Jim StewartDESY
The HERMES ExperimentThe HERMES Experiment
for the Hermes collaboration
•The HERMES ExperimentThe HERMES Experiment•Inclusive Structure FunctionsInclusive Structure Functions•Measurement of the Quark Helicity DistributionsMeasurement of the Quark Helicity Distributions•Transversity Measurements at HERMESTransversity Measurements at HERMES•Fragmentation FunctionsFragmentation Functions•SummarySummary
J Stewart
Hermes at HERAHermes at HERA
Beam Energy: 27.5 GeV
Electrons and positrons
Beam current
~50mA start of fill
~10mA end of fill
Polarized (<P>~53%)
P~45% now
Beam helicity reversable
Can be set at each expt.
Online measurement of beam Online measurement of beam polarization with two Compton polarization with two Compton polarimeters.polarimeters.
1.8 3.4% B
B
ΔP
P
J Stewart
The HERMES ExperimentThe HERMES Experiment
Fixed target experiment.Fixed target experiment. Polarized internal gas target.Polarized internal gas target. Magnetic spectrometer for Magnetic spectrometer for
momentum measurement.momentum measurement. Relatively large acceptance.Relatively large acceptance. Excellent particle identification.Excellent particle identification.
TargetTarget
J Stewart
The HERMES Polarized TargetThe HERMES Polarized Target
Longitudinal polarized H: <P>= 0.85 ± 0.03 =7.6 x 1013 nucl./cm2
Transverse polarized H: <P>= 0.78 ± 0.04 =1.1 x 1014 nucl./cm2
Long. Polarized D: =2.1 x 1014 nucl./cm2
→ <Pz+>=+0.85 ± 0.03 <Pz->= -0.84 ± 0.03
<Pzz+>= +0.89 ± 0.03 <Pzz->= -1.66 ± 0.05
Unpolarized gases used:
→ H2,D2,He,N2,Ne,Xe
J Stewart
The HERMES SpectrometerThe HERMES Spectrometer
21
175
1.0
2
x y
0.02 x 0.8 at Q GeV and W 2GeV
mrad, 4
Reconstruction :
Kinemati
0 mrad 140 mrad
p = 1.0 - 2.0%
c Ran
p
ge :
mrad
Particle Identification: TRD, Preshower, CalorimeterParticle Identification: TRD, Preshower, Calorimeter
1997: Threshold Cherenkov 1998: RICH + Muon-ID 1997: Threshold Cherenkov 1998: RICH + Muon-ID
J Stewart
hadron/positron separationcombining signals from: TRD, calorimeter, preshower, RICHTRD, calorimeter, preshower, RICH
Aerogel; n=1.03
C4F10; n=1.0014
hadron separationDual radiator RICH for , K, p
Particle IdentificationParticle Identification
K
J Stewart
Semi-Inclusive Deep Inelastic ScatteringSemi-Inclusive Deep Inelastic Scattering
2
lab
2
lab
22
had
(k k )
E
Q
Qx
2ME
z
E
q
The cross section can be expressed as a convolution of a The cross section can be expressed as a convolution of a
distribution function and a fragmentation function.distribution function and a fragmentation function.
ep eh eq eq
q
p qq h~ D FF F
J Stewart
Virtual Photon Asymmetry and DISVirtual Photon Asymmetry and DIS
3/ 2
N
N q
~ q (x)
S S 3/ 2
S S
-1/ 2
N
N q
~ q (x)
S S 1/ 2
S S
+
•Virtual photon can only couple to quarks of opposite helicityVirtual photon can only couple to quarks of opposite helicity
•Select quark helicity by changing target polarization directionSelect quark helicity by changing target polarization direction
•Different targets give sensitivity to different quark flavors Different targets give sensitivity to different quark flavors
,q (x) (x) (x)
( : , , , , , )
f f fq q
f u d s u d s
#$
J Stewart
Cross Section in Deep Inelastic ScatteringCross Section in Deep Inelastic Scattering
L W
2 2
4
d σ E=
dΩdE 2MQ( , , ,) )
E, (
hadronicleptonic
k q s P q S
:L
1 2
1( ) ( )
g
i g
W
g
μ νμν 2 2
Symetric part Spin independent
2 2σ
Asymetric part Spi
1 2
σ σ
n dependent
p p(x,Q ) (x,Q )
qx,Q p q - qp x,QS S
. .
