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Synthesis, crystal structure and magnetic properties of Li2InMo3O8: A novel reduced molybdenum oxide containing magnetic Mo3 clusters

Identifieur interne : 000392 ( Main/Repository ); précédent : 000391; suivant : 000393

Synthesis, crystal structure and magnetic properties of Li2InMo3O8: A novel reduced molybdenum oxide containing magnetic Mo3 clusters

Auteurs : RBID : Pascal:14-0020145

Descripteurs français

English descriptors

Abstract

Powder samples and single crystals of Li2InMo3O8 were obtained by solid state reaction. The structure was determined by single-crystal X-ray diffraction (771 independent reflections for 33 refinable, R1 = 0.0158 and wR2 = 0.0354). Li2InMo3O8 is isomorphous with Li2SnMo3O8 and crystallizes in the hexagonal space group P63mc with unit-cell parameters a = 5.7931(2)Å, c=10.4681(4) Å and Z=2. The crystal structure consists of distorted hexagonal-close-packed oxygen layers with stacking sequence abac along [001] and that are held together by alternating lithium-indium and molybdenum layers. The Li+ and In3+ ions occupy, respectively, tetrahedral and octahedral sites in the ratio 2:1. The Mo atoms occupy octahedral sites and form strongly bonded triangular clusters involving three MoO6 octahedra that are each shared along two edges, constituting a Mo3O13 unit. The variations of the Mo-Mo and Mo-O bond lengths according to the number of electrons per Mo3 cluster are discussed. The trivalent oxidation state of the indium leads to one unpaired electron per Mo3 and thus gives rise to a paramagnetic spin behavior with an effective magnetic moment of 1.5 μB per Mo3 cluster. The magnetic susceptibility vs. temperature curve also shows a maximum at 25 K arising probably from an antiferromagnetic ordering between the Mo3 clusters.

