Chapter 4: Q28P (page 177)
For the most general normalized spinor (Equation 4.139),
compute
Short Answer
By solving we find the above value to be.
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Chapter 4: Q28P (page 177)
For the most general normalized spinor (Equation 4.139),
compute
By solving we find the above value to be.
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What is the probability that an electron in the ground state of hydrogen will be found inside the nucleus?
[Refer to. Problem 4.59for background.] Suppose and, where and Kare constants.
(a) Find the fields E and B.
(b) Find the allowed energies, for a particle of mass m and charge q , in these fields, Answer: Comment: If K=0this is the quantum analog to cyclotron motion; is the classical cyclotron frequency, and it's a free particle in the z direction. The allowed energies,, are called Landau Levels.
The (time-independent) momentum space wave function in three dimensions is defined by the natural generalization of Equation 3.54:
(a)Find the momentum space wave function for the ground state of hydrogen (Equation 4.80). Hint: Use spherical coordinates, setting the polar axis along the direction of p. Do the θ integral first. Answer:
(b) Check that is normalized.
(c) Use to calculate , in the ground state of hydrogen.
(d) What is the expectation value of the kinetic energy in this state? Express your answer as a multiple of , and check that it is consistent with the virial theorem (Equation 4.218).
Consider the observablesand .
(a) Construct the uncertainty principle for
(b) Evaluate in the hydrogen state .
(c) What can you conclude aboutin this state?
a) Check that satisfies the radial equation with and .
(b) Determine graphically the allowed energies for the infinite spherical well, when . Show that for large . Hint: First show that . Plot xandon the same graph, and locate the points of intersection.
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