Tables 2.1 Different cases and ways of expressing the basic quantum formalism page 71 Eigenstates and eigenvalues of Eigenvalues,for the three-dimensional harmonic oscillator 6.3 Values of jand m and the corresponding number of possible states 233 64 Clebsch-Gordan coefficients fori==1/2 Clebsch-Gordan coefficients for j=1 and j2=1/2 66 Clebsch-Gordan coefficients for j=j2=1 7 Fermions and bosons 12 Fermionic distributions 252 7.3 Bo sonic distributions 11.1 Ground-state energy of helioid atoms 13.1 Electromagnetic spectrum 17.1 Sequence transmission 23 Toffoli truth table Fredkin truth table 8 17.4 Classical error correction 668Tables 2.1 Different cases and ways of expressing the basic quantum formalism page 71 6.1 Eigenstates and eigenvalues of ˆlz 199 6.2 Eigenvalues, for the three-dimensional harmonic oscillator 215 6.3 Values of j and m and the corresponding number of possible states 233 6.4 Clebsch–Gordan coefficients for j1 = j2 = 1/2 238 6.5 Clebsch–Gordan coefficients for j1 = 1 and j2 = 1/2 238 6.6 Clebsch–Gordan coefficients for j1 = j2 = 1 238 7.1 Fermions and bosons 250 7.2 Fermionic distributions 252 7.3 Bosonic distributions 254 11.1 Ground-state energy of helioid atoms 429 13.1 Electromagnetic spectrum 456 17.1 Sequence transmission 648 17.2 Toffoli truth table 658 17.3 Fredkin truth table 658 17.4 Classical error correction 668