2.
    发明专利
    未知

    公开(公告)号:DE3876228T2

    公开(公告)日:1993-06-03

    申请号:DE3876228

    申请日:1988-01-15

    Applicant: IBM

    Abstract: A field-effect structure, formed on a substrate (20) and comprising a channel (21) with source (22) and drain (23) as well as a gate (25) that is separated from the channel by an insulating layer (24). The channel is made of a high-Tc metal-oxide superconductor, e.g., YBaCuO, having a carrier density of about 10 /cm and a correlation length of about .2 nm. The channel thickness is in the order of 1 nm, it is single crystalline and oriented such that the superconducting behaviour is strongest in the plane parallel to the substrate. With a signal of a few Volt applied to the gate, the entire channel cross-section is depleted of charge carriers whereby the channel resistance can be switched between "zero" (undepleted, superconducting) and "very high" (depleted).

    3.
    发明专利
    未知

    公开(公告)号:DE3876228D1

    公开(公告)日:1993-01-07

    申请号:DE3876228

    申请日:1988-01-15

    Applicant: IBM

    Abstract: The field-effect structure comprises a channel (21) with source (22) and drain (23) as well as a gate (25) that is separated from the channel by an insulating layer (24). The channel is made of a high- Tc metal-oxide superconductor, e.g. YBaCuO, having a carrier density of about 10 power 21/cm3 and a correlation length of about .2 nm. The channel thickness is in the order of 1 nm, it is single crystalline and oriented such that the superconducting behaviour is strongest in the plane parallel to the substrate. With a signal of a few Volt applied to the gate, the entire channel cross-section is depleted of charge carriers whereby the channel resistance can be switched betweeen "zero" (undepleted, superconducting) and "very high" (depleted).

    6.
    发明专利
    未知

    公开(公告)号:BR8900147A

    公开(公告)日:1989-09-12

    申请号:BR8900147

    申请日:1989-01-13

    Applicant: IBM

    Abstract: A field-effect structure, formed on a substrate (20) and comprising a channel (21) with source (22) and drain (23) as well as a gate (25) that is separated from the channel by an insulating layer (24). The channel is made of a high-Tc metal-oxide superconductor, e.g., YBaCuO, having a carrier density of about 10 /cm and a correlation length of about .2 nm. The channel thickness is in the order of 1 nm, it is single crystalline and oriented such that the superconducting behaviour is strongest in the plane parallel to the substrate. With a signal of a few Volt applied to the gate, the entire channel cross-section is depleted of charge carriers whereby the channel resistance can be switched between "zero" (undepleted, superconducting) and "very high" (depleted).

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