Backward diode
In semiconductor devices, a backward diode (also called back diode[2]) is a variation on a Zener diode or tunnel diode having a better conduction for small reverse biases (for example –0.1 to –0.6 V) than for forward bias voltages.
The reverse current in such a diode is by tunneling, which is also known as the tunnel effect.[3][4][5]
Current–voltage characteristics of backward diode[edit]
The forward I–V characteristic is the same as that of an ordinary P–N diode. The breakdown starts when reverse voltage is applied. In the case of Zener breakdown, it starts at a particular voltage. In this diode the voltage remains relatively constant (independent of current) when it is connected in reverse bias. The backward diode is a special form of tunnel diode in which the tunneling phenomenon is only incipient, and the negative resistance region virtually disappears. The forward current is very small and becomes equivalent to the reverse current of a conventional diode.
Applications of backward diodes[edit]
- Detector
- Since it has low capacitance and no charge storage effect,[4] and a strongly nonlinear small-signal characteristic, the backward diode can be used as a detector up to 40 GHz.
- Rectifier
- A backward diode can be used for rectifying weak signals with peak amplitudes of 0.1 to 0.7 V.
- Switch
- A backward diode can be used in high speed switching applications.
References[edit]
- ^ Stanley William Amos, Roger S. Amos (1999). Newnes Dictionary of Electronics. Newnes. ISBN 0-7506-4331-5.
- ^ Paul Horowitz, Winfield Hill (1989). The Art of Electronics, 2nd edition. p. 891.
- ^ Anwar A. Khan and Kanchan K. Dey (2006). A First Course in Electronics. Prentice Hall of India. ISBN 81-203-2776-4.
- ^ a b S.L. Kakani (2004). Electronics Theory and Applications. New Age Intl. Ltd. ISBN 81-224-1536-9.
- ^ Karlheinz Seeger (2004). Semiconductor Physics: An Introduction. Springer. ISBN 3-540-21957-9.