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For the wave function in Example 2.2, find the expectation value of H, at time t=0 ,the 鈥渙ld fashioned way:

H=(x,0)H^(x,0)dx.

Compare the result obtained in Example 2.3. Note: BecauseH is independent of time, there is no loss of generality in usingt=0

Short Answer

Expert verified

The expectation value ofHisrole="math" localid="1655393475453" 52ma2 which is same as Example .

Step by step solution

01

Definition of wave function

A wave function is a function that describes the probability of a particle's quantum state as a function of position, momentum, time or spin. The variable 唯 is widely used to represent wave functions.

02

Finding the value of  H^Ψ(x,0)

The expectation value of Hat the time t=0will be evaluated.

The value ofH^(x,0) have to be found for the calculation of expectation value of H:

H^(x,0)=22m2x2[Ax(ax]=A22mx(a2x)=A2m

03

Finding the value of H

The expectation value of H can be calculated as,

H=x,0H^(x,0)dx=A22m0ax(ax)dx=A22m(ax22x33)|0a=A22m(a22a33)=30a52ma36A==52ma2

Thus, the expectation value of His 52ma2which is same as Example 2.3.

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Most popular questions from this chapter

A particle in the infinite square well has the initial wave function

(X,0)={Ax,0xa2Aa-x,a2xa

(a) Sketch (x,0), and determine the constant A

(b) Find(x,t)

(c) What is the probability that a measurement of the energy would yield the valueE1 ?

(d) Find the expectation value of the energy.

Consider the moving delta-function well: V(x,t)=-伪未(x-vt)

where v is the (constant) velocity of the well. (a) Show that the time-dependent Schr枚dinger equation admits the exact solution (x,t)=尘伪he-尘伪|x-vt|lh2e-i[E+1/2mv2t-mvx]lhwhere E=-尘伪2l2h2 is the bound-state energy of the stationary delta function. Hint: Plug it in and check it! Use the result of Problem 2.24(b). (b) Find the expectation value of the Hamiltonian in this state, and comment on the result.

Question: Find the probability current, J (Problem 1.14) for the free particle wave function Equation 2.94. Which direction does the probability flow?

Normalize (x)the equation 2.151, to determine the constants D and F.

Prove the following three theorem;

a) For normalizable solutions the separation constant E must be real as E0+iand show that if equation 1.20 is to hold for all t, must be zero.

b) The time - independent wave function localid="1658117146660" (x) can always be taken to be real, This doesn鈥檛 mean that every solution to the time-independent Schrodinger equation is real; what it says is that if you鈥檝e got one that is not, it can always be expressed as a linear combination of solutions that are . So, you might as well stick to 鈥檚 that are real

c) If is an even function then (x)can always be taken to be either even or odd

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