Alpha-particle emission from the deep-inelastic reaction 1354 MeV <span class="aps-inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><mmultiscripts><mrow><mi mathvariant="normal">Ho</mi></mrow><mprescripts></mprescripts><mrow></mrow><mrow><mn>165</mn></mrow><mrow></mrow><mrow></mrow></mmultiscripts></mrow></math></span>+<span class="aps-inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><mmultiscripts><mrow><mi mathvariant="normal">Ta</mi></mrow><mprescripts></mprescripts><mrow></mrow><mrow><mn>181</mn></mrow><mrow></mrow><mrow></mrow></mmultiscripts></mrow></math></span>

L. G. Sobotka; R. J. McDonald; G. J. Wozniak; D. J. Morrissey; A. J. Pacheco; L. G. Moretto

doi:10.1103/PhysRevC.25.1693

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Alpha-particle emission from the deep-inelastic reaction 1354 MeV ${}^{165}{Ho}$ + ${}^{181}{Ta}$

L. G. Sobotka, R. J. McDonald, G. J. Wozniak, D. J. Morrissey, A. J. Pacheco, and L. G. Moretto

Phys. Rev. C 25, 1693(R) – Published 1 March 1982

Abstract

The in-plane correlation between projectilelike fragments and $α$ particles has been studied over a broad range of angles for the system 1354 MeV ${}^{165}{Ho}$ + ${}^{181}{Ta}$ . These data unambiguously indicate that the dominant sources of $α$ particles are the fully accelerated fragments.

NUCLEAR REACTIONS ${}^{181}{Ta}$ ( ${}^{165}{Ho}$ , $x$ ), $E = 1354$ MeV, measured $σ (E_{α}, θ)$ .

Received 8 October 1981

DOI:https://doi.org/10.1103/PhysRevC.25.1693

Authors & Affiliations

L. G. Sobotka, R. J. McDonald, G. J. Wozniak, D. J. Morrissey, A. J. Pacheco, and L. G. Moretto

Nuclear Science Division, Lawrence Berkeley Laboratory, University of California, Berkeley, California 94720

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Vol. 25, Iss. 3 — March 1982

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