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Use Equation 6.59 to estimate the internal field in hydrogen, and characterize quantitatively a "strong" and "weak" Zeeman field.

Short Answer

Expert verified

The value of internal magnetic field is 12 T .

The strong and weak Zeeman field is characterized as:

Bext≫Bintstrong Zeeman field

Bext≫Bintweak Zeeman field

Step by step solution

01

Expression for the internal magnetic field

The expression for the internal magnetic field in the hydrogen atom is given as follows,

B=14πε0.emc2r3L

Here,ε0is the permittivity of the free space with value role="math" localid="1658138846877" 8.9×10-10C2/N.m2,e is the charge on electron with value 1.6×10-19C,m, is the mass of the electron with value 9.1×10-31kg,c is the speed of light with value 3×108m/s,ris the Bohr’s radius with value 0.53×10-10m, and L=ħwhich is Planck’s constant with value 1.05×10-34J.s.

02

Determination of the internal magnetic field of the hydrogen atom

Assume r=a that is Bohr’s radius, and L=ħ.

Substitute the values in the expression for the internal magnetic field in the hydrogen atom.

B=14πε0.emec2a3ħ=14π8.9×10-10C2/N.m2×1N.m1J.1.6×10-19C1.05×10-34J.s9.1×10-31kg3×108m/s20.53×10-10m=12C.m/s×1T1C.m/s=12T

03

Quantitative characterization of strong and weak Zeeman field

It is known that the strong Zeeman field is Bext>>10Tand the weak Zeeman field is Bext≪10T. So,Bext≫BintandBext≪Bint .

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Most popular questions from this chapter

For the harmonic oscillator[Vx=1/2kx2], the allowed energies areEN=(n+1/2)ħӬ,(n=0.1.2,..),whererole="math" localid="1656044150836" Ӭ=k/mis the classical frequency. Now suppose the spring constant increases slightly:k→(1+ο')k(Perhaps we cool the spring, so it becomes less flexible.)

(a) Find the exact new energies (trivial, in this case). Expand your formula as a power series inο,, up to second order.

(b) Now calculate the first-order perturbation in the energy, using Equation 6.9. What ishere? Compare your result with part (a).

Hint: It is not necessary - in fact, it is not permitted - to calculate a single integral in doing this problem.

Two identical spin-zero bosons are placed in an infinite square well (Equation 2.19). They interact weakly with one another, via the potential

V(x1,x2)=-aV0δ(x1-x2). (2.19).

(where V0is a constant with the dimensions of energy, and a is the width of the well).

(a)First, ignoring the interaction between the particles, find the ground state and the first excited state—both the wave functions and the associated energies.

(b) Use first-order perturbation theory to estimate the effect of the particle– particle interaction on the energies of the ground state and the first excited state.

Question: In Problem 4.43you calculated the expectation value ofrsin the stateψ321. Check your answer for the special cases s = 0(trivial), s = -1(Equation 6.55), s = -2(Equation 6.56), and s = -3(Equation 6.64). Comment on the case s = -7.

Consider the (eight) n=2states, |2ljmj⟩. Find the energy of each state, under weak-field Zeeman splitting, and construct a diagram like Figure 6.11 to show how the energies evolve asBext increases. Label each line clearly, and indicate its slope.

Consider the (eight) n=2states,|2lmlms⟩.Find the energy of each state, under strong-field Zeeman splitting. Express each answer as the sum of three terms: the Bohr energy, the fine-structure (proportional toa2), and the Zeeman contribution (proportional toμBBext.). If you ignore fine structure altogether, how many distinct levels are there, and what are their degeneracies?

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