Add draft abstract and conclusion.
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\begin{document}
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\begin{abstract}
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We have simulated the two-dimensional time-dependent Schrödinger equation, to study
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variations of the double-slit experiment. To solve the partial differential equations
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we have applied the Crank-Nicolson scheme in 2+1 dimensions, to derive a discretized
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equation. In addition, we have used Dirichlet boundary conditions to express the
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equation in matrix form and solve it using the sparse matrix solver \verb|superlu|.
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Our implementation, and choice of solver method, resulted in conserved total
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probability $\sum_{\ivec, \jvec} p_{\ivec, \jvec}^{n}=1$ for both the single and
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double slit setup. To illustrate the time evolution of the probability function,
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we created colormap plots at time steps $t = [0, 0.001, 0.002]$. We also included
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separate plots for each time step of Re$(u_{\ivec, \jvec})$ and Im$(u_{\ivec, \jvec})$.
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In addition, we determined the normalized particle detection probability $p(y \ | \ x=0.8, t=0.002)$,
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for single-, double- and triple-slit.
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\end{abstract}
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\end{document}
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