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The Weak Production of Hypernuclei. D.D. van Niekerk (M.Sc. project) B.I.S. van der Ventel G.C. Hillhouse Department of Physics Stellenbosch University South Africa. Stellenbosch, South Africa. Outline. Motivation Our Model Formalism The Hadronic Vertex Kinematics - PowerPoint PPT Presentation
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The Weak Production of Hypernuclei
D.D. van Niekerk (M.Sc. project)B.I.S. van der VentelG.C. Hillhouse
Department of PhysicsStellenbosch UniversitySouth Africa
Stellenbosch, South Africa
Outline
Motivation
Our Model
Formalism
The Hadronic Vertex
Kinematics
The Transition Matrix
Leptonic Tensor
Hadronic Tensor
Constructing Wµ (Example)
Conclusion
Motivation Recent large scale interest in astrophysics and the role of neutrinos in
stellar processes (i.e. supernovae)
Neutrino osscillations (changing of flavour) BooNE / MiniBooNE (Fermilab)
J-PARC Super-Kamiokande (50 GeV)
Nucleon decay postulated by supersymmetry
Hyperon and hypernuclei production form important part of neutrino-
induced reaction cross sections
0
p K
n K
Our Model Based on relativistic Dirac equation
never been studied (nuclear process)
first attempt in a fully relativistic framework
Quasifree process (interaction takes place between neutrino and
single bound nucleon)
Bound state wave functions are calculated using relativistic mean
field formalism
Aim:
Obtain quantitive results that will give indication of nuclear
model uncertainties
Provide theoretical basis for interpretation of experimental
results
Types of Reactions: Charged Current (CC)
(S = strangeness)
ΔS = 0
ΔS = 1
Neutral Current
ΔS = 0
ΔS = 1 not observed
0n K
n K n
0 0n K
Y12 12ν + C + K + C
Formalism
Neutral Current (NC) Charged Current (CC)
1K( )p
( )P
( )P
( )X q
( )k
( ')k
0X Z X W
Modelling the Hadronic Vertex
Quasifree Region
Use form factors ( )p
( )X q
1meson ( )p
( )P
( )P
( )X q
1meson ( )pboundhyperon
boundnucleon
2( )p
( )p
Vertex
Approximation
K is kinematic factor determined from normalisation of flux etc.
First order diagram:
Lμν contains projectile information
Wμν contains nuclear information
(4) 3 3 3 21 1( ' ' ') ' ' ' | |d K k P k p P d p d P d k M
2 μνμν| M | L W
Kinematics CC
In CC reactions we can detect the outgoing muon.
1
1'1
32 2 2' '4
' 1'
2( )
i roots 'of ( )
1( )
(cos ') 2 2
1| |
| '( ) |p
k p kk
ip
f E
dE E M
dE d d
Mf E
Kinematics NC
In NC reactions we cannot detect the outgoing neutrino.
' max
' min
1
1'1
( ) 12
' '41' ( ) 1
2 2 2' ( )
i roots 'of ( )
1(cos ')
2 2
1( ) | |
| '( ) |
.k
k
p
E
k k
E
p k ip
f E
ddE d E
d
E M Mf E
Transition Matrix Element
Leptonic Current Parity not conserved
Left-handed neutrinos
Propagator Vector Boson (W+ or Z0)
Coupling strengths follow from GSW Theory (ηl and ηh)
5(1 )l
( ') ( ) ( )l f h iiM u k l k iD q K J
2boson
gD
M
2 2| | FM G L W
Leptonic Tensor Lepton spinor
normalised as
helicity representation
Neutrino: m = 0 and h = -1
Feynman trace techniques and identities of the gamma
matrices can be used to simplify the expression for Lμν
2
h
k
kh
k
kE m
u k h kE kE m
† 1u u
5 5( ') (1 ) ( ) ( ') (1 ) ( ) *
' ' ' '
S A
L u k k u k k
N k k k k k k g i k k
L L
Hadronic Tensor
The hadronic tensor is expanded in a basis consisting of the
independent four-momenta, the metric tensor and the Levi-Civita tensor
(
μν μν μ ν μ ν μ ν μ ν μ ν1 2 3 4 5
μ ν μ ν μ ν μ ν6 7
μ ν μ ν μ ν μ ν8 9
μ ν μ ν μναβ μναβ μναβ10 11 α β 12 α β 13 α β
μν μνS A
W =W g +W q q +W P P +W p' p' +W q P + P q
+W q p' + p' q +W P p' + p' P
+W q P - P q +W q p' - p' q
+W P p' - p' P +W ε q P +W ε q p' +W ε P p'
=W +W
( )
( ) )
( ) ( )
( )
1meson ( )p
( )P
( )P
( )X q
This expansion is model independent
The Wi expansion coefficients are the structure functions
Extract Wi:g W W
q q W X W
1
2
11
2
W g W
W X q q W
done once