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Pascal:14-0020145

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<title xml:lang="en" level="a">Synthesis, crystal structure and magnetic properties of Li
<sub>2</sub>
InMo
<sub>3</sub>
O
<sub>8</sub>
: A novel reduced molybdenum oxide containing magnetic Mo
<sub>3</sub>
clusters</title>
<author>
<name sortKey="Gall, Philippe" uniqKey="Gall P">Philippe Gall</name>
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<s1>Laboratoire de Chimie du Solide et Inorganique Moléculaire, UMR CNRS 6226-INSA, Université de Rennes 1, Avenue du Général Leclerc</s1>
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<name>RABIH AL RAHAL AL ORABI</name>
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<title level="j" type="abbreviated">J. solid state chem. : (Print)</title>
<title level="j" type="main">Journal of solid state chemistry : (Print)</title>
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<term>Antiferromagnetism</term>
<term>Atomic position</term>
<term>Bond lengths</term>
<term>Carrier density</term>
<term>Crystal structure</term>
<term>Crystallographic site</term>
<term>HCP lattices</term>
<term>Hexagonal lattices</term>
<term>Indium</term>
<term>Lattice parameters</term>
<term>Magnetic cluster</term>
<term>Magnetic moments</term>
<term>Magnetic properties</term>
<term>Magnetic structure</term>
<term>Magnetic susceptibility</term>
<term>Molybdenum</term>
<term>Molybdenum oxide</term>
<term>Monocrystals</term>
<term>Paramagnetism</term>
<term>Solid state reaction</term>
<term>Space groups</term>
<term>Stacking sequence</term>
<term>Valence</term>
<term>XRD</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr">
<term>Structure cristalline</term>
<term>Structure magnétique</term>
<term>Propriété magnétique</term>
<term>Oxyde de molybdène</term>
<term>Amas magnétique</term>
<term>Réaction état solide</term>
<term>Diffraction RX</term>
<term>Réseau hexagonal</term>
<term>Groupe espace</term>
<term>Paramètre cristallin</term>
<term>Mode empilement</term>
<term>Indium</term>
<term>Molybdène</term>
<term>Site cristallographique</term>
<term>Monocristal</term>
<term>Réseau hexagonal compact</term>
<term>Position atomique</term>
<term>Longueur liaison</term>
<term>Densité porteur charge</term>
<term>Valence</term>
<term>Paramagnétisme</term>
<term>Moment magnétique</term>
<term>Susceptibilité magnétique</term>
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<front>
<div type="abstract" xml:lang="en">Powder samples and single crystals of Li
<sub>2</sub>
InMo
<sub>3</sub>
O
<sub>8</sub>
were obtained by solid state reaction. The structure was determined by single-crystal X-ray diffraction (771 independent reflections for 33 refinable, R1 = 0.0158 and wR2 = 0.0354). Li
<sub>2</sub>
InMo
<sub>3</sub>
O
<sub>8</sub>
is isomorphous with Li
<sub>2</sub>
SnMo
<sub>3</sub>
O
<sub>8</sub>
and crystallizes in the hexagonal space group P6
<sub>3</sub>
mc with unit-cell parameters a = 5.7931(2)Å, c=10.4681(4) Å and Z=2. The crystal structure consists of distorted hexagonal-close-packed oxygen layers with stacking sequence abac along [001] and that are held together by alternating lithium-indium and molybdenum layers. The Li
<sup>+</sup>
and In
<sup>3+</sup>
ions occupy, respectively, tetrahedral and octahedral sites in the ratio 2:1. The Mo atoms occupy octahedral sites and form strongly bonded triangular clusters involving three MoO
<sub>6</sub>
octahedra that are each shared along two edges, constituting a Mo
<sub>3</sub>
O
<sub>13</sub>
unit. The variations of the Mo-Mo and Mo-O bond lengths according to the number of electrons per Mo
<sub>3</sub>
cluster are discussed. The trivalent oxidation state of the indium leads to one unpaired electron per Mo
<sub>3</sub>
and thus gives rise to a paramagnetic spin behavior with an effective magnetic moment of 1.5 μ
<sub>B</sub>
per Mo
<sub>3</sub>
cluster. The magnetic susceptibility vs. temperature curve also shows a maximum at 25 K arising probably from an antiferromagnetic ordering between the Mo
<sub>3</sub>
clusters.</div>
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<s1>Synthesis, crystal structure and magnetic properties of Li
<sub>2</sub>
InMo
<sub>3</sub>
O
<sub>8</sub>
: A novel reduced molybdenum oxide containing magnetic Mo
<sub>3</sub>
clusters</s1>
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<s0>Powder samples and single crystals of Li
<sub>2</sub>
InMo
<sub>3</sub>
O
<sub>8</sub>
were obtained by solid state reaction. The structure was determined by single-crystal X-ray diffraction (771 independent reflections for 33 refinable, R1 = 0.0158 and wR2 = 0.0354). Li
<sub>2</sub>
InMo
<sub>3</sub>
O
<sub>8</sub>
is isomorphous with Li
<sub>2</sub>
SnMo
<sub>3</sub>
O
<sub>8</sub>
and crystallizes in the hexagonal space group P6
<sub>3</sub>
mc with unit-cell parameters a = 5.7931(2)Å, c=10.4681(4) Å and Z=2. The crystal structure consists of distorted hexagonal-close-packed oxygen layers with stacking sequence abac along [001] and that are held together by alternating lithium-indium and molybdenum layers. The Li
<sup>+</sup>
and In
<sup>3+</sup>
ions occupy, respectively, tetrahedral and octahedral sites in the ratio 2:1. The Mo atoms occupy octahedral sites and form strongly bonded triangular clusters involving three MoO