S
+ .
F F
Purely electromagnetic Purely electromagnetic →→ Calculable in QED Calculable in QED
:1 2, F FUnpolarized Structure FunctionsUnpolarized Structure Functions Polarized Structure FunctionsPolarized Structure Functions
1 2, :g gbb11,b,b22,b,b33,b,b4 4 for spin 1 nucleon “Tensor structure functions”for spin 1 nucleon “Tensor structure functions”
Momentum distributionMomentum distribution Helicity distributionHelicity distribution
1 2
1( ) ( )
1
61
2
g
g
W
i g
μ νμν 2 2
2 2σ σ σ
2 2μν μν μν
2 2μν μν μν μ4
1
ν
1 2
3
2
p p(x,Q ) (x,Q )
qS x,Q p qS -S qp x,Q
x,Q r x,Q s + t +u
1x,Q s -u +
b
x,Q s
F
b
b2
F
b - t
J Stewart
Structure Functions and Measured AsymmetriesStructure Functions and Measured Asymmetries
2 2e e 1 f f ff f
1 1F = q x q x q x
2 2 2 2g e e 1 f f ff f
1 1(x) = q x - q x q x
2 2
Momentum distribution of the QuarksMomentum distribution of the Quarks Helicity distribution of the QuarksHelicity distribution of the Quarks
A =
1 2A = D A + A
A =
2 1A = d A A
With D,d,R,With D,d,R, being being kinematic factorskinematic factors
Measurable AsymmetriesMeasurable Asymmetries
21 32 2 1 2
1 32 2
g g
11
AF
1 2g g
2 TL
1T
AF
Virtual Photon AsymmetriesVirtual Photon Asymmetries
J Stewart
World Data on World Data on
b t
1 N L -N LA =
P P N L -N L 1
21
g
2
A1A
F 1+ D
ProtonProton DeuteronDeuteron
Data shown at measured <QData shown at measured <Q22>:0.02-58 GeV>:0.02-58 GeV22
1 1g F
August 2005 J Stewart
Model-independent unfolding detector smearing QED radiative effects
)(
born
)(
born
meas
born
meas
ij
)(N
),(N
N
N
σ
σS
j
ji
radiative effects detector smearing
smearing within acceptance
kinematic migration insideacceptance for each spin state
systematic correlations between bins fully unfolded resulting (small) statistical correlations known
j=0 bin: kinematic migration into the acceptance
J Stewart
World Data on World Data on
Very precise proton dataVery precise proton data The most precise deuteron dataThe most precise deuteron data
The most precise neutron dataThe most precise neutron data
0.021-0.9 measured range:0.021-0.9 measured range:
1g2x (x,Q )
1 1 1p dg g g
3He
1 1 131 12 2
d p ndg g g w
1
1
0.1246 0.0032 0.0074
0.0452 0.0015 0.0017
p
d
g
g
J Stewart
The Structure Function bThe Structure Function b11(x,Q(x,Q22))
2 012
2 1b q
q
e q q q
0
1
1
02 3
2
dzzA
b
F
andand
J Stewart
First measurement of and First measurement of and at small xat small x In measured range (0.002-0.85)In measured range (0.002-0.85)
Qualitative agreement with Qualitative agreement with coherent double-scattering coherent double-scattering modelsmodels
The structure function bThe structure function b11(x,Q(x,Q22))
dzzA d
1bdzzA 0
dzzA 1%d1b 0
2d1 (1.05 0.34 0.35) 10b
hep-ex/0506018
3.2 M DIS events3.2 M DIS events<Pzz+>= +0.89 ± 0.03 <Pzz+>= +0.89 ± 0.03 <Pzz->= -1.66 ± 0.05<Pzz->= -1.66 ± 0.05
J Stewart
Quark PolarizationsQuark Polarizations
2 2 2
1/ 2 3/ 2
2 2
21 2
1/ 2 3/ 2
2 2
2 2
( ,Q ) ( ,Q )~ ~
( ,Q ) ( ,Q
( ) ( ,QA ( ,
)
)
(Q )
( )
) ( ,Q )
( , )
( )
hh hf f
hf f f f f
hq
hf f f f
h h hf f f f
he q x dzD z
e q
e q x dzD z
e q x x dzD z
x
dzD z
q x
q
z
xx
P
1, 1, 1, 1, 1,( ( ), ( ), ( ), ( ), ( ))Kp d p d dA A x A x A x A x A x
