−
2.6 The folding equation (HF+RT) (1.104) using the CDM3Y3 interaction with the elastic expansion 16O 12C to Elab = 200 MeV (the connecting line) is compared with the expansion of the HF component (the connecting line), the folding equation (HF+RT) is calibrated with the constant NR = 0.99 (the connecting line).
(see Table 2.2) . . 63
2.7 Above: The elastic recoil release rate of I Elab = 200 MeV [7] in the OM cavity with three folding modes (1.104) as shown in Figure 2.6, OP Eo section
−
as shown in Table 2.1. Below: Elastic and correct reinforcement helps form the Far-side reinforcement 16O 12C corresponding to different Eo reinforcement strengths. A1 priority and reverse
Airy's base was followed by the role of the Eagle. 64
−
2.8 The elastic recoil stress of 16O 12C to Elab = 170, and 181 MeV [7, 17, 18] in the OM cavity with the iron oxide was experimentally tested using the folding (HF+RT) and the
The WS is given by Table 2.2 (the internal joint). The Far-side reinforcement for the test sections W0 is given by the different Eo (the joint and the domed line), Ak is the pole.
Airy class 65
−
2.9 Similar to Figure 2.8, but for elastic 16O 12C
tI Elab = 230, 260, and 281 MeV [7, 17, 18]. 67
−
2.10 Similar to Figure 2.8, but for elastic bucket 16O 12C
tI Elab = 300, 330, and 608 MeV [18, 19, 76]. 68
2.11 The elastic and inelastic buckling (inter-core) buckling rates for a 12C-excited rod with an energy of Elab = 240 MeV by the CC method. The calculated results are compared with experimental results [12, 13]. The dot-dm, dot-dm, and dot-dm-dm curves are the equivalent buckling rates with the sub-supports K = 2, 0, and -2. The dot-dm curves are the Far-side buckling rates for the elastic buckling (2.2) and
elastic (2.6). 75
2.12 Similar to Figure 2.11 but for elastic and non-elastic forces.
elastic 16O−12C tI Elab = 200 MeV [7, 29]. 76
2.13 The calculation of CC is similar to Figure 2.12 but with elastic and non-elastic coefficients of the test method.
W → W0/3 78
2.14 Calculations of CC for the first batch of activated carbon
2
0+ (above) and 3−1 (below) based on 12C on the canopy
xXO 16O−12C tI Elab = 200 MeV. 80
v
en
−
3.1 The OM for the elastic 16O 12C Elab = 100, 115.9 MeV [20] with the combination of folding and WS equations is given in Table 3.1 (internal link).
Far-side beam deflection is given for calculating OM with different W0 supports (joint line)
and the line), Ak is the real Airy target. 85
−
3.2 The OM equation for the elastic 16O 12C electron beam Elab = 124, 132 MeV [16, 20] with the combination of folding and WS equations is given in Table 3.1 (internal link).
Far-side beam deflection is given for calculating OM with different W0 supports (joint line)
and the line), Ak is the real Airy target. 86
−
3.3 The OM model for elastic reinforcement 16O 12C tI Elab =
115.9 MeV [20] is given by the experimental method to match the experimental results.
OP mechanism (internal link). In the folding process, the Eo molecule consists of a volumetric flask and a particle size distribution. Different expressions of the fraction are used to determine the composition of the fraction.
Near-side pig elbow when changing tea basket to support milk aW87
−
3.4 Elastic displacement spectroscopy for 16O 12C with Elab = 100, 115.9 and 124.0 MeV [20] using the CRC method. Elastic displacement spectroscopy (dotted line) yields the OP calculation as shown in Table 3.1. Elastic displacement spectroscopy (dot line)
Let's calculate CRC with tea basket for practical purposes.
≈
Sα 1.96 93
3.5 Similar to Figure 3.4 but for elastic reinforcement
−
16O 12C tI Elab = 132 [7, 16] and 300 MeV [19]. Coherence school
Elab = 300 MeV, OP is given by Table 2.2 94
−
3.6 Two-channel CRC equations (inter-channel) for elastic recoil doses Elab = 115.9 MeV [20] and 132 MeV [7, 16]. The elastic recoil equation (3.6) for the 16O 12C system is decomposed into a Near-side component (inter-channel) and a Far-side component (inter-channel).
side(joint line) by Fuller method [71]. 96
−
3.7 Elastic force 16O 12C measured by Elab =
115.9 MeV [20] and 132 MeV [7, 16], using OP aligned with L
as shown in Figures 3.1 and 3.2 (dotted lines) and OP is added.
The coefficient of L according to the formula (3.10) (internal line) 97
en
−
3.8 The S-matrix's magnetic elements are given for the 16O 12C 132 MeV elastic mass OM calculation using the OP (linear) and the derivative (inter-linear) L calculation and the S-matrix's magnetic elements are given for the calculation.
Two-channel CRC (hyphenated line). 99
−
3.9 The Majorana neutron star was calculated using the multi-layer (conjugated) method for a 16O 12C to 132 MeV elastic mass [97]. This neutron star was compared with the
The Majorana is also like this (3.10). 100
−
3.10 The 10-channel reaction profile (5 channels of the upper edge and 5 channels of the lower edge) is taken into account in the CRC analysis of the 16O 12C elastic bucket, including the wood.
direct and indirect α-transfer processes. 102
−
3.11 New channel CRC calculations for elastic 16O 12C irradiation with Elab = 100 and 115.9 MeV [20] (internal path). These results are compared with the CC calculations for elastic 16O 12C irradiation, through the α-transition (root-channel path) or the two-channel direct CRC calculations (channel-channel path) and the four-channel direct and indirect CRC calculations through the α-transition (root-channel path).
