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SPIN EFFECTS IN
UNPOLARIZED SIDIS
ati
10
Azimuthal cosine modulations
DIS unpolarized cross section
rdano
b
Francesca Giordano
SPIN 2012, Dubna, Russia
1
Francesca Giordano
Collinear case
target
polarization
beam
polarization virtual photon
polarization
d3
⇤
dxdydz =
2
xyQ2 1 + ⇥2
2x {A(y)FUU,T + B(y)FUU,L}
SEMI-INCLUSIVE DIS
2
Francesca Giordano
target
polarization
beam
polarization virtual photon
polarization
SEMI-INCLUSIVE DIS
2
Francesca Giordano
target
polarization
beam
polarization virtual photon
polarization
SEMI-INCLUSIVE DIS
Negative squared
4-momentum transfer to the target
Fractional energy of the virtual photon
Parton fractional momentum
Fractional energy transfer to the
produced hadron
2
TRANSVERSE MOMENTUM
DEPENDENT FUNCTIONS
DF
σ
FF
3
TRANSVERSE MOMENTUM
DEPENDENT FUNCTIONS
DF
σ
FF
distribution functions
PDF probabilistic interpretation
f q
1 (x)
gq
1 (x)
hq
1 (x)
legend
transverse and longitu
transverse and longitu
Table 2.1.: Pictorial representation and chiral properties of the
transverse longitudinal
nucleon spin
parton spin
TMDs - Pro
parton with transverse or longit
parton transverse momentum
nucleon with transverse or l
Proton goes out of
parton transverse
momentum
3
TRANSVERSE MOMENTUM
DEPENDENT FUNCTIONS
DF
σ
FF
distribution functions
fragmentation functions
PDF probabilistic interpretation
f q
1 (x)
gq
1 (x)
hq
1 (x)
legend
transverse and longitu
transverse and longitu
Table 2.1.: Pictorial representation and chiral properties of the
transverse longitudinal
nucleon spin
parton spin
TMDs - Pro
parton with transverse or longit
parton transverse momentum
nucleon with transverse or l
Proton goes out of
parton transverse
momentum
3
TRANSVERSE MOMENTUM
DEPENDENT FUNCTIONS
DF
σ
FF
distribution functions
fragmentation functions
PDF probabilistic interpretation
f q
1 (x)
gq
1 (x)
hq
1 (x)
legend
transverse and longitu
transverse and longitu
Table 2.1.: Pictorial representation and chiral properties of the
transverse longitudinal
nucleon spin
parton spin
TMDs - Pro
parton with transverse or longit
parton transverse momentum
nucleon with transverse or l
Proton goes out of
parton transverse
momentum
3
TRANSVERSE MOMENTUM
DEPENDENT FUNCTIONS
DF
σ
FF
distribution functions
fragmentation functions
Boer-Mulders DF
PDF probabilistic interpretation
f q
1 (x)
gq
1 (x)
hq
1 (x)
legend
transverse and longitu
transverse and longitu
Table 2.1.: Pictorial representation and chiral properties of the
transverse longitudinal
nucleon spin
parton spin
TMDs - Pro
parton with transverse or longit
parton transverse momentum
nucleon with transverse or l
Proton goes out of
parton transverse
momentum
3
TRANSVERSE MOMENTUM
DEPENDENT FUNCTIONS
DF
σ
FF
distribution functions
fragmentation functions
Boer-Mulders DF
Collins FF
PDF probabilistic interpretation
f q
1 (x)
gq
1 (x)
hq
1 (x)
legend
transverse and longitu
transverse and longitu
Table 2.1.: Pictorial representation and chiral properties of the
transverse longitudinal
nucleon spin
parton spin
TMDs - Pro
parton with transverse or longit
parton transverse momentum
nucleon with transverse or l
Proton goes out of
parton transverse
momentum
3
Francesca Giordano
PDF probabilistic interpretation
f q
1 (x)
gq
1 (x)
hq
1 (x)
legend
transverse and longitu
transverse and longitu
Table 2.1.: Pictorial representation and chiral properties of the
transverse longitudinal
nucleon spin
parton spin
TMDs - Pro
parton with transverse or longit
parton transverse momentum
nucleon with transverse or l
Proton goes out of
parton transverse
momentum
LEADING TWIST TERMS
implicit sum over quark flavors
distribution functions
fragmentation functions
4
Francesca Giordano
LEADING AND
NEXT-TO-LEADING TWIST TERMS
implicit sum over quark flavors
distribution functions
PDF probabilistic interpretation
f q
1 (x)
gq
1 (x)
hq
1 (x)
legend
transverse and longitu
transverse and longitu
Table 2.1.: Pictorial representation and chiral properties of the
transverse longitudinal
nucleon spin
parton spin
TMDs - Pro
parton with transverse or longit
parton transverse momentum
nucleon with transverse or l
Proton goes out of
parton transverse
momentum
fragmentation functions
5
Francesca Giordano
LEADING AND
NEXT-TO-LEADING TWIST TERMS
implicit sum over quark flavors
distribution functions
PDF probabilistic interpretation
f q
1 (x)
gq
1 (x)
hq
1 (x)
legend
transverse and longitu
transverse and longitu
Table 2.1.: Pictorial representation and chiral properties of the
transverse longitudinal
nucleon spin
parton spin
TMDs - Pro
parton with transverse or longit
parton transverse momentum
nucleon with transverse or l
Proton goes out of
parton transverse
momentum
fragmentation functions
5
Francesca Giordano
LEADING AND
NEXT-TO-LEADING TWIST TERMS
implicit sum over quark flavors
interaction dependent
terms neglected
distribution functions
PDF probabilistic interpretation
f q
1 (x)
gq
1 (x)
hq
1 (x)
legend
transverse and longitu
transverse and longitu
Table 2.1.: Pictorial representation and chiral properties of the
transverse longitudinal
nucleon spin
parton spin
TMDs - Pro
parton with transverse or longit
parton transverse momentum
nucleon with transverse or l
Proton goes out of
parton transverse
momentum
fragmentation functions
5
Francesca Giordano
LEADING AND
NEXT-TO-LEADING TWIST TERMS
implicit sum over quark flavors
interaction dependent
terms neglected
+M2
Q2 C[
2
T
M2 f1D1 + ...]
distribution functions
PDF probabilistic interpretation
f q
1 (x)
gq
1 (x)
hq
1 (x)
legend
transverse and longitu
transverse and longitu
Table 2.1.: Pictorial representation and chiral properties of the
transverse longitudinal
nucleon spin
parton spin
TMDs - Pro
parton with transverse or longit
parton transverse momentum
nucleon with transverse or l
Proton goes out of
parton transverse
momentum
fragmentation functions
5
Francesca Giordano
BOER-MULDERS EFFECT
/ C[ h?
1 H?
1 ]Boer-Mulders effect
kT
kT
Ph?
Ph? sT
sT
6
Francesca Giordano
BOER-MULDERS EFFECT
/ C[ h?
1 H?
1 ]Boer-Mulders effect
kT
kT
Ph?
Ph? sT
sT
correlations between quark transverse spin &
transverse momentum
6
Francesca Giordano
BOER-MULDERS EFFECT
/ C[ h?
1 H?
1 ]Boer-Mulders effect
kT
kT
Ph?
Ph? sT
sT
correlations between quark transverse spin &
transverse momentum
SPIN Effect!
6
Francesca Giordano
BOER-MULDERS EFFECT
/ C[ h?
1 H?
1 ]Boer-Mulders effect
kT
kT
Ph?
Ph? sT
sT
chiral odd chiral odd
chiral even!
}
correlations between quark transverse spin &
transverse momentum
h?
1 H?
1
chiral odd functions
SPIN Effect!
6
Francesca Giordano
BOER-MULDERS EFFECT
/ C[ h?
1 H?
1 ]Boer-Mulders effect
kT
kT
Ph?
Ph? sT
sT
correlations between quark transverse spin &
transverse momentum
chiral odd functions
naive Time reversal odd
SPIN Effect!
6
Francesca Giordano
BOER-MULDERS EFFECT
/ C[ h?
1 H?
1 ]Boer-Mulders effect
kT
kT
Ph?
Ph? sT
sT
Final State Interactions
correlations between quark transverse spin &
transverse momentum
chiral odd functions
naive Time reversal odd
SPIN Effect!
6
u
FSI
u
Francesca Giordano
BOER-MULDERS EFFECT
/ C[ h?
1 H?
1 ]Boer-Mulders effect
kT
kT
Ph?
Ph? sT
sT
Final State Interactions
correlations between quark transverse spin &
transverse momentum
chiral odd functions
naive Time reversal odd
Spatial distortions due to
spin-orbit correlations
SPIN Effect!
6
u
FSI
u
Francesca Giordano
BOER-MULDERS EFFECT
/ C[ h?
1 H?
1 ]Boer-Mulders effect
kT
kT
Ph?
Ph? sT
sT
Final State Interactions
correlations between quark transverse spin &
transverse momentum
chiral odd functions
naive Time reversal odd
Spatial distortions due to
spin-orbit correlations
Collins FF H1 (z,kT
2) correlates transverse spin of fragm
and transverse momentum Ph of produced hadron h
““CollinsCollins--effect”effect”
h
h
q q
left-right (azimuthal) asymmetry in the direction
outgoing hadron
our observable: singleour observable: single--spinspin azimuthalazimuthal asymmasymm
Collins effect
SPIN Effect!
6
u
FSI
u
Francesca Giordano
BOER-MULDERS EFFECT
/ C[ h?
1 H?
1 ]Boer-Mulders effect
kT
kT
Ph?
Ph? sT
sT
Final State Interactions
correlations between quark transverse spin &
transverse momentum
Spatial distortions due to
spin-orbit correlations
Collins FF H1 (z,kT
2) correlates transverse spin of fragm
and transverse momentum Ph of produced hadron h
““CollinsCollins--effect”effect”
h
h
q q
left-right (azimuthal) asymmetry in the direction
outgoing hadron
our observable: singleour observable: single--spinspin azimuthalazimuthal asymmasymm
Collins effect
SPIN Effect!
access to Collins effect
6
u
FSI
u
Francesca Giordano
BOER-MULDERS EFFECT
/ C[ h?
1 H?
1 ]Boer-Mulders effect
kT
kT
Ph?
Ph? sT
sT
correlations between quark transverse spin &
transverse momentum
Cahn effect / C[f1D1]
Ph?
Ph?kT
kT
SPIN Effect!
access to Collins effect
7
Francesca Giordano
BOER-MULDERS EFFECT
/ C[ h?
1 H?
1 ]Boer-Mulders effect
kT
kT
Ph?
Ph? sT
sT
correlations between quark transverse spin &
transverse momentum
Cahn effect / C[f1D1]
Ph?
Ph?kT
kT
kinematic effect generated by parton intrinsic
transverse motion
SPIN Effect!
access to Collins effect
7
Francesca Giordano
BOER-MULDERS EFFECT
/ C[ h?
1 H?
1 ]Boer-Mulders effect
kT
kT
Ph?
Ph? sT
sT
correlations between quark transverse spin &
transverse momentum
Cahn effect / C[f1D1]
Ph?
Ph?kT
kT
kinematic effect generated by parton intrinsic
transverse motion
hq
T i ! cos q
h ! cos H
h
SPIN Effect!
access to Collins effect
7
Francesca Giordano
BOER-MULDERS EFFECT
/ C[ h?
1 H?
1 ]Boer-Mulders effect
kT
kT
Ph?
Ph? sT
sT
correlations between quark transverse spin &
transverse momentum
Cahn effect / C[f1D1]
Ph?
Ph?kT
kT
kinematic effect generated by parton intrinsic
transverse motion
access to parton transverse momenta
hq
T i ! cos q
h ! cos H
h
SPIN Effect!
access to Collins effect
7
Francesca GiordanoFrancesca Giordano
HERMES @ HERA
8
Francesca Giordano
DESY
Francesca Giordano
HERMES @ HERA
8
Francesca Giordano
DESY
Francesca Giordano
HERMES @ HERA
27.6 GeV (e+/e-) lepton
beam off D/H target
8
Francesca Giordano
HERMES
The HERMES Spectrometer
!
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RICH
RICH
DIPOLE
DIPOLE
9
Francesca Giordano
HERMES
The HERMES Spectrometer
!
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EF
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3@:2ABCD
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3;:2ABCD
#"&%2+&0&'*&9.'
27.6 GeV e±
beam
RICH
RICH
DIPOLE
DIPOLE
9
Francesca Giordano
HERMES
The HERMES Spectrometer
!
"
#
!!
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$
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=$0.2,%6!.
1/&%(
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EF
5@<G26E7
3;:2ABCD
3@:2ABCD
3@:2ABCD
3;:2ABCD
#"&%2+&0&'*&9.'
27.6 GeV e±
beam
H/D target
RICH
RICH
DIPOLE
DIPOLE
9
Francesca Giordano
HERMES
The HERMES Spectrometer
!
"
#
!!
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$
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*+,#-./'
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=$0.2,%6!.
1/&%(
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EF
5@<G26E7
3;:2ABCD
3@:2ABCD
3@:2ABCD
3;:2ABCD
#"&%2+&0&'*&9.'
27.6 GeV e±
beam
H/D target
RICH
RICH
DIPOLE
DIPOLE
tracking detectors: momentum resolution <2.5%
9
Francesca Giordano
HERMES
The HERMES Spectrometer
!
"
#
!!
!#
$
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*+,#-./'
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=$0.2,%6!.
1/&%(
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EF
5@<G26E7
3;:2ABCD
3@:2ABCD
3@:2ABCD
3;:2ABCD
#"&%2+&0&'*&9.'
27.6 GeV e±
beam
H/D target
particle identification: lepton/hadron separation
RICH
RICH
DIPOLE
DIPOLE
tracking detectors: momentum resolution <2.5%
9
Francesca Giordano
HERMES
The HERMES Spectrometer
!
"
#
!!
!#
$
!"#$%&'$()
*+,#-./'
0/$1(
1*2345
(,/6.(
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5@<G26E7
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3@:2ABCD
3@:2ABCD
3;:2ABCD
#"&%2+&0&'*&9.'
27.6 GeV e±
beam
H/D target
RICH: discrimination between charged "/ K / p
particle identification: lepton/hadron separation
RICH
RICH
DIPOLE
DIPOLE
tracking detectors: momentum resolution <2.5%
9
Francesca Giordano
HERMES
The HERMES Spectrometer
!
"
#
!!
!#
$
!"#$%&'$()
*+,#-./'
0/$1(
1*2345
(,/6.(
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9/.'+&=./2>+5?
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=$0.2,%6!.
1/&%(
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EF
5@<G26E7
3;:2ABCD
3@:2ABCD
3@:2ABCD
3;:2ABCD
#"&%2+&0&'*&9.'
27.6 GeV e±
beam
H/D target
RICH: discrimination between charged "/ K / p
particle identification: lepton/hadron separation
RICH
RICH
DIPOLE
DIPOLE
tracking detectors: momentum resolution <2.5%
9
Francesca Giordano
ACCEPTANCE CORRECTION
w = (x, y, z, Ph?)
0
w[1 + 2hcos hiw + 2hcos 2 hiw]
10
Francesca Giordano
ACCEPTANCE CORRECTION
w = (x, y, z, Ph?)
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
10
Francesca Giordano
ACCEPTANCE CORRECTION
w = (x, y, z, Ph?)
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
10
Francesca Giordano
ACCEPTANCE CORRECTION
w = (x, y, z, Ph?)
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
34
MC
RAD
MCMCMC
accLn εε=
MC
0σ

