Chapter 11: Q19P (page 419)
Prove the optical theorem, which relates the total cross-section to the imaginary part of the forward scattering amplitude:
Short Answer
Hence, it’s proved.
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Chapter 11: Q19P (page 419)
Prove the optical theorem, which relates the total cross-section to the imaginary part of the forward scattering amplitude:
Hence, it’s proved.
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Nothing that show that the determinant of a Hermitian matrix is real, the determinant of a unitary matrix has modulus 1 (hence the name), and the determinant of an orthogonal matrix is or .
A particle of massand energyrole="math" localid="1656064863125" is incident from the left on the potential
(a) If the incoming wave is(where), find the reflected wave.
(b) Confirm that the reflected wave has the same amplitude as the incident wave.
(c) Find the phase shift(Equation 11.40) for a very deep well.
Rutherford scattering. An incident particle of charge andkinetic energy scatters off a heavy stationary particle of charge .
(a) Derive the formula relating the impact parameter to the scattering angle. 2 Answer:
.
(b) Determine the differential scattering cross-section. Answer:
(c) Show that the total cross-section for Rutherford scattering is infinite. We say that the potential has "infinite range"; you can't escape from a Coulomb force.
Calculate the total cross-section for scattering from a Yukawa potential, in the Born approximation. Express your answer as a function of E.
Find the Green's function for the one-dimensional Schrödinger equation, and use it to construct the integral form (analogous to Equation 11.67).
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