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Synthesis, magnetic and transport pr...
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Gonen, Zehra Serpil.
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Synthesis, magnetic and transport properties of transition metal sulfides and oxides.
Record Type:
Electronic resources : Monograph/item
Title/Author:
Synthesis, magnetic and transport properties of transition metal sulfides and oxides./
Author:
Gonen, Zehra Serpil.
Description:
215 p.
Notes:
Source: Dissertation Abstracts International, Volume: 63-06, Section: B, page: 2836.
Contained By:
Dissertation Abstracts International63-06B.
Subject:
Chemistry, Inorganic. -
Online resource:
http://pqdd.sinica.edu.tw/twdaoeng/servlet/advanced?query=3055569
ISBN:
0493711570
Synthesis, magnetic and transport properties of transition metal sulfides and oxides.
Gonen, Zehra Serpil.
Synthesis, magnetic and transport properties of transition metal sulfides and oxides.
- 215 p.
Source: Dissertation Abstracts International, Volume: 63-06, Section: B, page: 2836.
Thesis (Ph.D.)--University of Maryland College Park, 2002.
The low temperature physical properties of known ternary sulfide phases, BaFe<sub>2</sub>S<sub>3</sub> and Ba<sub>6</sub>Fe<sub>8</sub>S<sub>15</sub>, have been studied. They show spin-glass like behavior at low temperatures and are semiconductors. BaFe<sub>2</sub>S<sub>3</sub> is a rare example of a magnetoresistive sulfide that is one dimensional. Sr substitution into BaMnS<sub> 2</sub> structure produces Ba<sub>0.93</sub>Sr<sub>0.07</sub>MnS<sub>2</sub>. Sr changes the coordination environment of Ba<super>2+</super>/Sr<super>2+ </super> and induces short range magnetic ordering. New perovskites and perovskite related oxides were prepared with Mn/Ru, Ni/V and Cu/V at the B site and La, Ba, Ca at the A site of ABO<sub>3</sub> lattice. The compounds show a wide range of magnetic and transport properties. Ba<sub>3</sub>MnRu<sub>2</sub>O<sub> 9</sub> adopts a hexagonal 9R structure. It displays spin-glass like behavior at low temperatures and shows temperature dependent spin at high temperatures due to metal-metal bonding. The Ca<sub>3</sub>MnRu<sub>2</sub>O<sub> 9</sub> and LaMn<sub>x</sub>Ru<sub>1−x</sub>O<sub>3</sub> (0 < x < 1) series adopt GdFeO<sub>3</sub> type perovskite structure. Ca<sub> 3</sub>MnRu<sub>2</sub>O<sub>9</sub> is a ferrimagnetic semiconductor with very low room temperature resistivity. The LaMn<sub>x</sub>Ru<sub>1−x </sub>O<sub>3</sub> series shows spin-glass like behavior with varying dominant interactions from antiferromagnetism (x ≤ 0.25) to ferrimagnetism (x > 0.25). There is an insulator to metal transition at x = 0.05. La<sub>3</sub>Ni<sub> 2</sub>VO<sub>9</sub> also has a GdFeO<sub>3</sub> structure and is a semiconductor. The magnetic susceptibility of this compound displays a spin-glass like behavior with suppressed effective magnetic moment. “LaCu<sub>2</sub>VO<sub> 9</sub>” possess a superstructure and the composition is best described as La<sub>13</sub>V<sub>4</sub>Cu<sub>9</sub>O<sub>38.5</sub>. It has a hexagonal structure with Cu<sub>3</sub> cluster units and V and Cu are trigonal bipyramidally coordinated. This compound is a semiconductor and the magnetic susceptibility follows the Curie-Weiss law with S = 1/2 per Cu<super>2+</super> (T > 220K) to S = 1/2 per Cu<sub>3</sub> units (T < 50K). La<sub>14</sub>V<sub>6</sub>CuO<sub> 36.5</sub> is a decomposition product of La<sub>13</sub>V<sub>4</sub>Cu<sub> 9</sub>O<sub>38.5</sub>. It is a transparent copper oxide which contains [OCuO]<super> 3−</super> sticks. Soft chemical synthesis methods have been utilized to prepare new metastable compounds. The ion exchange reactions of AMCuS<sub> 2</sub> (A = Rb, Cs; M = Mn, Fe) with various salts are complicated by the stability of the decomposition products. Concerted cation anion extraction from K<sub>2</sub>La<sub>2</sub>Ti<sub>3</sub>O<sub>10</sub> with PPh<sub> 4</sub>Br results in preparation of two metastable compounds, KLa<sub>2</sub>Ti<sub> 3</sub>O<sub>9.5</sub> and La<sub>2</sub>Ti<sub>3</sub>O<sub>9</sub>. In the oxide system, Cs<sub>0.5</sub>LaNb<sub>2</sub>O<sub>6.5</sub>X<sub>0.5</sub> (X = Cl, Br), Cs<sub>0.5</sub>Mg<sub>0.25</sub>LaNb<sub>2</sub>O<sub>7</sub>, and Cs<sub>0.5</sub>Mg<sub>0.5</sub>La<sub>5/6</sub>Nb<sub>2</sub>O<sub>7 </sub> can be prepared via ion exchange of CsLaNb<sub>2</sub>O<sub>7</sub> with PPh<sub>4</sub>X, MgCl<sub>2</sub> and MgCl<sub>2</sub>.6H<sub>2</sub>O.
