- Page 1: Effects of
- Page 5 and 6: Chapter 1 The elements existing in
- Page 7 and 8: observed the rapid fall-of<
- Page 9 and 10: Figure 1-1 illustrates the compound
- Page 11 and 12: smaller than the extra-extra push e
- Page 13 and 14: fusion and quasi-fission processes
- Page 15 and 16: In the present chapter we have pres
- Page 17 and 18: higher collective velocities to rep
- Page 19 and 20: 2.1 General considerations We want
- Page 21 and 22: couplings. Diabatic basis states ψ
- Page 23 and 24: Chapter 3 The synthesis of<
- Page 25 and 26: is calculated within the TCSM using
- Page 27 and 28: E adiab (MeV) n E diab (MeV) n 30 2
- Page 29 and 30: E diab (MeV) n 60 55 50 45 40 100Mo
- Page 31 and 32: 3-5: Diabatic potentials for the sy
- Page 33 and 34: 3-7: The same as in Fig. 3-6 for th
- Page 35 and 36: The estimated collective velocities
- Page 37 and 38: 3-10: Diabatic contributions as a f
- Page 39 and 40: effects give a justification for th
- Page 41 and 42: The similarity of
- Page 43 and 44: 4.1.3 Alternative microscopical met
- Page 45 and 46: to the DNS concept [18, 34], cross
- Page 47 and 48: U (MeV) 28 27 26 25 24 23 22 21 20
- Page 49 and 50: U (MeV) 35 30 25 20 15 10 90Zr + 12
- Page 51 and 52: 4-1: Fusion barriers B Table TCSM
- Page 53 and 54:
U (MeV) 40 30 20 10 20 10 0 a) b) 9
- Page 55 and 56:
experimental separation energy allo
- Page 57 and 58:
means a neglect of
- Page 59 and 60:
the case of an ind
- Page 61 and 62:
single particle density matrix exte
- Page 63 and 64:
following ratio in the limit <stron
- Page 65 and 66:
5-1: Dependence of
- Page 67 and 68:
the microscopical mass parameter <s
- Page 69 and 70:
5-3: Mass parameter Mεε as a func
- Page 71 and 72:
5-4: Mass parameter Mεε as a func
- Page 73 and 74:
the approximate expressions (Eqs. (
- Page 75 and 76:
(10 3 m fm 2) M , M λλ εε 25 20
- Page 77 and 78:
(10 3 m fm 2) M εε M (10 λλ 4 m
- Page 79 and 80:
~ f k (MeV -1) 0,20 0,15 0,10 0,05
- Page 81 and 82:
V (MeV) 30 25 20 15 10 5 0 -5 -10 1
- Page 83 and 84:
to the dependence of</stron
- Page 85 and 86:
where the lifetime t 0 of</
- Page 87 and 88:
6-2: a) Time-dependent dynamical po
- Page 89 and 90:
Table 6-1: Quasi-fission and inner
- Page 91 and 92:
6-3: Time-dependent average width <
- Page 93 and 94:
Chapter 7 In the quasi-fission proc
- Page 95 and 96:
The value of t0 is
- Page 97 and 98:
Y Z Y A 0,10 0,08 0,06 0,04 0,02 0,
- Page 99 and 100:
estimated from the difference betwe
- Page 101 and 102:
elements from Z=104 to Z=112 in the
- Page 103 and 104:
fission process is an important fac
- Page 105 and 106:
the neck coordinate ε and
- Page 107 and 108:
• The time-dependent transition b
- Page 109 and 110:
Appendix A For describing nucleus-n
- Page 111 and 112:
where The volume is V0 = 1 2 m0ϖ 2
- Page 113 and 114:
ϕ nz(z) = ⎧ ⎪⎨ ⎪⎩ C−1
- Page 115 and 116:
Appendix B The collective response
- Page 117 and 118:
[1] S.G.Nilsson et al., Phys. Lett.
- Page 119 and 120:
[27] N.V.Antonenko et al., in 1 st
- Page 121 and 122:
[63] Yu.F.Smirnov and Yu.M.Tchuvil
- Page 123 and 124:
[97] H. Hofmann et