Generated in 4⇡
ωφωε dMC
RAD
),()
),(),( φωεφωε RADacc)2cos)( φωB ωd
Inside acceptance
MC
MC simulation of spectrometers to correct for
acceptance/QED radiation
10
Francesca Giordano
ACCEPTANCE CORRECTION
w = (x, y, z, Ph?)
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
34
MC
RAD
MCMCMC
accLn εε=
MC
0σ

Generated in 4⇡
ωφωε dMC
RAD
),()
),(),( φωεφωε RADacc)2cos)( φωB ωd
Inside acceptance
MC
MC simulation of spectrometers to correct for
acceptance/QED radiation
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
n =
Z
L⇥0
w
acc
w, h
rad
w, h
dw
10
Francesca Giordano
ACCEPTANCE CORRECTION
w = (x, y, z, Ph?)
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
34
MC
RAD
MCMCMC
accLn εε=
MC
0σ

Generated in 4⇡
ωφωε dMC
RAD
),()
),(),( φωεφωε RADacc)2cos)( φωB ωd
Inside acceptance
MC
MC simulation of spectrometers to correct for
acceptance/QED radiation
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
n =
Z
L⇥0
w
acc
w, h
rad
w, h
dw
10
Francesca Giordano
ACCEPTANCE CORRECTION
w = (x, y, z, Ph?)
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
34
MC
RAD
MCMCMC
accLn εε=
MC
0σ

Generated in 4⇡
ωφωε dMC
RAD
),()
),(),( φωεφωε RADacc)2cos)( φωB ωd
Inside acceptance
MC
Not allowed!
MC simulation of spectrometers to correct for
acceptance/QED radiation
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
n =
Z
L⇥0
w
acc
w, h
rad
w, h
dw
10
Francesca Giordano
ACCEPTANCE CORRECTION
w = (x, y, z, Ph?)
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
34
MC
RAD
MCMCMC
accLn εε=
MC
0σ

