Supraleitender Verstaerker, welcher mehrere Kryotronstufen aufweist

1,077,357. Superconductive amplifiers. GENERAL ELECTRIC CO. Oct. 12, 1964 [Oct. 17, 1963], No. 41601/64. Heading H3B. In a superconductive amplifier comprising a plurality of cascaded cryotron stages, each stage including two cryotrons, an inductance is coupled between the output of the amplifier an...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Hauptverfasser: EDWARDS HAROLD HENRY, NEWHOUSE VERNON LEOPOLD
Format: Patent
Sprache:ger
Schlagworte:
Online-Zugang:Volltext bestellen
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
Beschreibung
Zusammenfassung:1,077,357. Superconductive amplifiers. GENERAL ELECTRIC CO. Oct. 12, 1964 [Oct. 17, 1963], No. 41601/64. Heading H3B. In a superconductive amplifier comprising a plurality of cascaded cryotron stages, each stage including two cryotrons, an inductance is coupled between the output of the amplifier and each of the cryotrons of a stage of the amplifier respectively so as to provide negative feedback. As shown in Fig. 1 a plurality of stages of cryotrons are connected so that the gate of a cryotron is connected to the control grid of a succeeding cryotron. The cryotrons are biased by current sources 21-30 so that the gates are between a condition of superconductivity and a condition of normal resistance. For each stage one of the current sources 40-45 supplies gate current I G to each gate of the stage which returns to ground after flowing through the control grids of the following stage. An input signal I in from generator 37 applied to terminals 31, 32 adds to the bias I bias in grid 11 resulting in gate 1 becoming more resistive so that the current from generator 40 does not divide equally but more flows through gate 2 and control grid 14 of the following stage. Gate 4 is now more resistive than gate 3, causing a larger proportion of current from 42 to flow through gate 3 and through succeeding grid 15. In this manner the remaining stages are driven in succession and due to the steep resistance VS grid current characteristic of each cryotron and because the control grids are narrow with respect to the cryotron gates an amplified output voltage appears across terminals 35, 36. In order to counteract the effect of low frequency noise voltages due to temperature fluctuations negative feedback at the frequency of the noise voltages is provided between the output of the amplifier and the input by means of inductances 38, 39. The width of the output cryotron grids 19, 20 are increased relative to the preceding cryotrons and in order to obtain a high output voltage the number of grid crossings is also increased. In the arrangement of Fig. 2 (not shown) current sources 40 to 45 and 21 to 30 are replaced by a single source which is connected between the common point of the control grids 11, 12 and the common point of the gates 1, 2. The arrangement of Fig. 3 (not shown) uses separate cryotrons for supplying the output voltage and for providing the feedback voltage. In this ease inductances (38), (39) are connected to the gates (50), (51) of two additional cryotrons