Seminar: Statistical Decay of Complex Systems (Nuclei)
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Transcript Seminar: Statistical Decay of Complex Systems (Nuclei)
FermiGasy
Addition of Angular Momenta
Angular momenta L1, L2 , direction undetermined
Projections conserved :m1, m2 , m m1 m2 L1 L2 L L1 L2
(t )
1 const.
2 const.
1(t ), 2(t ) L(t ), (t ), (t )
2
i (t ) i Larmor frequency
2
L L(t ) Classical Probability :
Angular Momentum Coupling
2
P(L) L t
1
2
2L L t
1
L2 m2 L21 sin2 1 L22 sin2 2
1
L1L2 sin 1 sin 2 cos(1 2 )
If (L1) (L2 ) dipole interaction : L1 couples with L2 L
Coherent motion : m conserved, const. (t ) L L(t )
W. Udo Schröder, 2005
At large r
1 2 r1 r2
3
decoupling
Angular Momentum Coupling
Quantal angular momentum eigen states j1 j2 ??
j
j
ˆ
J12 , ˆ
J1z : 1 ; ˆ
J22 , ˆ
J2 z : 2
m1
m2
3
Max alignment :
j1
j2
j1
j2
dim (2 j1 1)(2 j2 1) dimensionality
:
j1
j2
j1
j2
ˆ
2 j1
J
j1
j2
j2
??
??
j1
j2
j1
j2
2
Angular Momentum Coupling
Use ˆ
J 2 ˆ
J1 ˆ
J2 ˆ
J12 ˆ
J22 2ˆ
J1 ˆ
J2 ˆ
J12 ˆ
J22 ˆ
J1 ˆ
J2 ˆ
J1 ˆ
J2 2ˆ
J1z ˆ
J2 z
ˆ
2 j1
J
j1
j2
j2
2
j1( j1 1)
2
( j1 j2 )( j1 j2 1)
J
ˆ
Jz
j1
j2
j1
j2
W. Udo Schröder, 2005
j2 ( j2 1) 0 0 2 j1 j2
( j1 j2 )
J 1
j1
j2
j1
j2
j1
j2
j1
j2
m
2
j1
j2
j1
j2
j1
j2
j1
j2
J( J 1)
j1
j2
j1
j2
The first
ˆ
J2, ˆ
Jz
eigen state
Constructing J Eigen States
J , for example
Construct m J spectrum successively by applying ˆ
ˆ
J
j1
j2
j1
j2
J j1 j2
4
J2
J1 ˆ
ˆ
m J 1
2 j1
j1
j2
j1
j2
j1
j2
j1 1
j2
2 j1
+ 2 j2
j1
j2
j1 1
j2
2 j2
j1
j2
j1
j2 1
j1
j2
eigen state
j1
j2 1
J j1 j2 , m J 1
Can you show this??
This is one specific linear combination of 2 states j1 , m1 and
j2 , m2
Angular Momentum Coupling
What about the other ? There should be 2 orthogonal combinations.
And : Further application of ˆ
J yields again only one specific linear
combination of 3 independent components
J j1 j2
m J 2
j1
j2
j1 2
j2
+
j1
j2
j1 1
j2 1
+
j1
j2
j1
j2 2
What about others ? There should be 3 orthogonal combinations.
W. Udo Schröder, 2005
Constructing J-1 Eigen States
We have this state:
J j1 j2
2 j1
m J 1
j1
j2
j1 1
j2
+ 2 j2
j1
j2
eigen state
j1
j2 1
J j1 j2 , m J 1
Two basis states j1 , m1 , j2 , m2 2 new orthogonal states
5
J ??
m J 1
2 j1
j1
j2
j1 1
j2
- 2 j2
j1
j2
j1
j2 1
Angular Momentum Coupling
Apply ˆ
J2 ˆ
J12 ˆ
J22 ˆ
J1 ˆ
J2 ˆ
J1 ˆ
J2 2 ˆ
J1z ˆ
J2 z
Use
ˆ
J1
j1
j2
m1
m2
J j1 j2 1
m J
2 j1
j1
j2
j1 1
j2
- 2 j2
ˆ
J
to
m1 j1 m1 1
j1
is orthogonal
j1
j2
m1
m2
j1
j2
j1
j2 1
j1
j2
j1
j2
etc.
