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2004,Torino Aram Kotzinian 1
Neutrino Scattering
Neutrino interactionsNeutrino-electron scatteringNeutrino-nucleon quasi-elastic scatteringNeutrino-nucleon deep inelastic scattering
VariablesCharged currentQuark content of nucleonsSum rulesNeutral current
2004,Torino Aram Kotzinian 2
NeutrinoNeutrino--electron scatteringelectron scattering−− +→+ ee ee ννTree level Feynman diagrams:
0Z
eν eν
−e−e
−W
eν
eν−e
−e
Effective Hamiltonian:
[ ][ ]{ }eggeGAVee
F ))1(1()1(2 55 γγνγγν µ
µ +−+−=
[ ][ ] [ ][{ }eggeeeGH AVeeeeF
eff )()1()1()1(2 5555 γγνγγννγγγγν µ
µµ
µ −−+−−= ]
(through a Fierz transformation)
2004,Torino Aram Kotzinian 3
Only charged current:
−W
µν
eν−e
−µ
−− +→+ µνν µ ee
( ) )()(2)()( 2 LABinEmepps e µµ νν =+=
( )22 )()( µν µ ppqt −==
( ))(
)()()(
)()()()()(
LABinE
EEpep
ppepy
µ
µ
µ
µ
νµν
νµν −
=⋅
−⋅=
)()(2)( 2
22
22
LABinEmGmq
msGdy
ed eF
W
WFCCµ
µ νππ
νσ≈
−=
−
Inelasticity variable (0<y<1)
2432
10104.0)( cm
MeVEsGe F
CC
×== −−
πνσ µ
(cross-section proportional to energy!)
Total cross-section:
2004,Torino Aram Kotzinian 4
Only neutral current:−
−−
−
+→+ ee µµ νν)()(
0Z
µν)(−
−e
µν)(−
−e
eegeegegge RLAV )1()1()( 555 γγγγγγ µµµ ++−=−
WAVL ggg θ2sin21)(
21
+−=+=
WAVR ggg θ2sin)(21
=−=
−+
+−
−=
−24
22
22
22
)1(sinsin21)(
ymq
msGdy
edWW
Z
ZFNC θθπ
νσ µ
+−
+−
−=
−
WWZ
ZFNC ymq
msGdy
edθθ
πνσ µ 42
22
22
22
sin)1(sin21)(
2004,Torino Aram Kotzinian 5
Only neutral current (total cross-section):
24342
22
101015.0sin
31sin
21)( cm
MeVEsGe WW
FNC
×=
+
+−= −− ν
µ θθπ
νσ
24342
22
101014.0sinsin
21
31)( cm
MeVEsGe WW
FNC
×=
+
+−= −− ν
µ θθπ
νσ
−−
−−
+→+ ee µµ νν)()(
Can obtain value of sin2θWfrom neutrino electron scattering (CHARM II):
0059.00058.02324.0sin2 ±±=Wθ
)1(22 ymE ee −=Θ
2004,Torino Aram Kotzinian 6
Back to (charged and neutral currents)−− +→+ ee ee νν
WWAVL ggg θθ 22 sin211sin
21)11(
21
+=++−=+++=
1WAVR ggg θ2sin))1(1(
2=+−+=
Then: ( )
−+
+=
−24
22
2
1sinsin21)( ysG
dyed
WWFe θθπ
νσ
24342
22
10109.0sin
31sin
21)( cm
MeVEsGe WW
Fe
×=
+
+=⇒ −− νθθ
πνσ
This cross-section is a consequence of the interference of the charged and neutral current diagrams.
2004,Torino Aram Kotzinian 7
Neutrino pair production: eeee νν +→+ −+
Contribution from both W and Z graphs.
