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Universit à degli studi di Ferrara. Measurement of azimuthal asymmetries of the unpolarized cross-section at HERMES. Francesca Giordano Charlottesville, USA, SPIN2008. Unpolarized Semi-Inclusive DIS (SIDIS). Unpolarized SIDIS : collinear approximation. - PowerPoint PPT Presentation
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Measurement of azimuthal asymmetries of the unpolarized cross-
section at HERMES
Francesca GiordanoCharlottesville, USA, SPIN2008
Università degli studi di Ferrara
Unpolarized Semi-Inclusive DIS (SIDIS)
)1()(
)2/11()( 2
yyB
yyyA
Unpolarized SIDIS :collinear approximation
),,( 2...... zQxFF
LUUTUU FyBFyAxxyQdzdydx
d,,
2
2
23
)()(2
1
TUUF , LUUF ,
Unpolarized SIDIS :non-collinear cross-section
),,,( 2...... hPzQxFF
yyyC
yyB
yyyA
1)2()(
)1()(
)2/11()( 2
2coscos 2cos)(cos)( UUUU FyBFyC 2cosUUFcos
UUF
LUUTUUh
FyBFyAxxyQdPddzdydx
d,,
2
2
2
2
5
)()(2
1
TUUF , LUUF ,
Unpolarized SIDIS :non-collinear cross-section
2coscos 2cos)(cos)( UUUU FyBFyC 2cosUUFcos
UUF
d
dnPzyxn h )5(
)5(cos),,,(cos
LUUTUUh
FyBFyAxxyQdPddzdydx
d,,
2
2
2
2
5
)()(2
1
TUUF , LUUF ,
Leading twist expansion
11 Df
DF FF
TUUF ,
Leading twist expansion
N / q U L T
U
L
T
q/h U
U
T
1D1H
Distribution Functions (DF)
Fragmentation Functions
(FF)
1h
Tg1
1g Lh1
1hTh1,
Tf1
1f11 Df
DF FF
TUUF ,
Leading twist expansion
= Boer-Mulders = Boer-Mulders
functionfunctionCHIRAL-ODDCHIRAL-ODD
1h
N / q U L T
U
L
T
q/h U
U
T
1D1H
Distribution Functions (DF)
Fragmentation Functions
(FF)
1h
Tg1
1g Lh1
1hTh1,
Tf1
1f
Leading twist expansion
= Boer-Mulders = Boer-Mulders
functionfunctionCHIRAL-ODDCHIRAL-ODD
1h
11 Hh
CHIRAL-CHIRAL-
EVENEVEN!
chiral-odd
DF
chiral-oddFF
N / q U L T
U
L
T
q/h U
U
T
1D1H
Distribution Functions (DF)
Fragmentation Functions
(FF)
1h
Tg1
1g Lh1
1hTh1,
Tf1
1f
112cos )ˆ)(ˆ(2
HhMM
pkphkhF
h
TTTTUU
C
Structure functions expansion at
leading twist
(Implicit sum over quark flavours)
z
Hh
M
MDxf
M
kh
z
Df
M
MxhH
M
ph
Q
MF hTh
h
TUU
~ˆ~ˆ21111
cos
C
112cos )ˆ)(ˆ(2
HhMM
pkphkhF
h
TTTTUU
C
Structure functions expansion
at twist 3
(Implicit sum over quark flavours)
z
Hh
M
MDxf
M
kh
z
Df
M
MxhH
M
ph
Q
MF hTh
h
TUU
~ˆ~ˆ21111
cos
C
112cos )ˆ)(ˆ(2
HhMM
pkphkhF
h
TTTTUU
C
Structure functions expansion
at twist 3
(Implicit sum over quark flavours)
z
Hh
M
MDxf
M
kh
z
Df
M
MxhH
M
ph
Q
MF hTh
h
TUU
~ˆ~ˆ21111
cos
C
Structure functions expansion
at twist 3
12
2~h
Mhx T
1
~ffx
112cos )ˆ)(ˆ(2
HhMM
pkphkhF
h
TTTTUU
C
(Implicit sum over quark flavours)
z
Hh
M
MDxf
M
kh
z
Df
M
MxhH
M
ph
Q
MF hTh
h
TUU
~ˆ~ˆ21111
cos
C
Structure functions expansion
at twist 3
12
2~h
Mhx T
1
~ffx
112cos )ˆ)(ˆ(2
HhMM
pkphkhF
h
TTTTUU
C
(Implicit sum over quark flavours)
...neglecting interaction dependent terms....