ISBN: 0493711570Subjects--Topical Terms:
517253
Chemistry, Inorganic.
Synthesis, magnetic and transport properties of transition metal sulfides and oxides.
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Source: Dissertation Abstracts International, Volume: 63-06, Section: B, page: 2836.
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Thesis (Ph.D.)--University of Maryland College Park, 2002.
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The low temperature physical properties of known ternary sulfide phases, BaFe<sub>2</sub>S<sub>3</sub> and Ba<sub>6</sub>Fe<sub>8</sub>S<sub>15</sub>, have been studied. They show spin-glass like behavior at low temperatures and are semiconductors. BaFe<sub>2</sub>S<sub>3</sub> is a rare example of a magnetoresistive sulfide that is one dimensional. Sr substitution into BaMnS<sub> 2</sub> structure produces Ba<sub>0.93</sub>Sr<sub>0.07</sub>MnS<sub>2</sub>. Sr changes the coordination environment of Ba<super>2+</super>/Sr<super>2+ </super> and induces short range magnetic ordering. New perovskites and perovskite related oxides were prepared with Mn/Ru, Ni/V and Cu/V at the B site and La, Ba, Ca at the A site of ABO<sub>3</sub> lattice. The compounds show a wide range of magnetic and transport properties. Ba<sub>3</sub>MnRu<sub>2</sub>O<sub> 9</sub> adopts a hexagonal 9R structure. It displays spin-glass like behavior at low temperatures and shows temperature dependent spin at high temperatures due to metal-metal bonding. The Ca<sub>3</sub>MnRu<sub>2</sub>O<sub> 9</sub> and LaMn<sub>x</sub>Ru<sub>1−x</sub>O<sub>3</sub> (0 < x < 1) series adopt GdFeO<sub>3</sub> type perovskite structure. Ca<sub> 3</sub>MnRu<sub>2</sub>O<sub>9</sub> is a ferrimagnetic semiconductor with very low room temperature resistivity. The LaMn<sub>x</sub>Ru<sub>1−x </sub>O<sub>3</sub> series shows spin-glass like behavior with varying dominant interactions from antiferromagnetism (x ≤ 0.25) to ferrimagnetism (x > 0.25). There is an insulator to metal transition at x = 0.05. La<sub>3</sub>Ni<sub> 2</sub>VO<sub>9</sub> also has a GdFeO<sub>3</sub> structure and is a semiconductor. The magnetic susceptibility of this compound displays a spin-glass like behavior with suppressed effective magnetic moment. “LaCu<sub>2</sub>VO<sub> 9</sub>” possess a superstructure and the composition is best described as La<sub>13</sub>V<sub>4</sub>Cu<sub>9</sub>O<sub>38.5</sub>. It has a hexagonal structure with Cu<sub>3</sub> cluster units and V and Cu are trigonal bipyramidally coordinated. This compound is a semiconductor and the magnetic susceptibility follows the Curie-Weiss law with S = 1/2 per Cu<super>2+</super> (T > 220K) to S = 1/2 per Cu<sub>3</sub> units (T < 50K). La<sub>14</sub>V<sub>6</sub>CuO<sub> 36.5</sub> is a decomposition product of La<sub>13</sub>V<sub>4</sub>Cu<sub> 9</sub>O<sub>38.5</sub>. It is a transparent copper oxide which contains [OCuO]<super> 3−</super> sticks. Soft chemical synthesis methods have been utilized to prepare new metastable compounds. The ion exchange reactions of AMCuS<sub> 2</sub> (A = Rb, Cs; M = Mn, Fe) with various salts are complicated by the stability of the decomposition products. Concerted cation anion extraction from K<sub>2</sub>La<sub>2</sub>Ti<sub>3</sub>O<sub>10</sub> with PPh<sub> 4</sub>Br results in preparation of two metastable compounds, KLa<sub>2</sub>Ti<sub> 3</sub>O<sub>9.5</sub> and La<sub>2</sub>Ti<sub>3</sub>O<sub>9</sub>. In the oxide system, Cs<sub>0.5</sub>LaNb<sub>2</sub>O<sub>6.5</sub>X<sub>0.5</sub> (X = Cl, Br), Cs<sub>0.5</sub>Mg<sub>0.25</sub>LaNb<sub>2</sub>O<sub>7</sub>, and Cs<sub>0.5</sub>Mg<sub>0.5</sub>La<sub>5/6</sub>Nb<sub>2</sub>O<sub>7 </sub> can be prepared via ion exchange of CsLaNb<sub>2</sub>O<sub>7</sub> with PPh<sub>4</sub>X, MgCl<sub>2</sub> and MgCl<sub>2</sub>.6H<sub>2</sub>O.
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