Show that if hQ^h=Q^hhfor all functionsh(in Hilbert space), thenfQ^g=Q^fgfor allrole="math" localid="1655395250670" fandg(i.e., the two definitions of "Hermitian" -Equations 3.16 and 3.17- are equivalent).

Short Answer

Expert verified

Hermitian equations have two definitions, both of which are equivalent.

fQ^g=Q^fg

gQ^f=Q^gf

Step by step solution

01

Concept used

For a Hermitian operator (say Q), the following condition must be satisfied:

abg*Qfdx=abf(Qg)*dx


02

Given information from question

For a Hermitian operator (say Q), the following condition must be satisfied:

abg*Qfdx=abf(Qg)*dx

This condition can be written as: Using the more compact bracket notation, this condition can be written as:

gQ^f=Q^gf

03

Explanation

Start with a less restrictive condition that is:

hQh=Qhh......(1)

Let ,h=f+gso:

hQ^h=f+gQ^f+Q^g......(2)=fQ^f+gQ^g+fQ^g+gQ^f......(3)

We can also write this equation as:

Q^hh=Q^f+Q^gf+g......(4)=Q^ff+Q^gg+Q^fg+Q^gf......(5)

Use assumption hQ^h=Q^hhfor all functions, we have fQ^f=Q^ffand gQ^g=QQ^ggso, equating (2) and (3) and cancel out the common terms, we get:fQ^g+gQ^f=Q^fg+Q^gf

Now we do the same to above but with h=f+ig, so:

hQh^=f+igQ^f+iQ^g=fQ^f+(i)(i)gQ^g+ifQ^gigQ^f=fQ^f+gQ^g+ifQ^gigQ^f......(6)Qhh=Q^ff+Q^gg+iQ^fgiQgf......(7)

Using the assumption hQ^h=Q^hhfor all functions, we have fQ^f=Q^fand gQ^g=Q^gso, equating (2) and (3) and cancel out the common terms, we get:fQ^ggQ^f=Q^fgQ^gf......(8)

Add equation (4) and (8), we get,

fQ^g=Q^fg

If we subtract equation (8) from equation (4), we get,

gQ^f=Q^gf

Thus, the given statement is proved, i.e., gQ^f=Q^gf.

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Most popular questions from this chapter

Findthemomentum-spacewavefunctionϕn(p,t)forthenthstationarystateoftheinfinitesquarewell.Graph|ϕ1(p,t)|2and|ϕ2(p,t)|2,asfunctionsofp(payparticularattentiontothepointsp=±nπh/a).Useϕn(p,t)tocalculatetheexpectationvalueofp2.CompareyouranswertoProblem2.4.

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ψn=1n!(a^+)nψ0(2.68).

a_|α>=α|a>(the Eigen value α can be any complex number).

(a)Calculate <x>,<x2>,<p>,<p2>in the state |α〉. Hint: Use the technique in Example 2.5, and remember that is the Hermitian conjugate of a-. Do not assume α is real.

(b) Find σx; show that σxσp=h/2.

(c) Like any other wave function, a coherent state can be expanded in terms of energy Eigen states: |α>=n=0Cn|n>.

Show that the expansion coefficients arecn=αnn!c0.

(d) Determine by normalizing |α〉. Answer: exp(-α2/2)

(e) Now put in the time dependence: |n>e-iEntIh|n>,

and show that |αt|remains an Eigen state of a-, but the Eigen value evolves in time:α(t)=e-iωt So a coherent state stays coherent, and continues to minimize the uncertainty product.

(f) Is the ground state (n=0>)itself a coherent state? If so, what is the Eigen value?

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

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

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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.

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