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    • 75. 发明授权
    • Planar in-line resistors for superconductor circuits
    • 用于超导体电路的平面直线电阻器
    • US5912503A
    • 1999-06-15
    • US785031
    • 1997-01-02
    • Hugo W. ChanArnold H. Silver
    • Hugo W. ChanArnold H. Silver
    • H01L39/22H01L39/24H01L39/00H01B12/00B32B12/00
    • H01L39/2464Y10S438/923
    • A method of fabricating a low-inductance, in-line resistor includes the steps of: depositing a superconductive layer 12 on a base layer 14; patterning an interconnect region 16 on the superconductive layer 12; and converting the interconnect region 16 of the superconductive layer 12 to a resistor material region 18. The resistor region 18 and the superconductive layer 12 are substantially in the same plane. The method can further include the steps of depositing a conductive layer 22 on the resistor region 18 and on the photo-resist layer 20, and lifting off the photo-resist layer 20 to leave the conductive layer 22 on the resistor region 18. As such, the conductive layer 22 provides a low sheet resistivity for the resistor region 18. In another embodiment, the method includes the steps of: depositing in-situ a superconductive layer 12 on a base layer 14; depositing in-situ a conductive layer 22 on the superconductive layer 12 to form a bi-layer 24; patterning an interconnect region 16 on the bi-layer 24; and converting the interconnect region 16 of the bi-layer 24 to a resistor material region 18.
    • 制造低电感直列电阻器的方法包括以下步骤:在基极层14上沉积超导层12; 图案化超导层12上的互连区域16; 并且将超导层12的互连区域16转换成电阻材料区域18.电阻器区域18和超导层12基本上在同一平面内。 该方法还可以包括以下步骤:在电阻器区域18和光致抗蚀剂层20上沉积导电层22,并且提起光致抗蚀剂层20以将导电层22留在电阻器区域18上。同样地 导电层22为电阻器区域18提供低的薄层电阻率。在另一个实施例中,该方法包括以下步骤:在基底层14上原位沉积超导层12; 在导电层12上原位沉积导电层22以形成双层24; 图案化双层24上的互连区域16; 并将双层24的互连区域16转换成电阻材料区域18。
    • 78. 发明授权
    • Single-electron controlling magnetoresistance element
    • 单电子控制磁阻元件
    • US5877511A
    • 1999-03-02
    • US940194
    • 1997-09-29
    • Tetsufumi TanamotoShuichi Iwabuchi
    • Tetsufumi TanamotoShuichi Iwabuchi
    • G01R33/09H01L29/66H01L43/08H01L29/06H01L39/00
    • B82Y10/00H01L43/08
    • A single-electron controlling magnetoresistance element which comprises, a couple of first ferromagnetic bodies each magnetized in a first direction, a second ferromagnetic body magnetized in a second direction in an initial direction and sandwiched between the couple of first ferromagnetic bodies with a tunnel junction interposed therebetween respectively, and means for directing the magnetization direction of the second ferromagnetic body to a direction different from the second direction, wherein a charging energy E.sub.c of a single electron in at least one of the tunnel junctions interposed between the first ferromagnetic body and the second ferromagnetic body meets the following conditions:E.sub.c >>k.sub.B T (2)E.sub.c >>h/R.sub.t C (3)wherein k.sub.B T is a thermal energy at an operation temperature, h is a Planck's constant, R.sub.t is a junction tunnel resistance, and C is a junction capacity.