, , , , , 0u d u d s s
Qu d u d s s
Correlation between detected hadron Correlation between detected hadron and the struck quark allows and the struck quark allows flavor flavor separationseparation
Linear System in Linear System in Q
QA P
Inclusive DIS Inclusive DIS →→Semi-inclusiveSemi-inclusive →→ , , , ,u u d d s
J Stewart
The Measured Hadron AsymmetriesThe Measured Hadron Asymmetries
DEUTERIUMDEUTERIUM
PROTONPROTON
is an all sea
object and
K us
1,A 0Kd
J Stewart
Polarized Quark DensitiesPolarized Quark Densities
Polarized parallel to the protonPolarized parallel to the proton
q x q x q x #$
u(x) 0
Polarized anti-parallel to the protonPolarized anti-parallel to the proton
d(x)<0
Good agreement with LO-QCD fitGood agreement with LO-QCD fit
u(x) and Δd(x)
u(x) and d(x) ~ 0
s < 0
No indication for No indication for
→0.028 ± 0.033 ± 0.009 In 0.028 ± 0.033 ± 0.009 In
the measured rangethe measured range
A. Airapetian et al, Phys. Rev D 71 A. Airapetian et al, Phys. Rev D 71 (2005) 012003(2005) 012003
J Stewart
Polarized SeaPolarized Sea
d u 0 Unpolarized data on sea shows the Gottfried sum rule is broken Unpolarized data on sea shows the Gottfried sum rule is broken
Reanalyze polarized data: Reanalyze polarized data:
Polarized data favor a symmetric sea ,but large uncertaintiesPolarized data favor a symmetric sea ,but large uncertaintiesd u
u d u- d s= , ,Fit ,
u d u-d for
s Q
J Stewart
Distribution FunctionsDistribution Functions
)()()( xqxqxq$ )()( xqxqq
$
)()( xqxqq
HERMES 1996-2000HERMES 1996-2000 HERMES >2002HERMES >2002
Leading TwistLeading Twist
3 distribution functions survive the integration over transverse quark momentum3 distribution functions survive the integration over transverse quark momentum
unpolarized DFunpolarized DF Helicity DFHelicity DF Transversity DFTransversity DF
1F (x) 1g (x)
vector charge axial charge tensor charge
5 5
1 1 1( ) ( ) ( ) ( )
2 2 2x q x P q x P q x P S 5 5
1 1 1( ) ( ) ( ) ( )
2 2 2x q x P q x P q x P S
Transversity Transversity
basisbasis
J Stewart
Properties of the Transversity DFsProperties of the Transversity DFs For non-relativistic quarks For non-relativistic quarks q(x)=q(x)=q(x)q(x)
→ q(x) probes the relativistic nature of the q(x) probes the relativistic nature of the quarksquarks
Due to Angular Momentum ConservationDue to Angular Momentum Conservation→ Different QCD evolutionDifferent QCD evolution→ No gluon componentNo gluon component
→ Predominately sensitive to valence quarksPredominately sensitive to valence quarks
BoundsBounds Soffer Bound: Soffer Bound:
T-evenT-even Chiral oddChiral odd
→ Not measurable in inclusive DISNot measurable in inclusive DIS
( ) ( ) ( )q
x q x q x
( ) ( )q x q x ( ) ( ) ( )q x q x q x
J Stewart
Measuring TransversityMeasuring Transversityep eh eq eq
q
p hq q~ D FF F Need a chiral odd fragmentation function: ‘Collins FF’Need a chiral odd fragmentation function: ‘Collins FF’
•ForbiddenForbidden •Need chiral odd Need chiral odd fragmentation functionfragmentation function
Transverse quark polarization affects transverse hadron momentumTransverse quark polarization affects transverse hadron momentum Observed asymmetry in azimuthal angle about lepton scattering Observed asymmetry in azimuthal angle about lepton scattering
