Tunnel diode, also known as Esaki diode, is a special semiconductor element that relies on the quantum mechanical tunneling effect to achieve the characteristic of "negative impedance". This technology was invented by Nobita Ogasawara and Yukiko Kurose in 1957. The design of the tunnel diode gives it unique advantages in microwave technology and high-frequency applications, making the development of this technology an important milestone in the field of electronic components.
The negative differential resistance of tunnel diodes enables them to be used as oscillators and amplifiers, bringing unexpected applications.
The key to the tunnel diode is its highly doped P-N structure, which makes the entire structure only about 10 nanometers wide. This structure creates a ruptured band gap between the electron state in the conduction band and the hole state in the valence band, thereby realizing the quantum tunneling effect. This allows tunnel diodes to far exceed the capabilities of conventional diodes and transistors in the microwave frequency range, enabling them to be used in a variety of high-frequency applications.
The "negative differential resistance" property of the tunnel diode enables it to act as an oscillator and amplifier within certain operating ranges. Specifically, these components have very low capacitance, which means they can operate at microwave frequencies and provide a high degree of efficiency. Although tunnel diodes have limited output power, with frequencies of hundreds of milliwatts, they can achieve low latency and high speed in newly designed components.
Even though the performance of tunnel diodes has been surpassed by more traditional semiconductor components in many applications, their potential in microwave technology cannot be ignored.
In microwave technology, tunnel diodes have been used in many fields, including local oscillators in UHF TV tuners, trigger circuits in oscilloscopes, high-speed counter circuits, etc. These applications demonstrate its excellent performance in high-speed and low-noise amplification. In 1977, microstrip tunnel diode amplifiers were used in Intelsat V satellite receivers, which operated in the 14 to 15.5 GHz range and outperformed any transistor-based front-end design.
For a conventional semiconductor diode, when the P-N junction is forward biased, it conducts normally, but when it is reverse biased, it blocks the flow of current. This process is also accompanied by the existence of possible reverse breakdown voltage. However, the design of the tunnel diode greatly increases the concentration of dopants, making it conductive even under reverse bias, and under forward bias, a voltage and current behavior opposite to each other occurs. This is the concept of "negative impedance". This phenomenon can be effectively used in solid-state Dynatron oscillators.
In addition to being an amplifier at microwave frequencies, tunnel diodes also have excellent radiation resistance, making them particularly suitable for use in high-radiation environments, such as in space.
The durability of tunnel diodes is another outstanding feature. Decades later, components originally manufactured in the 1960s still work flawlessly today. According to Esaki and his collaborators, the semiconductor components are extremely stable and their lifespan is expected to be "infinite" as long as they are kept at room temperature. However, overheating is its worst enemy, so you need to be extra careful when soldering.
Although more modern semiconductor devices have surpassed the performance of tunnel diodes in many applications, their potential in microwave technology remains worth exploring. With the development of new tunnel effect mechanisms, such as resonant tunnel diodes and MIIM diodes, future applications in high-frequency fields may even open up new technological prospects.Will we be able to witness new breakthroughs and applications of tunnel diodes in microwave technology?