Introduction to solid state physics |
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Page 517
Nuclear Demagnetization The result of the preceding discussion of cooling by
adiabatic demagnetization of a paramagnetic salt is that T2, the final temperature
reached, is given as in Fig. 10 by B/Ti = BJT2, or T2 = Tt(BJB) (34) where Ba ...
Nuclear Demagnetization The result of the preceding discussion of cooling by
adiabatic demagnetization of a paramagnetic salt is that T2, the final temperature
reached, is given as in Fig. 10 by B/Ti = BJT2, or T2 = Tt(BJB) (34) where Ba ...
Page 588
In the nuclear spin problem the collisions are weak. In most optical problems the
collisions of atoms are strong enough to interrupt the phase of the oscillation. In
nuclear resonance the phase may vary smoothly in a collision, although the ...
In the nuclear spin problem the collisions are weak. In most optical problems the
collisions of atoms are strong enough to interrupt the phase of the oscillation. In
nuclear resonance the phase may vary smoothly in a collision, although the ...
Page 764
507 nuclear, 578 Magneton numbers, iron group, 510 lanthanide group, 508
Magnetoresistance, 290, 342 Magnetostriction, 573 Magnons, 538, 542 an ti
ferromagnetic 559 thermal excitation, 544, 572 Maser, 622 Mass action law, 367
...
507 nuclear, 578 Magneton numbers, iron group, 510 lanthanide group, 508
Magnetoresistance, 290, 342 Magnetostriction, 573 Magnons, 538, 542 an ti
ferromagnetic 559 thermal excitation, 544, 572 Maser, 622 Mass action law, 367
...
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Contents
CRYSTAL STRUCTURE | 1 |
CRYSTAL DIFFRACTION AND THE RECIPROCAL LATTICE | 43 |
CRYSTAL BINDING | 95 |
Copyright | |
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absolute zero absorption alkali alloy antiferromagnet applied field applied magnetic field atoms axis boundary Brillouin zone calculated Chapter charge components conduction band conduction electrons critical field crystal structure cubic defined density dielectric constant diffraction dipole direction dislocation dispersion relation elastic electric field electron gas energy gap entropy equation equilibrium excited exciton experimental F center Fermi surface ferroelectric ferromagnetic Figure free electron frequency function given heat capacity hole impurity interaction ionic ions lattice constant lattice points low temperatures magnetic field magnon Meissner effect metal momentum motion nearest neighbors neutron normal nuclear nucleus optical orbital paramagnetic particle phase phonon Phys physics plane polarizability polarization positive potential primitive cell quantum reciprocal lattice vector region resonance result room temperature scattering semiconductor shown in Fig solid specimen sphere spin superconducting susceptibility theory thermal tion transition temperature unit vacancies valence band velocity wave wavefunction wavelength wavevector x-ray