Encyclopedia
In
electronics, a
diode is a
component that restricts the direction of movement of charge carriers. Essentially, it allows an electric current to flow in one direction, but blocks it in the opposite direction. Thus, the diode can be thought of as an electronic version of a
check valve. Circuits that require current flow in only one direction will typically include one or more diodes in the circuit design.
Early diodes included "cat's whisker" crystals and
vacuum tube devices . Today the most common diodes are made from
semiconductor materials such as
silicon or
germanium.
History
Thermionic and solid state diodes developed in parallel. The principle of operation of
thermionic diodes was discovered by Frederick Guthrie in 1873 . The principle of operation of crystal diodes was discovered in 1874 by the German scientist,
Karl Ferdinand Braun .
Thermionic diode principles were rediscovered by
Thomas Edison on February 13, 1880 and he took out a patent in 1883 , but developed the idea no further. Braun patented the crystal rectifier in 1899 . The first radio receiver using a crystal diode was built around 1900 by Greenleaf Whittier Pickard. The first thermionic diode was patented in Britain by John Ambrose Fleming on November 16, 1904 . Pickard received a patent for a silicon crystal detector on November 20, 1906 .
At the time of their invention such devices were known as
rectifiers. In 1919
William Henry Eccles coined the term
diode from Greek roots;
di means 'two', and
ode means 'path'.
Thermionic or gaseous state diodes
Thermionic diodes are
vacuum tube devices , which are arrangements of electrodes surrounded by a vacuum within a glass envelope, similar in appearance to
incandescent light bulbs.
In vacuum tube diodes, a current is passed through the
cathode, a filament treated with a mixture of barium and strontium oxides, which are oxides of alkaline earth metals. The current heats the filament, causing
thermionic emission of electrons into the vacuum envelope. In forward operation, a surrounding metal electrode, called the
anode, is positively charged, so that it electrostatically attracts the emitted electrons.
However, electrons are not easily released from the unheated anode surface when the voltage polarity is reversed and hence any reverse flow is a very tiny current.
For much of the 20th century vacuum tube diodes were used in analog signal applications, and as rectifiers in power supplies. Today, tube diodes are only used in niche applications, such as rectifiers in tube guitar and hi-fi amplifiers, and specialized high-voltage equipment.
Most modern diodes are based on
semiconductor p-n junctions. In a p-n diode,
conventional current can flow from the p-type side to the n-type side , but not in the opposite direction.
Another type of semiconductor diode, the
Schottky diode, is formed from the contact between a metal and a semiconductor rather than by a p-n junction.
A semiconductor diode's current-voltage, or I-V, characteristic curve is ascribed to the behavior of the so-called
depletion layer or
depletion zone which exists at the
p-n junction between the differing semiconductors. When a p-n junction is first created, conduction band electrons from the N-doped region diffuse into the P-doped region where there is a large population of holes with which the electrons "recombine". When a mobile electron recombines with a hole, the hole vanishes and the electron is no longer mobile. Thus, two charge carriers have vanished. The region around the p-n junction becomes depleted of charge carriers and thus behaves as an insulator.
However, the depletion width cannot grow without limit. For each electron-hole pair that recombines, a positively-charged dopant ion is left behind in the N-doped region, and a negatively charged dopant ion is left behind in the P-doped region. As recombination proceeds and more ions are created, an increasing electric field develops through the depletion zone which acts to slow and then finally stop recombination. At this point, there is a 'built-in' potential across the depletion zone.
If an external voltage is placed across the diode with the same polarity as the built-in potential, the depletion zone continues to act as an insulator preventing a significant electric current. This is the
reverse bias phenomenon. However, if the polarity of the external voltage opposes the built-in potential, recombination can once again proceed resulting in substantial electric current through the p-n junction. For silicon diodes, the built-in potential is approximately 0.6 V. Thus, if an external current is passed through the diode, about 0.6 V will be developed across the diode such that the P-doped region is positive with respect to the N-doped region and the diode is said to be 'turned on' as it has a
forward bias.