112cos )ˆ)(ˆ(2
HhMM
pkphkhF
h
TTTTUU
C
Cahn and Boer-Mulders effects
1111cos
ˆˆ2Dfx
M
khHhx
M
ph
Q
MF T
h
TUU
C
(Implicit sum over quark flavours)
...neglecting interaction dependent terms....
Cahn and Boer-Mulders effects
kT
kT
hP
hP
112cos )ˆ)(ˆ(2
HhMM
pkphkhF
h
TTTTUU
C
1111cos
ˆˆ2Dfx
M
khHhx
M
ph
Q
MF T
h
TUU
C
CAHN EFFECT
11Df
BOER-MULDERS EFFECT
Cahn and Boer-Mulders effectskT kT
sT
sT
hP
hP
kT
kT
hP
hP
112cos )ˆ)(ˆ(2
HhMM
pkphkhF
h
TTTTUU
C
1111cos
ˆˆ2Dfx
M
khHhx
M
ph
Q
MF T
h
TUU
C
CAHN EFFECT
11Df11 Hh
11 Hh
HERa MEasurement of Spin
HERA storage ring @ DESY
HERMES spectrometer
Resolution: p/p ~ 1-2% <~0.6 mrad
Electron-hadron separation efficiency ~ 98-99%
HERMES spectrometer
Resolution: p/p ~ 1-2% <~0.6 mrad
Electron-hadron separation efficiency ~ 98-99%
),,,( hPzyx
Experimental extraction
)2cos)(cos)(1()(0 BALnEXP d
Experimental extraction
),,,( hPzyx
)2cos)(cos)(1()(0 BALnEXP
2cos2B
cos2A),,,( hPzyx
d
Experimental extraction
),(),( RADacc
),,,( hPzyx
d
Experimental extraction
)2cos)(cos)(1()(0 BALnEXP
),(),( RADacc
),,,( hPzyx
)2cos)(cos)(1( BA LnEXP )(0 d
Experimental extraction
Why a fully differential analysis?
Standard Monte Carlo dLn MC
RAD
MCMCMCMC
acc ),(),()(0
Why a fully differential analysis? ),(),(
RADacc)2cos)(cos)(1( BA LnEXP )(0 d
Measured inside acceptance
Generated in 4
),,,( hPzyx
Why a fully differential analysis?
MCMC
RAD
MCMC
RAD
MC
EXP
L
L
n
n
acc
acc
),(),()(
),(),()(
0
0
d
d)2cos)(cos)(1( BA
dL
dL
n
nFLATMCMC
RAD
MCFLATMC
FLATMCMC
RAD
MCFLATMC
FLATMC
FLATMC
acc
acc
,2,2
,1,1
,2
,1
),(),()(
),(),()(
0
0
1- VS. Multi-dimensional analysis
dL
dL
n
nFLATMCMC
RAD
MCFLATMC
FLATMCMC
RAD
MCFLATMC
FLATMC
FLATMC
acc
acc
,2,2
,1,1
,2
,1
),(),()(
),(),()(
0
0
)(,1
0 FLATMC
)(,2
0 FLATMC
1- VS. Multi-dimensional analysis
MC1, FLATMC2, FLAT
1- VS. Multi-dimensional analysis
dL
dL
n
nFLATMCMC
RAD
MCFLATMC
FLATMCMC
RAD
MCFLATMC
FLATMC
FLATMC
acc
acc
,2,2
,1,1
,2
,1
),(),()(
),(),()(
0
0
)(,1
0 FLATMC
)(,2
0 FLATMC
1- VS. Multi-dimensional analysis
One-dimensional analysisMulti-dimensional analysis
dL
dL
n
nFLATMCMC
RAD
MCFLATMC
FLATMCMC
RAD
MCFLATMC
FLATMC
FLATMC
acc
acc
,2,2
,1,1
,2
,1
),(),()(
),(),()(
0
0
One-dimensional analysisMulti-dimensional analysis
1- VS. Multi-dimensional analysis
dL
dL
n
nFLATMCMC
RAD
MCFLATMC
FLATMCMC
RAD
MCFLATMC
FLATMC
FLATMC
acc
acc
,2,2
,1,1
,2
,1
),(),()(
),(),()(
0
0
Fully d
iffer
entia
l analys
is
Fully d
iffer
entia
l analys
is
is nee
ded
is nee
ded
The unfolding procedure
MCBORNMCEXPBgnSn '
MCBORNMCEXPBgnSn '
The unfolding procedure
'MC
S
Probability that an event generated with kinematics is measured with kinematics ’
’
MCBORNMCEXPBgnSn '
The unfolding procedure
'MC
S
Accounts for acceptance, radiative and smearing
effects
depends only on instrumental and radiative effects
Probability that an event generated with kinematics is measured with kinematics ’
’
MCBORNMCEXPBgnSn '
The unfolding procedure
MCBg
Includes the events smeared within kinematical cuts
Accounts for acceptance, radiative and smearing
effects
depends only on instrumental and radiative effects
