ATOMIC AND NUCLEAR PHYSICS PLEASE ANSWER ALL QUESTIONS Let us consider that the two particles interact via an attractive square well potential, i.e -Uo TSR V(r)= 0 r> R, where R = 1.2 fm(4/³+A), with A1 and A2, the particles' atomic masses. For the s-wave state (= 0), the above equation has the following form Csin(Kr) T≤R to(k,r) == sin(kr +80) r> R₁ where C is a normalization constant, K² = √(k+Uo), and do the scattering phase shift. Using the continuity of the wave function and its derivative at r= R, i.e Csin(KR) = sin(kR+ 8), d dR Csin(KR) = sin(kR+60), d dR (a) show that the phase phift is given by

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14
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Α Α΄
B-B-S ## T
AaBbCcDc AaBbCcDc AaBbC AaBbCc AaBl AaBbCcl
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트플
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Heading 2
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··2·1·1·1···1·1·2·1·3·1·4·1·5· 1 · 6 · 1 · 7 · 1 · 8 · 1 · 9 · 1 · 10 · |··11· |·12·|·13°||·14° | ・15° |-·\\ · |·17· |-•· 18 · |
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ATOMIC AND NUCLEAR PHYSICS
PLEASE ANSWER ALL QUESTIONS
Let us consider that the two particles interact via an attractive square well potential, i.e
-Uo
r≤R
V(r) =
{
0
r> R,
1/3
where R = 1.2 fm(4/³ + A/³), with A₁ and A2, the particles' atomic masses. For the s-wave state
(l=0), the above equation has the following form
uo(k,r):
Csin(Kr)
sin(kr + 8)
T≤R
r> R,
where C is a normalization constant, K² = √(k+Uo), and do the scattering phase shift. Using
the continuity of the wave function and its derivative at r = R, i.e
d
Csin(KR) = sin(kR+ 5),
d
dR
-Csin(KR)=
dR sin(kR+60),
(a) show that the phase phift is given by
tan d =
k tan(KR) - K tan(kR)
K+ k tan(kR) tan(KR)
(b) Calculate the phase shift 6 for 160+208 Pb reaction at an incident energy E = 20.0 MeV, consider
Uo 102.0 MeV.
Calibri (Body)
BIU
I U abe X₂ X²
Mailings
Aal
Aa
יד
Ef
Find
A
Час Replace
Change
Styles Select
G
Editing
R 90% Ⓒ
@?
E
OG
Transcribed Image Text:| W 07:37 PM 2022-05-24 W File 70 Paste 14+1+13+1+12+|+11·10 ·9·1·8·1·7·1·6·1·5·1·4·1·3·1·2·1·1····1·1·20 Home Insert Cut Copy Format Painter Clipboard Page: 1 of 1 Words: 8 Document1 - Microsoft Word (Product Activation Failed) Page Layout References Review View T 14 T Α Α΄ B-B-S ## T AaBbCcDc AaBbCcDc AaBbC AaBbCc AaBl AaBbCcl abe X, X² A ab T 트플 1 Normal No Spaci... Heading 1 Heading 2 Title Subtitle Font Paragraph G Styles ··2·1·1·1···1·1·2·1·3·1·4·1·5· 1 · 6 · 1 · 7 · 1 · 8 · 1 · 9 · 1 · 10 · |··11· |·12·|·13°||·14° | ・15° |-·\\ · |·17· |-•· 18 · | I I I I I ATOMIC AND NUCLEAR PHYSICS PLEASE ANSWER ALL QUESTIONS Let us consider that the two particles interact via an attractive square well potential, i.e -Uo r≤R V(r) = { 0 r> R, 1/3 where R = 1.2 fm(4/³ + A/³), with A₁ and A2, the particles' atomic masses. For the s-wave state (l=0), the above equation has the following form uo(k,r): Csin(Kr) sin(kr + 8) T≤R r> R, where C is a normalization constant, K² = √(k+Uo), and do the scattering phase shift. Using the continuity of the wave function and its derivative at r = R, i.e d Csin(KR) = sin(kR+ 5), d dR -Csin(KR)= dR sin(kR+60), (a) show that the phase phift is given by tan d = k tan(KR) - K tan(kR) K+ k tan(kR) tan(KR) (b) Calculate the phase shift 6 for 160+208 Pb reaction at an incident energy E = 20.0 MeV, consider Uo 102.0 MeV. Calibri (Body) BIU I U abe X₂ X² Mailings Aal Aa יד Ef Find A Час Replace Change Styles Select G Editing R 90% Ⓒ @? E OG
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