1970
DOI: 10.1103/physrevb.2.5035
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Thermal Conductivity of Double-Nitrate Crystals below 1°K

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1973
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Cited by 17 publications
(2 citation statements)
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“…With the thermal conduction model we calculated the dispersion and absorption curves at this temperature and field. In the calculations the crystal was represented by a cylinder with a radius of 1.5 mm, a specific heat C L = 1.26 × 10 3 j/m3K [3] and a thermal conductivity h L = 1.50 x 103 W/mK [4]. The spin specific heat C n and the paramagnetic saturation factor K = XT(H)/xT (O) were calculated with the molecular field model as CH = 1.45 × 103 j/m3K and K =0.94.…”
Section: Resultsmentioning
confidence: 99%
“…With the thermal conduction model we calculated the dispersion and absorption curves at this temperature and field. In the calculations the crystal was represented by a cylinder with a radius of 1.5 mm, a specific heat C L = 1.26 × 10 3 j/m3K [3] and a thermal conductivity h L = 1.50 x 103 W/mK [4]. The spin specific heat C n and the paramagnetic saturation factor K = XT(H)/xT (O) were calculated with the molecular field model as CH = 1.45 × 103 j/m3K and K =0.94.…”
Section: Resultsmentioning
confidence: 99%
“…In the experiment (6) A t >> T 2 and at Ce 25% the ESR line i s not inhomogeneous in the absence of a strong a c field. But in (12) lattice defects a r e reported to occur in CDN. It is shown in (13) that a homogeneous line (the more in the presence of lattice defects) is split intoindividual fine components (in a strong a c field) between which cross-ielaxation occurs "in the iotating coordinate system" with time T that generates phonons in the experiment (6).…”
mentioning
confidence: 99%