A diode's I-V characteristic can be approximated by two regions of operation. Below a certain difference in potential between the two leads, the depletion layer has significant width, and the diode can be thought of as an open circuit. As the potential difference is increased, at some stage the diode will become conductive and allow charges to flow, at which point it can be thought of as a connection with zero resistance. More precisely, the transfer function is
logarithmic, but so sharp that it looks like a corner on a zoomed-out graph .
In a normal silicon diode at rated currents, the voltage drop across a conducting diode is approximately 0.6 to 0.7
volts. The value is different for other diode types -
Schottky diodes can be as low as 0.2 V and
light-emitting diodes can be 1.4 V or more .
Referring to the I-V characteristics image, in the reverse bias region for a normal P-N rectifier diode, the current through the device is very low for all reverse voltages up to a point called the peak-inverse-voltage . Beyond this point a process called reverse breakdown occurs which causes the device to be damaged along with a large increase in current. For special purpose diodes like the avalanche or
zener diodes, the concept of PIV is not applicable since they have a deliberate breakdown beyond a known reverse current such that the reverse voltage is "clamped" to a known value . These devices however have a maximum limit to the current and power in the zener or avalanche region.
Shockley diode equation
The
Shockley ideal diode equation is the I-V characteristic of an ideal diode in either forward or reverse bias . It is derived with the assumption that the only processes giving rise to current in the diode are drift , diffusion, and thermal recombination-generation. It also assumes that the recombination-generation current in the depletion region is insignificant. This means that the Shockley equation doesn't account for the processes involved in reverse breakdown and photon-assisted R-G. Additionally, it doesn't describe the "leveling off" of the I-V curve at high forward bias due to internal resistance, nor does it explain the practical deviation from the ideal at very low forward bias due to R-G current in the depletion region.
,
where
- I is the diode current,
- IS is a scale factor called the saturation current,
- VD is the voltage across the diode
- VT is the thermal voltage
- and n is the emission coefficient.
The emission coefficient
n varies from about 1 to 2 depending on the fabrication process and semiconductor material and in many cases is assumed to be approximately equal to 1 . The
thermal voltage VT is approximately 25.2 mV at room temperature and is a known constant. It is defined by:
,
where
- e is the magnitude of charge on an electron ,
- k is Boltzmann's constant
...
,
- T is the absolute temperature of the p-n junction.
Types of semiconductor diode
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SCRThere are several types of semiconductor junction diodes:
Normal diodes
- which operate as described above. Usually made of doped silicon or, more rarely, germanium
Germanium is a chemical element [i] in the periodic table [i] that has the symbol
Ge and atomic number [i] ...
. Before the development of modern silicon power rectifier diodes,
cuprous oxide and later
selenium was used; its low efficiency gave it a much higher forward voltage drop , and required a large heat sink , much larger than a silicon diode of the same current ratings would require.
'
Gold doped' diodes
- As a dopant, gold acts as recombination centers, which help a fast recombination of minority carriers. This allows the diode to operate at signal frequencies, at the expense of a higher forward voltage drop . A typical example is the 1N914.
Zener diodes
- Diodes that can be made to conduct backwards. This effect, called Zener breakdown, occurs at a precisely defined voltage, allowing the diode to be used as a precision voltage reference. In practical voltage reference circuits Zener and switching diodes are connected in series and opposite directions to balance the temperature coefficient to near zero. Some devices labeled as high-voltage Zener diodes are actually avalanche diodes . Two Zeners in series and in reverse order, in the same package, constitute a transient absorber . They are named for Dr. Clarence Melvin Zener of Southern Illinois University, inventor of the device.
Avalanche diodes
- Diodes that conduct in the reverse direction when the reverse bias voltage exceeds the breakdown voltage. These are electrically very similar to Zener diodes, and are often mistakenly called Zener diodes, but break down by a different mechanism, the avalanche effect. This occurs when the reverse electric field across the p-n junction causes a wave of ionization, reminiscent of an avalanche, leading to a large current. Avalanche diodes are designed to break down at a well-defined reverse voltage without being destroyed. The difference between the avalanche diode and the Zener is that the channel length of the former exceeds the 'mean free path' of the electrons, so there are collisions between them on the way out. The only practical difference is that the two types have temperature coefficients of opposite polarities.
