Parity violating measurements of neutron densities - Jefferson Lab
Parity violating measurements of neutron densities - Jefferson Lab
Parity violating measurements of neutron densities - Jefferson Lab
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Analysis II: Weak form factor<br />
• Compare Rw to well measured Rch=5.503 fm implies weak charge skin<br />
Rw-Rch=0.32±0.18(exp)±0.03(model) fm. Experimental milestone: direct<br />
evidence that weak charge density is more extended than E+M charge<br />
density.<br />
• Rch slightly larger than point proton radius, Rch 2 =Rp 2 ++N/Z<br />
(neglecting small spin-orbit and meson exchange currents).<br />
• Proton size =0.769 fm 2 , <strong>neutron</strong> =-0.116 fm 2 --> Rp=5.45 fm.<br />
• (Qw/qnN)Rw 2 =Rn 2 +(qpZ/qnN)Rch 2 ++Z/N-(A/qnN)<br />
• Total weak charge Qw=Nqn+Zqp=-118.55. Radiative corrected <strong>neutron</strong><br />
weak charge is qn=-0.9878, proton qp=0.0721.<br />
• Nucleon strangeness radius ≤±0.04 fm 2 from HAPPEX, G0, A4...<br />
• From Rw deduce Rn=5.751 ±0.175(exp) ±0.026(model) ±0.005(strange) fm.<br />
• Neutron skin: Rn-Rp=0.302 ±0.175 ±0.026 fm, consistent with Analysis I,<br />
Rn-Rp=0.33 +0.16 -0.18 fm, within limitations <strong>of</strong> Helm model (≈ ± model error).<br />
-- Phys. Rev. C 85, 032501(R) (2012)