cédric lorcé
DESCRIPTION
Second International Summer School of the GDR PH-QCD “Correlations between partons in nucleons”. N. Cédric Lorcé. Multidimensional pictures of the nucleon (2/3). IFPA Liège. June 30-July 4, 2014, LPT, Paris-Sud University, Orsay, France. Reminder. Lecture 1. - PowerPoint PPT PresentationTRANSCRIPT
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Cédric LorcéIFPA Liège
Multidimensional pictures of the nucleon (2/3)
June 30-July 4, 2014, LPT, Paris-Sud University, Orsay, France
Second International Summer School of the GDR PH-QCD
“Correlations between partons in nucleons”
N
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Reminder
• Understanding nucleon internal structure is essential• Concept of phase space can be generalized to QM and QFT• Relativistic effects force us to abandon 1D in phase space
Lecture 1
2+3D
Transverse momentum
Transverse position
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Outline
• Nucleon 1D picture• Nucleon 2D picture• Nucleon 2+1D picture• Energy-momentum tensor
Lecture 2
• Introduction• Tour in phase space• Galileo vs Lorentz• Photon point of view
Lecture 1
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Deep inelastic scattering
Coherent scattering
1/31
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Deep inelastic scattering
Coherent scattering
Incoherent scattering
2/31
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Deep inelastic scattering
Coherent scattering
Incoherent scattering
FactorizationHard/perturbative
Soft/non-perturbative
3/31
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Deep inelastic scattering
Parton model
QCD corrections
Probability to find parton with momentum fraction
Non-perturbativeProcess-independent
PerturbativeProcess-dependent
+ virtual diagrams
4/31
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Deep inelastic scattering
Cross-section must not depend on
DGLAP evolution equations
Splitting functions
Non-p
ert
urb
ati
ve
5/31
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Parton distribution functions (PDFs)
Optical theorem
PDFs
Final-state cut
Constrained by Lorentz and discrete space-time
symmetries
PDF correlator
Parametrization
6/31
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Parton distribution functions (PDFs)
PDFs
Charges
VectorQuark number
TensorQuark
transversity
AxialQuark helicity
7/31
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Elastic scattering
Constructive interference (Bragg’s
law)
Scattered amplitude
Diffraction pattern
Crystal
Reconstructed charge distribution
Let’s replace the crystal by a nucleon !
Form factor Scatterer distribution
8/31
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Form factors (FFs)
FFs
FF correlator
Parametrization (electromagnetic case)
Sachs FFs
Pointlike Spatial structure
9/31
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FFs
Form factors (FFs)
PDFs
Charges
Electric charge
Anomalous magnetic moment
10/31
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Monopole
Form factors (FFs)
+ -
Proton Neutron
Negative core does not fit naive picture
!
Longitudinally polarized nucleon
[Miller (2007)]
11/31
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Proton Neutron
Form factors (FFs)
Transversely polarized nucleon
+-
+
Dipole
[Carlson, Vanderhaeghen (2008)]
Apparent electric dipole
!P & T
violations ???
No !!!
Monopole
12/31
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Form factors (FFs)
Transversely polarized nucleon
[Lorcé (2009)]
u
d
Origin of EDM : light-front artifact
d
Orbital angular momentum
Induced electric moment
Anomalous moment
[Burkardt (2003)]
13/31
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Compton scattering
Virtual Compton scattering (VCS)
Real Compton Scattering
Recoiling target
Compton wavelengt
h
interferes with
VCS Bethe-Heitler
Question : why are there 2 peaks?
14/31
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Compton FF
Generalized parton distributions (GPDs)
GPDs
Factorization
[Collins, Freund (1999)][Belitsky et al. (2000)]Evolution @
NLO
Deeply virtual Compton scattering (DVCS)
GPD correlator
[Diehl (2003)][Belitsky, Radyushkin (2005)]
[Boffi, Pasquini (2008)]
Reviews :
15/31
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FFsPDFs
Charges
GPDs
Nucleon tomography/imaging
[GPD]
PDF [FF]
Generalized parton distributions (GPDs) 16/31
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Generalized parton distributions (GPDs)
Flat in tNarrow in
b
Steep in tWide in b
[Guidal et al. (2013)]
[Weiss (2009)]
17/31
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Generalized parton distributions (GPDs)
Explicit Lorentz invariance is broken by the preferred light-front direction
Lorentz invariance
and dependences constrained by Lorentz invariance !
18/31
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Generalized parton distributions (GPDs)
Lowest moment
FFs
GPDs
19/31
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Generalized parton distributions (GPDs)
Generic moment in LF gauge
20/31
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Generalized parton distributions (GPDs)
Generic moment
Derivative of Wilson line Covariant derivatives
using
21/31
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Generalized parton distributions (GPDs)
Generic local operator
Symmetrization+ trace removal
Generic FFs
Polynomiality of GPDs
Constrained by Lorentz and discrete space-time
symmetries
22/31
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Generalized parton distributions (GPDs)
How to ensure polynomiality property?
Lorentz-invariant variables
« Covariantization »
23/31
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Generalized parton distributions (GPDs)
GPD parametrization
[Müller et al. (1994)][Radyushkin (1999)]
[Polyakov, Weiss (1999)]
Double distribution (DD) parametrization
Constraint :
Support :
24/31
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Generalized parton distributions (GPDs)
Relation between GPDs and DDs
[Müller et al. (1994)][Radyushkin (1999)]
[Polyakov, Weiss (1999)]
Polynomiality property
and dependences not constrained by Lorentz invariance !
25/31
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Energy-momentum tensor
A lot of interesting physics is contained in the EM tensor
Energy density
Momentum
density
Energy flux
Momentum flux
Shear stress
Normal stress (pressure)
[Polyakov, Shuvaev (2002)]
[Polyakov (2003)][Goeke et al. (2007)]
[Cebulla et al. (2007)]
In rest frame
26/31
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Energy-momentum tensor
In presence of spin density
In rest frame
No « spin » contribution !
Belinfante « improvement »
Spin density gradient Four-momentum circulation
27/31
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QCD Energy-momentum operator
Matrix elements Normalization
28/31Energy-momentum tensor
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Energy-momentum FFs
Momentum sum rule
Angular momentum sum rule
[Ji (1997)]
Vanishing gravitomagnetic moment !
29/31Energy-momentum tensor
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Energy-momentum FFs
Momentum sum rule
Angular momentum sum rule
[Ji (1997)]
Vanishing gravitomagnetic moment !
Non-conserved current
30/31Energy-momentum tensor
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Leading-twist component of
Link with GPDs
[Ji (1997)]
Accessible e.g. in DVCS !
31/31Energy-momentum tensor
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Summary
• PDFs provide 1D pictures of the nucleon• FFs provide 2D pictures of the nucleon• GPDs generalize both PDFs and FFs and give access to the EMT
Lecture 2
[GPD]
PDF [FF]
Energy density
Momentum density
Energy
flux
Momentum flux
Shear stress
Normal stress (pressure)
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Backup slides
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Nuclear charge densities and FFs
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Nucleon FFs
[Perdrisat et al. (2006)]
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Nucleon FFs
green : Rosenbluth data (SLAC, JLab)
Pun05Gay02
JLab/HallA
recoil polarization data