RAQUEL
MOLINA PERALTA
CONTRATADO/A DOCTOR/A
George Washington University
Washington, Estados UnidosPublicaciones en colaboración con investigadores/as de George Washington University (21)
2021
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The πf(500) decay of the a1(1260)
European Physical Journal C, Vol. 81, Núm. 9
2018
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Chiral Extrapolations of the ρ(770) Meson in Nf = 2 + 1 Lattice QCD Simulations
EPJ Web of Conferences
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Extraction of isoscalar ππ phase shifts from lattice QCD
Physical Review D, Vol. 98, Núm. 1
2017
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Chiral extrapolations of the ρ (770) meson in Nf=2+1 lattice QCD simulations
Physical Review D, Vol. 96, Núm. 3
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Model selection for Pion photoproduction
Proceedings of Science
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Model selection for pion photoproduction
Physical Review C, Vol. 95, Núm. 1
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On the chiral covariant approach to ρρ scattering
Chinese Physics C, Vol. 41, Núm. 12
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Phenomenology of baryon resonances
Proceedings of Science
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Role of the strange quark in the ρ (770) meson
EPJ Web of Conferences
2016
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Determination of the compositeness of resonances from decays: The case of the Bs0 →j /ψf1 (1285)
Physical Review D, Vol. 93, Núm. 11
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Evolution of the K N - π 'system with M π 2 in a box from UχPT
AIP Conference Proceedings
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Pole structure of the Λ (1405) in a recent QCD simulation
Physical Review D, Vol. 94, Núm. 5
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Production of X (4160), y (3940) and Z (3930) in the B 0 → K ∗ 0 X (Y Z) and B s 0 → i X (Y Z) decays
AIP Conference Proceedings
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Resonance Extraction from the Finite Volume
PROCEEDINGS OF THE 10TH INTERNATIONAL WORKSHOP ON THE PHYSICS OF EXCITED NUCLEONS (NSTAR2015)
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Rho resonance parameters from lattice QCD
Physical Review D, Vol. 94, Núm. 3
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Two-Flavor Simulations of ρ (770) and the Role of the K K - Channel
Physical Review Letters, Vol. 117, Núm. 12
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Two-flavor simulations of the ρ(770) and the role of the KK̄ channel
Proceedings of Science
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Weak decays of heavy hadrons into dynamically generated resonances
International Journal of Modern Physics E, Vol. 25, Núm. 1
2015
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Evolution of the KN -πΣ system with M2π in a box from UΧPT
Proceedings of Science
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Predictions for the B0→ K*0X(YZ) and B0s→ øX(YZ) with X(4160), Y(3940), Z(3930)
European Physical Journal A, Vol. 51, Núm. 5