Generated in 4⇡
ωφωε dMC
RAD
),()
),(),( φωεφωε RADacc)2cos)( φωB ωd
Inside acceptance
MC
Not allowed!
MC simulation of spectrometers to correct for
acceptance/QED radiation
only if fully differential ratio (4D binning)
and only in the limit of infinitely small bins
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
n =
Z
L⇥0
w
acc
w, h
rad
w, h
dw
10
Francesca Giordano
w = (x, y, z, Ph?)
(w)4-dimensional
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits #
x 0.023 0.042 0.078 0.145 0.27 0.6 5
y 0.2 0.3 0.45 0.6 0.7 0.85 5
z 0.2 0.3 0.4 0.5 0.6 0.75 1 6
0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph?
unfolding
ACCEPTANCE CORRECTION
11
Francesca Giordano
w = (x, y, z, Ph?)
(w)4-dimensional
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
nborn= S 1
[n B0]
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits #
x 0.023 0.042 0.078 0.145 0.27 0.6 5
y 0.2 0.3 0.45 0.6 0.7 0.85 5
z 0.2 0.3 0.4 0.5 0.6 0.75 1 6
0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph?
unfolding
ACCEPTANCE CORRECTION
11
Francesca Giordano
w = (x, y, z, Ph?)
(w)4-dimensional
describes the acceptance &
smearing between adjacent bins
events smeared in the sample
from outside the acceptance
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
nborn= S 1
[n B0]
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits #
x 0.023 0.042 0.078 0.145 0.27 0.6 5
y 0.2 0.3 0.45 0.6 0.7 0.85 5
z 0.2 0.3 0.4 0.5 0.6 0.75 1 6
0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph?
unfolding
ACCEPTANCE CORRECTION
11
Francesca Giordano
w = (x, y, z, Ph?)
(w)4-dimensional
describes the acceptance &
smearing between adjacent bins
events smeared in the sample
from outside the acceptance
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
A(1 + B cos h + C cos 2 h)
nborn= S 1
[n B0]
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits #
x 0.023 0.042 0.078 0.145 0.27 0.6 5
y 0.2 0.3 0.45 0.6 0.7 0.85 5
z 0.2 0.3 0.4 0.5 0.6 0.75 1 6
0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph?
unfolding
ACCEPTANCE CORRECTION
11
Francesca Giordano
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits #
x 0.023 0.042 0.078 0.145 0.27 0.6 5
y 0.2 0.3 0.45 0.6 0.7 0.85 5
z 0.2 0.3 0.4 0.5 0.6 0.75 1 6
0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph?
PION FIT & PROJECTION
w = (x, y, z, Ph?)
(w)4-dimensional
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
A(1 + B cos h + C cos 2 h)
unfolding
z
x
y
Ph?
12
Francesca Giordano
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits #
x 0.023 0.042 0.078 0.145 0.27 0.6 5
y 0.2 0.3 0.45 0.6 0.7 0.85 5
z 0.2 0.3 0.4 0.5 0.6 0.75 1 6
0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph?
0.023 0.042 0.078 0.145 0.27
0.3 0.45 0.6 0.7 0.85
0.2 0.3 0.4 0.5 0.6 0.75
0.05 0.2 0.35 0.5 0.7 1
PION FIT & PROJECTION
w = (x, y, z, Ph?)
(w)4-dimensional
n =
Z
L⇥0
w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc
w, h
rad
w, h
dw
A(1 + B cos h + C cos 2 h)
unfolding
z
x
y
Ph?
12
Francesca Giordano
Boer-Mulders
Cahn
COS2 : PIONS
Final! / C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
13
arXiv:1204.4161
Francesca Giordano
Cahn expected flavor blind
Boer-Mulders
Cahn
COS2 : PIONS
Final! / C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
13
arXiv:1204.4161
Francesca Giordano
Cahn expected flavor blind
different / amplitudes
Boer-Mulders effect
⇡+
⇡
Boer-Mulders
Cahn
COS2 : PIONS
Final! / C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
13
arXiv:1204.4161
Francesca Giordano
Cahn expected flavor blind
different / amplitudes
Boer-Mulders effect
⇡+
⇡
Boer-Mulders
Cahn
COS2 : PIONS
Final! / C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
SPIN Effect!13
arXiv:1204.4161
Francesca Giordano
Cahn expected flavor blind
different / amplitudes
Boer-Mulders effect
⇡+
⇡
Boer-Mulders
Cahn
Gamberg, Goldstein
Phys. Rev. D77:094016, 2008
COS2 : PIONS
Final! / C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
SPIN Effect!13
arXiv:1204.4161
Francesca Giordano
Cahn expected flavor blind
different / amplitudes
Boer-Mulders effect
⇡+
⇡
Boer-Mulders
Cahn
Zhang et al
Phys. Rev. D78:034035, 2008
Gamberg, Goldstein
Phys. Rev. D77:094016, 2008
COS2 : PIONS
Final! / C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
SPIN Effect!13
arXiv:1204.4161
Francesca Giordano
Cahn expected flavor blind
different / amplitudes
Boer-Mulders effect
⇡+
⇡
Boer-Mulders
Cahn
Barone et al
Phys. Rev. D78:045022, 2008
Zhang et al
Phys. Rev. D78:034035, 2008
Gamberg, Goldstein
Phys. Rev. D77:094016, 2008
COS2 : PIONS
Final! / C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
SPIN Effect!13
arXiv:1204.4161
Francesca Giordano
Cahn expected flavor blind
different / amplitudes
Boer-Mulders effect
⇡+
⇡
Boer-Mulders
Cahn
COS2 : PIONS
Final! / C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
Hydrogen vs Deuterium
SPIN Effect!14
arXiv:1204.4161
Francesca Giordano
Cahn expected flavor blind
different / amplitudes
Boer-Mulders effect
⇡+
⇡
Boer-Mulders
Cahn
COS2 : PIONS
Final! / C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
h?,u
1 ⇡ h?,d
1
Hydrogen vs Deuterium
SPIN Effect!14
arXiv:1204.4161
Francesca Giordano
Cahn expected flavor blind
different / amplitudes
Boer-Mulders effect
⇡+
⇡
COS : PIONS
Final!
/ 2M
Q C[ h?
1 H?
1
f1D1 + ....]
15
arXiv:1204.4161
Francesca Giordano
Cahn
Boer-Mulders
Cahn expected flavor blind
different / amplitudes
Boer-Mulders effect
⇡+
⇡
COS : PIONS
Final!
/ 2M
Q C[ h?
1 H?
1
f1D1 + ....]
15
arXiv:1204.4161
Francesca Giordano
Cahn
/01&"#2'3" 456785988:.#;88<
=>?"#/01&"#@" $A67A5A.#;885
!"
x
-1
10
UU
〉)
h
φcos(〈2
-0.2
-0.1
0
0.1
−
π
+π
y
0.4 0.6 0.8
-0.2
-0.1
0
0.1 Xπe→e p
z
0.4 0.6
-0.2
-0.1
0
0.1
[GeV]⊥h
P
0.2 0.4 0.6 0.8 1
-0.2
-0.1
0
0.1 HERMES preliminary
#$%φ& '$()*+,-$. [ ]...
2
1111
cos
+−−∝ ⊥⊥
DfHh
Q
M
F h
UU Cφ
!"#$%&'()*%+#', -(".#
/01&"#2'3" 456785988:.#;88<
=>?"#/01&"#@" $A67A5A.#;885
Fcos h
UU / C[h?
1 H?
1 f1D1+....]Fcos h
UU / C[h?
1 H?
1 f1D1+....]
Cahn only
Too large!

x
-1
10
UU
〉)
h
φcos(〈2
-0.2
-0.1
0
0.1
−
π
+π
y
0.4 0.6 0.8
-0.2
-0.1
0
0.1 Xπe→e p
z
0.4 0.6
-0.2
-0.1
0
0.1
[GeV]⊥h
P
0.2 0.4 0.6 0.8 1
-0.2
-0.1
0
0.1 HERMES preliminary
φ  [ ]...
2
1111
cos
+−−∝ ⊥⊥
DfHh
Q
M
F h
UU Cφ
 
 
 