eigen state
J j1 j2 1 ...etc.
m J
Condon-Shortley
Normalization conditions leave open phase factors choose
asymmetrically <|J1z|> ≥ 0 and <a|J2z|b> ≤ 0
W. Udo Schröder, 2005
Clebsch-Gordan Coefficients
General scheme : Unitary transformation (between bases)
j1
j2 j j1
m
m1 , m2 m1 m2 m m1
j2
j
6
j
m
j1
m1 , m2
m1
j2 j1
m2 m1
m2
j1
m1 , m2 m1
j
m2 m
j2
m1 , m2
j j1
m2 m m1
j2
j1
j2
j1
m1
m2
m1
j2
m2
j2
j
m2 m
ˆ
Representations of identity operator 1
j1 j2 :
Angular Momentum Coupling
m1 , m2
j1
j2
j1
j2
m1
m2
m1
m2
ˆ
1
j1 j2
j,m
j
j
m
m
ˆ
1
j1 j2
Orthogonality relations of CG coefficients :
j j1
m1 , m2 m m1
j2 j1
m2 m1
j
m2 m
j2
m1 ,m2
j2
j j1
m m1 m2
j1
j2
j
m1 m2 m
j j mm
=1
j1
j , m m1
W. Udo Schröder, 2005
j2 j j j1
m2 m m m1
j2
j1
m2 j,m m1
j2 j
m2 m
j1
j2
m m1
m2
j
=1
m1 m1 m2 m2
Recursion Relations
j2 j1
j2 j
j1
j2
j1
j2
j
m1 m2
m
m
m1 , m2 m1 m2 m1 m2 m
m1 , m2 m1 m2
j1
j2
j1
j2
j
j
j
j
ˆ
ˆ
J
J
m1 m2 m - 1 m - 1
m
m
m1 , m2 m1 m2
j1
j
7
ˆ
P
j , m 1
j
m-1
ˆ
J
j
m
m1 , m2
j1
m1
j2
j1
j2
m2 m 1 m1
m2
j
Angular Momentum Coupling
j m j m 1
ˆ
J1- + ˆ
J2-
m
j
m1 , m2
j1
m1
j2
j
m2 m
j1
m1 - 1
ˆ
J1
j1
m1
j1
j2
m1 - 1 m2
j1 m1 j1 m1 1
C jm :
j m j m 1
W. Udo Schröder, 2005
m1 , m2
j1
m1
j2
j
m2 m
j2
m2 - 1
ˆ
J2
j2
j1
j2
m2
m1
m2 - 1
j2 m2 j2 m2 1
Recursion Relations for CG Coefficients
C jm
j1
m1
8
j1
j2
m2 m 1 m1
m2
j
j1
C j1m1 1
j2
j
j1
j2
m1 1 m2 m
m1
m2
j m j m 1
C jm :
j1
C j2m2 1
m1
j2
j
j1
j2
m2 1 m
m1
m2
j2
j
Projecting on <j1,j2,m1,m2| yields
C jm
Angular Momentum Coupling
j2
j1
j2
m1
j
m2 m 1
C j1m1 1
j1
j2
j
m1 1 m2 m
C j2m2 1
j1
m1 m2 1 m
Using ˆ
J ˆ
J1 ˆ
J2
C jm 1
j1
m1
j2
j
m2 m 1
C j1m1
j1
j2
j
m1 1 m2 m
C j2m2
j1
j2
j
m1 m2 1 m
Special values :
j 0 j
1
m 0 m
W. Udo Schröder, 2005
j1 j1 0 (1) j1 m1
m
m
2 j1 1
1 0
1
0
0
???
