Central Potential Scattering and Phase Shifts

Quantum Mechanics A

Schrödinger Equation The most fundamental equation of quantum mechanics; given a Hamiltonian Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \mathcal{H}} , it describes how a state Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |\Psi\rangle} evolves in time.

Physical Basis of Quantum Mechanics

Basic Concepts and Theory of Motion UV Catastrophe (Black-Body Radiation) Photoelectric Effect Stability of Matter Double Slit Experiment Stern-Gerlach Experiment The Principle of Complementarity The Correspondence Principle The Philosophy of Quantum Theory

Schrödinger Equation

Brief Derivation of Schrödinger Equation Relation Between the Wave Function and Probability Density Stationary States Heisenberg Uncertainty Principle Some Consequences of the Uncertainty Principle

Operators, Eigenfunctions, and Symmetry

Linear Vector Spaces and Operators Commutation Relations and Simultaneous Eigenvalues The Schrödinger Equation in Dirac Notation Transformations of Operators and Symmetry Time Evolution of Expectation Values and Ehrenfest's Theorem

Motion in One Dimension

One-Dimensional Bound States Oscillation Theorem The Dirac Delta Function Potential Scattering States, Transmission and Reflection Motion in a Periodic Potential Summary of One-Dimensional Systems

Discrete Eigenvalues and Bound States

Harmonic Oscillator Spectrum and Eigenstates Analytical Method for Solving the Simple Harmonic Oscillator Coherent States Charged Particles in an Electromagnetic Field WKB Approximation

Time Evolution and the Pictures of Quantum Mechanics

The Heisenberg Picture: Equations of Motion for Operators The Interaction Picture The Virial Theorem

Angular Momentum

Commutation Relations Angular Momentum as a Generator of Rotations in 3D Spherical Coordinates Eigenvalue Quantization Orbital Angular Momentum Eigenfunctions

Central Forces

General Formalism Free Particle in Spherical Coordinates Spherical Well Isotropic Harmonic Oscillator Hydrogen Atom WKB in Spherical Coordinates

The Path Integral Formulation of Quantum Mechanics

Feynman Path Integrals The Free-Particle Propagator Propagator for the Harmonic Oscillator

Continuous Eigenvalues and Collision Theory

Differential Cross Section and the Green's Function Formulation of Scattering Central Potential Scattering and Phase Shifts Coulomb Potential Scattering

We will now discuss scattering from a central potential in a different way. Recall that the wave function for an incident and scattered wave for a central potential is given by

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \psi_k(\mathbf{r})=\psi_k^{(0)}(\mathbf{r})=\psi_k^{(0)}(\mathbf{r})+f_k(\theta)\frac{e^{ikr}}{r},}

where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \psi_k^{(0)}(\mathbf{r})\!} is the incoming wave and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle f_k(\theta)\!} is the scattering amplitude.

To determine Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle f_k(\theta),\!} we start with the Schrödinger equation,

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left( -\frac{\hbar^2 }{2m}\nabla^2+V(r) \right) \psi=\frac{\hbar^2 k^2 }{2m}\psi .}

As before, this equation may be reduced to an effective one-dimensional equation,

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left( -\frac{\hbar^2 }{2m}\frac{d^2 }{dr^2 }+\frac{\hbar^2 l(l+1)}{2mr^2}+V(|\mathbf{r}|) \right) u_l(r) =\frac{\hbar^2 k^2 }{2m}u_l(r),}

with the full wave function given by Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \psi(\mathbf{r})=\frac{u_l(r)}{r}Y_l^m(\theta,\phi).}

For a potential with a finite range Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle d,\!} we know that, for Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle r \gg d,\!} the problem reduces to that of a free particle, and thus

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left( -\frac{\hbar^2 }{2m}\frac{d^2 }{dr^2 }+\frac{\hbar^2 l(l+1)}{2mr^2} \right) u_l(r) =\frac{\hbar^2 k^2 }{2m}u_l(r).}

The solution of this equation is a linear combination of the spherical Bessel functions and the spherical Neumann functions,

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle u_l(r)=A_l j_l(kr) +B_l n_l(kr).\!}

When Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle r\to\infty,\!} we use the asymptotic approximations of the spherical Bessel functions and the spherical Neumann functions, obtaining

