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Solve Equation 3.67 for Ψ(x) . Note that <x>and<p> are constants.

Short Answer

Expert verified

Equation 3.67 for ΨxisAe-ax-x2l2heipxlh

Step by step solution

01

The Uncertainty principle.

The uncertainty principle also called the Heisenberg uncertainty principle, or indeterminacy principle says that the position and the velocity of an object cannot be measured precisely, at the same time, even in theory.

For the position-momentum uncertainty principle becomes:

(hiddx-p)Ψ=ia(x-x)Ψ.

02

Solve equation 3.67 for  Ψ.

Solve equation 3.67 for Ψ, which is given by:

(hiddx-<p>)Ψ=ia(x-<x>)Ψ.

Now write the equation as:

»åΨdx=ihiax-iax+pΨ=ah-x+x+iapΨ

The above equation can be written as,

»åΨΨah-x+x+ipadx

Integrate both sides to get:

lnΨ=-22hx-x2+ipxh+lnA

Exponentiation both sidesthe result is,

Ae-ax-x2l2heipxlh

In any stationary state P=0, so any system in which there is a stationary state that has a gaussian wave function will have minimum position-momentum uncertainty.

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Most popular questions from this chapter

(a) Suppose that f(x)and g(x)are two eigenfunctions of an operatorQ^ , with the same eigenvalue q . Show that any linear combination of f andgis itself an eigenfunction of Q^, with eigenvalue q .

(b) Check that f(x)=exp(x)andg(x)=exp(-x) are eigenfunctions of the operatord2/dx2 , with the same eigenvalue. Construct two linear combinations of and that are orthogonal eigenfunctions on the interval(-1.1) .

(a) Show that the sum of two hermitian operators is hermitian.

(b) SupposeQ^is hermitian, andαis a complex number. Under what condition (onα) islocalid="1655970881952" αQ^hermitian?

(c) When is the product of two hermitian operators hermitian?

(d) Show that the position operator (x^=x)and the hamiltonian operator

localid="1655971048829" H^=-h22md2dx2+V(x)are hermitian.

(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.

Solve Equation 3.67 for Ψ(x). Note that ⟨x⟩and ⟨p⟩are constants.

Virialtheorem.Use3.71toshowthatddt<xp>=2<T>-<xdVdx>whereTisthekineticenergy(H=T+V).Inastationarystatetheleftsideiszero(why?)so2<T>=<xdVdx>Thisiscalledthevirialtheorem.Useittoprovethat<T>=<V>forstationarystatesoftheharmonicoscillator,andcheckthatthisisconsistentwiththeresultsyougotinProblem2.11and2.12.

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