Symmetries of CG Coefficients
Coupling depends on sequence ˆ
J1 , ˆ
J2
9
Phase convention : non diag. ˆ
J1z 0, ˆ
J2 z 0
j1 j2 j
j j j
(1) 1 2
m1 m2 m
j2 j1 j
m
m
2 1 m
Angular Momentum Coupling
j1 j2 j3
j3 j1
j2 m2 2 j3 1 j2
(1)
m
m
m
m
m
m
2
j
1
3
2
1
1
1 2 3
j1 j2 j3
j1 j2
j1 m1 2 j3 1 j3
(1)
m
m
m
m
m
m
2
j
1
1
2
2
1 2 3
3
j1 j2 j3
j j j
(1) 1 2 3
m1 m2 m3
m(m3 ) m1 m2
Triangular relation
Condon-Shortley :
Matrix elements of
J1z and J2z have
different signs
j1 j2
j3
m
m
m
3
1
2
Calculate CGs starting from max alignment : m j
Then use recursion relations to obtain all
W. Udo Schröder, 2005
j, m j
Explicit Expressions
A. R. Edmonds, Angular Momentum in Quantum Mechanics
j1 j2 j
m, m1 m2
m
m
m
1 2
10
12
2 j 1 j1 j2 j !( j1 m1 )!( j2 m2 )!( j m)!( j m)!
j
j
j
1
!
j
j
j
!
j
j
j
!(
j
m
)!(
j
m
)!
1
2
1
2
1
2
1
1
2
2
j m
( j1 m1 s)!( j2 j m1 s)!
s j m
1 1 1
s !( j1 m1 s)!( j m s)!( j2 j m1 s)!
s 0
Angular Momentum Coupling
12
j1 j2 j1 j2 2 j1 ! 2 j2 ! j1 j2 m1 m2 ! j1 j2 m1 m2 !
m
m
m
m
2
j
2
j
!
j
m
!
j
m
!
j
m
!
j
m
!
2
1
2
1
1
1
1
2
2
2
2
1 2 1
j1 j2
j
j1 m j1 m
12
2 j 1 ! 2 j1 ! j1 j2 j ! j1 j2 m !( j m)!
j
j
j
!
j
j
j
!
j
j
j
1
!
j
j
m
!
j
m
!
2
1
2
1
2
1
2
1
W. Udo Schröder, 2005
2 Particles in j Shell (jj-Coupling)
Look for 2-part. wfs of lowest energy in same j-shell, Vpair(r1,r2) < 0
spatially symmetric jj1(r) = jj2(r). Construct consistent spin wf.
J
11
JM j j
M
j j 0 J j j 2j
j j J
JM (r1, r2 ) N
jm1 (r1 ) jm2 (r2 ) jm2 (r1 ) jm1 (r2 )
m1, m2 m1 m2 M
N = normalization factor
Angular Momentum Coupling
Which J = j1+j2 (and M) are allowed? antisymmetric WF JM
j1 j2 j
j j j
Use Pauli Principle and
(1) 1 2
m1 m2 m
j2 j1 j
for 12 : 1 2
m
m
m
2 1
j j J j j J
JM (r1 , r2 ) N
jm1 (r1 ) jm2 (r2 )
m
m
m
m
m1 , m2
1 2 M 2 1 M
W. Udo Schröder, 2005
j j J
N 1 (1)2 j J
(r )
(r )
m , m m m M jm1 1 jm2 2 For j1 j2 5 2
2
1 2 1
2 j1 j 5 j odd
N 12
j 0, 2, 4
Symmetry of 2-Particle WFs in jj Coupling
Antisymmetric function of 2 equivalent nucleons (2 neutrons or 2
protons) in j shell in jj coupling.
