Chapter 3: 3.20P (page 118)
Show that the energy-time uncertainty principle reduces to the "your name" uncertainty principle (Problem 3.14), when the observable in question is x.
Short Answer
The energy-time uncertainty principle reduces to
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Chapter 3: 3.20P (page 118)
Show that the energy-time uncertainty principle reduces to the "your name" uncertainty principle (Problem 3.14), when the observable in question is x.
The energy-time uncertainty principle reduces to
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(a) Check that the eigenvalues of the hermitian operator in Example 3.1 are real. Show that the eigenfunctions (for distinct eigenvalues) are orthogonal.
(b) Do the same for the operator in Problem 3.6.
(a) Show that the set of all square-integrable functions is a vector space (refer to Section A.1 for the definition). Hint: The main problem is to show that the sum of two square-integrable functions is itself square-integrable. Use Equation 3.7. Is the set of all normalized functions a vector space?
(b) Show that the integral in Equation 3.6satisfies the conditions for an inner product (Section A.2).
(a) For what range of is the function in Hilbert space, on the interval ? Assume is real, but not necessarily positive.
(b) For the specific case , is in this Hilbert space? What about? How about ?
Show that the energy-time uncertainty principle reduces to the "your name" uncertainty principle (Problem 3.14), when the observable in question is x.
The Hermitian conjugate (or adjoint) of an operator is the operatorsuch that
(A Hermitian operator, then, is equal to its Hermitian conjugate:)
(a)Find the Hermitian conjugates of x, i, and.
(b) Construct the Hermitian conjugate of the harmonic oscillator raising operator,(Equation 2.47).
(c) Show that.
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