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The Long Way from QCD gauge sector to pion's and nucleon's GPDs Trento; 12-16 October, 2015 J. Rodríguez-Quintero Univ. Huelva & CAFPE

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Page 1: Pepe Rodriguez

The Long Way from QCD gauge sector to pion's and nucleon's GPDs

Trento; 12-16 October, 2015

J. Rodríguez-QuinteroUniv. Huelva & CAFPE

Page 2: Pepe Rodriguez

In collaboration with:

Chang Lei Cedric Mezrag Hervé Moutarde Craig D. Roberts Frank Sabatié Sebastian M. Schmidt Peter Tandy

Published in:

Phys. Lett. B735 (2014) 3239 Phys. Lett. B190 (2015) 731

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From gauge sector to hadron phenomenology

Quark propagator gap equation:

D. Binosi, L. Chang, J. Papavassiliou, C.D. Roberts, Phys. Lett. B, 183 (2015)

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From gauge sector to hadron phenomenology

Quark propagator gap equation:

Interaction kernel:

D. Binosi, L. Chang, J. Papavassiliou, C:D. Roberts, Phys. Lett. B, 183 (2015)

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From gauge sector to hadron phenomenology

Quark propagator gap equation:

Interaction kernel:

D. Binosi, L. Chang, J. Papavassiliou, C.D. Roberts, Phys. Lett. B, 183 (2015)

IR matter interaction kernel:

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From gauge sector to hadron phenomenologyD. Binosi, L. Chang, J. Papavassiliou, C.D. Roberts, Phys. Lett. B, 183 (2015)

IR matter interaction kernel:Current models of the interaction kernel yields ground- and excited-states hadron masses within a 10-15% of accuracy compared to experiments!!!C.D. Roberts et al. Few Body Sys. 51, 1 (2011)

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From gauge sector to hadron phenomenologyD. Binosi, L. Chang, J. Papavassiliou, C.D. Roberts, Phys. Lett. B, 183 (2015)

IR matter interaction kernel:

IR gauge-sector interaction kernel:More details in Binosi's Friday talk!!!

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From gauge sector to hadron phenomenologyD. Binosi, L. Chang, J. Papavassiliou, C.D. Roberts, Phys. Lett. B, 183 (2015)

IR matter interaction kernel:

IR gauge-sector interaction kernel:More details in Binosi's Friday talk!!!

Top-down approach

bottom-up approach

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From gauge sector to hadron phenomenologyD. Binosi, L. Chang, J. Papavassiliou, C.D. Roberts, Phys. Lett. B, 183 (2015)

IR matter interaction kernel:

IR gauge-sector interaction kernel: More details in Binosi's Friday talk!!!

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From gauge sector to hadron phenomenologyVery preliminary results!!!

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From gauge sector to hadron phenomenologyVery preliminary results!!!

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Why GPDs?3D imaging of the nucleon's partonic content but also...

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Why GPDs?3D imaging of the nucleon's partonic content but also...

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Why GPDs?3D imaging of the nucleon's partonic content but also...

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Why GPDs?3D imaging of the nucleon's partonic content but also...

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Why GPDs?3D imaging of the nucleon's partonic content but also...

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Why GPDs?3D imaging of the nucleon's partonic content but also...

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Pion GPDDefinition and symmetry properties:

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Pion GPDForm factors and parton distribution functions:

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Pion GPDForm factors and parton distribution functions:

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Pion GPDForm factors and parton distribution functions:

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Pion GPDForm factors and parton distribution functions:

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Pion GPDForm factors and parton distribution functions:

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Pion GPDForm factors and parton distribution functions:

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Pion GPDForm factors and parton distribution functions:

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Pion GPDForm factors and parton distribution functions:

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Pion GPDForm factors and parton distribution functions:

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Pion GPDDouble distributions (DD), a natural parameterization for a covariant GPD:

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Pion GPDDouble distributions (DD), a natural parameterization for a covariant GPD:

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GPD in the DSE-BSE approachEvaluation via the triangle diagram approximation:

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GPD in the DSE-BSE approachEvaluation via the triangle diagram approximation:

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GPD in the DSE-BSE approachEvaluation via the triangle diagram approximation:

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GPD in the DSE-BSE approachEvaluation via the triangle diagram approximation:

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GPD in the DSE-BSE approachEvaluation via the triangle diagram approximation:

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GPD in the DSE-BSE approachEvaluation via the triangle diagram approximation:

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GPD in the DSE-BSE approachEvaluation via the triangle diagram approximation:

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GPD in the DSE-BSE approachRainbow-ladder and physical content:

