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    • 6. 发明申请
    • HIGH-EFFICIENCY HETEROSTRUCTURE THERMIONIC COOLERS
    • 高效结构冷凝器
    • WO0033354A9
    • 2001-07-19
    • PCT/US9927284
    • 1999-11-17
    • UNIV CALIFORNIA
    • SHAKOURI ALIBOWERS JOHN E
    • H01J45/00H01L29/205H01L29/267H01L29/861H01L35/28H01L35/30
    • H01L29/861H01J45/00H01L29/205H01L29/267
    • A heterostructure thermionic cooler and a method for making thermionic coolers, employing a barrier layer of varying conduction bandedge for n-type material, or varying valence bandedge for p-type material, that is placed between two layers of material. The barrier layer bandedge is at least kBT higher than the Fermi level of the semiconductor layer, which allows only selected, "hot" electrons, or electrons of high enough energy, across the barrier. The barrier layer is constructed to have an internal electric field such that the electrons that make it over the initial barrier are assisted in travel to the anode. Once electrons drop to the energy level at the anode, they lose energy to the lattice, thus heating the lattice of the anode. The barrier height of the barrier layer is high enough to prevent the electrons from traveling in the reverse direction.
    • 异质结构热离子冷却器和用于制造热离子冷却器的方法,使用放置在两层材料之间的用于n型材料的变化的导带的阻挡层或用于p型材料的变化的带状带。 阻挡层带边缘至少比半导体层的费米能级高kBT,其仅允许穿过势垒的选定的“热”电子或足够高能量的电子。 阻挡层被构造成具有内部电场,使得使其超过初始屏障的电子被辅助到行进到阳极。 一旦电子降到阳极的能级,它们就会失去能量到晶格,从而加热阳极的晶格。 阻挡层的势垒高度足够高以防止电子沿相反方向传播。
    • 7. 发明申请
    • HIGH-EFFICIENCY HETEROSTRUCTURE THERMIONIC COOLERS
    • 高效的异质结构超音速冷却器
    • WO0033354A3
    • 2001-05-31
    • PCT/US9927284
    • 1999-11-17
    • UNIV CALIFORNIA
    • SHAKOURI ALIBOWERS JOHN E
    • H01J45/00H01L29/205H01L29/267H01L29/861H01L35/28H01L35/30
    • H01L29/861H01J45/00H01L29/205H01L29/267
    • A heterostructure thermionic cooler and a method for making thermionic coolers, employing a barrier layer of varying conduction bandedge for n-type material, or varying valence bandedge for p-type material, that is placed between two layers of material. The barrier layer bandedge is at least kBT higher than the Fermi level of the semiconductor layer, which allows only selected, "hot" electrons, or electrons of high enough energy, across the barrier. The barrier layer is constructed to have an internal electric field such that the electrons that make it over the initial barrier are assisted in travel to the anode. Once electrons drop to the energy level at the anode, they lose energy to the lattice, thus heating the lattice of the anode. The barrier height of the barrier layer is high enough to prevent the electrons from traveling in the reverse direction.
    • 一种异质结构热电子冷却器和一种制造热离子冷却器的方法,对n型材料采用不同导电边界的阻挡层,或对p型材料采用变化的价带边缘,其置于两层材料之间。 势垒层边界至少比半导体层的费米能级高KT,这允许穿过势垒的选定的“热”电子或具有足够高能量的电子。 阻挡层被构造成具有内部电场,以使得在初始阻挡层上方的电子被辅助传送到阳极。 一旦电子下降到阳极的能量水平,它们就失去了晶格的能量,从而加热了阳极的晶格。 阻挡层的势垒高度足够高以防止电子沿相反方向行进。