Let Q^be an operator with a complete set of orthonormal eigenvectors:localid="1658131083682" Q^en>=qnen(n=1,2,3,....) Show thatQ^can be written in terms of its spectral decomposition:Q^=nqnen><en|

Hint: An operator is characterized by its action on all possible vectors, so what you must show is thatQ^={nqnen><en|} for any vector α>.

Short Answer

Expert verified

The operator can be written as a spectral decomposition operator Q^=nqnen><en|.

Step by step solution

01

Spectral decomposition operator

The underlying vector space on which the operator functions is further decomposed canonically by the spectral decomposition, which is provided by the spectral theorem. Every real, symmetric matrix is diagonalizable according to the spectral theorem for symmetric matrices, which was established by Augustin-Louis Cauchy.

02

Write the operator as a spectral decomposition operator

Consider an operatorQ^with a complete, orthonormal set of eigenvectors, that is:

Q^em>=qmem>

Whereqmis the eigenvalue. Write the operator as a spectral decomposition operator.

First, write any vectorα>in terms of the eigenvectors set, since the eigenvectors of form a complete, orthonormal set:

α>=mamem>

Here amis the coefficient of the basis vector em>. Now apply Q^on this equation and get the result as:

Q^α>=mamqmem>

Write Q^as:

Q^=nqne><en|

then:

role="math" localid="1658132420035" Q^α>=nqnen><en|mamem>=n,mqnamδnme><em|=mamqmem>

So:

Q=nqnen><en|

Thus, the operator can be written as a spectral decomposition operator Q=nqnen><en|.

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Most popular questions from this chapter

Find the momentum-space wave function, Φ(p,t),for a particle in the ground state of the harmonic oscillator. What is the probability (to 2significant digits) that a measurement of p on a particle in this state would yield a value outside the classical range (for the same energy)? Hint: Look in a math table under "Normal Distribution" or "Error Function" for the numerical part-or use Mathematica.

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(a) For a function f(x)that can be expanded in a Taylor series, show that f(x+x0)=eip^x0Ihf(x)

wherex_{0}

is any constant distance). For this reason, p^/his called the generator of translations in space. Note: The exponential of an operator is defined by the power series expansion: eQ^1+Q^+(1/2)Q^2+(1/3!)Q^3+...

(b) If ψ(x,t)satisfies the (time-dependent) Schrödinger equation, show that ψ(x,t+t0)=e-iH^t0/hψ(x,t)

where t_{0}is any constant time); -H^/his called the generator of translations in time.

(c) Show that the expectation value of a dynamical variableQ(x,p,t), at time , t+t0can be written34

<Q>t+t0=<ψx,t|eiH^t0/hQ^x^,p^,t+t0e-iH^t0/h|ψx,t>

Use this to recover Equation 3.71. Hint: Lett0=dt, and expand to first order in dt.

Solve Equation 3.67 for Ψ(x). Note that xand pare constants.

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