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1 | %\subsection{Transition to pre-compound modeling \editor{Johannes Peter}} |
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2 | In simulating light ion reactions, the initial state of the cascade is prepared |
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3 | in the form of two nuclei, as described in the above section on the nuclear |
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4 | model. |
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5 | |
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6 | The lighter of the collision partners is selected to be the projectile. The |
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7 | nucleons in the projectile are then entered, with position and momenta, into |
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8 | the initial state of the cascade. Note that before the first scattering of an |
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9 | individual nucleon, a projectile nucleon's Fermi-momentum is not taken into |
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10 | account in the tracking inside the target nucleus. The nucleon distribution |
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11 | inside the projectile nucleus is taken to be a representative distribution of |
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12 | its nucleons in configuration space, rather than an initial state in the sense |
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13 | of QMD. The Fermi momentum and the local field are taken into account in the |
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14 | calculation of the collision probabilities and final states of the binary |
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15 | collisions. |
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