This time we will improve the quantum well. Specifically, by adding a potential barrier to the center of the quantum well, we will make it play a more role as a quantum bit.
In order to treat the quantum well as a bit, the quantum well is improved here. Specifically, a potential wall is created at the center of the quantum well. If the height of this potential is $ V_b [eV] $ and the width is $ W $, the potential is expressed as follows.
V(x)=\left\{\begin{array}{ll}
V_b & (|x|\leq \frac{W}{2})\\
0 & (\frac{W}{2} < |x| \leq \frac{L}{2})\\
+\infty & (|x| > \frac{L}{2})
\end{array}
\right.
\quad (5.1)
Let's plot the state when the size $ V_b $ of the barrier between the ground state and the first excited state is increased by 3 [eV] little by little.
From the above results, it was found that it can be divided into two for about $ 30 [eV] $.
Using the above result, an electric field is applied to the quantum well with a barrier. If there is a barrier, the electric field applied to the quantum well will have an effect even if it is much smaller than before. Last time it was increased in 1.0e9 units, but this time it can be seen to change just by increasing it in 1.0e6 units. Let's check this.
It can be confirmed that the electric field is about 10e7 and almost all distribution is on the left.
It can be confirmed that the electric field is about 10e7 and almost all distribution is on the right.
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