Schottky Diode Characteristics & Specifications

- a overview of the characteristics and specifications for parameters describing Schottky Barrier Diode performance.

The Schottky diode is a very useful form of diode. It is widely used within electronics circuits because it has some particularly useful characteristics.

Its characteristics mean that it can be used where other forms of diode do not perform so successfully.

Schottky diode characteristics

The Schottky diode is what is called a majority carrier device. This gives it tremendous advantages in terms of speed because it does not rely on holes or electrons recombining when they enter the opposite type of region as in the case of a conventional diode. By making the devices small the normal RC type time constants can be reduced, making these diodes an order of magnitude faster than the conventional PN diodes. This factor is the prime reason why they are so popular in radio frequency applications.

The diode also has a much higher current density than an ordinary PN junction. This means that forward voltage drops are lower making the diode ideal for use in power rectification applications.

Its main drawback is found in the level of its reverse current which is relatively high. For many uses this may not be a problem, but it is a factor which is worth watching when using it in more exacting applications.

The overall I-V characteristic is shown below. It can be seen that the Schottky diode has the typical forward semiconductor diode characteristic, but with a much lower turn on voltage. At high current levels it levels off and is limited by the series resistance or the maximum level of current injection. In the reverse direction breakdown occurs above a certain level. The mechanism is similar to the impact ionisation breakdown in a PN junction.

Schottky diode IV characteristic

The IV characteristic is generally that shown below. In the forward direction the current rises exponentially, having a knee or turn on voltage of around 0.2 V. In the reverse direction, there is a greater level of reverse current than that experienced using a more conventional PN junction diode.

The IV characteristic of a Schottky diode showing the forward and reverse conduction areas
Schottky diode IV characteristic

The use of a guard ring in the fabrication of the diode has an effect on its performance in both forward and reverse directions. [see page on structure and fabrication]. Both forward and reverse characteristics show a better level of performance.

However the main advantage of incorporating a guard ring into the structure is to improve the reverse breakdown characteristic. There is around a 4 : 1 difference in breakdown voltage between the two - the guard ring providing a distinct improvement in reverse breakdown. Some small signal diodes without a guard ring may have a reverse breakdown of only 5 to 10 V.

Key specification parameters

In view of the particular properties of the Schottky diode there are several parameters that are of key importance when determining the operation of one of these diodes against the more normal PN junction diodes.

  • Forward voltage drop:   In view of the low forward voltage drop across the diode, this is a parameter that is of particular concern. As can be seen from the Schottky diode IV characteristic, the voltage across the diode varies according to the current being carried. Accordingly any specification given provides the forward voltage drop for a given current. Typically the turn-on voltage is assumed to be around 0.2 V.
  • Reverse breakdown:   Schottky diodes do not have a high breakdown voltage. Figures relating to this include the maximum Peak Reverse Voltage, maximum Blocking DC Voltage and other similar parameter names. If these figures are exceeded then there is a possibility the diode will enter reverse breakdown. It should be noted that the RMS value for any voltage will be 1/√2 times the constant value. The upper limit for reverse breakdown is not high when compared to normal PN junction diodes. Maximum figures, even for rectifier diodes only reach around 100 V. Schottky diode rectifiers seldom exceed this value because devices that would operate above this value even by moderate amounts would exhibit forward voltages equal to or greater than equivalent PN junction rectifiers.
  • Capacitance:   The capacitance parameter is one of great importance for small signal RF applications. Normally the junctions areas of Schottky diodes are small and therefore the capacitance is small. Typical values of a few picofarads are normal. As the capacitance is dependent upon any depletion areas, etc, the capacitance must be specified at a given voltage.
  • Reverse recovery time:   This parameter is important when a diode is used in a switching application. It is the time taken to switch the diode from its forward conducting or 'ON' state to the reverse 'OFF' state. The charge that flows within this time is referred to as the 'reverse recovery charge'. The time for this parameter for a Schottky diode is normally measured in nanoseconds, ns. Some exhibit times of 100 ps. In fact what little recovery time is required mainly arises from the capacitance rather than the majority carrier recombination. As a result there is very little reverse current overshoot when switching from the forward conducting state to the reverse blocking state.
  • Working temperature:   The maximum working temperature of the junction, Tj is normally limited to between 125 to 175°C. This is less than that which can be sued with ordinary silicon diodes. Care should be taken to ensure heatsinking of power diodes does not allow this figure to be exceeded.
  • Reverse leakage current:   The reverse leakage parameter can be an issue with Schottky diodes. It is found that increasing temperature significantly increases the reverse leakage current parameter. Typically for every 25°C increase in the diode junction temperature there is an increase in reverse current of an order of magnitude for the same level of reverse bias.

