Form Factors with Electrons and Positrons - Jefferson Lab

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Spatial distributions in transverse plane 26 Charge density ρ(b) in the transverse plane of the infinite momentum frame is a 2D Fourier transform of F 1 The transverse coordinates are not affected by the Lorentz boost Lorentz contraction Pancake G.A. Miller, Phys. Rev. Lett. 99, 112001 (2007)
Multipole expansion <strong>and</strong> charge radius 27 The proton charge radius is obtained as the slope of electric form factor at Q 2 = 0 Likewise for the magnetic radius
Page 1 and 2: HUGS2013, JLab, May 28 - June 14, 2
Page 3 and 4: Lorentz invariants 3 Energy transfe
Page 5 and 6: LAB frame kinematics 5
Page 7 and 8: CM frame kinematics 7
Page 9 and 10: Lepton-lepton scattering 9 Unpolar
Page 11 and 12: Lepton-lepton scattering 11 Matrix
Page 13 and 14: Lepton-nucleon scattering 13 Lepto
Page 15 and 16: Lepton-nucleon scattering 15 Lepto
Page 17 and 18: Sachs form factors 17 Rosenbluth fo
Page 19 and 20: Sachs form factors 19 Rosenbluth fo
Page 21 and 22: Sachs form factors 21 With Sachs f
Page 23 and 24: Rosenbluth method 23 τG M 2 G E 2
Page 25: Spatial distributions in the Breit
Page 29 and 30: Radiative corrections 29 Angular di
Page 31 and 32: Radiative corrections 31
Page 33 and 34: How radiative corrections matter at
Page 35 and 36: Form factors from Rosenbluth method
Page 37 and 38: G p E and Gp M from unpolarized dat
Page 39 and 40: G p E and Gp from unpolarized data
Page 41 and 42: Rosenbluth data and form factor sca
Page 43 and 44: Concept of spin and polarization 43
Page 45 and 46: Quantum mechanics without spin? 45
Page 47 and 48: Pauli exclusion principle 47 From
Page 49 and 50: Spin and magnetic moment 49 Magn
Page 51 and 52: Polarimetry 51 left Spin-zero nucle

Form Factors with Electrons and Positrons - Jefferson Lab

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