    • 一种单电子控制磁阻元件,其包括:一对第一铁磁体,每个第一铁磁体沿第一方向磁化;第二铁磁体,沿初始方向沿第二方向被磁化,并夹在所述一对第一铁磁体之间, 以及用于将第二铁磁体的磁化方向引导到与第二方向不同的方向的装置,其中插入在第一铁磁体和第二铁磁体之间的至少一个隧道结中的单个电子的充电能量Ec 铁磁体满足以下条件:Ec >> kBT(2)Ec >> h / RtC(3)其中kBT是工作温度下的热能,h是普朗克常数,Rt是结隧道电阻,C是 一个连接能力。
    • 79. 发明授权
    • Laminated superconducting ceramic composite conductors
    • 层压超导陶瓷复合导体
    • US5801124A
    • 1998-09-01
    • US701333
    • 1996-08-30
    • Bruce B. GambleGilbert N. Riley, Jr.John D. ScudiereMichael D. ManliefDavid M. BuczekGregory L. Snitchler
    • Bruce B. GambleGilbert N. Riley, Jr.John D. ScudiereMichael D. ManliefDavid M. BuczekGregory L. Snitchler
    • H01L39/14H01L39/24H01L39/00H01B12/00
    • H01L39/248H01L39/143Y10S428/93Y10S505/704
    • The invention provides a superconducting ceramic laminate including a superconducting tape mechanically coupled to, and compressively strained to 0.1% or more under a predetermined load by, at least one cladding tape. The material and thickness of the cladding tape or tapes are selected relative to the material and thickness of the superconducting tape to locate the neutral axis so that, under a predetermined heavy load, the maximum compressive strain on any superconducting portion of the superconducting tape is less than the critical compressive strain and the maximum tensile strain on any superconducting portion of the superconducting tape under a predetermined load is less than the critical tensile strain. By "heavy load" is meant a load on the laminate equivalent to a load on the unlaminated superconducting tape selected for the laminate including a surface bend strain on the unlaminated superconducting tape of at least 0.1%. The laminate provides high critical current capacity, improved strain tolerance, superior critical current retention, and high packing factors. Articles comprising the laminates, such as coils and cables, are also provided.
    • 本发明提供了一种超导陶瓷层压体,其包括机械地耦合到至少一个包覆带上并在预定负载下被压缩至0.1%或更多的超导带。 相对于超导带的材料和厚度来选择包覆带或带的材料和厚度以定位中性轴线,使得在预定的重负载下,超导带的任何超导部分上的最大压缩应变较小 超过在预定载荷下超导带的任何超导部分上的临界压应变和最大拉伸应变小于临界拉伸应变。 “重负荷”是指层压板上的载荷相当于在层压板上选择的非层压超导带上的载荷,其中包括非层压超导带上的表面弯曲应变为至少0.1%。 层压板提供高临界电流容量,改进的应变耐受性,优异的临界电流保持率和高填充因子。 还提供了包括层压材料,例如线圈和电缆的制品。
    • 80. 发明授权
    • Tunnel thin film electroluminescent device
    • 隧道薄膜电致发光器件
    • US5796120A
    • 1998-08-18
    • US577976
    • 1995-12-28
    • Christopher J. SummersBrent K. Wagner
    • Christopher J. SummersBrent K. Wagner
    • H05B3/22H05B33/12H05B33/14H01L29/06H01L39/00
    • H05B33/145H05B3/22H05B33/12
    • A low voltage tunnel thin film electroluminescent device (10) that comprises a conductive layer (13) that acts as a source of electrons, a first thin barrier layer (14) deposited on the conductive layer, a luminescent layer (16) deposited on the barrier layer a second thin barrier layer (14) deposited on said luminescent layer, and an electrode (18) deposited on the second barrier layer. Electrons from the source layer tunnel through the thin tunnel barrier layer into the luminescent layer which is doped with luminescent centers. The electrons that tunnel through the thin tunnel barrier layer into the luminescent layer have kinetic energy that is within a narrow energy distribution. The material comprising the first barrier layer is preferably chosen to have a positive conduction band off-set (22) with respect to the conductive layer and the material comprising the luminescent layer is chosen to have a negative conduction band off-set (24) with respect to said first barrier layer, wherein the negative conduction band off-set is greater than the positive conduction band off-set. Further, the different material layers are preferably lattice-matched and epitaxially grown in order to make the device more efficient.
    • 一种低电压隧道薄膜电致发光器件(10),其包括用作电子源的导电层(13),沉积在所述导电层上的第一薄势垒层(14),沉积在所述导电层上的发光层(16) 沉积在所述发光层上的第二薄势垒层(14)和沉积在所述第二阻挡层上的电极(18)。 来自源层的电子穿过薄隧道势垒层进入掺杂有发光中心的发光层。 穿过薄隧道势垒层进入发光层的电子具有处于窄能量分布内的动能。 包括第一阻挡层的材料优选被选择为相对于导​​电层具有正导带偏移(22),并且包括发光层的材料被选择为具有负导带偏移(24),具有带 相对于所述第一阻挡层,其中所述负导带偏移大于所述正导带偏移。 此外,为了使器件更有效,不同的材料层优选是晶格匹配和外延生长的。