Transient voltage suppression diodes
- These are avalanche diodes designed specifically to protect other semiconductor devices from high-voltage transients. Their p-n junctions have a much larger cross-sectional area than those of a normal diode, allowing them to conduct large currents to ground without sustaining damage.
Photodiodes
- Semiconductors are subject to optical charge carrier generation and therefore most are packaged in light blocking material. If they are packaged in materials that allow light to pass, their photosensitivity can be utilized. Photodiodes can be used as solar cells, and in photometry.
Light-emitting diodes
- In a diode formed from a direct band-gap semiconductor, such as gallium arsenide, carriers that cross the junction emit photons when they recombine with the majority carrier on the other side. Depending on the material, wavelengths from the infrared to the near ultraviolet may be produced. The forward potential of these diodes depends on the wavelength of the emitted photons: 1.2 V corresponds to red, 2.4 to violet. The first LEDs were red and yellow, and higher-frequency diodes have been developed over time. All LEDs are monochromatic; 'white' LEDs are actually combinations of three LEDs of a different color, or a blue LED with a yellow scintillator coating. LEDs can also be used as low-efficiency photodiodes in signal applications. An LED may be paired with a photodiode or phototransistor in the same package, to form an opto-isolator.
Laser diodes
- When an LED-like structure is contained in a resonant cavity formed by polishing the parallel end faces, a laser can be formed. Laser diodes are commonly used in optical storage devices and for high speed optical communication.
Schottky diodes
- Schottky diodes are constructed from a metal to semiconductor contact. They have a lower forward voltage drop than a standard PN junction diode. Their forward voltage drop at forward currents of about 1 mA is in the range 0.15 V to 0.45 V, which makes them useful in voltage clamping applications and prevention of transistor saturation. They can also be used as low loss rectifiers although their reverse leakage current is generally much higher than non Schottky rectifiers. Schottky diodes are majority carrier devices and so do not suffer from minority carrier storage problems that slow down most normal diodes. They also tend to have much lower junction capacitance than PN diodes and this contributes towards their high switching speed and their suitability in high speed circuits and RF devices such as mixers and detectors.
Snap-off or 'step recovery' diodes
- The term 'step recovery' relates to the form of the reverse recovery characteristic of these devices. After a forward current has been passing in an SRD and the current is interrupted or reversed, the reverse conduction will cease very abruptly . SRDs can therefore provide very fast voltage transitions by the very sudden disappearance of the charge carriers.
Esaki or
tunnel diodes
- these have a region of operation showing negative resistance caused by quantum tunneling, thus allowing amplification of signals and very simple bistable circuits. These diodes are also the type most resistant to nuclear radiation.
Gunn diodes
- these are similar to tunnel diodes in that they are made of materials such as GaAs or InP that exhibit a region of negative differential resistance. With appropriate biasing, dipole domains form and travel across the diode, allowing high frequency microwave oscillators to be built.
Peltier diodes
- are used as sensors, heat engines for thermoelectric cooling. Charge carriers absorb and emit their band gap energies as heat.
There are other types of diodes, which all share the basic function of allowing electrical current to flow in only one direction, but with different methods of construction.
Point-contact diodes
- These work the same as the junction semiconductor diodes described above, but its construction is simpler. A block of n-type semiconductor is built, and a conducting sharp-point contact made with some group-3 metal is placed in contact with the semiconductor. Some metal migrates into the semiconductor to make a small region of p-type semiconductor near the contact. The long-popular 1N34 germanium version is still used in radio receivers as a detector and occasionally in specialized analog electronics.
Cat's whisker or crystal diodes
- These are a type of point contact diode. The cat's whisker diode consists of a thin or sharpened metal wire pressed against a semiconducting crystal, typically galena or a lump of coal. The wire forms the anode and the crystal forms the cathode. Cat's whisker diodes were also called crystal diodes and found application in crystal radio receivers.
