00:01
So here in this case, if we consider this wave function, here wave function, it is si, it is equal to ax 1 minus x divided by the a, and the si it is equal to ax minus x squared divided by the a, it is here.
00:17
So what is happening? we are considering the boundary condition.
00:21
So first of all, we are looking at this boundary condition.
00:24
And what is happening in the boundary condition? we can say x it is equal to 0.
00:29
So what is happening? the si it is equal to a multiplied with this 0 minus 0 divided by the a so this particular thing it is 0 so here we can say at x it is equal to a psi it is equal to 0 so this particular thing it is here further what is happening we are looking at the cases here so the energy of a l the ellen wave function the island wave function it is here and it is having this defined by this rogen wave equation.
01:01
Further what is happening, we are considering this normalization of the function we are considering.
01:06
So we are having this normalization of the function it is here.
01:10
So when we talk about this normalization of the function here, it is summation b to a, integration b to a it is here.
01:18
So we can say, si star, psi, and here it is d x it is equal to 1.
01:24
So this particular thing it is considered here.
01:26
So what is happening in this case? we are having this equation...