12
JM (r1 , r2 )
j j J
jm1 (r1 ) jm2 (r2 )
m1, m2 m1 m2 M
J even
1) j1 = j2 = j half-integer spins J =even
wave functions with even 2-p. spin J are antisymmetric
Angular Momentum Coupling
wave functions with odd 2-p. spin J are symmetric
jj coupling LS coupling equivalent statements
2) l1=l2=l integer orbital angular momenta L
wave functions with even 2-p. L are spatially symmetric
wave functions with odd 2-p. L are spatially antisymmetric
W. Udo Schröder, 2005
Tensor and Scalar Products
Tensor product of sets of tensors T k1 and T k2
k
T
k
k1 k2 k k1
k1
k2
k
T (1) T (2)
T (1)T 2 (2)
2
1,2 1 2 1
13
Scalar product of sets of tensors T k (1) and T k (2) number
T00
k
k k 0 k
(
1)
k
T (1) T (2)
T (1)T (2)
Tk (1)Tk (2)
0 0
2k 1
k
k
0
Angular Momentum Coupling
Vectors u and v : Rank k 1 2k 1 3 spherical components
Spin 0 scalar product
1 ux iuy
u v 0
3
2
1
u v
3
0
W. Udo Schröder, 2005
v x iv y ux iuy v x iv y
uz v z
2
2
2
Transforms like a J=0 object = number
Example: HF Interaction
14
Addition Theorem of spherical harmonics :
P cos
4
*
Ym (1 , 1 )Ym (2 , 2 )
2 1m
1
4
4
Y m (2 , 2 )
Ym* (1 , 1 )
2 1
2 1
m
m
r1 , r2
Electron nucleus (sum over p) hyperfine interactions
Angular Momentum Coupling
ˆ
H
int
i , p,
ei ep
ri
1
1
m
m,
rp P (
ri rp
ri rp
)
4
4
*
ep rpYm ( p , p )
ei ri
p 2 1
i 2 1
0
Tp Ti scalar product of separated tensors
0
protons electrons
only
only
W. Udo Schröder, 2005
Y m ( i , i )
1
Wigner’s 3j Symbols
Coupling j1 j2 j3 equivalent to symmetric j1 j2 j3 0
j2
15
j1
j3
j2
j1
j3
j1 j2 j3 j3 j3 0 (1) j3 m3
j3 m1 m2 m3 m3 m3 0
2 j3 1
j1 j2 j3
m
m
m
3
1 2
Angular Momentum Coupling
Choose additional arbitrary phase factor for 3 j symbol
j1 j2 j3 (1) j1 j2 m3
2 j3 1
m1 m2 m3
j1 j2 j3
m
m
m
3
1 2
j1 j2 j3 j3 j1 j2 j2 j3 j1
all cyclic
m1 m2 m3 m3 m1 m2 m2 m3 m1
j1 j2 j3
j1 j2 j3
(
1)
m
m
m
1 2 3
W. Udo Schröder, 2005
j2 j1 j3
any 2 columns
m2 m1 m3
Explicit Formulas
16
j1 j2 j3 j1 j2 j3
1
j3 j3 m3m3
2 j3 1
m1 , m2 m1 m2 m3 m1 m2 m3
j1 j2 j3 j1 j2 j3
2
j
1
3
m m m m m m m1m1 m2m2
j3 , m3
1 2 3 1 2 3
Explicit (Racah 1942):
Angular Momentum Coupling
j1 j2 j3
j1 j2 m3
1
m1 m2 m3 , 0
m1 m2 m3
j1
j2 j3 ! j1 j2 j3 ! j1 j2 j3 !
j1 j2 j3 !
j1 m1 ! j1 m1 ! j2 m2 ! j2 m2 ! j3 m3 ! j3 m3 !
1 z ! j1 j2 j3 z ! j1 m1 z ! j2 m2 z !
z
z
All factorials must be ≥ 0
W. Udo Schröder, 2005
j3 j2 m1 z ! j3 j1 m2 z !
1
Spherical Tensors and Reduced Matrix Elements
Spherical tensor of rank j 2 j 1 operators Tmj (m j,...., j )
j ' transforming like angular momentum ops.
Tmj Dmj ' m , , T m
m'
17
Tmj transfers angular
momentum to I 0 state
,
I 0
M 0
Tmj
:
,
0
0
,
j
m
, , = Qu. #
characterizing
states
In general LC of basis states
Angular Momentum Coupling
Tmj
,
,
j2
m2
j1
m1
Tmj
, j3 , m3
,
j1
m1
N
j j1 j3
m m1 m3
, j3 , m3
N
,
j3
N
m3
j j1 j3
m m1 m3
,
j2
m2
,
degeneracy
not due to m3
j3
m3
N
W. Udo Schröder, 2005
j2
m2
Tmj ,
j1
m1
N
m3
j j1 j2
m m1 m2
Wigner-Eckart Theorem
,
,
j3
j j1 j2
dyn geometry
m m1 m2
Wigner-Eckart Theorem
,
j2
m2
Tmj
18
,
,
j2
m2
j1
m1
Tmj
j j1 j2
N
m m1 m2
,
j1
m1
(1) j2 m2
j j1 j2
j
j2 T j1
m m1 m2
Angular Momentum Coupling
Reduced (double bar ) Matrix Element
j2
j1
j
j2 T j j1 contains all physics.
