To illustrate the basic feature of the new Schrödinger equation of Real Quantum Mechanics RealQM, let us reduce from 3d to 2d, to get the following formulation for a molecule with $N$ electrons (like graphene):
Find the wave function $\Psi (x)$ with $x$ a 2d Euclidean coordinate, of the form
- $\Psi (x) = \Psi_1(x) + \Psi_2 (x) + + \Psi_N(x)$
where the $\Psi_n(x)$ for $n=1,2,...,N$ are one-electron wave functions with non-overlapping supports meeting a Bernoulli free boundary $\Gamma$, which minimizes the total energy
- $E(\Psi ) = \frac{1}{2}\sum_{n=1}^N\int \vert\nabla\Psi_n\vert^2dx-\int P(x)\Psi^2dx$ (kinetic + potential energy)
with $P(x)$ a potential with contribution from electron and kernel charges, under the side condition
- $\int\Psi_n^2 dx = 1$ for $n=1,2,...,N,$
and the Bernoulli free boundary condition:
- $\Psi (x)$ is continuous and
- the normal derivative of $\Psi_n(x)$ vanishes on $\Gamma$ for $n=1,2,...,N.$
This minimisation problem is solved with a gradient method realised as an explicit update consisting of three lines for iterative update of (i) wave function, (ii) level set function for $\Gamma$ and (iii) potential $P(x)$ realised in this code.
We consider a molecule consisting of two H atoms in green and one Beryllium atom with valence shell consisting of two electrons as two "half-shells" in red and blue. We start the iteration with the electrons concentrated into disks without overlap:
We compare with the atoms well separated with a total energy of -5.803 after energy minimisation.
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