W
+e
−e
eν
eνZ
+e−e
eν
eν
Then:
+
+=→−+
41sin2
21
12)(
22
2
WF
eesGee θ
πννσ
Only neutral current contribution to: µµ νν +→+ −+ ee
+
−=→−+
41sin2
21
12)(
22
2
WF sGee θπ
ννσ µµ
2004,Torino Aram Kotzinian 8
NeutrinoNeutrino--electron scattering electron scattering Summary neutrino electron scattering processes:
−− +→+ ee µµ νν
−− +→+ ee µµ νν
−− +→+ ee ee νν
( )
+− WW
F sG θθπ
4222
sin341sin2
4
( )
+− WW
F sG θθπ
4222
sin41sin231
4
( )
+− WW
F sG θθπ
4222
sin341sin2
4
( )
++ WW
F sG θθπ
4222
sin41sin231
4
πsGF
2
++ WW
F sG θθπ
422
sin4sin221
12
+− WW
F sG θθπ
422
sin4sin221
12
Total cross-sectionProcess
−− +→+ ee ee ννee νµν µ +→+ −−
eeee νν +→+ −+
µµ νν +→+ −+ ee
)()(2 frameLABtheinEms e µν=
2004,Torino Aram Kotzinian 9
Neutrino-nucleon quasi-elastic scatteringQuasi-elastic neutrino-nucleon scattering reactions (small q2):
−W
µν
pn
−µ
pn +→+ −µν µ pp +→+−−
µµ νν)()(
np +→+ +µν µ
+W
µν
p n
+µ0Z
µν)(−
p p
µν)(−
== − nHpM eff ,, µνµ
factorformvectorqFV =)( 2
factorformvectoraxialqFA −=)( 2)(975.0cos angleCabbiboC =θ
[ ] ( )[ ]nqFqFpGAV
cF5
225 )()()1(
2cos γγνγγµθ
µµµ +−
2004,Torino Aram Kotzinian 10
Neutrino-nucleon quasi-elastic scattering
028.02573.1)0( ±−== AA gF
Form factors introduced since proton, neutron not elementary. Depend on vector and axial weak charges of the proton and neutron.Two hypotheses:
- Conservation of Vector Current (CVC):- Partial conservation of Axial Current (PCAC):
( )22
2
71.0/1)0()(
qFqF V
V−
= 1)0( =VF
( )22
2
065.1/1)0()(
qFqF A
A−
=
For low energy neutrinos (Eν<<mN):( ) [ ]22
22
)0(3)0(cos)()( AVCF
ee FFEGpn +==πθνσνσ ν
22
42
101075.9 cm
MeVE
×≈ − ν
2004,Torino Aram Kotzinian 11
Inelastic neutrino-nucleon scattering• Parton model is used to make predictions for deep inelastic neutrino-nucleon scattering. • Neutrino beams from pion and kaon decays, dominated by muon neutrinos are used to study this process.
νµ + nucleon → µ+ + Xνµ + nucleon → µ− + X
Since parity is not conserved in weak interactions, there are more structure functions for weak processes, like neutrino scattering, than for electromagnetic processes, like electron scattering.Again the variables x = Q2/2Mν and y = ν /E can be used.
2004,Torino Aram Kotzinian 12
Weak structure functionsGeneral form for the neutrino-nucleon deep inelastic scattering cross-section, neglecting lepton masses and corrections of the order of M/E:
dσν,ν
dxdy=
GF2 MEπ
1− y( )F2νN + y 2xF1
νN m y −y2
2
xF3
νN
The functions F1 , F2 and F3 are the functions of Q2 and ν . In the scaling limit they are the functions of x only.
