Energy levels of A = 21–44 nuclei (VII)

Endt, P.M.

doi:10.1016/0375-9474(90)90598-g

Cited by 1,242 publications

(454 citation statements)

References 1,800 publications

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“…Resonances were measured for E R cm \ 17È1937 keV, and the corresponding experimental energies and strengths have been adopted from Endt (1990Endt ( , 1998 and E R cm º 121 references therein. Two threshold states, corresponding to resonance energies of and 95 keV, have been considered.…”

Section: Appendix B Nuclear Physics Inputmentioning

confidence: 99%

“…Resonances were measured for E R cm \ 72È3819 keV. Measured strengths have been adopted from Endt (1990) and Chronidou et al (1999) and were normalized by E R cm º 195 using the absolute uc values of Table 1. The contributions of four threshold states have been taken into account.…”

Section: B4 the 27al( P C)28si Reactionmentioning

confidence: 99%

“…Resonances were measured for keV E R cm \ 52È2929 E R cm \ 483 and the measured strengths, adopted from Endt (1990) and references therein, were normalized by using the absolute uc values listed in Table 1. The contributions of six threshold states have been taken into account.…”

Section: B7 the 30si( P C)31p Reactionmentioning

confidence: 99%

“…First, at very high stellar temperatures, we have frequently adopted the results of Hauser-Feshbach calculations, normalized to our experimental reaction rates. a Endt (1990Endt ( , 1998. b Resonance strength deÐned by equation (16).…”

Section: Introductionmentioning

confidence: 99%

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Proton‐induced Thermonuclear Reaction Rates for A = 20–40 Nuclei

Iliadis

D’Auria

Starrfield

et al. 2001

ASTROPHYS J SUPPL S

284

419

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Proton-induced reaction rates on 26 stable and 29 unstable target nuclei in the mass A \ 20È40 region have been evaluated and compiled. Recommended reaction rates, assuming that all interacting nuclei are in the ground state, are presented in tabular form on a temperature grid in the range T \ 0.01È10.0 GK. Most reaction rates involving stable targets were normalized to a set of measured standard resonance strengths in the sd shell. For the majority of reaction rates, experimental information from transfer reaction studies has been used consistently. Our results are compared with recent statistical model (HauserFeshbach) calculations. Reaction rate uncertainties are presented and amount to several orders of magnitude for many of the reactions. Several of these reaction rates and/or their corresponding uncertainties deviate from results of previous compilations. In most cases, the deviations are explained by the fact that new experimental information became available recently. Examples are given for calculating reaction rates and reverse reaction rates for thermally excited nuclei from the present results. The survey of literature for this review was concluded in 2000 August.

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Section: Appendix B Nuclear Physics Inputmentioning

confidence: 99%

Section: B4 the 27al( P C)28si Reactionmentioning

confidence: 99%

Section: B7 the 30si( P C)31p Reactionmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

See 2 more Smart Citations

Proton‐induced Thermonuclear Reaction Rates for A = 20–40 Nuclei

Iliadis

D’Auria

Starrfield

et al. 2001

ASTROPHYS J SUPPL S

284

419

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“…The value differs from the present SM value by about 3 standard deviations. Whether this is an indication of new physics reflected in new interactions in β-decay, this depends strongly on the β/(β + γ) decay branching ratio for which some 5 measurements exists which in part disagree significantly [ 43] New measurements are needed.…”

Section: Correlations In β-Decaysmentioning

confidence: 99%

Fundamental Symmetries and Interactions

Jungmann

2005

Nuclear Physics A

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In nuclear physics numerous possibilities exist to investigate fundamental symmetries and interactions. In particular, the precise measurements of properties of fundamental fermions, searches for new interactions in β-decays, and violations of discrete symmeties offer possibilities to search for physics beyond standard theory. Precise measurements of fundamental constants can be carried out. Low energy experiments allow to probe New Physics at mass scales far beyond the reach of present accelerators or such planned for the future and at which predicted new particles could be produced directly.

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Doping of Silicon with Phosphorus Using the30Si(p, γ)31P Resonant Nuclear Reaction

Heredia-Ávalos

García-Molina

Abril

et al. 1999

phys. stat. sol. (a)

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We discuss the production of phosphorus atoms in a natural silicon target when it is bombarded with an energetic proton beam, as a consequence of the 30Si(p, γ)31P resonant nuclear reaction. The depth concentration of phosphorus is analysed as a function of proton energy. Our calculation shows that the shape and the location of the phosphorus profile can be accurately described if the proton beam energy is properly controlled.

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Energy levels of A = 21–44 nuclei (VII)

Cited by 1,242 publications

References 1,800 publications

Proton‐induced Thermonuclear Reaction Rates for A = 20–40 Nuclei

Proton‐induced Thermonuclear Reaction Rates for A = 20–40 Nuclei

Fundamental Symmetries and Interactions

Doping of Silicon with Phosphorus Using the30Si(p, γ)31P Resonant Nuclear Reaction

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