The contraction of hadronic and leptonic tensors is done considering symmetric and anti-symmetric contractions separately
General equation Model is needed for guidance
2 2
21 3
| | ( ) ( )
' ( ') ( )
F S A
F
M G L W L W
G W k k W
Construction of hµ
Born Term Model (s,t and u channels)
Propagators: spin ½
spin 0
Vertices: Strong coupling (baryon-baryon-meson) in s,t,u channels
Coupling constant
Weak coupling (meson-meson) in t channel Phenomenological meson form factorsMecklenberg W., Acta Physica Austriaca 48, 293 (1976)
Weak coupling (baryon-baryon) in s,u channel Form factors
Weak Current Operator
μ μ μν μWK 1 2 ν A 5
iJ = f γ + f σ q - g γ γ
2m
p m
p m
2 2
2 2
1
p - m
*,N Ym m
W h h
+1K ( )p
12 ( )C P
12* ( )C P
( )X q
0K
nW
0K
K
n
0
W
W
np
0
K
s
t
u
12 - + 12ν + C μ + K + C
d np
- 0 +ν + n μ + Λ + KElementary process:
s-channel
neutron-proton vertex
1μ μ μνCC V 1 2 ν +2
ip J + n = p j + ij n = u' γ + σ q τ u
2mf f( )
Form Factors
0n
K W
p
- 0 +ν + n μ + Λ + K
CVC relates weak vector form factors to isovector form factors
of EM current
EM isovector current
Axial form factor determined phenomenologically
(p) (nμ μ) (p) (n)1 1 2 2
μν 3EM ν
τiN' J N = u' γ + σ q u
2mF - F F -
2F
(p) (n)1 1 1
(p) (n)2 2 2
f = F - F
f = F - F
-22Dipole
A,CC A A2A
qg = g 1 - = 1.26 G
m
Total (for s-channel)
s d cosμ1 2 A
μ μν μn Λ C ,Cν C 5f f
ih = p θ γ + σ q - γ
2m
p×
g γ
+ - 5 n2 2 K p
+ mG γ
p -m
(p) (n)1 1 1
(p) (n)2 2 2
DipoleA,CC A
f = F - F
f = F - F
g = 1.26 G
u-channel
Vertex:
Weak current i.t.o. SU(3) octet currents
μ μ μ μ μ μ μ μ μCC 1 2 1 2 c 4 5 4 5 c
ΔS=0 ΔS=1
J = V ± iV - A ± iA θ + V ± iV - A ± iA θ ( ) ( ) cos ( ) ( ) sin
0ˆ ( ) ?CCJ
n
0 K
W
- 0 +ν + n μ + Λ + K
where
and λi = 3X3 generators of SU(3) γμ = 4X4 Dirac matrices
μ μ μ μ μ μ μ μ μCC 1 2 1 2 c 4 5 4 5 c
ΔS=0 ΔS=1
J = V ± iV - A ± iA θ + V ± iV - A ± iA θ ( ) ( ) cos ( ) ( ) sin
u x
q x = d x
s x
( )
( ) ( )
( )
μ μi i
μ μi i 5
iV = q x λ γ q x
2i
A = q x λ γ γ q x2
( ) ( )
( ) ( )
EM current
For Oj any octet current operator
For EM current
Comparison yields
μ μ μEM 3 8
1J =V + V
3
( ) ( ) ( ) ( )i j k ijk i k ijk i kB O B = if U B FU B + d U B DU B
ˆ
ˆ
D D1
μ μ μνEM ν
μ μ μνE
2
D DF
M νF1 2
1 2
2 in J n = - D = u' γ + σ q u
3 2m
D ip J p
2- F F3
F FF + F +
3= F + = u' γ + σ
3q u
3 2m
D (n)1 1
D (n)2 2
3F = - F
23
F = - F2
F (p) (n)1 1 1
F (p) (n)2 2 2
1F = F + F
21
F = F + F2
For weak current
Belongs to same octet as EM current
Axial form factor From s-channel
F μ F μν F μ1 2 ν 5
D μ D μν D μ1 2 ν 5
iF = f γ + f σ q - g γ γ
2mi
D = f γ + f σ q - g γ γ2m
D,F D,F1,2 1,2f = F
ˆ F D1 1 A,C
μ μ μCC A C5 5p J + n = u' γ γ u = u' γ γg + g g u( )
(0) (0)D F D F Dipole1 1 1 1 Ag + g = g + g G
u-channel weak baryon-baryon vertex:
propagator:
strong baryon-baryon-meson vertex:
ˆ ( )
1
20 μ - D μ D μν D μ
CC Λ 1 2 ν 1 5 Σ
2 iΛ J + Σ = f γ + f σ q - g γ γ
3 2m
+ - 5K nΣG γ
p2 2
+ m
p -m
- 0 +ν + n μ + Λ + K
n
0 K
W
Total (for u-channel)
u d cos D
1
2μ μ μν μ
n Λ C ν 5D D
1 2 1
2 ih = p θ γf f g+ σ q - γ γ
3 2m
p
+ - 5 n2 2 K nΣ
+ mG γ
p -m
D (n)1 1
D (n)2 2
D D1 1 A,CC
3f = - F
23
f = - F2
g = g (0)g
Summary(4) 3 3 3 2
1 1( ' ' ') ' ' ' | |d K k P k p P d p d P d k M
2 2
21 3
| | ( ) ( )
' ( ') ( )
F S A
F
M G L W L W
G W k k W
11
2
W g W
W X q q W
s t u
*
+h h h h
W h h
Conclusion We are constructing a relativistic model for the
description of weak hypernuclei production of relevance
to experiments at Fermilab (BooNE) and J-PARC
Hadronic tensor parametrised in model independent way
to facilitate different hadronic models through structure
functions
Code written in Fortran 95 and Mathematica. In process
of obtaining results: We are investigating the relation between the structure
functions Wi and the kaon scattering angle as well as
dependence of Wi on the momentum transfer
Calculate the cross sectionemail: [email protected]