2004,Torino Aram Kotzinian 13
Scaling behaviour
Compilation of the data on structure functions in deep inelastic neutrino scattering (1983)
2004,Torino Aram Kotzinian 14
Neutrino proton CC scattering:= number of u-quarks in proton between x and x+dx
Some of the quarks are from sea:
For proton (uud):
Xppp +′→+ − )()( µν µ
[ ]∫∫ =−=1
0
1
02)()()( dxxuxudxxuV
Scattering off quarks:
dxxu )(
)()()( xuxuxu SV += )()()( xdxdxd SV +=)()( xuxuS = )()( xdxdS =
[ ]∫∫ =−=1
0
1
01)()()( dxxdxddxxdV
πνσνσ µµ EmG
dyqd
dyqd qFCCCC
22)()(==
( )22
12)()(
yEmG
dyqd
dyqd qFCCCC −==
πνσνσ µµ
( )θcos1211 −=
′−=
EEywith
2004,Torino Aram Kotzinian 15
Scattering off proton:
[ ] [ ]{ }22
)1()()()()(2)(
yxcxuxsxdxMEGdxdy
pd FCC −+++=π
νσ µ
[ ] [ ]{ })()()1()()(2)( 2
2
xsxdyxcxuxMEGdxdy
pd FCC ++−+=π
νσ µ
Structure functions:Callan-Gross relationship: )()(2 21 xFxxF =
[ ])()()()(2)(2 xcxsxuxdxxF p +++=ν
[ ])()()()(2)(3 xcxsxuxdxxxF p −+−=ν
[ ])()()()(2)(2 xsxdxcxuxxF p +++=ν
[ ])()()()(2)(3 xsxdxcxuxxxF p −−+=ν
Neutron (isospin symmetry):[ ])()()()(2)(2 xcxsxdxuxxF n +++=ν
[ ])()()()(2)( xcxsxdxuxxxF n −+−=ν3
2004,Torino Aram Kotzinian 16
Scattering off isoscalar target (equal number neutrons and protons):
csduq +++≡ csduq +++≡
[ ])()()(2 xqxqxxF N +=ν
( )[ ])()(2)()()(3 xcxsxqxqxxxF N −+−=ν
( )[ ])()(2)()()(3 xcxsxqxqxxxF N −−−=ν
{ }22
)1()()()(
yxqxqxMEGdxdy
Nd FCC −+=π
νσ µ
{ })()1)(()( 2
2
xqyxqxMEGdxdy
Nd FCC +−=π
νσ µ
Total cross-section:
GeVcmQQMGEN FCC /1067.0
31/)( 238
2−×=
+=
πνσ µ
GeVcmQQMGEN FCC /1034.0
31/)( 238
2−×=
+=
πνσ µ
2004,Torino Aram Kotzinian 17
2004,Torino Aram Kotzinian 18
Rise of mean q2 with energy
Mean q2 was found to be linear function in neutrino (antineutrino) energy.
2004,Torino Aram Kotzinian 19
Quark content of nucleons from CC cross-sectionsDefine:
Experimental values from y distribution of cross-sections yields:
If
.,)(1
0etcdxxxuU ∫=
03.015.0 ±=+ QQQ
03.000.0 ±=+ QQS
01.016.0 ±=++
QQSQ
)(495.0)()( measured
NNr
CC
CC =≡νσνσ
19.03
13≈
−−
=⇒r
rQQ
33.0≈−= QQQV08.0≈== QQQ SS
49.0)(1
0 2 ≈+=∫ QQdxxF Nν
Quarks and antiquarks carry 49% of proton momentum, valence quarks only 33% and sea quarks only 16%.
2004,Torino Aram Kotzinian 20
Some details
Note that for right-handed incident anti-neutrinos the e term changes sign. Note also that the e term is orthogonal to the asymmetric hadronicterm that is proportional to since q = l – l’ and gives zero when dotted into
where both signs for the last term appear in the literature.
2004,Torino Aram Kotzinian 21
To obtain these expressions we have used
2004,Torino Aram Kotzinian 22
Finally we can put the pieces together to obtain the corresponding cross sections(in the limit )
We recognize this to be similar to the EM result but with replacements, an extra factor of 4 and the (new)
term.
2004,Torino Aram Kotzinian 23
We now consider the scaling limit
Substituting in terms of the scaling variables
we find the result
2004,Torino Aram Kotzinian 24
For scattering on structureless fermions/antifermions (e.g., point particle quarks) we have
Thus measures the difference between quarks and antiquarks.
2004,Torino Aram Kotzinian 25
For elastic neutrino scattering from quark and antiquark we have:
and
Working the details out explicitly in terms of the parton momentum and mass, we find
Thus for pointlike quarks we have
2004,Torino Aram Kotzinian 26
Gross-Llewellyn-Smith (2 names) sum rule
In terms of the parton distributions in the proton we have
Thus we have
and hence