Question: Verify the correctness of the normalization constant of the radial wave function given in Table 7.4 as

1(2a0)3/23a0

Short Answer

Expert verified

Answer

It has been proved that the normalization for the case 2pstateis correct.

Step by step solution

01

Given data

The radial wave function corresponding to the state is,

Rn/lr=re-r2a02a03/23a0

02

Normalization condition

The radial part of the Hydrogen atom wave function should satisfy the condition as,

0{Rn/lr}2r2dr=1

03

Determining whether the given normalization constant is correct

Check equation (I) with the given wave function as:

=12a033a00r4e-ra0dr=124a030r4e-ra0dr

Let us assume,

r/a0=zr=a0zdr=a0dz

Then the integral becomes

=124a05a050z4e-zdz=Γ524=4!24=2424=1

Here Γ5 is the gamma function.

Thus the normalization is correct.

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Most popular questions from this chapter

To conserve momentum, an atom emitting a photon must recoil, meaning that not all of the energy made available in the downward jump goes to the photon. (a) Find a hydrogen atom's recoil energy when it emits a photon in a n = 2 to n = 1 transition. (Note: The calculation is easiest to carry out if it is assumed that the photon carries essentially all the transition energy, which thus determines its momentum. The result justifies the assumption.) (b) What fraction of the transition energy is the recoil energy?

Calculate the “series limit” of the Lyman series of spectral lines. This is defined as the shortest wavelength possible of a photon emitted in a transition from a higher initial energy level to the ni=1 final level. (Note: In figure 7.5, the spectral lines of the series “crowd together” at the short-wavelength end of the series).

Here we Pursue the more rigorous approach to the claim that the property quantized according to ml is Lz,

(a) Starting with a straightforward application of the chain rule,

φ=xφ/x+yφy+zφz

Use the transformations given in Table 7.2 to show that

φ=-yx+xy

(b) Recall that L = r x p. From the z-component of this famous formula and the definition of operators for px and py, argue that the operator for Lz is -ihφ..

(c) What now allows us to say that our azimuthal solutioneimlφ has a well-defined z-component of angular momentum and that is value mlh.

Consider an electron in the ground state of a hydrogen atom. (a) Sketch plots of E and U(r) on the same axes (b) Show that, classically, an electron with this energy should not be able to get farther than 2a0from the proton. (c) What is the probability of the electron being found in the classically forbidden region?

Which electron transitions in singly ionized helium yield photon in the 450 - 500 nm(blue) portion of the visible range, and what are their wavelengths?

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