Boer-Mulders
Cahn expected flavor blind
different / amplitudes
Boer-Mulders effect
⇡+
⇡
COS : PIONS
Final!
/ 2M
Q C[ h?
1 H?
1
f1D1 + ....]
15
arXiv:1204.4161
Francesca Giordano
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits #
x 0.023 0.042 0.078 0.145 0.27 0.6 5
y 0.2 0.3 0.45 0.6 0.7 0.85 5
z 0.2 0.3 0.4 0.5 0.6 0.75 1 6
0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph?
KAON FIT & PROJECTION
(w)4-dimensional
A(1 + B cos h + C cos 2 h)
unfolding
z
x
y
Ph?
16
Francesca Giordano
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Binning
900 kinematic bins x 12 -bins
Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits #
x 0.023 0.042 0.078 0.145 0.27 0.6 5
y 0.2 0.3 0.45 0.6 0.7 0.85 5
z 0.2 0.3 0.4 0.5 0.6 0.75 1 6
0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph?
KAON FIT & PROJECTION
0.042 0.078 0.145 0.27
0.3 0.45 0.6 0.7
0.3 0.4 0.5 0.6
0.2 0.35 0.5 0.7
(w)4-dimensional
A(1 + B cos h + C cos 2 h)
unfolding
z
x
y
Ph?
16
Francesca GiordanoFrancesca Giordano
COS2 KAONS & PIONS
Final! / C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
17
arXiv:1204.4161
Francesca GiordanoFrancesca Giordano
COS2 KAONS & PIONS
Final!
Boer-Mulders
Cahn
/ C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
17
arXiv:1204.4161
Francesca GiordanoFrancesca Giordano
COS2 KAONS & PIONS
Final!
Boer-Mulders
Cahn
/ C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
No predictions for Kaons!
17
arXiv:1204.4161
Francesca GiordanoFrancesca Giordano
COS2 KAONS & PIONS
Final!
Boer-Mulders
Cahn
/ C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
No predictions for Kaons! Favored dominance for & .
same sign
K+
⇡+
?
17
arXiv:1204.4161
Francesca GiordanoFrancesca Giordano
COS2 KAONS & PIONS
Final!
Boer-Mulders
Cahn
/ C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
No predictions for Kaons! Favored dominance for & .
same sign
K+
⇡+
?
fully sea object!
both favored&unfavored fragmentation
K
17
arXiv:1204.4161
Francesca GiordanoFrancesca Giordano
COS2 KAONS & PIONS
Final!
Boer-Mulders
Cahn
/ C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
No predictions for Kaons! Favored dominance for & .
same sign
K+
⇡+
?
fully sea object!
both favored&unfavored fragmentation
K
Non trivial!
17
arXiv:1204.4161
Francesca GiordanoFrancesca Giordano
COS2 KAONS & PIONS
Final!
Boer-Mulders
Cahn
/ C[ h?
1 H?
1
+
2
T
Q2
f1D1 + ....]
No predictions for Kaons! Favored dominance for & .
same sign
K+
⇡+
?
fully sea object!
both favored&unfavored fragmentation
K
Non trivial!
Collins FF for kaons
soon from Belle
17
arXiv:1204.4161
Francesca Giordano
COS KAONS & PIONS
Final!
No predictions for Kaons!
Similar trends for Pion-Kaon
/ 2M
Q C[ h?
1 H?
1
f1D1 + ....]
18
arXiv:1204.4161
Francesca Giordano
COS KAONS & PIONS
Final!
No predictions for Kaons!
Similar trends for Pion-Kaon ?
Cahn
Boer-Mulders
/ 2M
Q C[ h?
1 H?
1
f1D1 + ....]
18
arXiv:1204.4161
Francesca Giordano
MULTI-D RESULTS
http://durpdg.dur.ac.uk
First 6 bins
19
Francesca Giordano
MULTI-D RESULTS
http://durpdg.dur.ac.uk
First 6 bins
1st x bin
20
Francesca Giordano
MULTI-D RESULTS
http://durpdg.dur.ac.uk
First 6 bins
1st x bin
2nd x bin
20
Francesca Giordano
MULTI-D RESULTS
http://durpdg.dur.ac.uk
First 6 bins
1st x bin
2nd x bin
3rd x bin
20
Francesca Giordano
MULTI-D RESULTS
http://durpdg.dur.ac.uk
First 6 bins
1st x bin
2nd x bin
3rd x bin 4th x bin
20
Francesca Giordano
MULTI-D RESULTS
http://durpdg.dur.ac.uk
First 6 bins
1st x bin
2nd x bin
3rd x bin 4th x bin 5th x bin
20
Francesca Giordano
MULTI-D RESULTS
http://durpdg.dur.ac.uk
First 6 bins
1st x bin
2nd x bin
3rd x bin 4th x bin 5th x bin
HYDROGEN, .
⇡+
DEUTERIUM, .
⇡+
20
Francesca Giordano
MULTI-D RESULTS
http://durpdg.dur.ac.uk
First 6 bins
1st x bin
2nd x bin
3rd x bin 4th x bin 5th x bin
HYDROGEN, .
⇡+
HYDROGEN, .
⇡
DEUTERIUM, .
⇡+
DEUTERIUM, .
⇡
HYDROGEN, .KHYDROGEN, .
K+
DEUTERIUM, .KDEUTERIUM, .
K+
HYDROGEN, .
HYDROGEN, .
DEUTERIUM, .
DEUTERIUM, .
h+
h+
h
h
20
Francesca Giordano
MULTI-D RESULTS
http://durpdg.dur.ac.uk
First 6 bins
1st x bin
2nd x bin
3rd x bin 4th x bin 5th x bin
HYDROGEN, .
⇡+
HYDROGEN, .
⇡
DEUTERIUM, .
⇡+
DEUTERIUM, .
⇡
HYDROGEN, .KHYDROGEN, .
K+
DEUTERIUM, .KDEUTERIUM, .
K+
HYDROGEN, .
HYDROGEN, .
DEUTERIUM, .
DEUTERIUM, .
THERE’S
AN EASIER WAY!
h+
h+
h
h
20
Francesca Giordano
A USEFUL TOOL
http://www-hermes.desy.de/cosnphi/
New!
21
Francesca Giordano
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits #
x 0.02 0.04 0.08 0.15 0.27 0.6 5
y 0.2 0.3 0.45 0.6 0.7 0.85 5
z 0.2 0.3 0.4 0.5 0.6 0.75 1 6
0.05 0.2 0.35 0.5 0.7 1 1 6Ph?
A USEFUL TOOL
New!
z
x
y
Ph?
22
Francesca Giordano
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits #
x 0.02 0.04 0.08 0.15 0.27 0.6 5
y 0.2 0.3 0.45 0.6 0.7 0.85 5
z 0.2 0.3 0.4 0.5 0.6 0.75 1 6
0.05 0.2 0.35 0.5 0.7 1 1 6Ph?
A USEFUL TOOL
New!
z
x
y
Ph?
22
Francesca Giordano
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Binning
900 kinematic bins x 12 - bins
Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits #
x 0.02 0.04 0.08 0.15 0.27 0.6 5
y 0.2 0.3 0.45 0.6 0.7 0.85 5
z 0.2 0.3 0.4 0.5 0.6 0.75 1 6
0.05 0.2 0.35 0.5 0.7 1 1 6Ph?
A USEFUL TOOL
New!
z
x
y
Ph?
22
Francesca Giordano
A USEFUL TOOL
New!
23
Francesca Giordano
UU
cos22
-0.2
-0.1
0
0.1
+h
x
-1
10
UU
cos22
-0.2
-0.1
0
0.1
-
h
y
0.4 0.6 0.8
z
0.4 0.6 0.8
e h Xe p
[GeV]hP
0.2 0.4 0.6 0.8 1 1.2
Systematic errors not shown
Systematic errors not shown
A USEFUL TOOL
New!
23
Francesca Giordano
UU
cos22
-0.2
-0.1
0
0.1
+h
x
-1
10
UU
cos22
-0.2
-0.1
0
0.1
-
h
y
0.4 0.6 0.8
z
0.4 0.6 0.8
e h Xe p
[GeV]hP
0.2 0.4 0.6 0.8 1 1.2
Systematic errors not shown
Systematic errors not shown
A USEFUL TOOL
New!
23
Francesca Giordano
PIONS: MORE PROJECTIONSFull z-dependence
24
Francesca Giordano
PIONS: MORE PROJECTIONSFull z-dependence
24
Francesca Giordano
PIONS: MORE PROJECTIONSFull z-dependence Full -dependencePh?
24
Francesca Giordano
KAONS: MORE PROJECTIONS
Larger z-dependence Larger -dependencePh?
25
Francesca Giordano
KAONS: MORE PROJECTIONS
Larger z-dependence Larger -dependencePh?
25
Francesca Giordano
SUMMARY
To date provides the most complete data
set available for Boer-Mulders and Cahn effects!
 
  



2009 Madrid, 26-30 April 2009
26
Francesca Giordano
Different behavior for with respect to pions:
large signals and same sign for modulation: indication of
same sign for favored/unfavored strange Collins fragmentation
functions?
K+
/K
cos 2 h
SUMMARY
To date provides the most complete data
set available for Boer-Mulders and Cahn effects!
 
  



2009 Madrid, 26-30 April 2009
26
Francesca Giordano
Different behavior for with respect to pions:
large signals and same sign for modulation: indication of
same sign for favored/unfavored strange Collins fragmentation
functions?
K+
/K
cos 2 h
Differences between :
evidence of a non-zero Boer-Mulders function:
confirms opposite sign for favored and unfavored pion Collins
fragmentation functions
+
/
SUMMARY
To date provides the most complete data
set available for Boer-Mulders and Cahn effects!
 
  



2009 Madrid, 26-30 April 2009
26
Francesca Giordano
Different behavior for with respect to pions:
large signals and same sign for modulation: indication of
same sign for favored/unfavored strange Collins fragmentation
functions?
K+
/K
cos 2 h
Differences between :
evidence of a non-zero Boer-Mulders function:
confirms opposite sign for favored and unfavored pion Collins
fragmentation functions
+
/
Similar results for deuterium & hydrogen data
suggest a Boer-Mulders function with same sign for u and d quark
SUMMARY
To date provides the most complete data
set available for Boer-Mulders and Cahn effects!
 
  



2009 Madrid, 26-30 April 2009
26
Francesca Giordano
Different behavior for with respect to pions:
large signals and same sign for modulation: indication of
same sign for favored/unfavored strange Collins fragmentation
functions?
K+
/K
cos 2 h
Differences between :
evidence of a non-zero Boer-Mulders function:
confirms opposite sign for favored and unfavored pion Collins
fragmentation functions
+
/
Thank you!
Similar results for deuterium & hydrogen data
suggest a Boer-Mulders function with same sign for u and d quark
SUMMARY
To date provides the most complete data
set available for Boer-Mulders and Cahn effects!
 