Conditions for non zero :
3 angular momenta j1 , j, j2
" couple to zero " m2 m1 m
Take the simplest ME to calculate
W. Udo Schröder, 2005
j2 T j j1
Examples for Reduced ME
Example 1 : const. operator 1
19
,
j2
m2
1 ,
j1
m1
j1 j2 m1m2
0 j1 j1
j2 1 j1
m
m
0
1
1
j1 j1 0 (1) j1 m1
Remember
2 j1 1
m1 m1 0
Angular Momentum Coupling
(1) j1 m1
j2 1 j1 2 j1 1 j1 j2
Example 2 : Vector operator ˆ
J ˆ
J
,
j2
m2
Jz ,
j1
m1
m1 j1 j2 m1m2
j 1 j1
Look up 1
m1 0 m1
W. Udo Schröder, 2005
ˆ
J
use
ˆ
Jz
ˆ
Jz
simplest
(1) j1 m1
j1 1 j1
j2 J j1
m
m
10 1
(1) j1 m1 m1
j1 j1 1 2 j1 2
j2 J j1
j1 j1 1 2 j1 2 j1 j2
Reduced MEs of Spherical Harmonics
2
m2
YML
1
m1
L 1 2
(1) 2 m2
m
m
M
1
2
2
YL
1
*
L
d Ym2 ( , ) YM ( , )Ym11( , )
20
2
(2
YML ( , )Ym1 ( , )
Angular Momentum Coupling
1
,
2
Y
L
1
1
1)(2L 1)(2 1) 1 L 1 L *
Y ( , )
4
m1 M 0 0 0
( ) Y ( , )
(1)
2
(2
1
1)(2
2
2 L 1
1)
0
0
0
Important for the calculation of gamma and particle transition probabilities
W. Udo Schröder, 2005
Isospin
Charge independence of nuclear forces neutron and proton states
of similar WF symmetry have same energy n, p = nucleons
Choose a specific representation in abstract isospin space:
Angular Momentum Coupling
21
1
Proton : 1 2
0
0
Neutron : 1 2
1
0 1
0 i
1 0
Isospin matrices SU(2) 1
;
;
2
3
1
0
i
0
0
1
1
Nucleon charge q 1 3
2
1
Isospin operators tˆi : i (i 1,2,3) analog to spin
2
tˆi , tˆj i tˆk (cyclic i, j, k ) spherical tensor (vector ) tˆ1 : tˆ (tˆ1 itˆ2 ), tˆ3
Transforms in isospin space like angular momentum in coordinate space
use angular momentum formalism for isospin coupling.
W. Udo Schröder, 2005
2-Particle Isospin Coupling
22
Use spin/angular momentum formalism: t (2t+1) iso-projections
t1
t2
mt1
mt 2
:
t1
t2
mt1
mt 2
Total isospin states T , MT
Iso antisymmetric :
0
Angular Momentum Coupling
can couple to t1 t2 T t1 t2
1
T 1, MT 0
0
W. Udo Schröder, 2005
1
0
mt 2
1(singlet ) state
(MT 1, 0,1)
MT
1
t2
1 2 (1)1 2 (2) 1 2 (2)1 2 (1)
2
T 1
1
MT
t1 t2 T t1
mt 1 , mt 2 mt 1 mt 2 MT mt1
1
0
Iso symmetric :
1
MT 0
0
T 0, MT 0
0
T 1, MT 1
1
T 0
T
3(triplet ) states
1
1 2 (1)1 2 (2) T 1, MT 1
1
1
1
1
1 2 (1) 1 2 (2) 1 2 (2) 1 2 (1)
2
1 2 (1)1 2 (2)
2-Particle Spin-Isospin Coupling
Both nucleons in j shell lowest E states have even J T=1 !
