In light-front holographic QCD the nucleon gravitational form factor B_N(t) vanishes exactly in the symmetric limit due to an antisymmetric longitudinal factor and remains strongly suppressed for realistic nucleon wave functions, explaining its observed smallness.
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Introducing an energy scale in AdS space changes the topological class of black holes, corresponding to confined and deconfined phases separated by a Hawking-Page transition at finite critical temperature.
Mechanical properties of the proton including transverse pressure and shear forces for u and d quarks are computed in momentum space via gravitational TMDs in the light-cone spectator diquark model, revealing strong binding at low momentum.
citing papers explorer
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Origin of the nucleon gravitational form factor $B_N(t)$: Exposition in light-front holographic QCD
In light-front holographic QCD the nucleon gravitational form factor B_N(t) vanishes exactly in the symmetric limit due to an antisymmetric longitudinal factor and remains strongly suppressed for realistic nucleon wave functions, explaining its observed smallness.
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Topological charges and confined-deconfined phase transition in holography
Introducing an energy scale in AdS space changes the topological class of black holes, corresponding to confined and deconfined phases separated by a Hawking-Page transition at finite critical temperature.
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Mechanical properties of proton in the momentum space
Mechanical properties of the proton including transverse pressure and shear forces for u and d quarks are computed in momentum space via gravitational TMDs in the light-cone spectator diquark model, revealing strong binding at low momentum.