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Anisotropic Phase Diagram for Quadrupole Ordering and Possible Crystal Field Level Structure in TmTe

Identifieur interne : 001457 ( Main/Exploration ); précédent : 001456; suivant : 001458

Anisotropic Phase Diagram for Quadrupole Ordering and Possible Crystal Field Level Structure in TmTe

Auteurs : Ryousuke Shiina [Japon] ; Tatsuya Nagao [Japon]

Source :

RBID : Pascal:09-0127170

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English descriptors

Abstract

The origin of an anisotropic phase diagram for the antiferro-quadrupolar (AFQ) order in TmTe is studied using a realistic J = 7/2 multiplet model, based on a previous analysis for the classical limit J → oo. Assuming the Γ3-type AFQ order parameters, a quantitative comparison of the phase diagram with the experiments is presented for a few candidates of the crystal field (CF) level schemes. It is shown that a scheme with a sequence from low- to high-energy levels, Γ867, naturally explains the observed field dependence and anisotropy of the phase diagram. The resonant x-ray scattering signals in the AFQ phase are studied to explore a possibility of identifying the order parameter and the CF scheme experimentally.


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<term>Anisotropy</term>
<term>Antiferromagnetism</term>
<term>Crystal field</term>
<term>Magnetic field effects</term>
<term>Order parameters</term>
<term>Ordering</term>
<term>Phase transformations</term>
<term>Quadrupole interactions</term>
<term>Resonance scattering</term>
<term>Thulium tellurides</term>
<term>X-ray scattering</term>
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<term>Anisotropie</term>
<term>Antiferromagnétisme</term>
<term>Relation ordre</term>
<term>Champ cristallin</term>
<term>Interaction quadripolaire</term>
<term>Paramètre ordre</term>
<term>Diffusion résonnante</term>
<term>Diffusion RX</term>
<term>Transformation phase</term>
<term>Effet champ magnétique</term>
<term>Tellurure de thulium</term>
<term>TmTe</term>
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<div type="abstract" xml:lang="en">The origin of an anisotropic phase diagram for the antiferro-quadrupolar (AFQ) order in TmTe is studied using a realistic J = 7/2 multiplet model, based on a previous analysis for the classical limit J → oo. Assuming the Γ
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