1
2+ core 12C (joint line). 105
3.12 Similar to Figure 3.11 but for the bucket with a bucket-shaped opening.
The measured elasticities are Elab = 132 MeV [7, 16] and 300 MeV [19]. . 106
−
−
3.13 The new CRC channel (inter-channel) based on the 16O 12C elastic band was measured at Elab = 115.9 and 124 MeV [20]. The 16O 12C elastic band (3.6) is decomposed into Near-side and Far-side components.
Fuller's method [71]. 109
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Side List
1.1 The parameters c and a and ρ0 are the two-parameter Fermi distribution function for a nuclear fusion furnace with a base price
rms
Rr.ms tea is comparable to Rex
practice
is a quadrilateral electron transport [50]. 35
≈
1.2 The parameters of the CDM3Yn interaction function F0(ρ) (1.96) and the corresponding correction function ∆F0(ρ) (1.102) are given by the corresponding coefficients. The core K obtained in the HF calculation of the symmetric core K is the coefficient of the CDM3Yn interaction function ρ0
0.17 fm−3 43
−
−
2.1 The WS parameters of the OP are determined by fitting experimental data to the 12C elastic mass at energies Elab = 139.5 360 MeV. NR is the standard coefficient of the folding reaction using the CDM3Y3 interaction, JV and JW are respectively the volume integrals of the reaction and the OP Eo reaction, σR is
the sound of the wind. 57
−
−
2.2 The WS parameters of the OP are determined by fitting experimental data to the 16O 12C elastic mass flow at energies Elab = 170 608 MeV. NR is the standard coefficient of the folding reaction using the CDM3Y3 interaction, JV and JW are respectively the volume integrals of the reaction and the OP's Eo reaction, σR is
the sound of the wind. 66
1
2.3 The OP parameters used in the CC calculation are the elastic and inelastic coefficients of the 2+12C mechanism. These parameters are experimentally adapted to JV and JW respectively.
Volumetric analysis of food and fertilizers OP 74
− −
3.1 Parameters for fitting OP theory in OM analysis of elastic 16O 12C Elab = 100 132
MeV. NR is the standard constant of the folding method used.
CDM3Y3, JV and JW interactions are volume integrals.
OP and σR are the displacements of the reaction vessels. . 84
ix
x
−
3.2 The coefficient of the elastic coefficient of the two-channel analysis of the elastic coefficient of the 160 12C transition, the tea basket obtained was compared with the previous analysis of the DWBA and CRC analyses for the 12C transition.
(16O,12C)16O. 95
3.3 Tea baskets Sα are used in the CRC analysis, including the direct and indirect α transfer process through the base and the base size 16O. These tea baskets are obtained according to the SM calculation[40]. The ratio quantities N and angular moments L correspond to
The α+12C configuration is given by the Wildermuth equation (3.3). 102
→
1
3.4 The reaction constant Saα is predicted for different axial models for the 16O α+12C atom, in which the 12C core is located in the base metal and the 2+ excitation is 4.44 MeV. The constant
−
The Saα coefficient used in the CRC calculation analyzes this 16O 12C elastic mass (final value) obtained in the calculation.
SM math [40]. 104
− −
3.5 The OP parameters according to expression (2.13) are used in the analysis of the new channel CRC (including direct and indirect α-transfer) with the elastic coefficient 16O 12C tI Elab = 100 300
MeV. 107
x
xi
xii
List of symbols, typefaces
Sign,
pencil
English | Vietnamese | |
AMD | Antisymmetric Molecular Dynamics | Percentage distribution ratio contrast |
BHF | Brueckner-Hartree-Fock | Brueckner-Hartree-Fock |
BM | Bohr-Mottelson | Bohr-Mottelson |
CC | Coupled Channel | Cross-channel |
CM | Center of Mass | Block |
CRC | Coupled Reaction Channel | Contact us |
DDM3Y | Density Dependent M3Y interaction | M3Y Interaction tired |
DPP | Dynamic Polarization Potential | The main part |
DWBA | Distorted Waves Born Approximation | XĐp x¿ Born gun mo |
el. | elastic | flock |
Exp. | Experiment | Practice |
HF | Hartree-Fock | Hartree-Fock |
HvH | Hugenholtz van Hove | Hugenholtz van Hove |
ine | inelastic | Non-elastic |
lab | laboratory | paradox |
NN | Nucleon-Nucleon | Nucleon-Nucleon |
OCM | Orthogonality Condition Model | The witch is a model of direct communication. |
BRAISED | Optical Modelxii | Arc light |
OP | Optical Potential | Lake of Light |
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RGM
Resonating Group Method | The witch looked at the crowd. | |
rms | root mean square | square root |
RT | Rearrangement Term | Number of garlic cloves |
SM | Shell Model | Color |
VLHN | Core physics | |
WS | Woods-Saxon | Woods-Saxon |
xiii