Probability that an event generated with kinematics is measured with kinematics ’
MCEXPMCBORN
BgnSn 1'
The unfolding procedure
MCBORNMCEXPBgnSn '
x bin=2x bin=3
The multi-dimensional analysis
Z hP
x bin=1
x bin=5
....x4 as the y binning is missing
here!
x bin=4
BINNING
400 kinematical bins x 12 -bins
Variable Bin limits #
x 0.023 0.042 0.078 0.145 0.27 1 5
y 0.3 0.45 0.6 0.7 0.85 4
z 0.2 0.3 0.45 0.6 0.75 1 5
PhT 0.05 0.2 0.35 0.5 0.75 4
Z hP
....x4 as the y binning is missing
here!
The multi-dimensional analysis
cos
x bin=2x bin=3
x bin=1
x bin=5x bin=4
unfoldin
g
)(
cos)()(cos
4
4
bi
bibi
xx
xxxx
bx
Z hP
....x4 as the y binning is missing
here!
The multi-dimensional analysis
cos
x bin=2x bin=3
x bin=1
x bin=5x bin=4
projecti
on
Z hP
The multi-dimensional analysis
)(
cos)()(cos
475.0
05.0
275.0
2.0
85.0
3.0
475.0
05.0
275.0
2.0
85.0
3.0
bi
bibi
xxh
xxxxh
b
dPdzdy
dPdzdyx
cos
x bin=2x bin=3
x bin=1
x bin=5x bin=4
)(
cos)()(cos
4
4
bi
bibi
xx
xxxx
bx
),(),( RADacc)2cos)(cos)(1( BA LnEXP )(0 d
RAD
EXP
accLn )1(0 UUFA0CAHNn
Model for the ‘Cahn Model for the ‘Cahn effect’ effect’
in Monte Carloin Monte Carlo
The multi-dimensional analysisCAHNn
Monte Carlo check
RAD
EXP
accLn )1(0 CAHNn 0 )1(UUFA
The multi-dimensional analysisMonte Carlo check
Measured inside acceptance
Generated in 4
MC
RAD
MCMCMC
accLn MC
0RAD
EXP
accLn )1(0 CAHNn 0 )1(UUFA
The multi-dimensional analysisMonte Carlo check
Measured inside acceptance
Generated in 4
MC
RAD
MCMCMC
accLn MC
0RAD
EXP
accLn )1(0 CAHNn 0 )1(UUFA
The multi-dimensional analysisMonte Carlo check
Measured inside acceptance
Generated in 4
MCMCBgS ,'
Monte Carlo Test
Cahn ModelUnfolded
Results
Statistics
Target Type Hadron charge #SIDIS
(Million)
Hydrogen h+ 1.46
h- 0.82
Deuterium h+ 1.53
h- 1.00
Hydrogen target
)(
cos)()(cos
475.0
05.0
275.0
2.0
85.0
3.0
475.0
05.0
275.0
2.0
85.0
3.0
bi
bibi
xxh
xxxxh
b
dPdzdy
dPdzdyx
112cos )ˆ)(ˆ(2
HhMM
pkphkhF
h
TTTTUU
C
Cahn and Boer-Mulders effects
1111cos
ˆˆ2Dfx
M
khHhx
M
ph
Q
MF T
h
TUU
C
(interaction dependent terms neglected)
Cahn and Boer-Mulders effects
fav
u
unf
uHH ,
,1
,
,1
112cos )ˆ)(ˆ(2
HhMM
pkphkhF
h
TTTTUU
C
1111cos
ˆˆ2Dfx
M
khHhx
M
ph
Q
MF T
h
TUU
C
cos2 interpretation
cos2 interpretation
V. Barone et al. Phys.Rev.D78:045022,2008
cos2 interpretation
Boer-Mulders
All contribution
sCahn (twist
4)
cos interpretation
Hydrogen VS. Deuterium
du hh ,1,1
h+
Hydrogen VS. Deuterium
du hh ,1,1
h+
Hydrogen VS. Deuteriumh-
du hh ,1,1
SummaryAccounting for the intrinsic quark transverse motion in the unpolarized cross-section gives origin to an azimuthal asymmetry in the hadron production direction;In particular it was stressed the existence of the
Cahn effect: an (higher twist) azimuthal modulation related to the existence of quark intrinsic motion;Boer-Mulders effect: a leading twist asymmetry originated by the correlation between the quark transverse motion and spin (a kind of spin-orbit effect).
Monte Carlo studies show that: A fully differential analysis together with an unfolding procedure is able to disentangle the ‘physical’ azimuthal asymmetry from the acceptance and radiative modulations of the cross-section.
