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Calculate the electric dipole moment p and estimate the transition time for a hydrogen atom electron making an electric dipole transition from the

(n,l,m)=(3,2,0)to the (2,1,0) state.

Short Answer

Expert verified

The electric dipole moment, p=1.04x10-29Cm

The transition time1.2×10-7s

Step by step solution

01

Given Formula:

Initial state is (n,l,ml)=(3,2,0) and the final state is (2,1,0).

Where, n is the principal quantum number, l is the azimuthal quantum number, ml is the magenetic quantum number.

Here, the electric dipole moment is given by,

p=-eRe(r¯Ψ2,1,0*(r¯)Ψ3,2,0(r¯)r2sinθdrdθdϕ) ….. (1)

Where,Ψis the wave function, θ is the colatitude, ϕ is the azimuth, and r is the radius.

02

Wave functions:  

Wave functions can be calculated by,

Ψ2,1,0*r¯Ψ3,2,0r¯=1a03/2r3a0e-r/a034πcosθ13a03/222r2275a02e-r/2a0516π3cos2θ-1=1a0312213322r33a0e-5r/6a014π3×54cosθ3cos2θ-1=38π35a06r3e-5r/6a0cosθ3cos2θ-1

03

Integration of  r:

r¯=18.39/2a060r6e-5r/6a0dr0π3cos4θ-cos2θsinθdr=18.39/2a066!5/6a07-35cos5θ+13cos3θ=7206a078.39/2a065765-23

r¯=1.23a0 ….. (2)

04

Finding electric dipole moment:

From eq. (1) and eq. (2), you get

p=-1.23a0costE/h

Youalso know that,

role="math" localid="1659870308402" E=(-13.6eV)132-122=1.89eV

Hence,

p=-(1.23a0)cost1.89eV/h=1.6×10-19C1.23×0.0529×10-9m=1.04×10-29Cm

05

Finding Transition time:

Define the angular frequency as below.

ω=Ei-Efh=1.89eV×1.6x10-19J/eV6.63×10-34J.s=2.86×1015s-1

Hence, the transition time will be given by

Transitiontime128.85×10-12C2/Nm23×108m/s31.055×10-34J.s1.04×10-29Cm22.86×1015s-131.2×10-7s

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Most popular questions from this chapter

Question: The kinetic energy of hydrogen atom wave functions for which lis its minimum value of 0 is all radial. This is the case for the 1s and 2s states. The 2 p state has some rotational kinetic energy and some radial. Show that for very large n, the states of largest allowed lhave essentially no radial kinetic energy. Exercise 55 notes that the expectation value of the kinetic energy (including both rotational and radial) equals the magnitude of the total energy. Compare this magnitude with the rotational energy alone,L2/2mr2
,assuming that n is large. That lis as large as it can be, and thatrn2a0.

Explicitly verify that the simple function Rr=Aebrcan be made to satisfy radial equation (7-31), and in so doing, demonstrate what its angular momentum and energy must be.

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?

When applying quantum mechanics, we often concentrate on states that qualify as “orthonormal”, The main point is this. If we evaluate a probability integral over all space of ϕ1*ϕ1or of ϕ2*ϕ2, we get 1 (unsurprisingly), but if we evaluate such an integral forϕ1*ϕ2orϕ2*ϕ1 we get 0. This happens to be true for all systems where we have tabulated or actually derived sets of wave functions (e.g., the particle in a box, the harmonic oscillator, and the hydrogen atom). By integrating overall space, show that expression (7-44) is not normalized unless a factor of 1/2is included with the probability.

A particular vibrating diatomic molecule may be treated as a simple harmonic oscillator. Show that a transition from that n=2state directly to n=0ground state cannot occur by electric dipole radiation.

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