Schottky diode characteristics summary

The Schottky diode is used in many applications as a result of its characteristics that differ appreciable from several aspects of the more widely used standard PN junction diode.

Comparison of Characteristics of Schottky Diode and PN Diode
Characteristic Schottky Diode PN Junction Diode
Forward current mechanism Majority carrier transport. Due to diffusion currents, i.e. minority carrier transport.
Reverse current Results from majority carriers that overcome the barrier. This is less temperature dependent than for standard PN junction. Results from the minority carriers diffusing through the depletion layer. It has a strong temperature dependence.
Turn on voltage Small - around 0.2 V. Comparatively large - around 0.7 V.
Switching speed Fast - as a result of the use of majority carriers because no recombination is required. Limited by the recombination time of the injected minority carriers.

Example Schottky diode characteristics

To give some idea of the characteristics to be expected from Schottky diodes a couple of real examples are provided below. These summarise the main specifications and give an idea of their performance

  • 1N5711 Schottky barrier switching diode   This diode is described as an ultra-fast switching diode with high reverse breakdown, low forward drop voltage and a guard ring for junction protection.
Typical 1N5711 Characteristics / Specifications
Characteristic Typical Value Unit Details
Max DC Blocking Voltage, Vr 70 V
Max forward continuous current, Ifm 15 mA
Reverse breakdown voltage, V(BR)R 70 V @ reverse current of 10µA
Reverse leakage current, IR 200 µA At VR=50V
Forward voltage drop, VF 0.41

V at IF = 1.0 mA

Junction capacitance, Cj 2.0 pF VR = 0V, f=1MHz
Reverse recovery time, trr 1 nS
  • 1N5828 Schottky barrier power rectifier diode   This diode is described as a Schottky diode, stud type, i.e. for power rectification.
Typical 1N5258 Shottky Diode Characteristics / Specifications
Characteristic Typical Value Unit Details
Maximum recurrent peak reverse voltage 40 V
Maxim DC blocking voltage 40 V
Average forward current, IF (AV) 15 A T = 100°C
Peak forward surge current, IFSM 500 A
Maximum instantaneous forward voltage, VF 0.5 V At IFM = 15A and Tj = 25°C
Maximum instantaneous reverse current at rated blocking voltage, IR 10

mA Tj= 25°C

Tj = 125°C

Even though the example here gives a reverse voltage characteristic of 40 V which is fairly typical, the maximum that can normally be obtained is around 100 V.

It should be noted that even though these figures are given as examples of the figures that may be expected for typical Schottky diodes, figures even for a given device number will also vary slightly between different manufacturers.

By Ian Poole

<< Previous   |   Next >>

Share this page

Want more like this? Register for our newsletter

Investment in sensor technology is helping to ensure continued technological evolution Matthias Oettl | Heilind
Investment in sensor technology is helping to ensure continued technological evolution
Sensor technology is key to the successful operation of many automated processes - sensor information enables the systems to detector what is happening and enable feedback to be provided.
Acquiring an Analog Signal: Bandwidth, Nyquist Sampling Theorem & Aliasing
In this white paper from National Instruments learn all you need to know about analog signal sampling: bandwidth, amplitude error, rise time, sample rate, Nyquist Sampling Theorem, aliasing & resolution.

More whitepapers
 is operated and owned by Adrio Communications Ltd and edited by Ian Poole. All information is © Adrio Communications Ltd and may not be copied except for individual personal use. This includes copying material in whatever form into website pages. While every effort is made to ensure the accuracy of the information on, no liability is accepted for any consequences of using it. This site uses cookies. By using this site, these terms including the use of cookies are accepted. More explanation can be found in our Privacy Policy