Elastic scattering of electrons from a light nucleus is measured at two small angles

PHYSICS · Multi-part · Fermi University Physics · Nuclear Physics · Nuclear constituents, size and binding · Nuclear constituents, size and binding

The Nucleus Resolved, Ch How big a nucleus is, and what the mass surface knows

Problem

Elastic scattering of 300 MeV300\,\mathrm{MeV} electrons from a light nucleus is measured at two small angles, and the form factor is extracted at each. The results are F(q12)=0.9494F(q_1^2) = 0.9494 at θ1=6∘\theta_1 = 6^\circ and F(q22)=0.7980F(q_2^2) = 0.7980 at θ2=12∘\theta_2 = 12^\circ. Someone sets out to find the rms charge radius from the small-qq expansion F(q2)=1−q2⟨r2⟩/6F(q^2) = 1 - q^2\langle r^2\rangle/6, and writes: "The momentum transfer at angle θ\theta is q=2ksin⁡θq = 2k\sin\theta, with k=E/ℏck = E/\hbar c. For E=300 MeVE = 300\,\mathrm{MeV}, k=300/197.327=1.520 fm−1k = 300/197.327 = 1.520\,\mathrm{fm^{-1}}. So q1=2(1.520)sin⁡6∘=0.318 fm−1q_1 = 2(1.520)\sin 6^\circ = 0.318\,\mathrm{fm^{-1}} and q2=2(1.520)sin⁡12∘=0.632 fm−1q_2 = 2(1.520)\sin 12^\circ = 0.632\,\mathrm{fm^{-1}}. The slope is F(q22)−F(q12)q22−q12=0.7980−0.94940.3996−0.1010=−0.507 fm2.\frac{F(q_2^2) - F(q_1^2)}{q_2^2 - q_1^2} = \frac{0.7980 - 0.9494}{0.3996 - 0.1010} = -0.507\,\mathrm{fm^2}. Since F=1−q2⟨r2⟩/6F = 1 - q^2\langle r^2\rangle /6, ⟨r2⟩=−6×(−0.507)=3.04 fm2\langle r^2\rangle = -6\times(-0.507) = 3.04\,\mathrm{fm^2}, so ⟨r2⟩1/2=1.74 fm\langle r^2\rangle^{1/2} = 1.74\,\mathrm{fm}." ((a)) Find the error in this working. ((b)) Keeping the same leading-order small-qq model, with higher powers of qq neglected, give the corrected estimate of ⟨r2⟩1/2\langle r^2\rangle^{1/2} for this nucleus.

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