  



2009 Madrid, 26-30 April 2009
26

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F Giordano: spin-dependent effects in spin-averaged DIS

  • 1. SPIN EFFECTS IN UNPOLARIZED SIDIS ati 10 Azimuthal cosine modulations DIS unpolarized cross section rdano b Francesca Giordano SPIN 2012, Dubna, Russia 1
  • 2. Francesca Giordano Collinear case target polarization beam polarization virtual photon polarization d3 ⇤ dxdydz = 2 xyQ2 1 + ⇥2 2x {A(y)FUU,T + B(y)FUU,L} SEMI-INCLUSIVE DIS 2
  • 3. Francesca Giordano target polarization beam polarization virtual photon polarization SEMI-INCLUSIVE DIS 2
  • 4. Francesca Giordano target polarization beam polarization virtual photon polarization SEMI-INCLUSIVE DIS Negative squared 4-momentum transfer to the target Fractional energy of the virtual photon Parton fractional momentum Fractional energy transfer to the produced hadron 2
  • 6. TRANSVERSE MOMENTUM DEPENDENT FUNCTIONS DF σ FF distribution functions PDF probabilistic interpretation f q 1 (x) gq 1 (x) hq 1 (x) legend transverse and longitu transverse and longitu Table 2.1.: Pictorial representation and chiral properties of the transverse longitudinal nucleon spin parton spin TMDs - Pro parton with transverse or longit parton transverse momentum nucleon with transverse or l Proton goes out of parton transverse momentum 3
  • 7. TRANSVERSE MOMENTUM DEPENDENT FUNCTIONS DF σ FF distribution functions fragmentation functions PDF probabilistic interpretation f q 1 (x) gq 1 (x) hq 1 (x) legend transverse and longitu transverse and longitu Table 2.1.: Pictorial representation and chiral properties of the transverse longitudinal nucleon spin parton spin TMDs - Pro parton with transverse or longit parton transverse momentum nucleon with transverse or l Proton goes out of parton transverse momentum 3
  • 8. TRANSVERSE MOMENTUM DEPENDENT FUNCTIONS DF σ FF distribution functions fragmentation functions PDF probabilistic interpretation f q 1 (x) gq 1 (x) hq 1 (x) legend transverse and longitu transverse and longitu Table 2.1.: Pictorial representation and chiral properties of the transverse longitudinal nucleon spin parton spin TMDs - Pro parton with transverse or longit parton transverse momentum nucleon with transverse or l Proton goes out of parton transverse momentum 3
  • 9. TRANSVERSE MOMENTUM DEPENDENT FUNCTIONS DF σ FF distribution functions fragmentation functions Boer-Mulders DF PDF probabilistic interpretation f q 1 (x) gq 1 (x) hq 1 (x) legend transverse and longitu transverse and longitu Table 2.1.: Pictorial representation and chiral properties of the transverse longitudinal nucleon spin parton spin TMDs - Pro parton with transverse or longit parton transverse momentum nucleon with transverse or l Proton goes out of parton transverse momentum 3
  • 10. TRANSVERSE MOMENTUM DEPENDENT FUNCTIONS DF σ FF distribution functions fragmentation functions Boer-Mulders DF Collins FF PDF probabilistic interpretation f q 1 (x) gq 1 (x) hq 1 (x) legend transverse and longitu transverse and longitu Table 2.1.: Pictorial representation and chiral properties of the transverse longitudinal nucleon spin parton spin TMDs - Pro parton with transverse or longit parton transverse momentum nucleon with transverse or l Proton goes out of parton transverse momentum 3
  • 11. Francesca Giordano PDF probabilistic interpretation f q 1 (x) gq 1 (x) hq 1 (x) legend transverse and longitu transverse and longitu Table 2.1.: Pictorial representation and chiral properties of the transverse longitudinal nucleon spin parton spin TMDs - Pro parton with transverse or longit parton transverse momentum nucleon with transverse or l Proton goes out of parton transverse momentum LEADING TWIST TERMS implicit sum over quark flavors distribution functions fragmentation functions 4
  • 12. Francesca Giordano LEADING AND NEXT-TO-LEADING TWIST TERMS implicit sum over quark flavors distribution functions PDF probabilistic interpretation f q 1 (x) gq 1 (x) hq 1 (x) legend transverse and longitu transverse and longitu Table 2.1.: Pictorial representation and chiral properties of the transverse longitudinal nucleon spin parton spin TMDs - Pro parton with transverse or longit parton transverse momentum nucleon with transverse or l Proton goes out of parton transverse momentum fragmentation functions 5
  • 13. Francesca Giordano LEADING AND NEXT-TO-LEADING TWIST TERMS implicit sum over quark flavors distribution functions PDF probabilistic interpretation f q 1 (x) gq 1 (x) hq 1 (x) legend transverse and longitu transverse and longitu Table 2.1.: Pictorial representation and chiral properties of the transverse longitudinal nucleon spin parton spin TMDs - Pro parton with transverse or longit parton transverse momentum nucleon with transverse or l Proton goes out of parton transverse momentum fragmentation functions 5
  • 14. Francesca Giordano LEADING AND NEXT-TO-LEADING TWIST TERMS implicit sum over quark flavors interaction dependent terms neglected distribution functions PDF probabilistic interpretation f q 1 (x) gq 1 (x) hq 1 (x) legend transverse and longitu transverse and longitu Table 2.1.: Pictorial representation and chiral properties of the transverse longitudinal nucleon spin parton spin TMDs - Pro parton with transverse or longit parton transverse momentum nucleon with transverse or l Proton goes out of parton transverse momentum fragmentation functions 5
  • 15. Francesca Giordano LEADING AND NEXT-TO-LEADING TWIST TERMS implicit sum over quark flavors interaction dependent terms neglected +M2 Q2 C[ 2 T M2 f1D1 + ...] distribution functions PDF probabilistic interpretation f q 1 (x) gq 1 (x) hq 1 (x) legend transverse and longitu transverse and longitu Table 2.1.: Pictorial representation and chiral properties of the transverse longitudinal nucleon spin parton spin TMDs - Pro parton with transverse or longit parton transverse momentum nucleon with transverse or l Proton goes out of parton transverse momentum fragmentation functions 5
  • 16. Francesca Giordano BOER-MULDERS EFFECT / C[ h? 1 H? 1 ]Boer-Mulders effect kT kT Ph? Ph? sT sT 6
  • 17. Francesca Giordano BOER-MULDERS EFFECT / C[ h? 1 H? 1 ]Boer-Mulders effect kT kT Ph? Ph? sT sT correlations between quark transverse spin & transverse momentum 6
  • 18. Francesca Giordano BOER-MULDERS EFFECT / C[ h? 1 H? 1 ]Boer-Mulders effect kT kT Ph? Ph? sT sT correlations between quark transverse spin & transverse momentum SPIN Effect! 6
  • 19. Francesca Giordano BOER-MULDERS EFFECT / C[ h? 1 H? 1 ]Boer-Mulders effect kT kT Ph? Ph? sT sT chiral odd chiral odd chiral even! } correlations between quark transverse spin & transverse momentum h? 1 H? 1 chiral odd functions SPIN Effect! 6
  • 20. Francesca Giordano BOER-MULDERS EFFECT / C[ h? 1 H? 1 ]Boer-Mulders effect kT kT Ph? Ph? sT sT correlations between quark transverse spin & transverse momentum chiral odd functions naive Time reversal odd SPIN Effect! 6
  • 21. Francesca Giordano BOER-MULDERS EFFECT / C[ h? 1 H? 1 ]Boer-Mulders effect kT kT Ph? Ph? sT sT Final State Interactions correlations between quark transverse spin & transverse momentum chiral odd functions naive Time reversal odd SPIN Effect! 6 u FSI u
  • 22. Francesca Giordano BOER-MULDERS EFFECT / C[ h? 1 H? 1 ]Boer-Mulders effect kT kT Ph? Ph? sT sT Final State Interactions correlations between quark transverse spin & transverse momentum chiral odd functions naive Time reversal odd Spatial distortions due to spin-orbit correlations SPIN Effect! 6 u FSI u
