High critical temperature superconductors in the system La3-ZMezBa3Ca1−vNcvCu7O16+x where Me=a rare earth or alkaline metal ion and Nc is a Mg, Cd ion
    1.
    发明授权
    High critical temperature superconductors in the system La3-ZMezBa3Ca1−vNcvCu7O16+x where Me=a rare earth or alkaline metal ion and Nc is a Mg, Cd ion 失效
    系统中的高临界温度超导体La3-ZMezBa3Ca1-vNcvCu7O16 + x其中Me =稀土或碱金属离子,Nc是Mg,Cd离子

    公开(公告)号:US06275716B1

    公开(公告)日:2001-08-14

    申请号:US09363490

    申请日:1999-07-29

    Abstract: Compounds of the of the general formula La3−zMezBa3Ca1−vNcvCu7O16+x, wherein Me can be a rare earth metal or an alkaline metal ion selected from the group consisting of yttrium (Y), ytterbium (Yb), sodium (Na) and Nc can be a 2+ ion selected from the group consisting of magnesium (Mg) and cadmium (Cd) have been prepared as the HTSC in thin film superconductors. These compounds can be used as thin film high critical superconductors in thin film high critical temperature superconducting structures and antennas and in multilayered structures and devices such as Josephson junctions, broadband impedance transformers and both flux flow and field effect transistors TABLE 1 Properties of La3-zMezBa3Ca1-vCu7O16+x Compounds. Lattice Parameter (Å) Onset Compound c &agr; Tc (K.) La3Ba3CaCu7O16+x 11.650 3.865 72  11.680*  80* La3Ba3CaCu7O16+x/LSAT 11.665 La3Ba3CaCu7O16+x/GGG 11.540 La3Ba3CaCu7O16+x/LaAlO3 11.660 35 La2YBa3CaCu7O16+x 11.580 3.850 72 LaY2Ba3CaCu7O16+x 11.630 3.868 74 LaY2Ba3CaCu7O16+x/LSAT 11.703 Nd3Ba3CaCu7O16+x 11.614 3.874 42 Nd3Ba3CaCu7O16+x/LSAT 40 La2YbBa3CaCu7O16+x 11.530 3.843 74 La2YbBa3CaCu7O16+x/LSAT 11.628 45 La2YbBa3CaCu7O16+x/LaAlO3 11.630 La2YbBa3CaCu7O16+x/GGG 11.683 La2.5Na.5Ba3CaCu7O16+x 11.630 3.870 68 La2.5Na.5Ba3CaCu7O16+x/LaAlO3 11.662 65 La2.5Na.5Ba3CaCu7O16+x/GGG 11.664 La3Ba3Ca.5Cd.5Cu7O16+x 11.661 3.881 55 La3Ba3Ca.5Cd.5Cu7O16+x/LSAT 11.720 La3Ba3Ca.5Cd.5Cu7O16+x/LaAlO3 11.265 70 La3Ba3Ca.5Cd.5Cu7O16+x/GGG 11.730 La3Ba3Ca.5Mg.5Cu7O16+x 11.661 3.890 35 La3Ba3Ca.5Mg.5Cu7O16+x/LaAlO3 11.650 La3Ba3Ca.5Mg.5Cu7O16+x/GGG 11.692 &Dgr;Tc Observed Compound (K.) Reflections La3Ba3CaCu7O16+x 4 La3Ba3CaCu7O16+x/LSAT 003, 005, 006, 007, 0012 La3Ba3CaCu7O16+x/GGG 003, 005, 006, 007, 009 La3Ba3CaCu7O16+x/LaAlO3 15 003, 004, 005, 006, 007, 009, 0011, 0012 La2YBa3CaCu7O16+x 3 LaY2Ba3CaCu7O16+x 6 LaY2Ba3CaCu7O16+x/LSAT 002, 005, 006, 007 Nd3Ba3CaCu7O16+x Nd3Ba3CaCu7O16+x/LSAT 20 La2YbBa3CaCu7O16+x 5 La2YbBa3CaCu7O16+x/LSAT >20 003, 005, 006, 007, 009, 0010, 0011 La2YbBa3CaCu7O16+x/LaAlO3 003, 005, 006, 007, 008, 009, 0010, 0011 La2YbBa3CaCu7O16+x/GGG 003, 005, 006, 007 La2.5Na.5Ba3CaCu7O16+x 18 [multiphase] La2.5Na.5Ba3CaCu7O16+x/LaAlO3 >40 003, 005, 006, 007 La2.5Na.5Ba3CaCu7O16+x/GGG 006, 009 La3Ba3Ca.5Cd.5Cu7O16+x La3Ba3Ca.5Cd.5Cu7O16+x/LSAT 003, 006 La3Ba3Ca.5Cd.5Cu7O16+x/LaAlO3 >45 003, 006 La3Ba3Ca.5Cd.5Cu7O16+x/GGG La3Ba3Ca.5Mg.5Cu7O16+x 15 La3Ba3Ca.5Mg.5Cu7O16+x/LaAlO3 003, 005, 006, 007, 009, 0010, 0011 La3Ba3Ca.5Mg.5Cu7O16+x/GGG 003, 005, 006, 007, 0011 *S. Engelsberg, Physica C, 176, 451 (1991)

