1971
DOI: 10.1002/pssb.2220430105
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Phonon Polarization Operator in the Random Phase Approximation

Abstract: In the random phase approximation the imaginary part of the phonon polarization o,mrator is calculated in the left vicinity of the Curie point as well aa the renormalization of the sound velocity due to the spin-phonon interaction of exchange origin in a cubic ferrodielectric.

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Cited by 9 publications
(2 citation statements)
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References 6 publications
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“…At higher temperatures the phonon spectrum may be investigated employing the general result of (6) for the self-energy A(qA, iq). On substituting into (5) we obtain The first term proportional to A,, which provides the only significant contribution for T < Tc as discussed in Section 3, arises due to fluctuations in the transverse spin components. The second term proportional to A, involves additional fluctuation effects in the longitudinal spin component Sz, and becomes more important as the temperature is increased.…”
Section: Results At Temperatures Close To T mentioning
confidence: 97%
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“…At higher temperatures the phonon spectrum may be investigated employing the general result of (6) for the self-energy A(qA, iq). On substituting into (5) we obtain The first term proportional to A,, which provides the only significant contribution for T < Tc as discussed in Section 3, arises due to fluctuations in the transverse spin components. The second term proportional to A, involves additional fluctuation effects in the longitudinal spin component Sz, and becomes more important as the temperature is increased.…”
Section: Results At Temperatures Close To T mentioning
confidence: 97%
“…The phonon energy shift Awq2 and damping Lq2 are then found by making the analytic continuation iq --f wql + i0+ in (8), substituting into (5), and finally taking real and imaginary parts using (28) of [ 11.…”
mentioning
confidence: 99%