For odd J total isospin T = 0
23
JM,TMT
T J
1
j1 j2 J
J T
j1m1 (1) j2m2 (2) (1) j1m1 (2) j2m2 (1)T ,MT
2 m1,m2 m1 m2 M
1
J 0 T 1
Angular Momentum Coupling
j1 j2 j 1
j2 JM ,T 1MT
j j 0
jm (1) j m (2) jm (2) j m (1)T 1,MT
m1 , m2 m m 0
3 states (MT=-1,0,+1) are degenerate, if
what should be true (nn, np forces are same)
ˆ, Tˆ 0
H
Different MT states belong to different nuclei T3 = (N-Z)/2
W. Udo Schröder, 2005
MT 1, 0,1
Angular Momentum Coupling
24
2-Particle Isobaric Analog (Isospin Multiplet) States
Corresponding
T=1levels in A=14
nuclei
T3=+
1
2n
W. Udo Schröder, 2005
T3=-1
2n holes
T3=0, pn
W. Udo Schröder, 2005
Angular Momentum Coupling
25
Separation of Variables: HF Interaction
26
Addition Theorem of spherical harmonics :
P cos
4
*
Ym (1 , 1 )Ym (2 , 2 )
2 1m
1
4
4
Y m (2 , 2 )
Ym* (1 , 1 )
2 1
2 1
m
m
r1 , r2
Electron nucleus (sum over p) hyperfine interactions
Angular Momentum Coupling
ˆ
H
int
i , p,
ei ep
ri
1
1
m
m,
rp P (
ri rp
ri rp
)
4
4
*
ep rpYm ( p , p )
ei ri
p 2 1
i 2 1
0
Tp Ti scalar product of separated tensors
0
protons electrons
only
only
W. Udo Schröder, 2005
Y m ( i , i )
1
Electric Quadrupole Moment of Charge Distributions
z
r arbitrary nuclear charge distribution with norm d3r r Z
1
Coulomb
V (r ) e2 d 3r p* r
p r
interaction
r r
Point
Charge e
r
r r
1
r r
1
27
|e|Z
r r
r r
2
1
r
r 1
2
1 cos
3 cos 1 ...
r
r
r
2
1 r
el
2 P2 (cos ) Q02
r
P (cos )
quadrupole
r 0 r
Nuclear Deform
Quadrupole moment Q T2= Q2 -ME in aligned state m=j
Qz :
j
j
Qz (m)
Q02
j
m
j
j j 2
2
j Q j
j
j j 0
Q02
Qz (m) (1) j m
W. Udo Schröder, 2004
spectroscopic Qz (m j )
j 2 j j 2
j j 2
2
j m j
j
Q
j
Q
(
1)
m
m
m
0
m
m
0
j
j
0
j
2
3m j( j 1)
Q
j(2 j 1)
Look up/calculate
3 j Symbol Qz 0 for j 1
Angular-Momentum Decomposition: Plane Waves
k
r k
z
in z direction : e ikz e ikr cos c mYm ( , )
m
symmetric about z axis c
m
m0
28
r
Plane wave can be decomposed into
spherical elementary waves
Spherical Bessel function
Angular Momentum Coupling
c 0 (r ) 2 d sin Y0 ( ) eikr cos i
0
eikz eikr cos c 0Y0 ( , ) i
4 (2 1) j (kr )
4 (2 1) j (kr ) Y0 ( , )
For arbitrary direction k use Addition Theorem for Ym :
e
ik r
m
i
W. Udo Schröder, 2005
m
4 (2 1) j (kr ) Ym ( r , r )Ym*( k , k )
j (kr )
j-Transfer Through Particle Emission/Absorption
P
29
T
Angular Momentum Coupling
p+T
W. Udo Schröder, 2005
Average Transition Probabilities
Fermi ' s Golden Rule : Pi f
i
Tk
mf
k
T
ji
mi
f (Ef )
If more than 1 initial state may be populated (e.g. diff. m)
average over initial states
30
Angular Momentum Coupling
jf
for one i state and f f states
f
1
P
2 j1 1 mi , mf
jf
mf
1
P
2 j1 1 2k 1
ji
k
T
2
mi
jf T
k
Sum over all components of
ji
Tk
2
ji k jf
1
2 j1 1 mi , mf mi mf
jf T
k
ji
const .
2
= total if Tk transition probability
W. Udo Schröder, 2005
2
2
1
P P
2 ji 1
jf T
k
ji
2
2
W. Udo Schröder, 2005
Angular Momentum Coupling
31
W. Udo Schröder, 2005
Angular Momentum Coupling
32
Translations
cmi m cni m VR n cmi Ei
Vmn
33
n
m 1,2,3
Angular Momentum Coupling
V(r)
V(x)
W. Udo Schröder, 2005
r
x