Varicap or
varactor diodes
- These are used as voltage-controlled capacitors. These were important in PLL and FLL circuits, allowing tuning circuits, such as those in television receivers, to lock quickly, replacing older designs that took a long time to warm up and lock. A PLL is faster than a FLL, but prone to integer harmonic locking . They also enabled tunable oscillators in early discrete tuning of radios, where a cheap and stable, but fixed-frequency, crystal oscillator provided the reference frequency for a voltage-controlled oscillator.
PIN diodes
- A PIN diode has a central un-doped, or intrinsic, layer, forming a p-type / intrinsic / n-type structure. They are used as radio frequency switches, similar to varactor diodes but with a more sudden change in capacitance. They are also used as large volume ionizing radiation detectors and as photodetectors. PIN diodes are also used in power electronics, as their central layer can withstand high voltages. Furthermore, the PIN structure can be found in many power semiconductor devices, such as IGBTs, power MOSFETs, and thyristors.
Current-limiting field-effect diodes
- These are actually a JFET with the gate shorted to the source, and function like a two-terminal current-limiting analog to the Zener diode; they allow a current through them to rise to a certain value, and then level off at a specific value. Also called CLDs, constant-current diodes, or current-regulating diodes. ,
Other uses for semiconductor diodes include sensing temperature, and computing analog
logarithms .
Related devices
Applications
Radio demodulation
The first use for the diode was the demodulation of
amplitude modulated radio broadcasts. The history of this discovery is treated in depth in the
radio article. In summary, an AM signal consists of alternating positive and negative peaks of voltage, whose
amplitude or 'envelope' is proportional to the original audio signal, but whose average value is zero. The diode
rectifies the AM signal, leaving a signal whose average amplitude is the desired audio signal. The average value is extracted using a simple
filter and fed into an audio transducer, which generates sound.
Power conversion
Rectifiers are constructed from diodes, where they are used to convert
alternating current electricity into
direct current . Similarly, diodes are also used in
Cockcroft-Walton voltage multipliers to convert AC into very high DC voltages.
Over-voltage protection
Diodes are frequently used to conduct damaging high voltages away from sensitive electronic devices. They are usually reverse-biased under normal circumstances, and become forward-biased when the voltage rises above its normal value. For example, diodes are used in
stepper motor and
relay circuits to de-energize coils rapidly without the damaging voltage spikes that would otherwise occur. Many
integrated circuits also incorporate diodes on the connection pins to prevent external voltages from damaging their sensitive transistors. Specialized diodes are used to protect from over-voltages at higher power .
Logic gates
Diodes can be combined with other components to construct
AND and
OR logic gates. This is referred to as
diode logic.
In addition to light, mentioned above,
semiconductor diodes are sensitive to more
energetic radiation. In
electronics,
cosmic rays and other sources of ionising radiation cause noise
pulses and single and multiple bit errors.
This effect is sometimes exploited by
particle detectors to detect radiation. A single particle of radiation, with thousands or millions of electron volts of energy, generates many charge carrier pairs, as its energy is deposited in the semiconductor material. If the depletion layer is large enough to catch the whole shower or to stop a heavy particle, a fairly accurate measurement of the particle's energy can be made, simply by measuring the charge conducted and without the complexity of a magnetic spectrometer or etc.
These semiconductor radiation detectors need efficient and uniform charge collection and low leakage current. They are often cooled by
liquid nitrogen. For longer range particles they need a very large depletion depth and large area. For short range particles, they need any contact or un-depleted semiconductor on at least one surface to be very thin. The back-bias voltages are near breakdown . Germanium and silicon are common materials. Some of these detectors sense position as well as energy.
They have a finite life, especially when detecting heavy particles, because of radiation damage. Silicon and germanium are quite different in their ability to convert
gamma rays to electron showers.
Semiconductor detectors for high energy particles are used in large numbers. Because of energy loss fluctuations, accurate measurement of the energy deposited is of less use.
Temperature measuring
A diode can be used as a temperature measuring device, since the forward voltage drop across the diode depends on temperature. This temperature dependence follows from the Shockley ideal diode equation given above.
Digital cameras and similar units use arrays of photo diodes, integrated with readout circuitry.
Additional
Diodes may also be referred to as
controlled rectifiers, abbreviated
CR on
printed wiring boards.
See also
Notes
External links
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