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Desai Chapter 9 notes and problems.

Posted by peeterjoot on November 29, 2010

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Chapter 9 notes for [1].



Problem 2.


On the basis of the results already derived for the harmonic oscillator, determine the energy eigenvalues and the ground-state wavefunction for the truncatedoscillator

\begin{aligned}V(x) &= \frac{1}{{2}} K x^2 \theta(x)\end{aligned}


We require u(0) = 0, so our solutions are limited to the truncated odd harmonic oscillator solutions. The normalization will be different since only the x>0 integration range is significant. Our energy eigenvalues are

\begin{aligned}E_n = \left( n + \frac{1}{{2}} \right) \hbar \omega, n = 1, 3, 5, \cdots\end{aligned} \hspace{\stretch{1}}(3.1)

And its wave function is

\begin{aligned}v_1(x) \propto u_1(x) \theta(x) = A x e^{-\alpha^2 x^2/2} \theta(x)\end{aligned} \hspace{\stretch{1}}(3.2)

where u_1(x) is the first odd wavefunction for the non-truncated oscillator. Normalizing this we find A^2 \sqrt{\pi}/4 \alpha^3 = 1, or

\begin{aligned}v_1(x) = 2 \left( \frac{\alpha^3}{\sqrt{\pi}}\right)^{1/2} x e^{-\alpha^2 x^2/2} \theta(x)\end{aligned} \hspace{\stretch{1}}(3.3)

Problem 3.


Show that for the harmonic oscillator in the state {\lvert {n} \rangle}, the following uncertainty product holds.

\begin{aligned}\Delta x \Delta p = \left( n + \frac{1}{{2}} \right) \hbar\end{aligned} \hspace{\stretch{1}}(3.4)


I tried this first explicitly with the first two wave functions

\begin{aligned}u_0(x) &= \left(\frac{\alpha^2}{\pi}\right)^{1/4} e^{- \alpha^2 x^2/2} \\ u_1(x) &= \sqrt{2 \alpha^2} \left(\frac{\alpha^2}{\pi}\right)^{1/4} x e^{- \alpha^2 x^2/2}\end{aligned} \hspace{\stretch{1}}(3.5)

For the {\lvert {0} \rangle} state we find easily that \left\langle{{X}}\right\rangle = 0

\begin{aligned}{\langle {0} \rvert} X {\lvert {0} \rangle} &=\int dx {\langle {0} \rvert} X {\lvert {x} \rangle} \left\langle{{x}} \vert {{0}}\right\rangle \\ &=\int dx x {\left\lvert{\left\langle{{x}} \vert {{0}}\right\rangle}\right\rvert}^2 \\ &=\int dx x {\left\lvert{u_0(x)}\right\rvert}^2 \\ &\propto\int dx x e^{-\alpha^2 x^2} \end{aligned}

and this is zero since we are integrating an odd function over an even range (presuming that we take the principle value of the integral).

For the {\lvert {1} \rangle} state this we have

\begin{aligned}{\langle {0} \rvert} X {\lvert {0} \rangle} \propto\int dx x^5 e^{-\alpha^2 x^2} = 0\end{aligned}

Since each u_n(x) is a polynomial times a e^{-\alpha^2 x^2/2} factor we have \left\langle{{X}}\right\rangle = 0 for all states {\lvert {n} \rangle}.

The momentum expecation values for states {\lvert {0} \rangle} and {\lvert {1} \rangle} are also fairly simple to compute. We have

\begin{aligned}{\langle {n} \rvert} P {\lvert {n} \rangle} &=\int dx {\langle {n} \rvert} P {\lvert {x} \rangle}\left\langle{{x}} \vert {{n}}\right\rangle \\ &=\int dx' dx \left\langle{{n}} \vert {{x'}}\right\rangle {\langle {x} \rvert} P {\lvert {x} \rangle} \left\langle{{x}} \vert {{n}}\right\rangle \\ &=-i \hbar \int dx' dx u_n^{*}(x') \delta(x-x') \frac{\partial {}}{\partial {x}} u_n(x) \\ &=-i \hbar \int dx u_n^{*}(x) \frac{\partial {}}{\partial {x}} u_n(x) \\ \end{aligned}

For the {\lvert {0} \rangle} state our derivative is odd since a factor of x is brought down, and we are again integrating an odd function over an even range. For the {\lvert {1} \rangle} case our derivative is proportional to

\begin{aligned}\frac{\partial {}}{\partial {x}} u_1(x) \propto\frac{\partial {}}{\partial {x}} \left( x e^{-\alpha^2 x^2 } \right)=\left( 1 -2 \alpha^2 x^2 \right) e^{-\alpha^2 x^2 } \end{aligned}