  • 23. Francesca Giordano BOER-MULDERS EFFECT / C[ h? 1 H? 1 ]Boer-Mulders effect kT kT Ph? Ph? sT sT Final State Interactions correlations between quark transverse spin & transverse momentum chiral odd functions naive Time reversal odd Spatial distortions due to spin-orbit correlations Collins FF H1 (z,kT 2) correlates transverse spin of fragm and transverse momentum Ph of produced hadron h ““CollinsCollins--effect”effect” h h q q left-right (azimuthal) asymmetry in the direction outgoing hadron our observable: singleour observable: single--spinspin azimuthalazimuthal asymmasymm Collins effect SPIN Effect! 6 u FSI u
  • 24. Francesca Giordano BOER-MULDERS EFFECT / C[ h? 1 H? 1 ]Boer-Mulders effect kT kT Ph? Ph? sT sT Final State Interactions correlations between quark transverse spin & transverse momentum Spatial distortions due to spin-orbit correlations Collins FF H1 (z,kT 2) correlates transverse spin of fragm and transverse momentum Ph of produced hadron h ““CollinsCollins--effect”effect” h h q q left-right (azimuthal) asymmetry in the direction outgoing hadron our observable: singleour observable: single--spinspin azimuthalazimuthal asymmasymm Collins effect SPIN Effect! access to Collins effect 6 u FSI u
  • 25. Francesca Giordano BOER-MULDERS EFFECT / C[ h? 1 H? 1 ]Boer-Mulders effect kT kT Ph? Ph? sT sT correlations between quark transverse spin & transverse momentum Cahn effect / C[f1D1] Ph? Ph?kT kT SPIN Effect! access to Collins effect 7
  • 26. Francesca Giordano BOER-MULDERS EFFECT / C[ h? 1 H? 1 ]Boer-Mulders effect kT kT Ph? Ph? sT sT correlations between quark transverse spin & transverse momentum Cahn effect / C[f1D1] Ph? Ph?kT kT kinematic effect generated by parton intrinsic transverse motion SPIN Effect! access to Collins effect 7
  • 27. Francesca Giordano BOER-MULDERS EFFECT / C[ h? 1 H? 1 ]Boer-Mulders effect kT kT Ph? Ph? sT sT correlations between quark transverse spin & transverse momentum Cahn effect / C[f1D1] Ph? Ph?kT kT kinematic effect generated by parton intrinsic transverse motion hq T i ! cos q h ! cos H h SPIN Effect! access to Collins effect 7
  • 28. Francesca Giordano BOER-MULDERS EFFECT / C[ h? 1 H? 1 ]Boer-Mulders effect kT kT Ph? Ph? sT sT correlations between quark transverse spin & transverse momentum Cahn effect / C[f1D1] Ph? Ph?kT kT kinematic effect generated by parton intrinsic transverse motion access to parton transverse momenta hq T i ! cos q h ! cos H h SPIN Effect! access to Collins effect 7
  • 31. Francesca Giordano DESY Francesca Giordano HERMES @ HERA 27.6 GeV (e+/e-) lepton beam off D/H target 8
  • 32. Francesca Giordano HERMES The HERMES Spectrometer ! " # !! !# $ !"#$%&'$() *+,#-./' 0/$1( 1*2345 (,/6.( *.!! 07* #*23!8 +&0&'*&9.2+: #&%$(&/ -*2345 -*284; (/0 9/&9< *+,#-./' 1$.!02*!,#9' 9/.'+&=./2>+5? '(..!29!,(. *,!&/$#.(./ 0/$1(2*+,#-./' (/$66./2+&0&'*&9.2+3 " ! # % & ' ( ) * + !" /$*+ 5@:2ABCD 5@:2ABCD #"&%2+&0&'*&9. =$0.2,%6!. 1/&%( #"&% +&0& #,6%.( $ $/&%2=,!! EF 5@<G26E7 3;:2ABCD 3@:2ABCD 3@:2ABCD 3;:2ABCD #"&%2+&0&'*&9.' RICH RICH DIPOLE DIPOLE 9
  • 33. Francesca Giordano HERMES The HERMES Spectrometer ! " # !! !# $ !"#$%&'$() *+,#-./' 0/$1( 1*2345 (,/6.( *.!! 07* #*23!8 +&0&'*&9.2+: #&%$(&/ -*2345 -*284; (/0 9/&9< *+,#-./' 1$.!02*!,#9' 9/.'+&=./2>+5? '(..!29!,(. *,!&/$#.(./ 0/$1(2*+,#-./' (/$66./2+&0&'*&9.2+3 " ! # % & ' ( ) * + !" /$*+ 5@:2ABCD 5@:2ABCD #"&%2+&0&'*&9. =$0.2,%6!. 1/&%( #"&% +&0& #,6%.( $ $/&%2=,!! EF 5@<G26E7 3;:2ABCD 3@:2ABCD 3@:2ABCD 3;:2ABCD #"&%2+&0&'*&9.' 27.6 GeV e± beam RICH RICH DIPOLE DIPOLE 9
  • 34. Francesca Giordano HERMES The HERMES Spectrometer ! " # !! !# $ !"#$%&'$() *+,#-./' 0/$1( 1*2345 (,/6.( *.!! 07* #*23!8 +&0&'*&9.2+: #&%$(&/ -*2345 -*284; (/0 9/&9< *+,#-./' 1$.!02*!,#9' 9/.'+&=./2>+5? '(..!29!,(. *,!&/$#.(./ 0/$1(2*+,#-./' (/$66./2+&0&'*&9.2+3 " ! # % & ' ( ) * + !" /$*+ 5@:2ABCD 5@:2ABCD #"&%2+&0&'*&9. =$0.2,%6!. 1/&%( #"&% +&0& #,6%.( $ $/&%2=,!! EF 5@<G26E7 3;:2ABCD 3@:2ABCD 3@:2ABCD 3;:2ABCD #"&%2+&0&'*&9.' 27.6 GeV e± beam H/D target RICH RICH DIPOLE DIPOLE 9
  • 35. Francesca Giordano HERMES The HERMES Spectrometer ! " # !! !# $ !"#$%&'$() *+,#-./' 0/$1( 1*2345 (,/6.( *.!! 07* #*23!8 +&0&'*&9.2+: #&%$(&/ -*2345 -*284; (/0 9/&9< *+,#-./' 1$.!02*!,#9' 9/.'+&=./2>+5? '(..!29!,(. *,!&/$#.(./ 0/$1(2*+,#-./' (/$66./2+&0&'*&9.2+3 " ! # % & ' ( ) * + !" /$*+ 5@:2ABCD 5@:2ABCD #"&%2+&0&'*&9. =$0.2,%6!. 1/&%( #"&% +&0& #,6%.( $ $/&%2=,!! EF 5@<G26E7 3;:2ABCD 3@:2ABCD 3@:2ABCD 3;:2ABCD #"&%2+&0&'*&9.' 27.6 GeV e± beam H/D target RICH RICH DIPOLE DIPOLE tracking detectors: momentum resolution <2.5% 9
  • 36. Francesca Giordano HERMES The HERMES Spectrometer ! " # !! !# $ !"#$%&'$() *+,#-./' 0/$1( 1*2345 (,/6.( *.!! 07* #*23!8 +&0&'*&9.2+: #&%$(&/ -*2345 -*284; (/0 9/&9< *+,#-./' 1$.!02*!,#9' 9/.'+&=./2>+5? '(..!29!,(. *,!&/$#.(./ 0/$1(2*+,#-./' (/$66./2+&0&'*&9.2+3 " ! # % & ' ( ) * + !" /$*+ 5@:2ABCD 5@:2ABCD #"&%2+&0&'*&9. =$0.2,%6!. 1/&%( #"&% +&0& #,6%.( $ $/&%2=,!! EF 5@<G26E7 3;:2ABCD 3@:2ABCD 3@:2ABCD 3;:2ABCD #"&%2+&0&'*&9.' 27.6 GeV e± beam H/D target particle identification: lepton/hadron separation RICH RICH DIPOLE DIPOLE tracking detectors: momentum resolution <2.5% 9
  • 37. Francesca Giordano HERMES The HERMES Spectrometer ! " # !! !# $ !"#$%&'$() *+,#-./' 0/$1( 1*2345 (,/6.( *.!! 07* #*23!8 +&0&'*&9.2+: #&%$(&/ -*2345 -*284; (/0 9/&9< *+,#-./' 1$.!02*!,#9' 9/.'+&=./2>+5? '(..!29!,(. *,!&/$#.(./ 0/$1(2*+,#-./' (/$66./2+&0&'*&9.2+3 " ! # % & ' ( ) * + !" /$*+ 5@:2ABCD 5@:2ABCD #"&%2+&0&'*&9. =$0.2,%6!. 1/&%( #"&% +&0& #,6%.( $ $/&%2=,!! EF 5@<G26E7 3;:2ABCD 3@:2ABCD 3@:2ABCD 3;:2ABCD #"&%2+&0&'*&9.' 27.6 GeV e± beam H/D target RICH: discrimination between charged "/ K / p particle identification: lepton/hadron separation RICH RICH DIPOLE DIPOLE tracking detectors: momentum resolution <2.5% 9
  • 38. Francesca Giordano HERMES The HERMES Spectrometer ! " # !! !# $ !"#$%&'$() *+,#-./' 0/$1( 1*2345 (,/6.( *.!! 07* #*23!8 +&0&'*&9.2+: #&%$(&/ -*2345 -*284; (/0 9/&9< *+,#-./' 1$.!02*!,#9' 9/.'+&=./2>+5? '(..!29!,(. *,!&/$#.(./ 0/$1(2*+,#-./' (/$66./2+&0&'*&9.2+3 " ! # % & ' ( ) * + !" /$*+ 5@:2ABCD 5@:2ABCD #"&%2+&0&'*&9. =$0.2,%6!. 1/&%( #"&% +&0& #,6%.( $ $/&%2=,!! EF 5@<G26E7 3;:2ABCD 3@:2ABCD 3@:2ABCD 3;:2ABCD #"&%2+&0&'*&9.' 27.6 GeV e± beam H/D target RICH: discrimination between charged "/ K / p particle identification: lepton/hadron separation RICH RICH DIPOLE DIPOLE tracking detectors: momentum resolution <2.5% 9
  • 39. Francesca Giordano ACCEPTANCE CORRECTION w = (x, y, z, Ph?) 0 w[1 + 2hcos hiw + 2hcos 2 hiw] 10
  • 40. Francesca Giordano ACCEPTANCE CORRECTION w = (x, y, z, Ph?) n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw 10
  • 41. Francesca Giordano ACCEPTANCE CORRECTION w = (x, y, z, Ph?) n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw 10
  • 42. Francesca Giordano ACCEPTANCE CORRECTION w = (x, y, z, Ph?) n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw 34 MC RAD MCMCMC accLn εε= MC 0σ  Generated in 4⇡ ωφωε dMC RAD ),() ),(),( φωεφωε RADacc)2cos)( φωB ωd Inside acceptance MC MC simulation of spectrometers to correct for acceptance/QED radiation 10
  • 43. Francesca Giordano ACCEPTANCE CORRECTION w = (x, y, z, Ph?) n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw 34 MC RAD MCMCMC accLn εε= MC 0σ  Generated in 4⇡ ωφωε dMC RAD ),() ),(),( φωεφωε RADacc)2cos)( φωB ωd Inside acceptance MC MC simulation of spectrometers to correct for acceptance/QED radiation n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw n = Z L⇥0 w acc w, h rad w, h dw 10
  • 44. Francesca Giordano ACCEPTANCE CORRECTION w = (x, y, z, Ph?) n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw 34 MC RAD MCMCMC accLn εε= MC 0σ  Generated in 4⇡ ωφωε dMC RAD ),() ),(),( φωεφωε RADacc)2cos)( φωB ωd Inside acceptance MC MC simulation of spectrometers to correct for acceptance/QED radiation n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw n = Z L⇥0 w acc w, h rad w, h dw 10
