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The power of the Finite Difference Approximation is that it can be used for potentials that are not analytically solvable! Consider the following potential as
The power of the Finite Difference Approximation is that it can be used for potentials that are not analytically solvable! Consider the following potential as a crude approximation to the harmonic oscillator potential (V(x)=21kx2) with k=1 : V(x)=29029x=3x=0x=3 (A) (2 points) Using the N=3 Finite Difference Approximation, write down the 3x3 matrix representation of the Hamiltonian, H, for the above potential. The final matrix should include the "t" value in the lecture notes - no need to plug anything else in - just keep it as "t". (B) (2 points) Calculate, by hand, the characteristic polynomial of the matrix in (A) by calculating det(HI)=0. Write down this characteristic polynomial but do not solve it. (C) (2 points) It's pretty crazy how complicated this expression already is for such a simple system. You can try to find the roots by hand, or you can use Mathematica's Solve function (Solve [f(x)==0,x] ) function to find the three roots of this equation. These are the three eigenvalues of the Hamiltonian
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