Excitation of negative parity states (1-, 3-, T = 0) in 16O in inelastic alpha scattering

M. N. Harakeh; J. R. Comfort; A. Van der Woude

doi:10.1016/0370-2693(76)90492-5

Excitation of negative parity states (1^-, 3^-, T = 0) in ¹⁶O in inelastic alpha scattering

M. N. Harakeh, J. R. Comfort, A. Van der Woude

Research output: Contribution to journal › Article

13 Scopus citations

Abstract

The rather strong excitation of the E_x = 7.12 MeV 1^-, T = 0 state in ¹⁶O by inelastic α-particle scattering, which forbidden in the long wavelength approximation, can be explained by a DWBA calculation using a microscopic form-factor generated in the framework of a 1p-1h model with 1hω excitation.

Original language	English (US)
Pages (from-to)	155-158
Number of pages	4
Journal	Physics Letters B
Volume	62
Issue number	2
DOIs	https://doi.org/10.1016/0370-2693(76)90492-5
State	Published - May 24 1976
Externally published	Yes

ASJC Scopus subject areas

Nuclear and High Energy Physics

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Harakeh, M. N., Comfort, J. R., & Van der Woude, A. (1976). Excitation of negative parity states (1^-, 3^-, T = 0) in ¹⁶O in inelastic alpha scattering. Physics Letters B, 62(2), 155-158. https://doi.org/10.1016/0370-2693(76)90492-5

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abstract = "The rather strong excitation of the Ex = 7.12 MeV 1-, T = 0 state in 16O by inelastic α-particle scattering, which forbidden in the long wavelength approximation, can be explained by a DWBA calculation using a microscopic form-factor generated in the framework of a 1p-1h model with 1hω excitation.",

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AU - Harakeh, M. N.

AU - Comfort, J. R.

AU - Van der Woude, A.

PY - 1976/5/24

Y1 - 1976/5/24

N2 - The rather strong excitation of the Ex = 7.12 MeV 1-, T = 0 state in 16O by inelastic α-particle scattering, which forbidden in the long wavelength approximation, can be explained by a DWBA calculation using a microscopic form-factor generated in the framework of a 1p-1h model with 1hω excitation.

AB - The rather strong excitation of the Ex = 7.12 MeV 1-, T = 0 state in 16O by inelastic α-particle scattering, which forbidden in the long wavelength approximation, can be explained by a DWBA calculation using a microscopic form-factor generated in the framework of a 1p-1h model with 1hω excitation.

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