1997
DOI: 10.1039/a702244a
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Multiply bridged organodiantimony(V) compounds; crystal structures of [(SbR2)2(μ-O)2(μ -O2AsMe2)2] (R = Ph or p-tolyl) and [(SbR3)2(μ-O)(μ-O2 MR′2)2] (R = Ph, M = P, R′ = Me; R = Ph, M = As, R′ = Me or Ph; R = p-tolyl, M = P, R′ = Me)

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Cited by 24 publications
(10 citation statements)
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“…There is a range of SNe II models available in the literature. In the present situation, there are large differences in the predicted yields since there is a wide variety of input physics (e.g., criterion for convection, reaction rates, and the way to initiate the shock wave) (Aufderheide et al 1991;Gibson et al 1997).…”
Section: Models Of Sne Ia and Sne IImentioning
confidence: 97%
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“…There is a range of SNe II models available in the literature. In the present situation, there are large differences in the predicted yields since there is a wide variety of input physics (e.g., criterion for convection, reaction rates, and the way to initiate the shock wave) (Aufderheide et al 1991;Gibson et al 1997).…”
Section: Models Of Sne Ia and Sne IImentioning
confidence: 97%
“…The bounds for SNe II progenitors are taken to be m l = 10M ⊙ and m u = 50M ⊙ , respectively, and an IMF slope x = 1.35 (Salpeter 1955) is adopted throughout. While this slope is of prime importance for arguments concerning the absolute mass of elements in the ICM (e.g., , it is less so for abundance ratios (Gibson et al 1997).…”
Section: Models Of Sne Ia and Sne IImentioning
confidence: 99%
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