    Abstract translation: 通式La3-zMezBa3Ca1-vNcvCu7O16 + x的化合物,其中Me可以是选自钇(Y),镱(Yb),钠(Na)和Nc的稀土金属或碱金属离子 可以选自镁(Mg)和镉(Cd)中的2+离子作为HTSC在薄膜超导体中制备。 这些化合物可用作薄膜高临界温度超导结构和天线中的薄膜高临界超导体,以及多层结构和器件,如约瑟夫逊结,宽带阻抗变压器和通量流场效应晶体管

    MICROWAVE CAVITY WITH DIELECTRIC REGION AND METHOD THEREOF
    3.
    发明申请
    MICROWAVE CAVITY WITH DIELECTRIC REGION AND METHOD THEREOF 有权
    具有介电区域的微波炉及其方法

    公开(公告)号:US20130063158A1

    公开(公告)日:2013-03-14

    申请号:US13230108

    申请日:2011-09-12

    CPC classification number: G01R27/2658 G01N22/00

    Abstract: A method and apparatus for obtaining dielectric constant and other measurements of a sample, comprising an open cavity resonator; a microwave energy generator for creating a resonating microwave in the open cavity resonator; a predetermined dielectric material having a high dielectric constant in the range of 2 to 100,000 substantially filling the region in which a microwave resonates; the dielectric material adapted to receive a sample for measurement of the dielectric properties of the sample; whereby during operation the resonating microwave beam is substantially immersed in the predetermined dielectric material such that the effective electrical spot size and beam cross-section along the cylindrical axis of the resonating microwave is reduced as a function of the inverse of the square root of the predetermined dielectric material dielectric constant. The dielectric constant or loss tangent of the sample may be determined based upon the change in the cavity's resonant frequency modes.

    Abstract translation: 一种用于获得样品的介电常数和其它测量的方法和装置,包括开放式腔谐振器; 微波能量发生器,用于在开放式腔谐振器中产生谐振微波; 具有高介电常数在2至100,000范围内的预定电介质材料,其基本上填充微波共振的区域; 所述电介质材料适于接收用于测量所述样品的介电性质的样品; 由此在操作期间,谐振微波束基本上浸没在预定介电材料中,使得沿共振微波的圆柱轴线的有效电斑尺寸和光束横截面作为预定的平面根的倒数的函数而减小 介电常数介电材料。 样品的介电常数或损耗角正切可以根据空腔谐振频率模式的变化来确定。

    Ferroelectric-tunable microwave branching couplers
    5.
    发明授权
    Ferroelectric-tunable microwave branching couplers 失效
    铁电可调微波分支耦合器

    公开(公告)号:US06335662B1

    公开(公告)日:2002-01-01

    申请号:US09405303

    申请日:1999-09-21

    CPC classification number: H01P5/04

    Abstract: The invention discloses the utilization of various transmission lines that entail a ferroelectric material as dielectric substrate to introduce an impedance shift by means of an externally applied d.c. bias, which alters the effective length between the input and output signals of the transmission lines of microwave couplers.

    Abstract translation: 本发明公开了利用铁电材料作为介质基板的各种传输线路,通过外部施加的直流电流引入阻抗偏移。 偏置,其改变微波耦合器的传输线的输入和输出信号之间的有效长度。

    C-axis oriented high temperature superconductors deposited onto new
compositions of garnet
    6.
    发明授权
    C-axis oriented high temperature superconductors deposited onto new compositions of garnet 失效
    C轴取向的高温超导体沉积在新的石榴石组合物上

    公开(公告)号:US5691279A

    公开(公告)日:1997-11-25

    申请号:US423173

    申请日:1995-04-18

    CPC classification number: H01L39/2458 Y10S428/93 Y10S505/701

    Abstract: c-axis oriented high temperature superconductors are deposited onto new compositions of garnets using pulsed laser deposition (PLD) with conditions of 85 mTorr of oxygen partial pressure; a block temperature of 730.degree. C., a substrate surface temperature of 790.degree. C. and a laser fluence of 1 to 2 Joules/cm.sup.2 at the target, a laser repetition rate of 10 Hz and a target to substrate distance of 7 cm and in which the a and b lattice parameters of the new compositions of garnets exhibit a mismatch of less than 7 percent with the a and b lattice parameters of the HTSC.

    Abstract translation: c轴取向的高温超导体使用脉冲激光沉积(PLD)沉积到具有85mTorr氧分压条件的新型石榴石组合物上; 块温度为730℃,基材表面温度为790℃,激光注量为1至2焦耳/平方厘米,激光重复频率为10赫兹,目标与基板距离为7厘米, 其中新组合物的a和b晶格参数与HTSC的a和b晶格参数呈现小于7%的失配。

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