© 2015 IJIRT | Volume 1 Issue 12 | ISSN: 2349-6002 PN DIODE Siddhartha Nair,Shubham Sharma,Sunil Sharma ECE department, Dronacharya College of Engineering, Gurgaon ABSTRACT The main aim of this research paper is to understand the basic working, biasing and the breakdown mechanism of a PN diode. Keywords- Diode, Forward Biased, Reverse Biased, Depletion Region Introduction A PN junction can be fabricated by implanting or diffusing (See Figure) donors into a P-type substrate such that a layer of semiconductor is converted into N type. Converting a layer of an N-type semiconductor into P type withacceptors would also create a PN junction. A PN junction has rectifying current–voltage (I–V or IV) characteristics as shown in Fig. 4–2. As a device, it is called a rectifier or a diode. The PN junction is the basic structure of solar cell, light-emitting diode, and diode laser, and is present in all types of transistors. In addition, PN junction is a vehicle for studying the theory IJIRT 101825 PN junction diode is symbolically represented as shown in picture. The direction of arrow is the direction of conventional current flow (under forward bias). Now let us try applying an external voltage to the PN junction diode. The process of applying an external voltage is called as “biasing”. There are two ways in which we can bias a PN junction diode. 1) Forward bias 2) Reverse bias The basic difference between a forward bias and reverse bias is in the direction of applying external voltage. The direction of external voltage applied in reverse bias is opposite to that of external voltage applied in forward bias. FORWARD BIASED When a diode is connected in a Forward Bias condition, a negative voltage is applied to the Ntype material and a positive voltage is applied to the P-type material. If this external voltage becomes greater than the value of the potential barrier, approx. 0.7 volts for silicon and 0.3 volts for germanium, the potential barriers opposition will be overcome and current will start to flow. This is because the negative voltage pushes or repels electrons towards the junction giving them the energy to cross over and combine with the holes being pushed in the opposite direction towards the junction by the positive voltage. This results in a characteristics curve of zero current flowing up to this voltage point, called the “knee” on the static curves and then a high current flow through the diode with little increase in the external voltage as shown below. Forward Characteristics Curve for a Junction Diode INTERNATIONAL JOURNAL OF INNOVATIVE RESEARCH IN TECHNOLOGY 99 © 2015 IJIRT | Volume 1 Issue 12 | ISSN: 2349-6002 The forward biasing voltage on the junction diode results in the depletion layer becomes very thin and narrow which represents a low impedance path through the junction thereby allowing high currents to flow. The point at which this sudden increase in current takes place is represented on the static I-V characteristics curve above as the “knee” point. Reduction in the Depletion Layer due to Forward Bias This condition represents the low resistance path through the PN junction allowing very large currents to flow through the diode with only a small increase in bias voltage. The actual potential difference across the junction or diode is kept constant by the action of the depletion layer at approximately 0.3v for germanium and approximately 0.7v for silicon junction diodes. Since the diode can conduct “infinite” current above this knee point as it effectively becomes a short circuit, therefore resistors are used in series with the diode to limit its current flow. Exceeding its maximum forward current specification causes the device to dissipate more power in the form of heat than it was designed for resulting in a very quick failure of the device.the device will burn if it exceeds the forward current. 2) Reverse Biased PN Junction Diode IJIRT 101825 When a diode is connected in a Reverse Bias condition, a positive voltage is applied to the Ntype material and a negative voltage is applied to the P-type material. The positive voltage applied to the N-type material attracts electrons towards the positive electrode and away from the junction, while the holes in the P-type end are also attracted away from the junction towards the negative electrode. The net result is that the depletion layer grows wider due to a lack of electrons and holes and presents a high impedance path, almost an insulator. The result is that a high potential barrier is created thus preventing current from flowing through the semiconductor material. 3) Increase in the Depletion Layer due to Reverse Bias This condition represents a high resistance value to the PN junction and practically zero current flows through the junction diode with an increase in bias voltage. However, a very small leakage current does flow through the junction which can be measured in microamperes, ( μA ). One final point, if the reverse bias voltage Vr applied to the diode is increased to a sufficiently high enough value, it will cause the diode’s PN junction to overheat and fail due to the avalanche effect around the junction. This may cause the diode to become shorted and will result in the flow of maximum circuit current, and this shown as a step downward slope in the reverse static characteristics curve below. 4) Reverse Characteristics Curve for a Junction Diode INTERNATIONAL JOURNAL OF INNOVATIVE RESEARCH IN TECHNOLOGY 100 © 2015 IJIRT | Volume 1 Issue 12 | ISSN: 2349-6002 Sometimes this avalanche effect has practical applications in voltage stabilizing circuits where a series limiting resistor is used with the diode to limit this reverse breakdown current to a preset maximum value thereby producing a fixed voltage output across the diode. These types of diodes are commonly known as Zener Diodes and are discussed in a later tutorial. PN Junction Breakdown Electrical break down of any material (say metal, conductor, semiconductor or even insulator) can occur due to two different phenomena. Those two phenomena are 1) Zener breakdown 2) Avalanche breakdown These two phenomena are quite like a natural occurrence. It even applies to our daily life while lightning. We all know air is an insulator under normal conditions. But when lightning occurs (an extremely high voltage), it charges the air molecules nearby and charges get transferred via air medium. Now that’s a kind of electrical break down of an insulator. A similar kind of situation arises in zener and avalanche breakdown as well. Let see what’s it all about! Zener Breakdown When we increase the reverse voltage across the PN junction diode, what really happens is that the electric field across the diode junction increases (both internal & external). This results in a force of attraction on the negatively charged electrons at junction. This force frees electrons from its covalent bond and moves those free electrons to conduction band. When the electric field increases (with applied voltage), more and more electrons are freed from its covalent bonds. This results in drifting of electrons across the junction and electron hole recombination occurs. So a net current is developed and it increases rapidly with increase in electric field. IJIRT 101825 Zener breakdown phenomena occur in a PN junction diode with heavy doping & thin junction (means depletion layer width is very small). Zener breakdown does not result in damage of diode. Since current is only due to drifting of electrons, there is a limit to the increase in current as well. Avalanche Breakdown Avalanche breakdown occurs in a pn junction diode which is moderately doped and has a thick junction (means its depletion layer width is high). Avalanche breakdown usually occurs when we apply a high reverse voltage across the diode (obviously higher than the Zener breakdown voltage, sayVz). So as we increase the applied reverse voltage, the electric field across junction will keep increasing. If applied reverse voltage is Va and the depletion layer width is d then the generated electric field can be calculated as Ea =Va/d. This generated electric field exerts a force on the electrons at junction and it frees them from covalent bonds. These free electrons will gain acceleration and it will start moving across the junction with high velocity. This results in collision with other neighboring atoms. These collisions in high velocity will generate further free electrons. These electrons will start drifting and electron-hole pair recombination occurs across the junction. This results in net current that rapidly increases. We learned that avalanche breakdown occurs at a voltage (Va) which is higher than Zener breakdown voltage (Vz). The reason behind this is simple. We know avalanche phenomena occur in a diode which is moderately doped and junction width (say d) is high. A Zener break down occurs in a diode with heavy doping and thin junction (here d is small). The electric field that occur due to applied reverse voltage (say V) can be calculated as E = V/d. REFERENCES [1] www.google.co.in [2] www.wikipedia.com [3] Electronic Devices and Circuits- By JB Gupta [4] Notes by- Prof Poonam Kaushik [5] Notes by- Dr. K.K Saini INTERNATIONAL JOURNAL OF INNOVATIVE RESEARCH IN TECHNOLOGY 101