Measurement of (Interference) Fragmentation Functions in e + e - at Anselm Vossen and Di-Hadron Correlations and DiFF Mini Workshop Pavia, Italy, September.

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Measurement of (Interference) Fragmentation Functions in

e+e- at

Anselm Vossen

and Di-Hadron Correlations

and

DiFF Mini WorkshopPavia, Italy, September 5th - 8th 2011

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Outline• IFF measurements at Belle

– Observables– Kinematic Distributions– Flavor decomposition (Charm Contributions)– Results– Future Plans

• Phenix– Experiment– Results

• Star– Current status– Future possibilities

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Interference FF in Quark Fragmentation

q

qs

k

R

Interference Fragmentation Function:Fragmentation of a transversely polarizedquark q into two spin-less hadron h1, h2 carries anazimuthal dependence:

R

sin

T qk R s

1h

2h

𝑘𝑠𝑞

𝑅𝑅𝑇

𝑧𝑝𝑎𝑖𝑟

= 2 𝐸𝑝𝑎𝑖𝑟 / √ 𝑠𝑚

: quark   momentum:quark   spin  : momentum   difference𝑝h 1−𝑝h 2

transverse   hadron   momentum  difference  ¿𝐸𝑝𝑎𝑖𝑟 /𝐸𝑞

: relative   hadron   pair   momentum: hadron   pair   invariant  mass

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o Quark spin direction unknown: measurement of Interference Fragmentation function in one hemisphere is not possible

sin φ modulation will average out.

o Correlation between two hemispheres with sin φRi single spin asymmetries results in cos(φR1+φR2) modulation of the observed di-hadron yield.

Measurement of azimuthal correlations for di-pion pairs around the jet axis in two-jet events!

Spin Dependent FF in e+e- : NeedCorrelation between Hemispheres !

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q1

quark-1 spin

Interference effect in e+e-

quark fragmentation will lead to azimuthalasymmetries in di-hadron correlation measurements!

Experimental requirements:

Small asymmetries very large data sample!

Good particle ID to high momenta.

Hermetic detector Observable:cos(φR1+φR2)

modulation measures

Measuring di-Hadron CorrelationsIn e+e- Annihilation into Quarks

electron

positron

q2

quark-2 spin

( )

z1,2 relative pion pair momenta

z2 z1

( )

11H H

φR1φR2

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KEKB: L>2.11 x 1034cm-2s-1 !!• Asymmetric collider• 8GeV e- + 3.5GeV e+

• √s = 10.58GeV (U(4S))• e+e-U(4S)BB• Off-resonance production:

10.52 GeV• e+e-qq (u,d,s,c)• Integrated Luminosity: > 1000 fb-1

• >70 fb-1 => continuum

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Belle detectorKEKB

7Large acceptance, good tracking and particle identification!

He/C2H6

Interference Fragmentation–thrust methode+e- (+-)jet1()jet2X

transverse spin projection8 21221111 m,zHm,zHA cos

2

2

sin

1 cos

2

1

1hP

2hP

2h1h PP

q

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• Similar to previous method• Observe angles j1R+j2R between the event-plane (beam, two-

pion-axis) and the two two-pion planes.

• Theoretical guidance by Boer,Jakob,Radici

jR2

-p jR1

1hP

2hP

3hP

4hP

2h1h PP

4h3h PP

Interference Fragmentation – “ f0 “ method

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Cuts and Binning

• Similar to Collins analysis, full off-resonance and on-resonance data(7-55): ~73 fb-1 + 588 fb-1

• Visible energy >7GeV • PID: Purities in for di-pion pairs > 90% • Same Hemisphere cut within pair (p+p-), opposite hemisphere between

pairs• All 4 hadrons in barrel region:-0.6 < cos (q) <0.9• Thrust axis in central area: cosine of thrust axis around beam <0.75• Thrust > 0.8 to remove B-events < 1% B events in sample• zhad1,had2>0.1

