Nuclear structure and heavy-ion dynamics: Varenna on Lake Como, Villa Monastero, 27 July-6 August 1982 |
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Page 174
The probability to find the system in the vicinity d»'x(T) around x(T), P(x(T)) &Mx(T
), is equal to the probability to find the system in the phase-space volume dMp(0)
which is mapped onto dMx(T) as the system develops in time. But, since at t = 0 ...
The probability to find the system in the vicinity d»'x(T) around x(T), P(x(T)) &Mx(T
), is equal to the probability to find the system in the phase-space volume dMp(0)
which is mapped onto dMx(T) as the system develops in time. But, since at t = 0 ...
Page 258
This behaviour is seen as an indication that the reactions proceed stepwise with
the same probability of occurrence whether a proton or a neutron is transferred.
In addition, some transfers are energetically less favoured, thus dropping their ...
This behaviour is seen as an indication that the reactions proceed stepwise with
the same probability of occurrence whether a proton or a neutron is transferred.
In addition, some transfers are energetically less favoured, thus dropping their ...
Page 305
For a Markovian system with a short memory time the information about the
fluctuating force is contained fully in the conditional-probability distribution W(p, t;
p + tj, t + A<) which tells us about the probability of finding the system with a
relative ...
For a Markovian system with a short memory time the information about the
fluctuating force is contained fully in the conditional-probability distribution W(p, t;
p + tj, t + A<) which tells us about the probability of finding the system with a
relative ...
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Contents
Introduction | 3 |
Relation with the collective model | 12 |
A Faesslee Competition between collective and singlepar | 30 |
Copyright | |
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Common terms and phrases
a-particle alignment amplitude angle angular distributions angular momentum anisotropy approximation band barrier beam bombarding energy boson calculated Casimir operator classical trajectory coincidence collisions component compound nucleus configuration corresponding Coulomb Coulomb barrier coupling cross-section curve decay deep inelastic deformation degrees of freedom detector dissipation edited effect eigenstates ejectiles emission equations evaporation excitation energy excitation functions exit channel experimental Fermi Fermi surface fermion fission fluctuations fragment spin given Hamiltonian incomplete fusion inertia interaction kinetic energy Lett matrix elements measured momenta neutron neutron emission Nucl nuclear nuclei nucleons observed obtained orbital pairing parameters particles phase space Phys polarization potential probability projectile proton Q-value quadrupole quantum number quasi-particle region residual resonance rotational saddle point scattering shape shell model shown in fig shows single-particle spectra spectrum statistical structure target tion transfer transitions values velocity width y-ray yrast zero