Titlebook: Crystal Field Effects in Metals and Alloys; A. Furrer Book 1977 Plenum Press, New York 1977 Holmium.Praseodym.Terbium.Ytterbium.cobalt.cry

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書目名稱Crystal Field Effects in Metals and Alloys影響因子(影響力)




書目名稱Crystal Field Effects in Metals and Alloys影響因子(影響力)學(xué)科排名




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書目名稱Crystal Field Effects in Metals and Alloys網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Crystal Field Effects in Metals and Alloys被引頻次




書目名稱Crystal Field Effects in Metals and Alloys被引頻次學(xué)科排名




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書目名稱Crystal Field Effects in Metals and Alloys年度引用學(xué)科排名




書目名稱Crystal Field Effects in Metals and Alloys讀者反饋




書目名稱Crystal Field Effects in Metals and Alloys讀者反饋學(xué)科排名

委托

Neutron Crystal-Field Spectroscopy in PrSn3 the paramagnetic molecular field parameter λ.=(1.8±0.3)×10. Oe./erg. The crystalfield parameters are consistent with susceptibility and zero-field magnetization data. The anomalous temperature dependence of the crystal-field transition line widths is interpreted in terms of spin-electron relaxation effects.

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尾隨

EPR of Gd3+ in Lu and Sc Single Crystalsor the axial crystal field parameter D = 3B.: . and the isothermal g-factors: . Sc:Gd is strongly bottlenecked, leading to an anormal angular dependence of the resonance field, which is explained in terms of available theories.

blithe

guzzle

Critical Behaviour of the Magnetization in TbSb and Tb0.6Y0.4Sbansition in TbSb should be of first order, since the Hamiltonian shows no stable fixed point within the ε-expansion. In pure TbSb we find the critical exponent β = 0.20±0.01 in the region 4×10. < (T.-T)/T.<2×10.. In Tb.Y.Sb the exponent is significantly different, we find a sharp transition with β = 0.37±0.05.

guzzle

Book 1977tal-field effects in metals and alloys. The crystal field plays an important role in the understanding of the energetic level structure of ions in condensed matter. In partic- ular, the magnetic properties of rare earth metals and alloys are strongly influenced by the crystal field. In the phenomeno

FAZE

Pantry

Design strategies for VLSI logic,tric; consequently the two modes are strongly mixed at long wavelengths and the low frequency response may be expressed in Debye form with a relaxation time that diverges at T.. Results are in agreement with dynamic susceptibility theories of Buyers and Lines.

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