Again, this is an even function, while u_1(x) is odd, so we have zero. Noting that we can express each u_n(x) in terms of Hankel functions

\begin{aligned}u_n(x) &= \left( \frac{ \alpha}{\sqrt{\pi} 2^n n!} \right)^{1/2} H_n(\alpha x) e^{ -\alpha^2 x^2/2}\end{aligned} \hspace{\stretch{1}}(3.7)

where H_{2n}(x) is even and H_{2n-1}(x) is odd, we note that this expectation value will always be zero since we will have an even times odd function in the integration kernel.

Knowing that the position and momentum expectation values are zero reduces this problem to the calculation of {\langle {n} \rvert} X^2 {\lvert {n} \rangle} {\langle {n} \rvert} P^2 {\lvert {n} \rangle}. Either of these expecation values are again not too hard to compute for n=0,1. However, we now have to keep track of the proportionality constants. As expected this yields

\begin{aligned}{\langle {0} \rvert} X^2 {\lvert {0} \rangle} {\langle {0} \rvert} P^2 {\lvert {0} \rangle} &= \hbar^2/4  \\ {\langle {1} \rvert} X^2 {\lvert {1} \rangle} {\langle {1} \rvert} P^2 {\lvert {1} \rangle} &= 9 \hbar^2/4\end{aligned} \hspace{\stretch{1}}(3.8)

These are respectively

\begin{aligned}\Delta x \Delta p &= \left( 0 + \frac{1}{{2}} \right) \hbar \\ \Delta x \Delta p &= \left( 1 + \frac{1}{{2}} \right) \hbar\end{aligned} \hspace{\stretch{1}}(3.10)

However, these integrals were only straightforward (albeit tedious) to calculate because we had explicit representations for u_0(x) and u_1(x). For the general wave function, what we have to work with is either the Hankel function representation of 3.7 or the derivative form

\begin{aligned}u_n(x) &= (-1)^n\left( \frac{ \alpha}{\sqrt{\pi} 2^n n!} \right)^{1/2} e^{ \alpha^2 x^2/2}\frac{d^n}{d (\alpha x)^n}e^{ -\alpha^2 x^2}\end{aligned} \hspace{\stretch{1}}(3.12)

Expanding this explicitly for arbitrary n isn’t going to be feasible. We can reduce the scope of the problem by trying to be lazy and see how some work can be avoided. One possible trick is noting that we can express the squared momentum expectation in terms of the Hamiltonian

\begin{aligned}{\langle {n} \rvert} P^2 {\lvert {n} \rangle}&={\langle {n} \rvert} 2m \left( H - \frac{1}{{2}} m \omega^2 X^2 \right) {\lvert {n} \rangle} \\ &=\left( n + \frac{1}{{2}} \right) 2 m \hbar \omega- m^2 \omega^2 {\langle {n} \rvert} X^2 {\lvert {n} \rangle} \\ &=\left( n + \frac{1}{{2}} \right) 2 \hbar^2 \alpha^2 - \hbar^2 \alpha^4 {\langle {n} \rvert} X^2 {\lvert {n} \rangle} \\ \end{aligned}

So we can get away with only calculating {\langle {n} \rvert} X^2 {\lvert {n} \rangle}, an exersize in integration by parts

