00:01
First, in this problem, we need to find and sketch the probability density.
00:06
Given a wave function, the probability density, p of x, is equal to the wave function times its complex conjugate si -star.
00:18
Thus, for our wave function, psi equals to square root 2 over a, e -to -the -minus x over a, for x greater than 0, and 0 for, x less than zero, this probability density function will be 2 over a times e to the minus x over a, times e to the minus x over a, which is equal to 2 over a, e to the minus 2x over a.
00:55
Part b asks us to find the probability that the particle will be at any point where x over a.
01:01
Part b asks us to find the probability that the particle will be at any point where x is less than zero.
01:06
Now, the probability density when x is less than zero will be zero because of the fact that our wave function is zero when x is less than zero, and when x is less than zero, so 0 times 0 is still 0.
01:34
Thus, for part b, the integral of the probability density function, dx, from minus infinity to 0, will be 0 because p of x in this range is 0.
01:50
Finally, we're asked to show that si is normalized and then find the probability of mining the particle between 0 and a.
01:58
First, to find that si is normalized, we need to integrate the probability density function from minus infinity to infinity...