  • 45. Francesca Giordano ACCEPTANCE CORRECTION w = (x, y, z, Ph?) n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw 34 MC RAD MCMCMC accLn εε= MC 0σ  Generated in 4⇡ ωφωε dMC RAD ),() ),(),( φωεφωε RADacc)2cos)( φωB ωd Inside acceptance MC Not allowed! MC simulation of spectrometers to correct for acceptance/QED radiation n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw n = Z L⇥0 w acc w, h rad w, h dw 10
  • 46. Francesca Giordano ACCEPTANCE CORRECTION w = (x, y, z, Ph?) n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw 34 MC RAD MCMCMC accLn εε= MC 0σ  Generated in 4⇡ ωφωε dMC RAD ),() ),(),( φωεφωε RADacc)2cos)( φωB ωd Inside acceptance MC Not allowed! MC simulation of spectrometers to correct for acceptance/QED radiation only if fully differential ratio (4D binning) and only in the limit of infinitely small bins n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw n = Z L⇥0 w acc w, h rad w, h dw 10
  • 47. Francesca Giordano w = (x, y, z, Ph?) (w)4-dimensional n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits # x 0.023 0.042 0.078 0.145 0.27 0.6 5 y 0.2 0.3 0.45 0.6 0.7 0.85 5 z 0.2 0.3 0.4 0.5 0.6 0.75 1 6 0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph? unfolding ACCEPTANCE CORRECTION 11
  • 48. Francesca Giordano w = (x, y, z, Ph?) (w)4-dimensional n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw nborn= S 1 [n B0] Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits # x 0.023 0.042 0.078 0.145 0.27 0.6 5 y 0.2 0.3 0.45 0.6 0.7 0.85 5 z 0.2 0.3 0.4 0.5 0.6 0.75 1 6 0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph? unfolding ACCEPTANCE CORRECTION 11
  • 49. Francesca Giordano w = (x, y, z, Ph?) (w)4-dimensional describes the acceptance & smearing between adjacent bins events smeared in the sample from outside the acceptance n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw nborn= S 1 [n B0] Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits # x 0.023 0.042 0.078 0.145 0.27 0.6 5 y 0.2 0.3 0.45 0.6 0.7 0.85 5 z 0.2 0.3 0.4 0.5 0.6 0.75 1 6 0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph? unfolding ACCEPTANCE CORRECTION 11
  • 50. Francesca Giordano w = (x, y, z, Ph?) (w)4-dimensional describes the acceptance & smearing between adjacent bins events smeared in the sample from outside the acceptance n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw A(1 + B cos h + C cos 2 h) nborn= S 1 [n B0] Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits # x 0.023 0.042 0.078 0.145 0.27 0.6 5 y 0.2 0.3 0.45 0.6 0.7 0.85 5 z 0.2 0.3 0.4 0.5 0.6 0.75 1 6 0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph? unfolding ACCEPTANCE CORRECTION 11
  • 51. Francesca Giordano Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits # x 0.023 0.042 0.078 0.145 0.27 0.6 5 y 0.2 0.3 0.45 0.6 0.7 0.85 5 z 0.2 0.3 0.4 0.5 0.6 0.75 1 6 0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph? PION FIT & PROJECTION w = (x, y, z, Ph?) (w)4-dimensional n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw A(1 + B cos h + C cos 2 h) unfolding z x y Ph? 12
  • 52. Francesca Giordano Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits # x 0.023 0.042 0.078 0.145 0.27 0.6 5 y 0.2 0.3 0.45 0.6 0.7 0.85 5 z 0.2 0.3 0.4 0.5 0.6 0.75 1 6 0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph? 0.023 0.042 0.078 0.145 0.27 0.3 0.45 0.6 0.7 0.85 0.2 0.3 0.4 0.5 0.6 0.75 0.05 0.2 0.35 0.5 0.7 1 PION FIT & PROJECTION w = (x, y, z, Ph?) (w)4-dimensional n = Z L⇥0 w[1 + 2hcos ⇤hiw + 2hcos 2⇤hiw] acc w, h rad w, h dw A(1 + B cos h + C cos 2 h) unfolding z x y Ph? 12
  • 53. Francesca Giordano Boer-Mulders Cahn COS2 : PIONS Final! / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] 13 arXiv:1204.4161
  • 54. Francesca Giordano Cahn expected flavor blind Boer-Mulders Cahn COS2 : PIONS Final! / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] 13 arXiv:1204.4161
  • 55. Francesca Giordano Cahn expected flavor blind different / amplitudes Boer-Mulders effect ⇡+ ⇡ Boer-Mulders Cahn COS2 : PIONS Final! / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] 13 arXiv:1204.4161
  • 56. Francesca Giordano Cahn expected flavor blind different / amplitudes Boer-Mulders effect ⇡+ ⇡ Boer-Mulders Cahn COS2 : PIONS Final! / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] SPIN Effect!13 arXiv:1204.4161
  • 57. Francesca Giordano Cahn expected flavor blind different / amplitudes Boer-Mulders effect ⇡+ ⇡ Boer-Mulders Cahn Gamberg, Goldstein Phys. Rev. D77:094016, 2008 COS2 : PIONS Final! / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] SPIN Effect!13 arXiv:1204.4161
  • 58. Francesca Giordano Cahn expected flavor blind different / amplitudes Boer-Mulders effect ⇡+ ⇡ Boer-Mulders Cahn Zhang et al Phys. Rev. D78:034035, 2008 Gamberg, Goldstein Phys. Rev. D77:094016, 2008 COS2 : PIONS Final! / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] SPIN Effect!13 arXiv:1204.4161
  • 59. Francesca Giordano Cahn expected flavor blind different / amplitudes Boer-Mulders effect ⇡+ ⇡ Boer-Mulders Cahn Barone et al Phys. Rev. D78:045022, 2008 Zhang et al Phys. Rev. D78:034035, 2008 Gamberg, Goldstein Phys. Rev. D77:094016, 2008 COS2 : PIONS Final! / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] SPIN Effect!13 arXiv:1204.4161
  • 60. Francesca Giordano Cahn expected flavor blind different / amplitudes Boer-Mulders effect ⇡+ ⇡ Boer-Mulders Cahn COS2 : PIONS Final! / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] Hydrogen vs Deuterium SPIN Effect!14 arXiv:1204.4161
  • 61. Francesca Giordano Cahn expected flavor blind different / amplitudes Boer-Mulders effect ⇡+ ⇡ Boer-Mulders Cahn COS2 : PIONS Final! / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] h?,u 1 ⇡ h?,d 1 Hydrogen vs Deuterium SPIN Effect!14 arXiv:1204.4161
  • 62. Francesca Giordano Cahn expected flavor blind different / amplitudes Boer-Mulders effect ⇡+ ⇡ COS : PIONS Final! / 2M Q C[ h? 1 H? 1 f1D1 + ....] 15 arXiv:1204.4161
  • 63. Francesca Giordano Cahn Boer-Mulders Cahn expected flavor blind different / amplitudes Boer-Mulders effect ⇡+ ⇡ COS : PIONS Final! / 2M Q C[ h? 1 H? 1 f1D1 + ....] 15 arXiv:1204.4161
  • 64. Francesca Giordano Cahn /01&"#2'3" 456785988:.#;88< =>?"#/01&"#@" $A67A5A.#;885 !" x -1 10 UU 〉) h φcos(〈2 -0.2 -0.1 0 0.1 − π +π y 0.4 0.6 0.8 -0.2 -0.1 0 0.1 Xπe→e p z 0.4 0.6 -0.2 -0.1 0 0.1 [GeV]⊥h P 0.2 0.4 0.6 0.8 1 -0.2 -0.1 0 0.1 HERMES preliminary #$%φ& '$()*+,-$. [ ]... 2 1111 cos +−−∝ ⊥⊥ DfHh Q M F h UU Cφ !"#$%&'()*%+#', -(".# /01&"#2'3" 456785988:.#;88< =>?"#/01&"#@" $A67A5A.#;885 Fcos h UU / C[h? 1 H? 1 f1D1+....]Fcos h UU / C[h? 1 H? 1 f1D1+....] Cahn only Too large!  x -1 10 UU 〉) h φcos(〈2 -0.2 -0.1 0 0.1 − π +π y 0.4 0.6 0.8 -0.2 -0.1 0 0.1 Xπe→e p z 0.4 0.6 -0.2 -0.1 0 0.1 [GeV]⊥h P 0.2 0.4 0.6 0.8 1 -0.2 -0.1 0 0.1 HERMES preliminary φ  [ ]... 2 1111 cos +−−∝ ⊥⊥ DfHh Q M F h UU Cφ       Boer-Mulders Cahn expected flavor blind different / amplitudes Boer-Mulders effect ⇡+ ⇡ COS : PIONS Final! / 2M Q C[ h? 1 H? 1 f1D1 + ....] 15 arXiv:1204.4161
  • 65. Francesca Giordano Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits # x 0.023 0.042 0.078 0.145 0.27 0.6 5 y 0.2 0.3 0.45 0.6 0.7 0.85 5 z 0.2 0.3 0.4 0.5 0.6 0.75 1 6 0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph? KAON FIT & PROJECTION (w)4-dimensional A(1 + B cos h + C cos 2 h) unfolding z x y Ph? 16
