Polyakov loops and finite-size effects of hadron masses in full lattice QCD

Polyakov type loops are responsible for the difference between quenched and unquenched finite size effects on the QCD mass spectrum. With a numerical simulation, using appropriate sea quark spatial boundary conditions, we show that we can align the phases of spatial Polyakov loops in a predelined di...

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Detalles Bibliográficos
Autores: Antonelli, S., Bellacci, M., Fernández Pérez, Luis Antonio, Muñoz Sudupe, Antonio, Ruiz Lorenzo, J. J., Sarno, R., Tarancón, A., Bartoloni, A., Battista, C., Cabibbo, N., Cabasino, S., Panizzi, E., Paolucci, P. S., Todeesco, G. M., Torelli, M., Tripiccione, R., Vicini, P.
Tipo de recurso: artículo
Fecha de publicación:1995
País:España
Institución:Universidad Complutense de Madrid (UCM)
Repositorio:Docta Complutense
Idioma:inglés
OAI Identifier:oai:docta.ucm.es:20.500.14352/60107
Acceso en línea:https://hdl.handle.net/20.500.14352/60107
Access Level:acceso abierto
Palabra clave:53
51-73
Física (Física)
Física-Modelos matemáticos
22 Física
Descripción
Sumario:Polyakov type loops are responsible for the difference between quenched and unquenched finite size effects on the QCD mass spectrum. With a numerical simulation, using appropriate sea quark spatial boundary conditions, we show that we can align the phases of spatial Polyakov loops in a predelined direction. Starting from these results, we propose a procedure to minimize fluctuations due to these effects in meson propagators.

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