• z1 = zhad1+zhad2 and z2 in 9x9 bins

• m 1pp and m 2pp in 8x8 bins: [0.25 - 2.0] GeV

• New: Mixed binning

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Kinematics

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Opening Cut and Energy Flow

Opening Cut of 0.8 Opening Cut of 0.9

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Zero tests: MC

• A small asymmetry seen due to acceptance effect• Mostly appearing at boundary of acceptance• Opening cut in CMS of 0.8 (~37 degrees) reduces

acceptance effect to the sub-per-mille level13

Ph

),cos(ˆ

nPP

nP

h

h

No opening cutOpening cut>0.7Opening cut >0.8

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(z1x m1) Binning

arXiv:1104.2425PRL 107, 072004(2011)

(m1x z1) Binning

arXiv:1104.2425PRL 107, 072004(2011)

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Subprocess contributions (MC)8x8 m1 m2 binning

tau contribution (only significant at high z)charged B(<5%, mostly at higher mass)Neutral B (<2%)charm( 20-60%, mostly at lower z)uds (main contribution)

Subprocess contributions (MC)

tau contribution (only significant at high z)charged B(<5%, mostly at higher mass)Neutral B (<2%)charm( 20-60%, mostly at lower z)uds (main contribution)

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9x9 z1 z2 binning

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Accessing QCD vacuum fluctuations in Quark Fragmentation

• QCD vacuum is superposition of theta vacua• On microscopic scale this could be accessible in experiments

– First results in STAR – Planned measurements in Belle: – Needed as a ‘tie breaker’– Model Calculations predict 2% effect

• Access to nonperturpative properties of QCD• Transition instantons/sphalerons: Role in Early Universe, baryogenesis …

Anselm Vossen

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q1

quark-1 spin

Event Topologyelectron

positron

q2

quark-2 spin

z2 z1

z1,2 relative pion momenta

Jet Axis

p+ p-

: Momentum : Spin

• Fragmentation in P-odd bubble leads to left right asymmetry– Difference in ‘Winding number’ gives effective increment in chirality– Spin alignment via chromomagnetic effect– Azimuthal event by event modulation– Measurement: Extract width of distribution of first moments

– Analysis already underway: Is there a Di-hadron Analogue?

1H 1H

Currently underway:• Belle II is a significant upgrade to

Belle and will sample 2 orders of magnitude higher luminosity

• High precision data will enable measurement of– P-odd FFs– Transverse momentum dependent FFs– Charm suppression possible

• IU will develop FEE for Barrel KLM detector crucial for high precision FF measurement of identified particles

Belle Fragmentation activityRIKEN/RBRC Illinois Indiana Titech

Unpol FFse+e-hX:

e+e-(hh)X,(h)(h)X,hhX:

Unpol kT dependence:

Neutral hadrons: (p0 ,h0) John KosterCharged di-hadrons: Ralf Seidl

Charged hadrons (p,K,P):Martin Leitgab

Martin Leitgab

Collins FFse+e-(h)(h)X:

kT dependence:

pp0 : John Kosterpr0: Ralf Seidlpp: Ralf Seidlpp0 : John Koster

pK,KK: Francesca GiordanoFrancesca Giordano

pr±: ?

Interference FF:e+e-(hh)(hh)X

Charged : pp Ralf Seidl

Charged pp: Anselm Vossenpp0 : Anselm Vossen

Charged pK,KK:Nori-aki Kobayashi

Local P :L(polFF,SSA) :Jet-jet asy:

Anselm Vossen

Black: about to startGreen: ongoingGrey: finished

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Same Hemisphere Correlations?