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{u(r)}{r}\approx A_l \frac{\sin(kr-l\frac{\pi}{2})}{kr} -B_l \frac{\cos(kr-l\frac{\pi}{2})}{kr}.}

Let us now define

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{B_l }{A_l }=-\tan\delta_l.}

The angle Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \delta_l\!} is known as the phase shift of the Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \ l^{\text{th}}} wave and it is the phase shift induced by scattering from the potential in the radial part of the wave function. Note that, in the absence of a scattering potential, the boundary condition that the wave function must be finite at the origin causes Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle B_l} to vanish for all values of Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle l.} Therefore, the magnitude of Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle B_l} compared to Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle A_l} is a meausre of the intensity of the scattering. We may rewrite the above expression as

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{u_l(r)}{r}=A_l\frac{\sin(kr-l\frac{\pi}{2} + \delta_l )}{kr}.}

Physically, we expect Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \delta_l < 0\!} for repulsive potentials and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \delta_l > 0\!} for attractive potentials. Also, if Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle l/k \gg d,\!} then the classical impact parameter is much larger than the range of the potential and in this case we expect Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \delta_l\!} to be small.

Because the scattering amplitude has azimuthal symmetry (i.e., it is independent of Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \phi\!} ), we can write the full solution of the Schrödinger equation as a superposition of Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle m=0\!} spherical harmonics only:

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \psi(\mathbf{r})=\sum_{l=0}^{\mathop{ \infty}}a'_l(k)P_l(\cos\theta) \frac{u_l(r)}{r}=\sum_{l=0}^{\mathop{ \infty}}a_l(k)P_l(\cos\theta) \frac{\sin(kr-l\frac{\pi}{2}+\delta_l )}{kr}.}

We now determine the coefficients Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle a_l(k)\!} by substituting in the wave function in terms of the scattering amplitude on the left-hand side:

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle e^{ikr\cos\theta}+f_k(\theta)\frac{e^{ikr}}{r}=\sum_{l=0}^{\mathop{ \infty}}a_l(k)P_l(\cos\theta) \frac{\sin(kr-l\frac{\pi}{2}+\delta_l )}{kr}}

Here, we assume that the incident wave propagates along the Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle z\!} direction. This must hold for large Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle r.\!} We may show that

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle e^{ikr\cos\theta}=\sum_{l=0}^{\mathop{ \infty}}(2l+1)i^l P_l(\cos\theta) \frac{\sin(kr-l\frac{\pi}{2} ) }{kr},}

so that

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sum_{l=0}^{\mathop{ \infty}}(2l+1)i^l P_l(\cos\theta) \frac{\sin(kr-l\frac{\pi}{2} ) }{kr}+f_k(\theta)\frac{e^{ikr}}{r}=\sum_{l=0}^{\mathop{ \infty}}a_l(k)P_l(\cos\theta) \frac{\sin(kr-l\frac{\pi}{2}+\delta_l )}{kr} .}

Using the fact that

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sin (x)=\frac{e^{ix}-e^{-ix}}{2i},\!}

we may rewrite this as

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{align} \sum_{l=0}^{\mathop{ \infty}}(2l+1)i^l P_l(\cos\theta) \frac{1}{kr} \frac{1}{2i} \left( e^{i\left( kr-l\frac{\pi}{2} \right)} - e^{-i\left( kr-l\frac{\pi}{2} \right)} \right) +f_k(\theta)\frac{e^{ikr}}{r} \\ = \sum_{l=0}^{\mathop{ \infty}}a_l(k)P_l(\cos\theta) \frac{1}{kr} \frac{1}{2i} \left( e^{i\left(kr-l\frac{\pi}{2}+\delta_l \right)} - e^{-i\left(kr-l\frac{\pi}{2}+\delta_l \right)}\right). \end{align} }

By matching the coefficients of Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle e^{-ikr}\!} , we get

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle a_l(k)=(2l+1)i^le^{i\delta_l},}

and doing the same for Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle e^{ikr}\!} yields

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle f_k(\theta)=\frac{1}{k}\sum_{l=0}^{\infty}(2l+1)e^{i\delta_l }\sin\delta_lP_l(\cos\theta) .}

Note that Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \delta_l\!} is a function of Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle k\!} and therefore a function of the incident energy. If Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \delta_l(k)\!} is known, then we can reconstruct the entire scattering amplitude and consequently the differential cross section. The phase shifts themselves must be determined by solving the Schrödinger equation.

