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Check the Equation 10.31 satisfies the time-dependent Schrodinger equation for the Hamiltonian in Equation 10.25. Also confirm Equation 10.33, and show that the sum of the squares of the coefficients is 1, as required for normalization.

Short Answer

Expert verified

Hence showed thatih饾湑x饾湑t=Hx

Step by step solution

01

Define Geometric phase.

Geometric phase is a phase difference gained during the course of a cycle when a system is subjected to cyclic adiabatic processes, which derives from the geometrical features of the Hamiltonian's parameter space in both classical and quantum mechanics.

02

Obtain the derivative of the function.

To show that : ih饾湑x饾湑t=Hx..(1)

Here, Equation 10.25....H=h12肠辞蝉伪ei蝇tsinei蝇tsin-肠辞蝉伪....(2)and

Equation10.31....x(t)=cos(t/2)-i(1-)sin(t/2)cos(/2)e-it/2cos(t/2)-i(1+)sin(t/2)sin(/2)e+it/2.....(3)

The derivative of the equation (3) with respect to t is,

role="math" localid="1656062904380" ih饾湑x饾湑t=ih2-sint2-i(1-)cost2cos2e-it/2-i2cost2-i(1-)sint2cos2e-it/22-sint2-i(1-)cost2sin2eit/2+2cost2-i(1-)sint2sin2eit/2

From (2) and (3), the equation (1) becomes,

Hx(t)=h12coscost2-i(1-)sint2cos2e-it/2+e-itsincost2-i(1-)sint2cos2eit/2e-itcoscost2-i(1-)sint2cos2e-it/2-coscost2-i(1-)sint2sin2eit/2

03

Show that the two matrices are identical.

Start the upper element:

ih2-sint2-i(1-)cost2cos2e-it/2-i2cost2-i(1-')sint2cos2e-it/2=h12coscost2-i(1-)sint2cos2eit/2+e-itcost2-i(1-)sint2sin2eit/2

Cancel the like terms and substitute 蝉颈苍伪=2sin2cos2in the last term to get:

role="math" localid="1656064057976" i-sint2-i(1-)cost2-i2cost2-i(1-')sint2..........(4)=1coscosl2-i(1-)sint2+2sin22cost2-i(1-)sint2

The sum of sine鈥檚 terms is zero, hence,

isint2[-2-12+21cos-1+2+(12-1)cos+(12+1)(1-cos)]=-isint2[-12-21cos-12+12cos-1cos+12+1-12cos-1cos=0Similarly,thesamethinforthelowertermisih饾湑x饾湑tHx.

04

Confirm the equation 10.33.

Let the equation 10.33 be, x(t)=cost2-i(1-cos)sint2e-it/2x+(t)+isinsint2e-it/2x-(t)

Here, x+(t)=cos(/2)eitsin(/2),x-(t)=e-itsin(/2)cos(/2).Thus,

cost2-i(1-cos)sint2e-it/2cos2-eitsin2isinsint2e-it/2sin2-eitcos2=

Here, localid="1656067456488" =cost2-i1sint2cos2+icoscos2+sinsin2sint2e-it/2butcoscos2+sinsin2=cos-2=cos2.=cost2-i(1-)sint2cos2e-it/2

Hence, the upper term of the equation (3) is confirmed.

For:=cost2-i1t2sin2+icossin2-sincos2sint2eit/2

role="math" localid="1656068970462" But,coscos2-sincos2=sin2-=-sin2.So,=cost2-i(1+)sint2sin2eit/2

Hence, the lower term of the equation (3) is confirmed.

The coefficients are normalized. Hence,

c+2+c-2=cos2t2+(1-cos)22sin2t2+sinsint22=cos2t2+sin2t2(1-cos)22+sin2=cos2t2+sin2t21+12-21cos2=cos2t2+sin2t22+12-21cos2+12-21cos

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Most popular questions from this chapter

Work out to analog to Equation 10.62 for a particle of spin I.