plane plane
2 (1/ 2)1
( , ) ( , )1,
( , ) ( , )
~ ( )si )( (n )
h S h S
UT ST h S h S
qqS
N NA
S N N
e q x H z
J Stewart
Sivers Function Sivers Function
Distribution functionDistribution function→ Naïve T-ODDNaïve T-ODD→ Chiral evenChiral even
a remnant of the quark transverse momentum a remnant of the quark transverse momentum can survive the photo-absorption and the can survive the photo-absorption and the fragmentation processfragmentation process
Can be inherited in the transverse momentum Can be inherited in the transverse momentum component component → influence azimuthal distributioninfluence azimuthal distribution
Non-vanishing Sivers function requires quark Non-vanishing Sivers function requires quark orbital angular momentumorbital angular momentum
Cross section depends on the angle between Cross section depends on the angle between the target spin direction and the hadron the target spin direction and the hadron production planeproduction plane
2 (1/ 2)UT 1 1A ~ (sin( ) ) ( )q
q TS qe f x D z
(1/ 2)1Tf
August 2005 J Stewart
Single target-spin asymmetry
angle of hadron relative to final quark spin
angle of hadron relative to initial quark spin
h S h SS
T h S h S
Collins SiversUT S UT S
N ( , ) N ( , )1( , )
| | N ( , ) N ( , )
A sin( ) A sin( )
S
hUTA
amplitudes fit simultaneously (prevents mixing effects due to acceptance)
J Stewart
Collins MomentCollins Moment Result is consistent with the Result is consistent with the
published Collins moment.published Collins moment.
Large negative Large negative -- moment moment unexpectedunexpected
One possibility One possibility
Additional information on the Collins Additional information on the Collins fragmentation function needed to fragmentation function needed to extract the transversity distribution. extract the transversity distribution. → BelleBelle
u 0
usin( ) 0s
sin( ) 0s
(1/ 2) (1/ 2)1 1( ) ( )unfavored favoredH z H z
J Stewart
Sivers MomentSivers Moment
++ sivers moment > 0! sivers moment > 0!→ Clear sign for non-zero Clear sign for non-zero
orbital angular orbital angular momentum!momentum!
Sivers moment for Sivers moment for -- is is consistent with zero.consistent with zero.→ Unfavored frag.?Unfavored frag.?
Unpolarized fragmentation Unpolarized fragmentation functions are known functions are known → Sivers function can be Sivers function can be
extracted.extracted.
ff1T1T
(x) DIS = - f(x) DIS = - f1T1T
(x) DY(x) DY→ UNIVERSALITYUNIVERSALITY
J Stewart
Why are Fragmentation functions important?Why are Fragmentation functions important?
In Semi-inclusive DIS:In Semi-inclusive DIS:
Important for Important for q,q,q, and q, and Test factorizationTest factorization Test universalityTest universality
DF FF
1Tf
12 2 h 2h 2 f f f0
f1DIS 2 2
f f0f
e dxq x,Q D z,QdN z,Q1
N dz e dxq x,Q
Extract Extract , K, and p multiplicities:, K, and p multiplicities:
J Stewart
Multiplicity ExtractionMultiplicity Extraction
Born Level Born Level
multiplicitiesmultiplicities
ExperimentalExperimental
Multiplicities Multiplicities
in acceptancein acceptance
MCMC
Excl. VM Corr.Excl. VM Corr.
