-
Notifications
You must be signed in to change notification settings - Fork 0
Expand file tree
/
Copy pathdthesis.out
More file actions
45 lines (45 loc) · 3.43 KB
/
dthesis.out
File metadata and controls
45 lines (45 loc) · 3.43 KB
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
\BOOKMARK [0][-]{chapter.1}{Introduction}{}% 1
\BOOKMARK [0][-]{chapter.2}{Nuclear excitations}{}% 2
\BOOKMARK [1][-]{section.2.1}{Collective excitations}{chapter.2}% 3
\BOOKMARK [1][-]{section.2.2}{Noncollective excitations}{chapter.2}% 4
\BOOKMARK [0][-]{chapter.3}{Coupled-channels method}{}% 5
\BOOKMARK [1][-]{section.3.1}{Coupled-channels equations}{chapter.3}% 6
\BOOKMARK [1][-]{section.3.2}{Iso-centrifugal approximation}{chapter.3}% 7
\BOOKMARK [1][-]{section.3.3}{Sudden tunneling limit}{chapter.3}% 8
\BOOKMARK [1][-]{section.3.4}{Barrier distribution method}{chapter.3}% 9
\BOOKMARK [1][-]{section.3.5}{Constant coupling approximation}{chapter.3}% 10
\BOOKMARK [1][-]{section.3.6}{Coupling to collective states}{chapter.3}% 11
\BOOKMARK [2][-]{subsection.3.6.1}{Vibrational coupling}{section.3.6}% 12
\BOOKMARK [2][-]{subsection.3.6.2}{Rotational coupling}{section.3.6}% 13
\BOOKMARK [2][-]{subsection.3.6.3}{Adiabatic potential renormalization}{section.3.6}% 14
\BOOKMARK [1][-]{section.3.7}{Full order coupling}{chapter.3}% 15
\BOOKMARK [0][-]{chapter.4}{Random matrix theory}{}% 16
\BOOKMARK [1][-]{section.4.1}{Introduction}{chapter.4}% 17
\BOOKMARK [1][-]{section.4.2}{Gaussian orthogonal ensemble\(GOE\)}{chapter.4}% 18
\BOOKMARK [1][-]{section.4.3}{Properties of GOE}{chapter.4}% 19
\BOOKMARK [1][-]{section.4.4}{Fluctuation measures of GOE}{chapter.4}% 20
\BOOKMARK [1][-]{section.4.5}{Random matrix theory for deep inelastic collision}{chapter.4}% 21
\BOOKMARK [0][-]{chapter.5}{Noncollective excitations in 16O + 208Pb reaction}{}% 22
\BOOKMARK [1][-]{section.5.1}{Current status of 16O + 208Pb reaction}{chapter.5}% 23
\BOOKMARK [1][-]{section.5.2}{Results}{chapter.5}% 24
\BOOKMARK [2][-]{subsection.5.2.1}{Single phonon calculation}{section.5.2}% 25
\BOOKMARK [2][-]{subsection.5.2.2}{Double phonon calculation}{section.5.2}% 26
\BOOKMARK [2][-]{subsection.5.2.3}{Anharmonicity of octupole phonon state in 208Pb}{section.5.2}% 27
\BOOKMARK [2][-]{subsection.5.2.4}{Q-value distribution}{section.5.2}% 28
\BOOKMARK [2][-]{subsection.5.2.5}{Mass-number dependence of the effect of noncollective excitations}{section.5.2}% 29
\BOOKMARK [0][-]{chapter.6}{Noncollective excitations in 20Ne + 90,92Zr reaction}{}% 30
\BOOKMARK [1][-]{section.6.1}{Quasi-elastic scattering for 20Ne + 90,92Zr systems}{chapter.6}% 31
\BOOKMARK [1][-]{section.6.2}{Random matrix model}{chapter.6}% 32
\BOOKMARK [1][-]{section.6.3}{Level density and strength distribution}{chapter.6}% 33
\BOOKMARK [1][-]{section.6.4}{Test of random matrix model with 16O + 208Pb reaction}{chapter.6}% 34
\BOOKMARK [1][-]{section.6.5}{Application to 20Ne + 90,92Zr systems}{chapter.6}% 35
\BOOKMARK [2][-]{subsection.6.5.1}{Parameters}{section.6.5}% 36
\BOOKMARK [2][-]{subsection.6.5.2}{Results}{section.6.5}% 37
\BOOKMARK [1][-]{section.6.6}{Prediction for 24Mg + 90,92Zr reaction}{chapter.6}% 38
\BOOKMARK [0][-]{chapter.7}{Summary and concluding remarks}{}% 39
\BOOKMARK [0][-]{appendix.A}{Classical expression for fusion cross section and the Wong formula}{}% 40
\BOOKMARK [0][-]{appendix.B}{Role of noncollective excitations in one-dimensional barrier penetration problem}{}% 41
\BOOKMARK [1][-]{section.B.1}{Random matrix model for one-dimensional coupled-channels equations}{appendix.B}% 42
\BOOKMARK [1][-]{section.B.2}{Results}{appendix.B}% 43
\BOOKMARK [0][-]{appendix.C}{Calculation of gaussian orthogonal ensemble\(GOE\)}{}% 44
\BOOKMARK [0][-]{appendix.D}{Interplay of collective and noncollective excitations}{}% 45