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
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
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
hq
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
hq
T i ! cos q
h ! cos H
h
SPIN Effect!
access to Collins effect
7
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
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
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