PID with the RICHPID with the RICH
UnpolarizedUnpolarized
H&D dataH&D data
AcceptanceAcceptance
Radiative effectsRadiative effects
J Stewart
MC tuningMC tuning
Monti Carlo:Monti Carlo:→ Lepto in combination with Lepto in combination with
JETSET; JETSET; → PDF: CTEQ-6LPDF: CTEQ-6L→ Fragmentation Fragmentation
parameters tuned to parameters tuned to HERMES multiplicities in HERMES multiplicities in the acceptancethe acceptance
Data: Data: → QQ22>1GeV>1GeV22, W, W22>10GeV>10GeV22, ,
z>0.2, 2GeV <p< 15GeV z>0.2, 2GeV <p< 15GeV ((, K, and P), K, and P)
Excellent Agreement even Excellent Agreement even at the cross section levelat the cross section level
→ DATA/MC <10%!DATA/MC <10%!
++ --
++ --
PP++ PP--
J Stewart
± ± Multiplicities vs zMultiplicities vs z
Systematic uncertainties mainly from hadron PID correctionSystematic uncertainties mainly from hadron PID correctionQQ22>1GeV>1GeV22, W, W22>10GeV>10GeV22
Comparison with EMC FF, Nucl. Phys. B321 (1989) 541Comparison with EMC FF, Nucl. Phys. B321 (1989) 541Reasonable agreement with FF from S. KretzerReasonable agreement with FF from S. Kretzer
J Stewart
KK±± Multiplicity vs z Multiplicity vs z
Charge separated Kaon multiplicitiesCharge separated Kaon multiplicities Systematic uncertainty mainly from hadron PIDSystematic uncertainty mainly from hadron PID Low KLow K-- statistics at high z statistics at high z will collect more data will collect more data
J Stewart
Agreement with existing Frag. Fns.Agreement with existing Frag. Fns.
J Stewart
Summary Summary
Longitudinally Polarized Target DataLongitudinally Polarized Target Data The structure functions have been measured.The structure functions have been measured.
→ First measurement of bFirst measurement of b11..
First direct measurement of the helicity distributionsFirst direct measurement of the helicity distributions
Transversely Polarized Target DataTransversely Polarized Target Data Collins:Collins:
→ Non-Zero asymmetries measured.Non-Zero asymmetries measured.→ Disfavored fragmentation functions appear to be Disfavored fragmentation functions appear to be
important and have opposite sign to the favored.important and have opposite sign to the favored. Sivers: Sivers:
→ ++ Amplitude is greater than zero. Amplitude is greater than zero.→ Orbital angular momentum must be non-zero!Orbital angular momentum must be non-zero!
0, 0, , , 0u d u d s
1 1 1, ,g gp d dand b
J Stewart
Outlook Outlook
Data taking with transverse polarized target will continue Data taking with transverse polarized target will continue till November.till November.
Expect about 5M DIS events in the final data set. Expect about 5M DIS events in the final data set. New multiplicities New multiplicities
→ New millennium extraction of New millennium extraction of q (purity free).q (purity free).→ New extraction using isoscalor methodNew extraction using isoscalor methodΔs+ Δs
J Stewart
Backup SlidesBackup Slides
J Stewart
q
q
J Stewart
Purities Purities -- -- --
J Stewart
J Stewart
J Stewart
Distribution and Fragmentation FunctionsDistribution and Fragmentation Functions
hqeqeqq
qHehXeH Df
J Stewart
Exclusive VM ContaminationExclusive VM Contamination
Exclusive vector meson (VM) Exclusive vector meson (VM) contribution estimated using Pythia-6contribution estimated using Pythia-6
Correct data set for VM contamination.Correct data set for VM contamination.→ Different process than SIDISDifferent process than SIDIS
Evaluate ratio:Evaluate ratio:
Large contamination for Large contamination for at high z at high z Contribution for K moderate vs zContribution for K moderate vs z Contribution grows for small x for both Contribution grows for small x for both
and K and K
h hexcl.VM excl.VMN (z)/N (z)