\begin{aligned}{\langle {n} \rvert} X^2 {\lvert {n} \rangle}&=\frac{ \alpha}{\sqrt{\pi} 2^n n!} \int dx x^2e^{ \alpha^2 x^2}\left(\frac{d^n}{d (\alpha x)^n}e^{ -\alpha^2 x^2}\right)^2 \\ &=\frac{ 1 }{\alpha^2 \sqrt{\pi} 2^n n!} \int dy y^2 e^{ y^2}\left(\frac{d^n}{d y^n}e^{ -y^2 }\right)^2 \\ &=\frac{ 1 }{\alpha^2 \sqrt{\pi} 2^n n!} \int dy \frac{1}{{2}} y \frac{ d}{dy} e^{ y^2}\left(\frac{d^n}{d y^n}e^{ -y^2 }\right)^2 \\ &=\frac{ 1 }{\alpha^2 \sqrt{\pi} 2^n n!} \frac{1}{{-2}}\int dy e^{ y^2}\frac{d}{dy} \left( y \left(\frac{d^n}{d y^n}e^{ -y^2 }\right)^2 \right)\\ &=\frac{ 1 }{\alpha^2 \sqrt{\pi} 2^n n!} \frac{1}{{-2}}\int dy e^{ y^2}\left( \left(\frac{d^n}{d y^n}e^{ -y^2 }\right)^2 + 2 y \frac{d^n}{d y^n}e^{ -y^2 }\frac{d^{n+1}}{d y^{n+1}}e^{ -y^2 }\right)\\ &=-\frac{1}{{2 \alpha^2}}-\frac{ 1 }{\alpha^2 \sqrt{\pi} 2^n n!} \frac{1}{{2}}\int dy \frac{d}{dy} e^{ y^2}\frac{d^n}{d y^n}e^{ -y^2 }\frac{d^{n+1}}{d y^{n+1}}e^{ -y^2 }\\ &=-\frac{1}{{2 \alpha^2}}+\frac{ 1 }{\alpha^2 \sqrt{\pi} 2^n n!} \frac{1}{{2}}\int dy e^{ y^2}\left(\frac{d^{n+1}}{d y^{n+1}}e^{ -y^2 }\frac{d^{n+1}}{d y^{n+1}}e^{ -y^2 }+\frac{d^n}{d y^n}e^{ -y^2 }\frac{d^{n+2}}{d y^{n+2}}e^{ -y^2 }\right)\\ \end{aligned}

The second term in this remaining integral is proportional to \left\langle{{n}} \vert {{n+2}}\right\rangle = 0, which leaves us with

\begin{aligned}{\langle {n} \rvert} X^2 {\lvert {n} \rangle}=-\frac{1}{{2 \alpha^2}} + \frac{n+1}{\alpha^2} = \frac{1}{{\alpha^2}}\left( n + \frac{1}{{2}} \right)\end{aligned} \hspace{\stretch{1}}(3.13)

Our squared momentum expectation value is then

\begin{aligned}{\langle {n} \rvert} P^2 {\lvert {n} \rangle}&=\left( n + \frac{1}{{2}} \right) 2 \hbar^2 \alpha^2 - \hbar^2 \alpha^4 {\langle {n} \rvert} X^2 {\lvert {n} \rangle} \\ &=\left( n + \frac{1}{{2}} \right) \hbar^2 \alpha^2 \end{aligned}

This completes the problem, and we are left with

\begin{aligned}\Delta x \Delta p = \left( n + \frac{1}{{2}} \right) \hbar.\end{aligned} \hspace{\stretch{1}}(3.14)

Problem 4.


Consider the following two-dimensional harmonic oscilator problem:

\begin{aligned}-\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial x^2}-\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial y^2}+ \frac{1}{{2}} K_1 x^2 u+ \frac{1}{{2}} K_2 y^2 u= E u\end{aligned} \hspace{\stretch{1}}(3.15)

where (x,y) are the coordinates of the particle. Use the separation of variables technique to obtain the energy eigenvalues. Discuss the degeneracy in the eigenvalues if K_1 = K_2.


Write u = A(x) B(y). Substitute and dividing throughout by u we have

\begin{aligned}\left( -\frac{\hbar^2}{2m} \frac{A''}{A} + \frac{1}{{2}} K_1 x^2 \right)+\left( -\frac{\hbar^2}{2m} \frac{B''}{B} + \frac{1}{{2}} K_2 y^2 \right)= E\end{aligned} \hspace{\stretch{1}}(3.16)

Introduction of a pair of constants E_1, E_2 for each of the independent terms we have

\begin{aligned}H_1 A &= -\frac{\hbar^2}{2m} A'' + \frac{1}{{2}} K_1 x^2 A = E_1 A \\ H_2 B &= -\frac{\hbar^2}{2m} B'' + \frac{1}{{2}} K_1 y^2 B = E_2 B \\ H &= H_1 + H_2 \\ E  &= E_1 + E_2\end{aligned} \hspace{\stretch{1}}(3.17)

For each of these equations we have a set of quantized eigenvalues and can write

\begin{aligned}E_{1m} &= \left(m + \frac{1}{{2}}\right) \hbar \sqrt{\frac{K_1}{m}} \\ E_{2n} &= \left(n + \frac{1}{{2}}\right) \hbar \sqrt{\frac{K_2}{m}} \\ H_1 A_m(x) &= E_{1m} A_m(x) \\ H_2 A_n(y) &= E_{2n} B_n(y)\end{aligned} \hspace{\stretch{1}}(3.21)