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GPD in the DSE-BSE approachRainbow-ladder and physical content:

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GPD in the DSE-BSE approachRainbow-ladder and physical content:

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GPD in the DSE-BSE approachRainbow-ladder and physical content:

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GPD in the DSE-BSE approachMost of the properties made sure by construction:

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GPD in the DSE-BSE approachMost of the properties made sure by construction:

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GPD in the DSE-BSE approachMost of the properties made sure by construction:

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GPD in the DSE-BSE approachMost of the properties made sure by construction:

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GPD in the DSE-BSE approachMost of the properties made sure by construction:

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GPD in the DSE-BSE approachMost of the properties made sure by construction:

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Algebraic DSE-BSE inspired GPD modelHave to deal with DSEs and BSEs solutions:

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Algebraic DSE-BSE inspired GPD modelA first intermediate step before dealing with numerical solutions:

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Algebraic DSE-BSE inspired GPD modelA first intermediate step before dealing with numerical solutions:

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Algebraic DSE-BSE inspired GPD modelA first intermediate step before dealing with numerical solutions:

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Algebraic DSE-BSE inspired GPD modelA first intermediate step before dealing with numerical solutions:

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Results for the pion GPDVerification of the theoretical constraints:

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Results for the pion GPDVerification of the theoretical constraints:

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Results for the pion GPDVerification of the theoretical constraints:

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Results for the pion GPDVerification of the theoretical constraints:

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Results for the pion GPDVerification of the theoretical constraints:

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Results for the pion GPDThe two-body problem:

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Results for the pion GPDThe two-body problem:

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Results for the pion GPDThe two-body problem:

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Results for the pion GPDThe two-body problem:

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Results for the pion GPDThe two-body problem:

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Results for the pion GPDThe two-body problem:

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Results for the pion GPDThe form factor and the dimensionful parameter:

400

C. Mezrag et al., Phys. Lett. B190 (2015) 741

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Results for the pion GPDThe parton distribution function:

0.40

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Results for the pion GPDThe off-forward (non-skewed) GPD:

C. Mezrag et al., Phys. Lett. B190 (2015) 741

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Results for the pion GPDThe off-forward (non-skewed) GPD:

C. Mezrag et al., Phys. Lett. B190 (2015) 741

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Results for the pion GPDThe off-forward (non-skewed) GPD:

C. Mezrag et al., Phys. Lett. B190 (2015) 741

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Results for the pion GPDThe off-forward (non-skewed) GPD:

C. Mezrag et al., Phys. Lett. B190 (2015) 741

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Results for the pion GPDThe off-forward (non-skewed) GPD:

C. Mezrag et al., Phys. Lett. B190 (2015) 741

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The overlap approachA first-principle connection with Light-Front Wave Function:

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The overlap approachA first-principle connection with Light-Front Wave Function:

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The overlap approachA first-principle connection with Light-Front Wave Function:

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The overlap approachA first-principle connection with Light-Front Wave Function:

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The overlap approachA first-principle connection with Light-Front Wave Function:

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The overlap approachA first-principle connection with Light-Front Wave Function:

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DGLAP to ERBL extension from the overlapBefore dealing with a nucleon GPD, one needs to solve the problem of the extension to :ξ>x

1CDD-scheme Radon transform:

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DGLAP to ERBL extension from the overlapBefore dealing with a nucleon GPD, one needs to solve the problem of the extension to :ξ>x

1CDD-scheme Radon transform:

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DGLAP to ERBL extension from the overlapBefore dealing with a nucleon GPD, one needs to solve the problem of the extension to :ξ>x

1CDD-scheme Radon transform:

Mathematical literature (a lot of) on the problem of computerized tomography:

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DGLAP to ERBL extension from the overlapBefore dealing with a nucleon GPD, one needs to solve the problem of the extension to :ξ>x

1CDD-scheme Radon transform:

Mathematical literature (a lot of) on the problem of computerized tomography:

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DGLAP to ERBL extension from the overlapBefore dealing with a nucleon GPD, one needs to solve the problem of the extension to :ξ>x

1CDD-scheme Radon transform:

Mathematical literature (a lot of) on the problem of computerized tomography:

Unicity: the knowledge of the GPD in DGLAP region allows the (unique) reconstruction of the GPD over the full range, , by capitalizing the polynomiality condition, and up to an ambiguity on the line .ξ , x∈R

β=0

... in progress!!!

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Conclusions:We just made a few modest steps in a very long way!!!

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Conclusions:We just made a few modest steps in a very long way!!!