For standard neutrinos, recent solar neutrino results together with the assumption of a nuclear powered Sun imply severe constraints on the individual components of the total neutrino flux: ΦBe≤0.7×109 cm-2 s-1, ΦCNO≤0.6×109 cm-2s-1, and 64×109 cm-2 s- 1≤Φpp+pep≤65×109 cm-2 s-1 (at 1σ level). The bound on ΦBe is in strong disagreement with the standard solar model (SSM) prediction ΦBeSSM5×109 cm-2 s-1. We study a large variety of nonstandard solar models with low inner temperature, finding that the temperature profiles T(m) follow the homology relationship T(m)=kTSSM(m), so that they are specified just by the central temperature Tc. There is no value of TC which can account for all the available experimental results. Even if we only consider the gallium and Kamiokande results, they remain incompatible. Lowering the cross section p+7Be→γ+8B is not a remedy. The shift of the nuclear fusion chain towards the pp-I termination could be induced by a hypothetical low energy resonance in the He3+3He reaction. This mechanism gives a somehow better, but still bad, fit to the combined experimental data. We also discuss what can be learned from new generation experiments, planned for the detection of monochromatic solar neutrinos, about the properties of neutrinos and of the Sun. © 1994 The American Physical Society.
Neutrinos from the Sun: experimental results confronted with solar models
FIORENTINI, Giovanni;RICCI, BarbaraUltimo
1994
Abstract
For standard neutrinos, recent solar neutrino results together with the assumption of a nuclear powered Sun imply severe constraints on the individual components of the total neutrino flux: ΦBe≤0.7×109 cm-2 s-1, ΦCNO≤0.6×109 cm-2s-1, and 64×109 cm-2 s- 1≤Φpp+pep≤65×109 cm-2 s-1 (at 1σ level). The bound on ΦBe is in strong disagreement with the standard solar model (SSM) prediction ΦBeSSM5×109 cm-2 s-1. We study a large variety of nonstandard solar models with low inner temperature, finding that the temperature profiles T(m) follow the homology relationship T(m)=kTSSM(m), so that they are specified just by the central temperature Tc. There is no value of TC which can account for all the available experimental results. Even if we only consider the gallium and Kamiokande results, they remain incompatible. Lowering the cross section p+7Be→γ+8B is not a remedy. The shift of the nuclear fusion chain towards the pp-I termination could be induced by a hypothetical low energy resonance in the He3+3He reaction. This mechanism gives a somehow better, but still bad, fit to the combined experimental data. We also discuss what can be learned from new generation experiments, planned for the detection of monochromatic solar neutrinos, about the properties of neutrinos and of the Sun. © 1994 The American Physical Society.File | Dimensione | Formato | |
---|---|---|---|
PhysRevD.50.4749.pdf
solo gestori archivio
Descrizione: Full text editoriale
Tipologia:
Full text (versione editoriale)
Licenza:
NON PUBBLICO - Accesso privato/ristretto
Dimensione
715.92 kB
Formato
Adobe PDF
|
715.92 kB | Adobe PDF | Visualizza/Apri Richiedi una copia |
9405064.pdf
accesso aperto
Descrizione: Pre-print
Tipologia:
Pre-print
Licenza:
Creative commons
Dimensione
356.01 kB
Formato
Adobe PDF
|
356.01 kB | Adobe PDF | Visualizza/Apri |
I documenti in SFERA sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.