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Imagine two noninteracting particles, each of mass m, in the infinite square well. If one is in the staten(Equation 2.28 ), and the other in state 1(ln), calculate localid="1658214464999" (x1-x2)2, assuming (a) they are distinguishable particles, (b) they are identical bosons, and (c) they are identical fermions.

Short Answer

Expert verified

a) The value of<(x1-x2)2>assuming that they are distinguishable particles is a216-1221n2+1m2.

b) The value of<(x1-x2)2>assuming that they are identical bosons is a216-1221n2+1m2-128a2m2n24m2-n24

c) The value of<(x1-x2)2>assuming that they are identical fermions is a216-1221n2+1m2-128a2m2n24m2-n24.

Step by step solution

01

Definition of identical bosons and identical fermions

According to Carroll, particles exist in two types: those that makeup matter, known as 'fermions,' and those that convey forces, known as 'bosons.

Bosons can be piled on top of one other, whereas fermions take up space.

02

(a) Determination of <(x1-x2)2> assuming that they are distinguishable particles

For distinguishable particles, use the following formula,

x1-x22=x2a+x2b-2xa(xnb~=a213-12蟿蟿苍2+a213-12蟿蟿苍2-2a2a2=a223-12-12蟿蟿21n2+1m2Evaluatethevalueofx1-x22.x1-x22=a216-12蟿蟿21n2+1m2Thus,thevalueofx1-x22assumingtheyaredistinguishableparticlesisa216-12蟿蟿21n2+1m2.

03

(b) Determination of<x1-x22>assuming that they are the identical Bosons

For the same Bosons, the equation is as follows,

x1-x22B=x2m+x2n-2a,xn~na,xn~m-2a,xn~nm2=x1-x22d-2a,xn~nm2

But it is known that a,xn~nm=-8amn2m2-n22. So, that expression is as follows,

a,xn~nm2=a,xn~nm2=a,xn~nma,xn~nmx1-x22B=a216-1221n2+1m2-128a2m2n24m2-n2Hence,thevalueofx1-x22dconsideringtheyareidenticalbosonsis.a216-12蟿蟿21n2+1m2-128a2m2n2蟿蟿4m2-n24

04

(c) Determination of<x1-x22>assuming that they are the identical fermions

ForFermionsthatareidentical,theequationisasfollows,x1-x2f2=xa2+xb2-2ax,n~aax,n~b+2ax,n~ab2=x1-x2d2+2ax,n~ab2=a216-12蟿蟿21n2+1m2+128a2m2n2蟿蟿4m2-n24Thus,thevalueofx1-x22dwhentheyareidenticalfermionsis.=a216-12蟿蟿21n2+1m2+128a2m2n2蟿蟿4m2-n24

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Show that most of the energies determined by Equation 5.64are doubly degenerate. What are the exceptional cases? Hint: Try it for N=1,2,3,4.... , to see how it goes. What are the possible values of cos(ka)in each case?

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