The complete eigenstates are then

\begin{aligned}u_{mn}(x,y) &= A_m(x) B_n(y)\end{aligned} \hspace{\stretch{1}}(3.25)

with total energy satisfying

\begin{aligned}H u_{mn}(x,y) &=\frac{\hbar}{\sqrt{m}} \left( \left(m + \frac{1}{{2}}\right) \sqrt{K_1} + \left(n + \frac{1}{{2}}\right) \sqrt{K_2} \right) u_{mn}(x,y)\end{aligned} \hspace{\stretch{1}}(3.26)

A general state requires a double sum over the possible combinations of states \Psi = \sum_{mn} c_{mn} u_{mn}, however if K_1 = K_2 = K, we cannot distinguish between u_{mn} and u_{nm} based on the energy eigenvalues

\begin{aligned}H u_{mn}(x,y) &= \hbar\sqrt{\frac{K}{m}} \left( m + n + 1 \right) u_{mn}(x,y) = H u_{nm}(x,y)\end{aligned} \hspace{\stretch{1}}(3.27)

In this case, we can write the wave function corresponding to a general state for the system as just \Psi = \sum_{m+ n = \text{constant}} c_{mn} u_{mn}. This reduction in the cardinality of this set of basis eigenstates is the degeneracy to be discussed.

Problem 5,6.


Consider now a variation on Problem 4 in which we have a coupled oscillator with the potential given by

\begin{aligned}V(x,y) = \frac{1}{{2}} K \Bigl( x^2 + y^2 + 2 \lambda x y \Bigr)\end{aligned} \hspace{\stretch{1}}(3.28)

Obtain the energy eigenvalues by changing variables (x,y) to (x', y') such that the new potential is quadratic in (x', y'), without the coupling term.


This has the look of a diagonalization problem so we write the potential in matrix form

\begin{aligned}V(x,y)= \frac{1}{{2}} K\begin{bmatrix}x & y\end{bmatrix}\begin{bmatrix}1 & \lambda \\ \lambda & 1\end{bmatrix}\begin{bmatrix}x \\  y\end{bmatrix} = \frac{1}{{2}} K \tilde{X} M X\end{aligned} \hspace{\stretch{1}}(3.29)

The similarity transformation required is

\begin{aligned}M = \frac{1}{{\sqrt{2}}}\begin{bmatrix}1 & 1 \\ 1 & -1\end{bmatrix}\begin{bmatrix}1+ \lambda & 0 \\ 0 & 1 - \lambda\end{bmatrix}\frac{1}{{\sqrt{2}}}\begin{bmatrix}1 & 1 \\ 1 & -1\end{bmatrix}\end{aligned} \hspace{\stretch{1}}(3.30)

Our change of variables is therefore

\begin{aligned}X' =\frac{1}{{\sqrt{2}}}\begin{bmatrix}1 & 1 \\ 1 & -1\end{bmatrix}X=\frac{1}{{\sqrt{2}}}\begin{bmatrix}x + y \\ x - y\end{bmatrix}\end{aligned} \hspace{\stretch{1}}(3.31)

Our Laplacian should also remain diagonal under this orthonormal transformation, but we can verify this by expanding out the partials explicitly

\begin{aligned}\frac{\partial {}}{\partial {x}} &=\frac{\partial {x'}}{\partial {x}}\frac{\partial {}}{\partial {x'}}+\frac{\partial {y'}}{\partial {x}}\frac{\partial {}}{\partial {y'}} = \frac{1}{{\sqrt{2}}} \left( \frac{\partial {}}{\partial {x'}} + \frac{\partial {}}{\partial {y'}} \right) \\ \frac{\partial {}}{\partial {y}} &=\frac{\partial {x'}}{\partial {y}}\frac{\partial {}}{\partial {x'}} +\frac{\partial {y'}}{\partial {y}}\frac{\partial {}}{\partial {y'}}= \frac{1}{{\sqrt{2}}}\left( \frac{\partial {}}{\partial {x'}} - \frac{\partial {}}{\partial {y'}} \right)\end{aligned} \hspace{\stretch{1}}(3.32)