SummaryAccounting for the intrinsic quark transverse motion in the unpolarized cross-section gives origin to an azimuthal asymmetry in the hadron production direction;In particular it was stressed the existence of the
Cahn effect: an (higher twist) azimuthal modulation related to the existence of quark intrinsic motion;Boer-Mulders effect: a leading twist asymmetry originated by the correlation between the quark transverse motion and spin (a kind of spin-orbit effect).
Monte Carlo studies show that: A fully differential analysis together with an unfolding procedure is able to disentangle the ‘physical’ azimuthal asymmetry from the acceptance and radiative modulations of the cross-section.
SummaryAccounting for the intrinsic quark transverse motion in the unpolarized cross-section gives origin to an azimuthal asymmetry in the hadron production direction;In particular it was stressed the existence of the
Cahn effect: an (higher twist) azimuthal modulation related to the existence of quark intrinsic motion;Boer-Mulders effect: a leading twist asymmetry originated by the correlation between the quark transverse motion and spin (a kind of spin-orbit effect).
Flavour dependent experimental results: Negative <cos> moments are extracted for positive and
negative hadrons, with a larger absolute value for the positive ones
The results for the <cos2> moments are negative for the positive hadrons and positive for the negative hadrons
- Evidence of a non-zero Boer-Mulders function
Monte Carlo studies show that: A fully differential analysis together with an unfolding procedure is able to disentangle the ‘physical’ azimuthal asymmetry from the acceptance and radiative modulations of the cross-section.
SummaryAccounting for the intrinsic quark transverse motion in the unpolarized cross-section gives origin to an azimuthal asymmetry in the hadron production direction;In particular it was stressed the existence of the
Cahn effect: an (higher twist) azimuthal modulation related to the existence of quark intrinsic motion;Boer-Mulders effect: a leading twist asymmetry originated by the correlation between the quark transverse motion and spin (a kind of spin-orbit effect).
Flavour dependent experimental results: Negative <cos> moments are extracted for positive and
negative hadrons, with a larger absolute value for the positive ones
The results for the <cos2> moments are negative for the positive hadrons and positive for the negative hadrons
- Evidence of a non-zero Boer-Mulders function
THANK
THANK
YOU!YOU!
Experimental status: cos
EMC
E665
ZEUS
c)
Negative results in all the existing measurements
No distinction between hadron type or charge
2cos
EMC
ZEUS collaborationXhHe
0.12.0 z
222 /7220180 cGeVQ 01.001.0 x 8.02.0 y
ZEUS
Drell-Yan
Experimental status:
Positive results in all the existing measurements
No distinction between hadron type or charge (in SIDIS experiments)
Indication of small Boer-Mulders function for the sea quark (from Drell-Yan experiments)
Compass results
Vector meson dilution