Preparation and Structure of Artificial Superlattices of Oxides and Selenides
Preparation and Structure of Artificial Superlattices of Oxides and Selenides
批准号:
61470045
负责人:
BANDO Yoshichika
金额:
$2.37万
依托单位:
依托单位国家:
日本
项目类别:
Grant-in-Aid for General Scientific Research (B)
财政年份:
1986
资助国家:
日本
项目状态:
已结题
起止时间:
1986 至 1987
中文摘要
我们投资the structural and magnetic properties on thigh quality single crystals of theartificial superlattices. High quality single crystal films have been epitaxially grown on a singlecrystal by the evaporation. Important informations on the artificial superlattices been1. substrate crystals, evaporation rates (r_r), Proper selection of substrate crystalssubstrate temperatures (t_s) must be taken for growth of good quality single crystals. forexample,optimum conditions for growth of PbSe/SnSe superlattice on the rock salt by evaporation are t_s of150 C, and d_r of 1a /s. Hile,optimum conditions for growth of C0O/NiO superlattice on sapphire c plane by the reactiveevaporation are t_s of 200 C and d_r less than than 1a /s. Under these optimum conditionsthe crystal may grow by layer growth mechanismand results in the monolayer controlled superlattice.2. the crystalline quality estimated from arocking curve significantly become higher with decreasing layer t…More hickness in PbSe/SnSe and CoO/NiO superlattices. It seems likely that a preudomorphouscrystal below a critical thickness grows on a substrate crystal and the mismatch is adsorbed in eachlayer as homogeneous elastic strain. When each layer thickness is large,the interface contains the misfit dislocations and strain.3. the superlattices (PbS)_m(SnSe)_n havethe SnSe type structure for m<equal or less than>6, n>(2/3)the PbSe type structure for m<equal or less than>4, n<(2/3)_m,and the PbSe and SnSe结构in each layer for m>12, n>4,respectively.4. (CoO)_m(NiO)_n superlattices stacked with (111) plane show a well-defined magneticpeak in neutron diffraction pattern. The magnetic axis of The superlattices is most probablyoriented within the film plane. the (CoO)_m(NiO)_n with m,n <equal or less than> 8 gives a unique t_n like a single phase material. However(CoO)_m(NiO)_n superlattices with m,20有两个magnetic phases with different Neel temperatures. Less <greater than or equal> 20有两个magnetic phases with different Neel temperatures. Less
英文摘要
We have investigated the structural and magnetic properties on thigh quality single crystals of the artificial superlattices. High quality single crystal films have been epitaxially grown on a single crystal by the evaporation. Important informations on the artificial superlattices have been obtained as follows.1. Proper selection of substrate crystals, evaporation rates (R_r), and substrate temperatures (T_s) must be taken for growth of good quality single crystals. For example, optimum conditions for growth of PbSe/SnSe superlattice on the rock salt by evaporation are T_s of 150゜C, and D_r of 1A/s. Hile, optimum conditions for growth of C0O/NiO superlattice on sapphire c plane by the reactive evaporation are T_s of 200゜C and D_r less than 1 A/s. Under these optimum conditions, the crystal may grow by layer growth mechanism, and results in the monolayer controlled superlattice.2. The crystalline quality estimated from a rocking curve significantly become higher with decreasing layer t … More hickness in PbSe/SnSe and CoO/NiO superlattices. It seems likely that a preudomorphous crystal below a critical thickness grows on a substrate crystal and the mismatch is adsorbed in each layer as homogeneous elastic strain. When each layer thickness is large, the interface contains the misfit dislocations and strain.3. The superlattices (PbS)_m(SnSe)_n have the SnSe type structure for m<equal or less than>6, n>(2/3)_m, the PbSe type structure for m<equal or less than>4, n<(2/3)_m, and the PbSe and SnSe structures in each layer for m>12, n>4, respectively.4. (CoO)_m(NiO)_n superlattices stacked with (111) plane show a well-defined magnetic peak in neutron diffraction pattern. The magnetic axis of the superlattices is most probably oriented within the film plane. The (CoO)_m(NiO)_n with m, n <equal or less than> 8 gives a unique T_n like a single phase material. However, (CoO)_m(NiO)_n superlattices with m, n <greater than or equal> 20 have two magnetic phases with different Neel temperatures. Less
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広井善二: 日本化学会誌. 9. 1665-1671 (1987)
Zenji Hiroi:日本化学会杂志 9. 1665-1671 (1987)。
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坂東尚周: "新しい材料" 出版科学総合研究所, 15 (1987)
坂东直志和:《新材料》出版科学研究所,15(1987)
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坂東尚周: 日本応用磁気学会誌. 10. 462-467 (1986)
Naoki Bando:日本应用磁学学会杂志。10. 462-467 (1986)
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T. Terashima: Thin Solid Films. 152. 455-463 (1987)
T. Terashima:固体薄膜。
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坂東尚周: 日本金属学会会報. 26. 783-792 (1987)
Naoki Bando:日本金属研究所通报。26. 783-792 (1987)
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共 35 条
Material Design for High-T_c Superconductors by MBE and Study for Electronic State Using Cross Sectional STM
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批准号:07454176
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项目类别:Grant-in-Aid for Scientific Research (B)
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资助金额:$0.7万
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财政年份:1995
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负责人:BANDO Yoshichika
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依托单位:
Research on High-T_c Superconductors with Relation to Anisotropy
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批准号:07309007
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项目类别:Grant-in-Aid for Scientific Research (A)
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资助金额:$6.46万
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财政年份:1995
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负责人:BANDO Yoshichika
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依托单位:
海外基金