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Phase transitions and incommensurability in the layered semiconductor TlInS2-an NMR study

Identifieur interne : 001706 ( Main/Repository ); précédent : 001705; suivant : 001707

Phase transitions and incommensurability in the layered semiconductor TlInS2-an NMR study

Auteurs : RBID : Pascal:12-0181968

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Abstract

We report on the first NMR study of powder and single crystal samples of thallium indium sulfide, TlInS2. The crystal under study is a pure single-layer TlInS2 polytype. Our findings show that transformation from the high temperature paraelectric phase to the low temperature ferroelectric phase occurs via an incommensurate phase that exists in the temperature range from Tc = 192 K to Ti = 205 K. On approaching the phase transition at Ti from above, the crystal exhibits a soft mode behavior. A discrepancy in the literature data on the phase transitions in TlInS2 is discussed and ascribed to polytypism of the TlInS2 crystals.

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Pascal:12-0181968

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<title xml:lang="en" level="a">Phase transitions and incommensurability in the layered semiconductor TlInS
<sub>2</sub>
-an NMR study</title>
<author>
<name sortKey="Panich, A M" uniqKey="Panich A">A. M. Panich</name>
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<s1>Department of Physics, Ben-Gurion University of the Negev, PO Box 653</s1>
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<s3>ISR</s3>
<sZ>1 aut.</sZ>
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<country>Israël</country>
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<name sortKey="Mogilyansky, D" uniqKey="Mogilyansky D">D. Mogilyansky</name>
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<s1>Institutes for Applied Research, Ben-Gurion University of the Negev</s1>
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<name sortKey="Sardarly, R M" uniqKey="Sardarly R">R. M. Sardarly</name>
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<s1>Institute for Radiation Problems, Azerbaijan National Academy of Sciences, B Vahabzadeh street 9</s1>
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<term>Ferroelectric transitions</term>
<term>Goldstone mode</term>
<term>Incommensurate phases</term>
<term>Indium Thallium Sulfides Mixed</term>
<term>Layered crystals</term>
<term>Monocrystals</term>
<term>Nuclear magnetic resonance</term>
<term>Polytypism</term>
<term>Quadrupole moments</term>
<term>Semiconductor materials</term>
<term>Soft modes</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr">
<term>Phase incommensurable</term>
<term>Résonance magnétique nucléaire</term>
<term>Polytypisme</term>
<term>Transition ferroélectrique</term>
<term>Mode mou</term>
<term>Moment quadripolaire</term>
<term>Mode Goldstone</term>
<term>Indium Thallium Sulfure Mixte</term>
<term>Semiconducteur</term>
<term>Monocristal</term>
<term>Cristal lamellaire</term>
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<div type="abstract" xml:lang="en">We report on the first NMR study of powder and single crystal samples of thallium indium sulfide, TlInS
<sub>2</sub>
. The crystal under study is a pure single-layer TlInS
<sub>2</sub>
polytype. Our findings show that transformation from the high temperature paraelectric phase to the low temperature ferroelectric phase occurs via an incommensurate phase that exists in the temperature range from T
<sub>c</sub>
= 192 K to T
<sub>i</sub>
= 205 K. On approaching the phase transition at T
<sub>i</sub>
from above, the crystal exhibits a soft mode behavior. A discrepancy in the literature data on the phase transitions in TlInS
<sub>2</sub>
is discussed and ascribed to polytypism of the TlInS
<sub>2</sub>
crystals.</div>
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<sub>2</sub>
-an NMR study</s1>
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<s1>PANICH (A. M.)</s1>
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<s1>MOGILYANSKY (D.)</s1>
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<sZ>1 aut.</sZ>
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<s0>We report on the first NMR study of powder and single crystal samples of thallium indium sulfide, TlInS
<sub>2</sub>
. The crystal under study is a pure single-layer TlInS
<sub>2</sub>
polytype. Our findings show that transformation from the high temperature paraelectric phase to the low temperature ferroelectric phase occurs via an incommensurate phase that exists in the temperature range from T
<sub>c</sub>
= 192 K to T
<sub>i</sub>
= 205 K. On approaching the phase transition at T
<sub>i</sub>
from above, the crystal exhibits a soft mode behavior. A discrepancy in the literature data on the phase transitions in TlInS
<sub>2</sub>
is discussed and ascribed to polytypism of the TlInS
<sub>2</sub>
crystals.</s0>
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<s0>Phase incommensurable</s0>
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<s0>Incommensurate phases</s0>
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<s0>Polytypism</s0>
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<s0>Transition ferroélectrique</s0>
<s5>05</s5>
</fC03>
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<s0>Ferroelectric transitions</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE">
<s0>Mode mou</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG">
<s0>Soft modes</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE">
<s0>Moment quadripolaire</s0>
<s5>07</s5>
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<s0>Quadrupole moments</s0>
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<s0>Mode Goldstone</s0>
<s5>08</s5>
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<s0>Goldstone mode</s0>
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<s0>Modo Goldstone</s0>
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</fC03>
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<s0>Indium Thallium Sulfure Mixte</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>11</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG">
<s0>Indium Thallium Sulfides Mixed</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>11</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA">
<s0>Mixto</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>11</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE">
<s0>Semiconducteur</s0>
<s5>15</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG">
<s0>Semiconductor materials</s0>
<s5>15</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE">
<s0>Monocristal</s0>
<s5>16</s5>
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<fC03 i1="10" i2="3" l="ENG">
<s0>Monocrystals</s0>
<s5>16</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE">
<s0>Cristal lamellaire</s0>
<s5>17</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG">
<s0>Layered crystals</s0>
<s5>17</s5>
</fC03>
<fN21>
<s1>135</s1>
</fN21>
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