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α-<i>d</i>capture with formation of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Li</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>6</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>and the isoscalar<i>E</i>1 multipole

G RyzhikhInstitute for Nuclear Research of the Russian Academy of Sciences, Moscow 117312, RussiaR.A. EramzhyanInstitute for Nuclear Research of the Russian Academy of Sciences, Moscow 117312, RussiaS. ShlomoInstitute for Nuclear Research of the Russian Academy of Sciences, Moscow 117312, Russia
1995lv
ABI

Annotatsiya

We present results of a calculation of the low-energy fusion reaction \ensuremath{\alpha}+d${\ensuremath{\rightarrow}}^{6}$Li+\ensuremath{\gamma}. In this calculation $^{6}\mathrm{Li}$ was treated as a three body \ensuremath{\alpha}-2N system in the framework of the multicluster dynamic model with Pauli projection (MDMP). To construct the $^{6}\mathrm{Li}$ wave function with a high precision a large basis is used for the radial wave function of \ensuremath{\alpha}-2N relative motion in the ground state of $^{6}\mathrm{Li}$. We pay special attention to the asymptotic region of this radial function. We obtained good agreement with experimental data on both angular distribution and total cross section by taking into account the contribution of the isoscalar E1 multipole.

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