  • 66. Francesca Giordano Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Binning 900 kinematic bins x 12 -bins Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits # x 0.023 0.042 0.078 0.145 0.27 0.6 5 y 0.2 0.3 0.45 0.6 0.7 0.85 5 z 0.2 0.3 0.4 0.5 0.6 0.75 1 6 0.05 0.2 0.35 0.5 0.7 1 1.3 6Ph? KAON FIT & PROJECTION 0.042 0.078 0.145 0.27 0.3 0.45 0.6 0.7 0.3 0.4 0.5 0.6 0.2 0.35 0.5 0.7 (w)4-dimensional A(1 + B cos h + C cos 2 h) unfolding z x y Ph? 16
  • 67. Francesca GiordanoFrancesca Giordano COS2 KAONS & PIONS Final! / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] 17 arXiv:1204.4161
  • 68. Francesca GiordanoFrancesca Giordano COS2 KAONS & PIONS Final! Boer-Mulders Cahn / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] 17 arXiv:1204.4161
  • 69. Francesca GiordanoFrancesca Giordano COS2 KAONS & PIONS Final! Boer-Mulders Cahn / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] No predictions for Kaons! 17 arXiv:1204.4161
  • 70. Francesca GiordanoFrancesca Giordano COS2 KAONS & PIONS Final! Boer-Mulders Cahn / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] No predictions for Kaons! Favored dominance for & . same sign K+ ⇡+ ? 17 arXiv:1204.4161
  • 71. Francesca GiordanoFrancesca Giordano COS2 KAONS & PIONS Final! Boer-Mulders Cahn / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] No predictions for Kaons! Favored dominance for & . same sign K+ ⇡+ ? fully sea object! both favored&unfavored fragmentation K 17 arXiv:1204.4161
  • 72. Francesca GiordanoFrancesca Giordano COS2 KAONS & PIONS Final! Boer-Mulders Cahn / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] No predictions for Kaons! Favored dominance for & . same sign K+ ⇡+ ? fully sea object! both favored&unfavored fragmentation K Non trivial! 17 arXiv:1204.4161
  • 73. Francesca GiordanoFrancesca Giordano COS2 KAONS & PIONS Final! Boer-Mulders Cahn / C[ h? 1 H? 1 + 2 T Q2 f1D1 + ....] No predictions for Kaons! Favored dominance for & . same sign K+ ⇡+ ? fully sea object! both favored&unfavored fragmentation K Non trivial! Collins FF for kaons soon from Belle 17 arXiv:1204.4161
  • 74. Francesca Giordano COS KAONS & PIONS Final! No predictions for Kaons! Similar trends for Pion-Kaon / 2M Q C[ h? 1 H? 1 f1D1 + ....] 18 arXiv:1204.4161
  • 75. Francesca Giordano COS KAONS & PIONS Final! No predictions for Kaons! Similar trends for Pion-Kaon ? Cahn Boer-Mulders / 2M Q C[ h? 1 H? 1 f1D1 + ....] 18 arXiv:1204.4161
  • 79. Francesca Giordano MULTI-D RESULTS http://durpdg.dur.ac.uk First 6 bins 1st x bin 2nd x bin 3rd x bin 20
  • 80. Francesca Giordano MULTI-D RESULTS http://durpdg.dur.ac.uk First 6 bins 1st x bin 2nd x bin 3rd x bin 4th x bin 20
  • 81. Francesca Giordano MULTI-D RESULTS http://durpdg.dur.ac.uk First 6 bins 1st x bin 2nd x bin 3rd x bin 4th x bin 5th x bin 20
  • 82. Francesca Giordano MULTI-D RESULTS http://durpdg.dur.ac.uk First 6 bins 1st x bin 2nd x bin 3rd x bin 4th x bin 5th x bin HYDROGEN, . ⇡+ DEUTERIUM, . ⇡+ 20
  • 83. Francesca Giordano MULTI-D RESULTS http://durpdg.dur.ac.uk First 6 bins 1st x bin 2nd x bin 3rd x bin 4th x bin 5th x bin HYDROGEN, . ⇡+ HYDROGEN, . ⇡ DEUTERIUM, . ⇡+ DEUTERIUM, . ⇡ HYDROGEN, .KHYDROGEN, . K+ DEUTERIUM, .KDEUTERIUM, . K+ HYDROGEN, . HYDROGEN, . DEUTERIUM, . DEUTERIUM, . h+ h+ h h 20
  • 84. Francesca Giordano MULTI-D RESULTS http://durpdg.dur.ac.uk First 6 bins 1st x bin 2nd x bin 3rd x bin 4th x bin 5th x bin HYDROGEN, . ⇡+ HYDROGEN, . ⇡ DEUTERIUM, . ⇡+ DEUTERIUM, . ⇡ HYDROGEN, .KHYDROGEN, . K+ DEUTERIUM, .KDEUTERIUM, . K+ HYDROGEN, . HYDROGEN, . DEUTERIUM, . DEUTERIUM, . THERE’S AN EASIER WAY! h+ h+ h h 20
  • 85. Francesca Giordano A USEFUL TOOL http://www-hermes.desy.de/cosnphi/ New! 21
  • 86. Francesca Giordano Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits # x 0.02 0.04 0.08 0.15 0.27 0.6 5 y 0.2 0.3 0.45 0.6 0.7 0.85 5 z 0.2 0.3 0.4 0.5 0.6 0.75 1 6 0.05 0.2 0.35 0.5 0.7 1 1 6Ph? A USEFUL TOOL New! z x y Ph? 22
  • 87. Francesca Giordano Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits # x 0.02 0.04 0.08 0.15 0.27 0.6 5 y 0.2 0.3 0.45 0.6 0.7 0.85 5 z 0.2 0.3 0.4 0.5 0.6 0.75 1 6 0.05 0.2 0.35 0.5 0.7 1 1 6Ph? A USEFUL TOOL New! z x y Ph? 22
  • 88. Francesca Giordano Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Binning 900 kinematic bins x 12 - bins Variable Bin limitsBin limitsBin limitsBin limitsBin limitsBin limitsBin limits # x 0.02 0.04 0.08 0.15 0.27 0.6 5 y 0.2 0.3 0.45 0.6 0.7 0.85 5 z 0.2 0.3 0.4 0.5 0.6 0.75 1 6 0.05 0.2 0.35 0.5 0.7 1 1 6Ph? A USEFUL TOOL New! z x y Ph? 22
  • 90. Francesca Giordano UU cos22 -0.2 -0.1 0 0.1 +h x -1 10 UU cos22 -0.2 -0.1 0 0.1 - h y 0.4 0.6 0.8 z 0.4 0.6 0.8 e h Xe p [GeV]hP 0.2 0.4 0.6 0.8 1 1.2 Systematic errors not shown Systematic errors not shown A USEFUL TOOL New! 23
  • 91. Francesca Giordano UU cos22 -0.2 -0.1 0 0.1 +h x -1 10 UU cos22 -0.2 -0.1 0 0.1 - h y 0.4 0.6 0.8 z 0.4 0.6 0.8 e h Xe p [GeV]hP 0.2 0.4 0.6 0.8 1 1.2 Systematic errors not shown Systematic errors not shown A USEFUL TOOL New! 23
  • 92. Francesca Giordano PIONS: MORE PROJECTIONSFull z-dependence 24
  • 93. Francesca Giordano PIONS: MORE PROJECTIONSFull z-dependence 24
  • 94. Francesca Giordano PIONS: MORE PROJECTIONSFull z-dependence Full -dependencePh? 24
  • 95. Francesca Giordano KAONS: MORE PROJECTIONS Larger z-dependence Larger -dependencePh? 25
  • 96. Francesca Giordano KAONS: MORE PROJECTIONS Larger z-dependence Larger -dependencePh? 25
  • 97. Francesca Giordano SUMMARY To date provides the most complete data set available for Boer-Mulders and Cahn effects!         2009 Madrid, 26-30 April 2009 26
  • 98. Francesca Giordano Different behavior for with respect to pions: large signals and same sign for modulation: indication of same sign for favored/unfavored strange Collins fragmentation functions? K+ /K cos 2 h SUMMARY To date provides the most complete data set available for Boer-Mulders and Cahn effects!         2009 Madrid, 26-30 April 2009 26
  • 99. Francesca Giordano Different behavior for with respect to pions: large signals and same sign for modulation: indication of same sign for favored/unfavored strange Collins fragmentation functions? K+ /K cos 2 h Differences between : evidence of a non-zero Boer-Mulders function: confirms opposite sign for favored and unfavored pion Collins fragmentation functions + / SUMMARY To date provides the most complete data set available for Boer-Mulders and Cahn effects!         2009 Madrid, 26-30 April 2009 26
  • 100. Francesca Giordano Different behavior for with respect to pions: large signals and same sign for modulation: indication of same sign for favored/unfavored strange Collins fragmentation functions? K+ /K cos 2 h Differences between : evidence of a non-zero Boer-Mulders function: confirms opposite sign for favored and unfavored pion Collins fragmentation functions + / Similar results for deuterium & hydrogen data suggest a Boer-Mulders function with same sign for u and d quark SUMMARY To date provides the most complete data set available for Boer-Mulders and Cahn effects!         2009 Madrid, 26-30 April 2009 26
  • 101. Francesca Giordano Different behavior for with respect to pions: large signals and same sign for modulation: indication of same sign for favored/unfavored strange Collins fragmentation functions? K+ /K cos 2 h Differences between : evidence of a non-zero Boer-Mulders function: confirms opposite sign for favored and unfavored pion Collins fragmentation functions + / Thank you! Similar results for deuterium & hydrogen data suggest a Boer-Mulders function with same sign for u and d quark SUMMARY To date provides the most complete data set available for Boer-Mulders and Cahn effects!         2009 Madrid, 26-30 April 2009 26