• Motivation: P-odd FF x Collins (in Single hadron) does not average out

p+p complementary and increased kinematic reach in x, z

• Kinematic reach of SIDIS data

• Kinematic reach in p+p for single pions at 3<eta<4

• Relative hadron momentum z for p+p (3<eta<4) collisions and SIDIS (COMPASS), only single hadron, di-hadron z1+z2 ‘less different’

z

Mean z: 0.64

PT

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Definition of Vectors and Angles

1 2

1 2

1 2

p+p c.m.s. = lab frame

, : momenta of protons

, : momenta of hadrons

( ) / 2

: proton spin orientation

A B

h h

C h h

C h h

B

P P

P P

P P P

R P P

S

))))))))))))))))))))))))))))

))))))))))))))))))))))))))))

))))))))))))))))))))))))))))))))))))))))))

))))))))))))))))))))))))))))))))))))))))))

))))))))))))))

1hP))))))))))))))

2hP))))))))))))))

100 GeVAP))))))))))))))

100 GeVBP))))))))))))))

CP))))))))))))))

BS))))))))))))))

pp hhX

1 2hadron plane: ,

scattering plane: ,

h h

C B

P P

P P

))))))))))))))))))))))))))))

)))))))))))))))))))))))))))) : from scattering plane

to hadron planeR : from polarization vector

to scattering plane S

Bacchetta and Radici, PRD70, 094032 (2004)

2 CR))))))))))))))

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PHENIX Detectors used for IFF Analysis

• Use 2 separate spectrometer arms at central rapidity,|h| < 0.35

• Azimuthal coverage: 90° + 90°• Electromagnetic Calorimeters

– PbSC + PbGl– High granularity DhDf=0.010.01

• Tracking of charged particles– Drift chamber, pad chambers

Little p_t dependence of x at mid rapidity, low x

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vs Invariant Mass of the PairsinUTA

First measurement of IFF in pp

Results and ProjectionsFrom run 12+13

Planned Transversity measurements at STAR

• Measurements with current detector– Transversity in Di-Hadron

correlations – p0 in FMS and Encap, p+ /p-

inTPC– Sivers effect in jets in EEMC– Explore jet –jet and gamma –

jet asymmetries

Full azimuth spanned with nearly contiguous electromagnetic calorimetry from -1<h<4

approaching full acceptance detector

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R&D for planned STAR forward upgrade

• Forward instrumentation optimized for p+A and transverse spin physics

– Charged Tracking upgrade covering FMS will enable di-hadron measurements and jet measurements

– Star decadal plans calls additionally for PID (e.g. RICH) and pi0/gamma separation (preshower)

FMS

~ 6 GEM disksTracking: 2.5 < η < 4

proton nucleus

• Transverse spin effect dominated by valence quarks accessed in forward direction

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Projections forBelle Measurements of IFF in STAR, Channel: (pp0) (pp0)

• Errors one order of magnitude smaller than average asymmetry in (pp)

Hadron pair in second hemisphere:0.77 GeV <Minv< 1.2 GeV

a 12

(580 fb-1 integrated luminosity)

-0.004

0.002

-0.002

0

3131

Measuring Light Quark Fragmentation Functions on the ϒ(4S) Resonance

ii

ii

p

npTThrust

ˆ

:

• small B contribution (<1%) in high thrust sample • >75% of X-section continuum under ϒ (4S) resonance• 73 fb-1 662 fb-1

9.44 9.46

e+e- Center-of-Mass Energy (GeV)

0

5

10

15

20

25

(e+

e-

had

ron

s)(n

b)

(1S)10.0010.02

0

5

10

15

20

25

(2S)10.34 10.37

0

5

10

15

20

25

(3S)10.54 10.58 10.62

0

5

10

15

20

25

(4S)9.44 9.46

e+e- Center-of-Mass Energy (GeV)

0

5

10

15

20

25

(e+

e-

had

ron

s)(n

b)

(1S)10.0010.02

0

5

10

15

20

25

(2S)10.34 10.37

0

5

10

15

20

25

5

10

15

20

25

(2S)10.34 10.37

0

5

10

15

20

25

(3S)10.54 10.58 10.62

0

5

10

15

20

(3S)10.54 10.58 10.62

0

5

10

15

20

25

(4S)BB00 BB

e+e-qq̅, q uds∈

e+e-cc̅

0.5 0.8 1.0

4s“off”