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| Exotic dynamically generated baryons with negative charm quantum number |
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| Charmed baryon resonances with heavy-quark symmetry |
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| Trace anomaly, thermal power corrections, and dimension two condensates in the deconfined phase |
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| CP violation in the effective action of the Standard Model |
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| Direct construction of the effective action of chiral gauge fermions in the anomalous sector |
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| s-wave charmed baryon resonances from a coupled-channel approach with heavy quark symmetry |
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| Phase space localization of antisymmetric functions |
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| The powers of deconfinement |
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| The invariant factor of the chiral determinant |
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| χ-SU(3) bethe salpeter model: Extension to SU(6) and SU(8) spin-flavor symmetries |
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| Derivative expansion of the heat kernel in curved space |
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| The existence of positive representations for complex weights |
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| Power corrections in the quark-antiquark potential at finite temperature |
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| Information-theoretic measures of hyperspherical harmonic |
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| Meson-baryon s-wave resonances with strangeness -3 |
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| Dimension-2 condensates and Polyakov Chiral Quark Models |
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| Large- N weinberg-tomozawa interaction and spin-flavor symmetry |
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| Resonances and the Weinberg-Tomozawa 56-baryon-35-meson interaction |
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| Comment on "A quantum-classical bracket that satisfies the Jacobi identity" [J. Chem. Phys. 124, 201104 (2006)] |
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| The method of covariant symbols in curved space-time |
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| Chiral Lagrangian at finite temperature from the Polyakov-chiral quark model |
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| Polyakov loop in chiral quark models at finite temperature |
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| Large Nc Weinberg-Tomozawa interaction and negative parity s-wave baryon resonances |
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| SU(6) extension of the Weinberg-Tomozawa meson-baryon Lagrangian |
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| Dimension two condensates and the Polyakov loop above the deconfinement phase transition |
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| Energy momentum tensor of chiral quark models at low energies |
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| Covariant derivative expansion of the heat kernel |
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| Low-energy chiral Lagrangian from the spectral quark model |
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| Thermal heat kernel expansion and the one-loop effective action of QCD at finite temperature |
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| Comment on "Quantum backreaction through the Bohmian particle" (multiple letters) |
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| The Polyakov loop and the heat kernel expansion at finite temperature |
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| Comment on “Quantum Backreaction through the Bohmian Particle |
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| On the cascade approach to the quantum multiscattering problem |
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| The induced Chern-Simons term at finite temperature |
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| Derivative expansion for the effective action of chiral gauge fermions. The abnormal parity component |
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| Derivative expansion for the effective action of chiral gauge fermions. The normal parity component |
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| Gauge invariant derivative expansion of the effective action at finite temperature and density and the scalar field in [Formula Presented] dimensions |
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| On the uniqueness of the expected stress-energy tensor in renormalizable field theories |
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| Impediments to mixing classical and quantum dynamics |
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| Parity breaking in 2 + 1 dimensions and finite temperature |
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| Chiral and scale anomalies of non local Dirac operators |
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| Non-mesonic weak decay of Λ hypernuclei |
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| Temperature dependence of the anomalous effective action of fermions in two and four dimensions |
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| Non-mesonic weak decay of Lambda hypernuclei |
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| Feynman diagrams with the effective action |
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| Minimum Uncertainty for Antisymmetric Wave Functions |
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| Elimination of the vacuum instability for finite nuclei in the relativistic [Formula Presented]-[Formula Presented] model |
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| Representation of complex probabilities |
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| Absence of classical and quantum mixing |
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| Wigner transformation for the determinant of Dirac operators |
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| Semiclassical treatment of the Dirac sea contribution for finite nuclei |
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| Semiclassical expansions up to ℏ<sup>4</sup>-order in relativistic nuclear physics |
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| Two nucleon induced Λ decay and the neutron to proton induced ratio |
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| Chiral anomaly and nucleon properties in the Nambu-Jona-Lasinio model with vector mesons |
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| Short-range correlations in the pion s-wave self-energy of pionic atoms |
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| A REVIEW ON MESONIC DECAY OF LAMBDA-HYPERNUCLEI |
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| Two nucleon induced decay and the neutron to proton induced ratio |
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| The low energy expansion of the Nambu-Jona-Lasinio model with vector mesons in the anomalous sector |
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| SEMICLASSICAL EXPANSION FOR DIRAC HAMILTONIANS |
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| Sixth order derivative expansion of one-loop effective actions |
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| Spurious solutions of the complex Langevin equation |
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| Inclusive (γ, π) reactions in nuclei |
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| Response functions for infinite fermion systems with velocity dependent interactions |
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| New Improvements for Mie Scattering Calculations |
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| Mean field solution of QCD<inf>2</inf> in the large-N limit |
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| Pion-nucleus elastic scattering in a local approximation to the delta-hole model |
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| Decay modes of sigma and lambda hypernuclei |
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| Calculation of the first-order s-wave optical potential in pionic atoms |
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| INCLUSIVE PION-NUCLEUS DOUBLE CHARGE-EXCHANGE |
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| COMPUTER-SIMULATION OF INCLUSIVE PION NUCLEAR-REACTIONS |
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| Experimental test of three-body pion absorption |
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| S-wave optical potential in pionic atoms |
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| DELTA SELF-ENERGY IN NUCLEAR-MATTER |
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| A decay in nuclei |
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| Effect of nuclear correlations on the Λ decay width in nuclei |
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| A THEORETICAL APPROACH TO PION NUCLEAR-REACTIONS IN THE RESONANCE REGION |
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| Mesonic and non-mesonic Λ-decay in nuclei |
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| Error sources in the standard numerical integration of the Schrödinger equation: An improved method |
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