An Interlude — Question 2

Section 44-2 · Physics pages 7314–7315

Question 2 Quantum statistics changes the number of two-particle occupations Two identical noninteracting particles can occupy three distinct one-particle states of equal energy. Each state includes every internal quantum number. Compare spinless bosons with fermions whose spin state is fixed. three complete one-particle states Schematic; labels, not drawing lengths, specify the data. (a) Count the allowed two-particle occupation patterns for each statistics. (b) For three particles in the same three states, repeat the count and explain the difference.
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Question 2 - Solution Quantum statistics changes the number of two-particle occupations three complete one-particle states (a) Method and calculation ΩB(2, 3) = ( 3 + 2 −1 2 ) = ( 4 2 ) = 6 . ΩF (2, 3) = ( 3 2 ) = 3 (ni = 0 or 1). (b) Interpretation and further calculation ΩB(3, 3) = ( 5 3 ) = 10, ΩF (3, 3) = ( 3 3 ) = 1 . ∑ i ni = N, ni ≥0 for bosons; ni ≤1 for identical fermions . Physical check The count concerns indistinguishable occupation patterns, not labeled-particle arrangements. Degenerate energy does not make distinct quantum states identical.

Question 2

Quantum statistics changes the number of two-particle occupations

Two identical noninteracting particles can occupy three distinct one-particle states of equal energy. Each state includes every internal quantum number. Compare spinless bosons with fermions whose spin state is fixed.

Diagram shown in the original SVG worksheet.

  1. Count the allowed two-particle occupation patterns for each statistics.

  2. For three particles in the same three states, repeat the count and explain the difference.

Question 2 - Solution

Quantum statistics changes the number of two-particle occupations

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ΩB(2,3)=(3+2−12)=(42)=6.\boxed{\Omega_B(2,3)=\binom{3+2-1}{2}=\binom42=6}.ΩF(2,3)=(32)=3(ni=0 or 1).\boxed{\Omega_F(2,3)=\binom32=3}\quad(n_i=0\text{ or }1).

(b) Interpretation and further calculation

ΩB(3,3)=(53)=10,ΩF(3,3)=(33)=1.\boxed{\Omega_B(3,3)=\binom53=10,\quad\Omega_F(3,3)=\binom33=1}.∑ini=N,ni≥0 for bosons;ni≤1 for identical fermions.\sum_i n_i=N,\quad\boxed{n_i\ge0\text{ for bosons};\ n_i\le1\text{ for identical fermions}}.

Physical check

The count concerns indistinguishable occupation patterns, not labeled-particle arrangements. Degenerate energy does not make distinct quantum states identical.