Squaring and summing we have

\begin{aligned}\frac{\partial^2}{\partial x^2} +\frac{\partial^2}{\partial y^2}&=\frac{1}{{2}} \left( \frac{\partial {}}{\partial {x'}} + \frac{\partial {}}{\partial {y'}} \right)^2+\frac{1}{{2}} \left( \frac{\partial {}}{\partial {x'}} - \frac{\partial {}}{\partial {y'}} \right)^2=\frac{\partial^2}{\partial {x'}^2} +\frac{\partial^2}{\partial {y'}^2}\end{aligned} \hspace{\stretch{1}}(3.34)

Our transformed Hamiltonian operator is thus

\begin{aligned}-\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial {x'}^2}-\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial {y'}^2}+ \frac{1}{{2}} K(1+\lambda) {x'}^2 u+ \frac{1}{{2}} K(1-\lambda) {y'}^2 u= E u\end{aligned} \hspace{\stretch{1}}(3.35)

So, provided {\left\lvert{\lambda}\right\rvert} < 1, the energy eigenvalue equation is given by 3.26 with K_1 = K(1+ \lambda), and K_2 = K(1 -\lambda).

Problem 7.


Consider two coupled harmonic oscillators in one dimension of natural length a and spring constant K connecting three particles located at x_1, x_2, and x_3. The corresponding Schr\”{o}dinger equation is given as

\begin{aligned}-\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial {x_1}^2}-\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial {x_2}^2}-\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial {x_3}^2}+ \frac{K}{2}\left((x_2 - x_1 - a)^2+(x_3 - x_2 - a)^2\right) u= E u\end{aligned} \hspace{\stretch{1}}(3.36)

Obtain the energy eigenvalues using the matrix method.


Let’s start with an initial simplifying substutition to get rid of the factors of a. Write

\begin{aligned}r_1 &= x_1 + a \\ r_2 &= x_2 \\ r_3 &= x_3 - a\end{aligned} \hspace{\stretch{1}}(3.37)

These were picked so that the differences in our quadratic terms involve only factors of r_k

\begin{aligned}x_2 - x_1 - a &= r_2 - r_1 \\ x_3 - x_2 - a &= r_3 - r_2\end{aligned} \hspace{\stretch{1}}(3.40)

Schr\”{o}dinger’s equation is now

\begin{aligned}-\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial {r_1}^2}-\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial {r_2}^2}-\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial {r_3}^2}+ \frac{K}{2}\left((r_2 - r_1)^2+(r_3 - r_2)^2\right) u= E u\end{aligned} \hspace{\stretch{1}}(3.42)

Putting our potential into matrix form, we have

\begin{aligned}V(r_1, r_2, r_3) &=\frac{K}{2}\left((r_2 - r_1)^2+(r_3 - r_2)^2\right)=\frac{K}{2}\begin{bmatrix}r_1 & r_2 & r_3\end{bmatrix}\begin{bmatrix}1 & -1 & 0 \\ -1 & 2 & -1 \\ 0 & -1 & 1\end{bmatrix}\begin{bmatrix}r_1 \\  r_2 \\  r_3\end{bmatrix}\end{aligned} \hspace{\stretch{1}}(3.43)

This symmetric matrix, let’s call it M

\begin{aligned}M=\begin{bmatrix}1 & -1 & 0 \\ -1 & 2 & -1 \\ 0 & -1 & 1\end{bmatrix}\end{aligned} \hspace{\stretch{1}}(3.44)

has eigenvalues 0,1,3, with orthonormal eigenvectors

\begin{aligned}e_0 &=\frac{1}{{\sqrt{3}}}\begin{bmatrix}1 \\ 1 \\ 1\end{bmatrix} \\ e_1 &=\frac{1}{{\sqrt{2}}}\begin{bmatrix}1 \\ 0 \\ -1\end{bmatrix} \\ e_3 &=\frac{1}{{\sqrt{6}}}\begin{bmatrix}1 \\ -2 \\ 1\end{bmatrix}\end{aligned} \hspace{\stretch{1}}(3.45)


\begin{aligned}U = [e_0 e_1 e_3]=\begin{bmatrix}\frac{1}{{\sqrt{3}}} & \frac{1}{{\sqrt{2}}}  & \frac{1}{{\sqrt{6}}}  \\ \frac{1}{{\sqrt{3}}} & 0  & -\frac{2}{\sqrt{6}}  \\ \frac{1}{{\sqrt{3}}} & -\frac{1}{{\sqrt{2}}}  & \frac{1}{{\sqrt{6}}}\end{bmatrix}\end{aligned} \hspace{\stretch{1}}(3.48)

\begin{aligned}M = U\begin{bmatrix}0 & 0 & 0 \\ 0 & 1 & 0 \\ 0 & 0 & 3\end{bmatrix}\tilde{U}=U D \tilde{U}\end{aligned} \hspace{\stretch{1}}(3.49)