<sub>6</sub>
octahedra that are each shared along two edges, constituting a Mo
<sub>3</sub>
O
<sub>13</sub>
unit. The variations of the Mo-Mo and Mo-O bond lengths according to the number of electrons per Mo
<sub>3</sub>
cluster are discussed. The trivalent oxidation state of the indium leads to one unpaired electron per Mo
<sub>3</sub>
and thus gives rise to a paramagnetic spin behavior with an effective magnetic moment of 1.5 μ
<sub>B</sub>
per Mo
<sub>3</sub>
cluster. The magnetic susceptibility vs. temperature curve also shows a maximum at 25 K arising probably from an antiferromagnetic ordering between the Mo
<sub>3</sub>
clusters.</s0>
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<s5>05</s5>
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<s5>05</s5>
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<s5>06</s5>
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<fC03 i1="06" i2="X" l="SPA">
<s0>Reacción estado sólido</s0>
<s5>06</s5>
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<fC03 i1="07" i2="3" l="FRE">
<s0>Diffraction RX</s0>
<s5>07</s5>
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<fC03 i1="07" i2="3" l="ENG">
<s0>XRD</s0>
<s5>07</s5>
</fC03>
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<s0>Réseau hexagonal</s0>
<s5>08</s5>
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<s0>Hexagonal lattices</s0>
<s5>08</s5>
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<s0>Groupe espace</s0>
<s5>09</s5>
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<s0>Space groups</s0>
<s5>09</s5>
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<s0>Paramètre cristallin</s0>
<s5>10</s5>
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<s0>Lattice parameters</s0>
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<s0>Mode empilement</s0>
<s5>11</s5>
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<s0>Stacking sequence</s0>
<s5>11</s5>
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<s5>11</s5>
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<s0>Indium</s0>
<s2>NC</s2>
<s5>12</s5>
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<fC03 i1="12" i2="3" l="ENG">
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<s2>NC</s2>
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<s0>Molybdène</s0>
<s2>NC</s2>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG">
<s0>Molybdenum</s0>
<s2>NC</s2>
<s5>13</s5>
</fC03>
<fC03 i1="14" i2="X" l="FRE">
<s0>Site cristallographique</s0>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="X" l="ENG">
<s0>Crystallographic site</s0>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="X" l="SPA">
<s0>Sitio cristalográfico</s0>
<s5>14</s5>
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<s0>Monocristal</s0>
<s5>15</s5>
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<fC03 i1="15" i2="3" l="ENG">
<s0>Monocrystals</s0>
<s5>15</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE">
<s0>Réseau hexagonal compact</s0>
<s5>16</s5>
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<s0>HCP lattices</s0>
<s5>16</s5>
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<s5>29</s5>
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<s0>Atomic position</s0>
<s5>29</s5>
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<s0>Posición atómica</s0>
<s5>29</s5>
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<s0>Longueur liaison</s0>
<s5>30</s5>
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<s0>Bond lengths</s0>
<s5>30</s5>
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<s0>Densité porteur charge</s0>
<s5>31</s5>
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<s0>Carrier density</s0>
<s5>31</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE">
<s0>Valence</s0>
<s5>32</s5>
</fC03>
<fC03 i1="20" i2="3" l="ENG">
<s0>Valence</s0>
<s5>32</s5>
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<s0>Paramagnétisme</s0>
<s5>33</s5>
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<fC03 i1="21" i2="3" l="ENG">
<s0>Paramagnetism</s0>
<s5>33</s5>
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<s0>Moment magnétique</s0>
<s5>34</s5>
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<s0>Magnetic moments</s0>
<s5>34</s5>
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<fC03 i1="23" i2="3" l="FRE">
<s0>Susceptibilité magnétique</s0>
<s5>35</s5>
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<fC03 i1="23" i2="3" l="ENG">
<s0>Magnetic susceptibility</s0>
<s5>35</s5>
</fC03>
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<s0>Antiferromagnétisme</s0>
<s5>36</s5>
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<s0>Antiferromagnetism</s0>
<s5>36</s5>
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<s0>6166</s0>
<s4>INC</s4>
<s5>71</s5>
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<fN21>
<s1>020</s1>
</fN21>
<fN44 i1="01">
<s1>OTO</s1>
</fN44>
<fN82>
<s1>OTO</s1>
</fN82>
</pA>
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   |texte=   Synthesis, crystal structure and magnetic properties of Li2InMo3O8: A novel reduced molybdenum oxide containing magnetic Mo3 clusters
}}

Wicri

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