The differential scattering cross section is

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{d\sigma}{d\Omega}=|f_k(\theta) |^2=\frac{1}{k^2 }\left|\sum_{l=0}^{\infty}(2l+1)e^{i\delta_l }\sin\delta_lP_l(\cos\theta) \right|^2.}

By integrating Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{d\sigma}{d\Omega}\!} over the solid angle Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \Omega, \!} we obtain the total scattering cross section:

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{align} \sigma_{tot} &= \int \frac{d\sigma}{d\Omega}\,d\Omega \\ &= \sum_{l=0}^{\infty}\sum_{l'=0}^{\infty}(2l+1)(2l'+1)e^{i\delta_l }e^{-i\delta_{l'}}\sin\delta_l\sin\delta_{l'} \int_{0}^{2\pi} d\phi\,\int_{0}^{\pi}d\theta\,\sin\theta P_l(\cos\theta)P_{l'}(\cos\theta) \\ &= \frac{4\pi}{k^2 }\sum_{l=0}^{\mathop{ \infty}}(2l+1)\sin^2\delta_l \end{align} }

The last equality follows from the orthogonality of the Legendre polynomials,

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \int_{-1}^{1}dxP_l(x) P_{l'}(x)=\frac{2}{(2l+1)}\delta_{ll'}.}

Finally, note that since $P_{l}(1)=1\!$ for all $l,\!$ we obtain

$f_{k}(0)={\frac {1}{k}}\sum _{l=0}^{\infty }\left(2l+1\right)e^{i\delta _{l}}\sin \delta _{l}P_{l}(1)={\frac {1}{k}}\sum _{l=0}^{\infty }\left(2l+1\right)e^{i\delta _{l}}\sin \delta _{l}.$

If we take the imaginary part of the scattering amplitude,then

$\Im m[f_{k}(0)]={\frac {1}{k}}\sum _{l=0}^{\infty }\left(2l+1\right)\sin ^{2}\delta _{l}={\frac {k}{4\pi }}\sigma _{tot}.$

Therefore,

$\sigma _{tot}={\frac {4\pi }{k}}\Im mf(0).$

This relationship is known as the optical theorem. The optical theorem is a general law of wave scattering theory that relates the forward scattering amplitude to the total cross section of the scattering. It was originally discovered independently by Sellmeier and Lord Rayleigh in 1871.

Referring back to the formula for the scattering amplitude, one more important quantity can be discussed:

$S_{l}(k)=e^{2i\delta _{l}(k)}$

This quantity, for now referred to as the partial scattering for angular momentum $l\!,$ is the ratio of the coefficients of the outgoing and incoming waves for a wave scattered on a potential of finite range $a.\!$

These ratios can simplify the problem of evaluating the continuity of the waveform at the boundary $r=a.\!$ In general, if the interior wave function is known to be smoothly continuous across the boundary at $r=a,\!$ then the phase shifts can be expressed in terms of the logarithmic derivatives evaluated at the boundary $r=a:\!$

$\beta _{l}=\left({\frac {a}{u_{l}(r)}}{\frac {du_{l}(r)}{dr}}\right)_{r=a}$

Using the above equations for the form of $u_{l}(r)$ beyond the region of scattering, the following relation is found:

$\beta _{l}=ka{\frac {j'_{l}(ka)\cos(\delta _{l})-n'_{l}(ka)\sin(\delta _{l})}{j_{l}(ka)\cos(\delta _{l})-n_{l}(ka)\sin(\delta _{l})}}$

Thus, after some algebra,

$S_{l}=e^{2i\delta _{l}}=-{\frac {j_{l}(ka)-in_{l}(ka)}{j_{l}(ka)+in_{l}(ka)}}{\frac {\beta _{l}-ka{\frac {j'_{l}(ka)-in'_{l}(ka)}{j_{l}(ka)-in_{l}(ka)}}}{\beta _{l}-ka{\frac {j'_{l}(ka)+in'_{l}(ka)}{j_{l}(ka)+in_{l}(ka)}}}}.$

Note that, if $\beta _{l}\to \infty ,\!$ which corresponds to $f_{l}(a)=0,\!$ then only the first portion of this expression survives. This is a special quantity corresponding to hard sphere scattering; we may define the phase angles $\xi _{l},\!$ known as the hard sphere phase shifts, as

$e^{2i\xi _{l}}=-{\frac {j_{l}(ka)-in_{l}(ka)}{j_{l}(ka)+in_{l}(ka)}}.$

Note that these phase shifts are present for any potential, not just that of a hard sphere.