Writing R' = \tilde{U} R, and \boldsymbol{\nabla}' = \tilde{U} \boldsymbol{\nabla}, we see that the Laplacian has no mixed partial terms after transformation

\begin{aligned}\boldsymbol{\nabla}' \cdot \boldsymbol{\nabla}' &= (\tilde{U} \boldsymbol{\nabla})^{\tilde{}} \tilde{U} \boldsymbol{\nabla} \\ &= \tilde{\boldsymbol{\nabla} } \boldsymbol{\nabla} \\ &= \boldsymbol{\nabla} \cdot \boldsymbol{\nabla}\end{aligned}

Schr\”{o}dinger’s equation is then just

\begin{aligned}\left( -\frac{\hbar^2}{2m} {\boldsymbol{\nabla}'}^2 + \frac{K}{2} \tilde{R'} D R' \right) u = E u\end{aligned} \hspace{\stretch{1}}(3.50)


\begin{aligned}-\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial {r_1'}^2}-\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial {r_2'}^2}-\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial {r_3'}^2}+ \frac{K}{2}\left({r_2'}^2+3 {r_3'}^2\right) u= E u\end{aligned} \hspace{\stretch{1}}(3.51)

Separation of variables provides us with one free particle wave equation, and two harmonic oscillator equations

\begin{aligned}-\frac{\hbar^2}{2m} \frac{\partial^2 u_1}{\partial {r_1'}^2} &= E_1 u_1 \\ -\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial {r_2'}^2} + \frac{K}{2} {r_2'}^2 u_2 &= E_2 u_2 \\ -\frac{\hbar^2}{2m} \frac{\partial^2 u}{\partial {r_3'}^2} + \frac{3 K}{2} {r_3'}^2 u_3 &= E_3 u_3\end{aligned} \hspace{\stretch{1}}(3.52)

We can borrow the Harmonic oscillator energy eigenvalues from problem 4 again with K_1 = K, and K_2 = 3 K.

Problem 8.


As a variation of Problem 7 assume that the middle particle at x_2 has a different mass M. Reduce this problem to the form of Problem 7 by a scale change in x_2 and then use the matrix method to obtain the energy eigenvalues.


We write \sqrt{M} x_2 = \sqrt{m} x_2', x_1 + a = x_1', x_3 - a = x_3', and then Schr\”{o}dinger’s equation takes the form

\begin{aligned}\left( -\frac{\hbar^2}{2m} {\boldsymbol{\nabla}'}^2 + V(X') \right) u &= E u \end{aligned} \hspace{\stretch{1}}(3.55)

\begin{aligned}V(X') = \frac{K}{2} \left( \left( \sqrt{\frac{m}{M}} x_2' - x_1' \right)^2+\left( -\sqrt{\frac{m}{M}} x_2' + x_3' \right)^2\right)\end{aligned} \hspace{\stretch{1}}(3.56)

With \mu = \sqrt{m/M}, we have

\begin{aligned}V(X') = \frac{K}{2} \tilde{X'}\begin{bmatrix}1 & -\mu & 0 \\ -\mu & 2 \mu^2 & -\mu \\ 0 & -\mu & 1\end{bmatrix}X'\end{aligned} \hspace{\stretch{1}}(3.57)

We find that this symmetric matrix has eigenvalues 0, 1, 1 + 2 \mu^2, and eigenvectors

\begin{aligned}e_0 &=\frac{1}{{\sqrt{1 + 2 \mu^2}}}\begin{bmatrix}\mu \\  1 \\  \mu\end{bmatrix} \\ e_1 &=\frac{1}{{\sqrt{2}}}\begin{bmatrix}1 \\  0 \\  -1\end{bmatrix} \\ e_{1+ 2 \mu^2} &=\frac{1}{{\sqrt{2 + 4 \mu^2}}}\begin{bmatrix}1 \\  -2 \mu \\  1\end{bmatrix} \end{aligned} \hspace{\stretch{1}}(3.58)

The rest of the problem is now no different than the tail end of Problem 7, and we end up with K_1 = K, K_2 = (1 + 2 \mu^2) K.


[1] BR Desai. Quantum mechanics with basic field theory. Cambridge University Press, 2009.


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