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Show that two noncommuting operators cannot have a complete set of common eigenfunctions. Hint: Show that if P^and Q^have a complete set of common eigenfunctions, then [P^.Q^]f=0for any function in Hilbert space.

Short Answer

Expert verified

A whole set of common eigenfunctions cannot be shared by two noncommuting operators.

Step by step solution

01

Concept used

The same complete set of common eigenfunctions:

P^fn=λnfnandQ^fn=μnfn

02

Calculation

Assuming the operators P^ and Q^have the same complete set of common eigenfunctions, that is:

P^fn=λnfnandQ^fn=μnfn

And suppose the set fnis complete, so that any function in Hilbert space f{x)can be expressed as a linear combination, that is:

f=∑cnfn

Solving for the above function,

P^,Q^f=P^Q^-Q^P^∑cnfn=P^∑cnμnfn-Q^∑cnλnfn=∑cnμnλnfn-∑cnλnμnfn=0

If two operators have the same set of eigenfunctions, the commutator will be zero.

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Most popular questions from this chapter

The Hermitian conjugate (or adjoint) of an operator Q^is the operatorQ^†such that

⟨f∣Q^g⟩=⟨Q^†f∣g⟩ (´Ú´Ç°ù²¹±ô±ôfandg).

(A Hermitian operator, then, is equal to its Hermitian conjugate:Q^=Q^†)

(a)Find the Hermitian conjugates of x, i, andd/dx.

(b) Construct the Hermitian conjugate of the harmonic oscillator raising operator,a+(Equation 2.47).

(c) Show that(Q^R^)†=R^†Q^†.

An anti-Hermitian (or skew-Hermitian) operator is equal to minus its Hermitian conjugate:

QÁåœt=-QÁåœ

(a) Show that the expectation value of an anti-Hermitian operator is imaginary. (b) Show that the commutator of two Hermitian operators is anti-Hermitian. How about the commutator of two anti-Hermitian operators?

The Hamiltonian for a certain three-level system is represented by the matrix

H=(a0b0c0b0a), where a, b, and c are real numbers.

(a) If the system starts out in the state |&(0)⟩=(010)what is |&(t) ?

(b) If the system starts out in the state|&(0)⟩=(001) what is|&(t) ?

(a) Write down the time-dependent "Schrödinger equation" in momentum space, for a free particle, and solve it. Answer: exp(-ip2t/2mh)Φ(p,0).

(b) Find role="math" localid="1656051039815" Φ(p,0)for the traveling gaussian wave packet (Problem 2.43), and construct Φ(p,t)for this case. Also construct |Φ(p,t)|2, and note that it is independent of time.

(c) Calculaterole="math" localid="1656051188971" pandrole="math" localid="1656051181044" p2by evaluating the appropriate integrals involvingΦ, and compare your answers to Problem 2.43.

(d) Show thatrole="math" localid="1656051421703" <H>=<p>2/2m+<H>0(where the subscript denotes the stationary gaussian), and comment on this result.

The Hamiltonian for a certain two-level system is

H^=oË™(1><1-2><2+1><2+2><1)

where1>,2>is an orthonormal basis and localid="1658120083298" oË™ is a number with the dimensions of energy. Find its eigenvalues and eigenvectors (as linear combinations oflocalid="1658120145851" 1> and2> . What is the matrix H representingH^ with respect to this basis?

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