Scattering by Square Well potential

Consider a beam of point particles of mass $m\!$ scattering from a finite spherical attractive well of depth $V_{0}\!$ and radius $a,\!$

$V(r)={\begin{cases}-V_{0},&r<a\\0,&r>a\end{cases}}$

The effective Schrödinger equation for $r<a\!$ is

${\frac {d^{2}R_{l}}{dr^{2}}}+{\frac {2}{r}}{\frac {dR_{l}}{dr}}-{\frac {l(l+1)}{r^{2}}}R_{l}+{\frac {2m}{\hbar ^{2}}}(E+V_{0})u_{l}=0.$

Its solution is

$u_{l}(r)=A_{l}j_{l}(\kappa r),\!$

where $\kappa ^{2}={\frac {2m}{\hbar ^{2}}}(E+V_{0}).\!$

In the region $r>a,\!$ $u_{l}\!$ is

$u_{l}(r)=Bj_{l}(kr)+Cn_{l}(kr).\!$

Here, $A,\!$ $B,\!$ and $C\!$ are arbitrary constants and $k^{2}={\frac {2m}{\hbar ^{2}}}E.\!$

For large $r,\!$

$u_{l}(r)\approx {\frac {\sin {(kr-l\pi /2+\delta _{l})}}{kr}},$

where

${\frac {C}{B}}=-\tan {\delta _{l}}.$

We now apply the boundary conditions at $r=a,\!$ which are continuity of $u_{l}\!$ and of its logarithmic derivative. We obtain

$-{\frac {C}{B}}=\tan {\delta _{l}}={\frac {kj_{l}'(ka)j_{l}(\kappa a)-\kappa j_{l}(ka)j_{l}'(\kappa a)}{kn_{l}'(ka)j_{l}(\kappa a)-\kappa n_{l}(ka)j_{l}'(\kappa a)}}.$

Let us now consider two limiting cases:

(a) $ka\ll l\!$ and $\kappa a\ll l:\!$ In this case, we find that, with some simplification, $\tan {\delta _{l}}\sim k^{2l+1}\sim E^{l+1/2}.\!$ This behavior is a result of the centrifugal barrier that keeps waves of energy far below the barrier from feeling the effect of the potential.

(b) When the phase shift is $\pi /2,\!$ the partial wave cross section $\sigma _{l}(k)={\frac {4\pi (2l+1)}{k^{2}}}\sin ^{2}{\delta _{l}}\!$ is maximized. This is known as a resonant scattering.

From (a), we see that the phase shift is small for $ka\!$ small. However, when $ka\!$ changes and passes through the resonance condition, the phase shift rises rapidly and has a sharp peak at resonant energy $E_{R}\!$. This can be represented as

$\tan {\delta _{l}}\approx {\frac {\gamma (ka)^{2l+1}}{E-E_{R}}},$

so that the partial wave cross section is

$\sigma _{l}={\frac {4\pi (2l+1)}{k^{2}}}{\frac {[\gamma (ka)^{2l+1}]^{2}}{(E-E_{R})^{2}+[\gamma (ka)^{2l+1}]^{2}}}.$

This is the Breit-Wigner formula for a resonant cross section.

Problems

(1) Consider the scattering of a particle from a real spherically symmetric potential. If ${\frac {d\sigma (\theta )}{d\Omega }}$ is the differential cross section and $\sigma$ is the total cross section, then show that

$\sigma \leq {\frac {4\pi }{k}}{\sqrt {\frac {d\sigma (0)}{d\Omega }}}$

for a general central potential using the partial-wave expansion of the scattering amplitude and the cross section.

Solution

(2) Consider an attractive delta shell potential ($\lambda >0\!$) of the form,

$V({\textbf {r}})=-{\frac {\hbar ^{2}\lambda }{2m}}\delta (r-a.)$

(a) Derive the equation for the phase shift caused by this potential for arbitrary angular momentum.

(b) Obtain the expression for the $s\!$ wave phase shift.

(c) Obtain the $s\!$ wave scattering amplitude.

Solution