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Momentum
213, 222, 317, 322 |
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–generalized
1488 |
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–see
angular, mechanical |
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–conjugate
213, 225, 1488 |
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Mossbauer
effect 1365 (e) |
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Multipole
moments 1059, 1090 (e) |
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Muon
524, 807, 811, 1266 |
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Muonic
atoms 524, 811, 1146 |
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Muonium
807, 1262 |
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Neumann
spherical functions 947 |
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Neutron
mass endpaper |
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Non-linear |
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–response
1323 |
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–susceptibility
1335 |
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Non-resonant
excitation 1315 |
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Norm |
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–of
a wave function 20, 96, 107 |
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–of
a state vector 111 |
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–conservation
237 |
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Normal
variables 578, 591, 607, 614 |
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Normal
modes of vibration 575, 586, 605 |
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Nuclear
finite mass effect 807 |
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Nucleus |
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–volume
effect 526, 812, 1141, 1248 |
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–finite
mass effect 807 |
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–spin
1070 |
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–multipole
moments 1070 |
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Numbers
(quantum) |
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–good
248 |
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–see
azimuthal, magnetic, principal, radial |
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Observables
136, 139, 215 |
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–measurement
215, 225 |
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–quantization
222 |
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–whose
commutator equals ih 187, 286 |
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–for
identical particles 1381, 1393 |
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–C.S.C.O.
(Complete Set of Commuting Observables) 143, 159, 206 (e), 235 |
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Occupation
number 1391 |
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Operators |
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–definition
96, 114 |
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–general
properties 166 |
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–eigenvalue
equation, diagonalization 132, 158, 420 |
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–representation
126 |
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–Hermitian
120, 136 |
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–unitary
176 |
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–function
of an operator 169 |
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–restriction
of an operator 168 |
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–density
295, 437 |
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–evolution
308 |
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–parity
192 |
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–translation
190, 556, 761 |
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–rotation
693, 983 |
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–scalar
705, 709 |
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–vector
705, 1048, 1089 (e) |
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–tensor
1089 (e), 1090 (e) |
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–creation
and annihilation 489, 498 |
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–permutation
1378, 1382 |
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Oppenheimer:
see Born |
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Optical
theorem 956 |
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Orbital |
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–angular
momentum 643, 644, 660 |
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–state
space 970 |
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Orbitals |
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–atomic
841, 1447 (e) |
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–molecular
1180, 1185 |
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–linear
combination of atomic orbitals 1151, 1173 |
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Orthonormal
basis 97, 105, 107, 122, 138 |
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Oscillation
between two states 412, 448, 1340 |
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 |
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Oscillator
(anharmonic) 487, 1102 |
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Oscillator
(harmonic) |
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 |
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–one-dimensional
483, 511 |
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–two-dimensional
727 |
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 |
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–three-dimensional
547, 814, 870 (e) |
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–in
an electric field 552 |
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 |
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–in
thermodynamic equilibrium 620 |
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 |
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|
–coupled
oscillators 575, 586 |
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 |
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|
–quasi-classical
states 559 |
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 |
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|
Oscillator
strength 1318 |
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 |
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|
Overlap
integral 1175 |
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 |
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|
Packet:
see wave packet |
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 |
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|
Paramagnetism
828, 870 (e), 1438 |
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 |
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|
Parity |
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|
 |
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|
–operator
192 |
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|
 |
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|
–of
the multipole operators 1065, 1066 |
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|
 |
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|
–of
a permutation 1383 |
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|
 |
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|
Parseval
' |
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|
 |
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|
|
–Parseval-Plancherel
relation 1465, 1475 |
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|
 |
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|
–Parseval-Bessel
relation 27, 1462 |
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|
 |
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|
Part
(principal) 1488 |
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|
 |
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|
Partial
waves (method of) 921, 929, 951, 960, 962 (e), 1450 (e) |
|
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|
 |
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|
Path
(space-time) 333, 1497 |
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|
 |
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|
Pauli |
|
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|
 |
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|
|
–matrices
417, 973 |
|
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|
 |
|
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|
|
–theory
970 |
|
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|
 |
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|
|
–Hamiltonian
991 (e) |
|
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|
 |
|
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|
|
–exclusion
principle 1389, 1396, 1414, 1433, 1436, 1445 |
|
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|
 |
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|
Penetrating
orbit 1414 |
|
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|
 |
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|
Periodic |
|
|
|
 |
|
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|
|
–function
1459 |
|
|
|
 |
|
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|
|
–potential
367, 1159 |
|
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|
 |
|
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|
|
–boundary
conditions 1165, 1440 |
|
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|
 |
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|
|
Permutation |
|
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|
 |
|
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|
|
–operators
1378, 1382 |
|
|
|
 |
|
|
|
|
–transformation
of observables by 1381, 1386 |
|
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|
 |
|
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|
|
–parity
of 1383 |
|
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|
 |
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|
Perturbations |
|
|
|
 |
|
|
|
|
–stationary
1094 |
|
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|
 |
|
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|
|
–time-dependent
1284 |
|
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|
 |
|
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|
|
Phase |
|
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|
 |
|
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|
|
–condition
of stationary 25, 58 |
|
|
|
 |
|
|
|
|
–see:
velocity |
|
|
|
 |
|
|
|
|
Phonons
586, 601 |
|
|
|
 |
|
|
|
|
Photoelectric
effect 1345, 1361 (e) |
|
|
|
 |
|
|
|
|
Photons
10, 605, 626, 1336 |
|
|
|
 |
|
|
|
|
–see
absorption |
|
|
|
|