Show that if n is real, the geometric phase vanishes. (Problems 10.3 and 10.4 are examples of this.) You might try to beat the rap by tacking an unnecessary (but perfectly legal) phase factor onto the eigenfunctions: n(t)e颈蠁苍n(t), wheren(R) is an arbitrary (real) function. Try it. You'll get a nonzero geometric phase, all right, but note what happens when you put it back into Equation 10.23. And for a closed loop it gives zero. Moral: For nonzero Berry's phase, you need (i) more than one time-dependent parameter in the Hamiltonian, and (ii) a Hamiltonian that yields nontrivially complex eigenfunctions.

A particle starts out in the ground state of the infinite square well (on the interval 0 鈮 x 鈮 a) .Now a wall is slowly erected, slightly off center:

V(x)=f(t)(x-a2-)

wheref(t)rises gradually from 0toAccording to the adiabatic theorem, the particle will remain in the ground state of the evolving Hamiltonian.

(a)Find (and sketch) the ground state att Hint: This should be the ground state of the infinite square well with an impenetrable barrier ata/2+ . Note that the particle is confined to the (slightly) larger left 鈥渉alf鈥 of the well.

(b) Find the (transcendental) equation for the ground state energy at time t.
Answer:

zsinz=T[cosz-cos(z)]zsinz,wherezka,Tmaf(t)/h2,2/a,andk2mE/h. zsinz=T[cosz-cos(z)]zsinz,wherezka,Tmaf(t)/h2,2/a,andk=2mE/h

(c) Setting 未 = 0 , solve graphically for z, and show that the smallest z goes from 蟺 to 2蟺 as T goes from 0 to 鈭. Explain this result.

(d) Now set 未 = 0.01 and solve numerically for z, using

T=0,1,5,20,100,and1000

(e) Find the probability Prthat the particle is in the right 鈥渉alf鈥 of the well, as a function of z and 未. Answer:

Pr=1/[1+I+II-]Pr=1/[1+I+II?],whereI+[1-(z1)sin2[z1/2]

. Evaluate this expression numerically for the T鈥檚 and 未 in part (d). Comment on your results.

(f) Plot the ground state wave function for those same values of T and 未.
Note how it gets squeezed into the left half of the well, as the barrier grows.

(a) Derive the equation 10.67 from Equation 10.65.

(b) Derive Equation 10.79, starting with Equation 10.78.

The case of an infinite square well whose right wall expands at a constant velocity (v) can be solved exactly. A complete set of solutions isn(x,t)2wsin(苍蟺ux)ei(mvx22Enint)/2w

Where w(t)a+vtis the (instantaneous) width of the well andEnin222/2ma2 is the nthallowed energy of the original well (width). The general solution is a linear combination of the's:

(x,t)=n=1cnn(x,t)

the coefficients cnare independent oft

a. Check that Equation \(10.3\) satisfies the time-dependent Schr枚dinger equation, with the appropriate boundary conditions.


(b) Suppose a particle starts outrole="math" localid="1659010978273" (t=0) in the ground state of the initial well:

role="math" localid="1659011031703" (x,0)=2asin(ax)

Show that the expansion coefficients can be written in the form

cn=20ei2sin(nz)sin(z)dz

Where mva/22is a dimensionless measure of the speed with which the well expands. (Unfortunately, this integral cannot be evaluated in terms of elementary functions.)

(c) Suppose we allow the well to expand to twice its original width, so the "external" time is given byw(Te)=2a The "internal" time is the period of the time-dependent exponential factor in the (initial) ground state. Determine TeandTi show that the adiabatic regime corresponds to 1sothatexp(iz2)1over the domain of integration. Use this to determine the expansion coefficients,Cn Construct (x,t)and confirm that it is consistent with the adiabatic theorem.

(d) Show that the phase factor inrole="math" localid="1659011579812" (x,t) can be written in the form

(t)=10tE1(t')dt'.

WhereEn(t)n222/2mw2 is the instantaneous eigenvalue, at timet Comment on this result.

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