SCHOTTKY BARRIER DIODE

•The Schottky diode (named after German physicist Walter H. Schottky; also known as hot carrier diode) is a semiconductor diode with a low forward voltage drop and a very fast switching action.

•When current flows through a diode there is a small voltage drop across the diode terminals. A normal silicon diode has a voltage drop between 0.6–1.7 volts, while a Schottky diode voltage drop is between approximately 0.15–0.45 volts. This lower voltage drop can provide higher switching speed and better system efficiency.

CONSTRUCTION

• A metal–semiconductor junction is formed between a metal and a semiconductor, creating a Schottky barrier (instead of a semiconductor–semiconductor junction as in conventional diodes).

• Typical metals used are molybdenum, platinum, chromium or tungsten; and the semiconductor would typically be N-type silicon.

• The metal side acts as the anode and N-type semiconductor acts as the cathode of the diode. This Schottky barrier results in both very fast switching and low forward voltage drop.

Reverse recovery time

• The most important difference between the p-n and Schottky diode is reverse recovery time, when the diode switches from conducting to non-conducting state. Where in a p-n diode the reverse recovery time can be in the order of hundreds of nanoseconds and less than 100 ns for fast diodes, Schottky diodes do not have a recovery time, as there is nothing to recover from (i.e. no charge carrier depletion region at the junction).

• The switching time is ~100 ps for the small signal diodes, and up to tens of nanoseconds for special high-capacity power diodes. With p-n junction switching, there is also a reverse recovery current, which in high-power semiconductors brings increased EMI noise. With Schottky diodes switching essentially instantly with only slight capacitive loading, this is much less of a concern.

CONSTRUCTION AND APPLICATIONS

• It is often said that the Schottky diode is a "majority carrier" semiconductor device. This means that if the semiconductor body is doped n-type, only the n-type carriers (mobile electrons) play a significant role in normal operation of the device. The majority carriers are quickly injected into the conduction band of the metal contact on the other side of the diode to become free moving electrons. Therefore no slow, random recombination of n- and p- type carriers is involved, so that this diode can cease conduction faster than an ordinary p-n rectifier diode. This property in turn allows a smaller device area, which also makes for a faster transition.

• This is another reason why Schottky diodes are useful in switch-mode power converters; the high speed of the diode means that the circuit can operate at frequencies in the range 200 kHz to 2 MHz, allowing the use of small inductors and capacitors with greater efficiency than would be possible with other diode types. Small-area Schottky diodes are the heart of RF detectors and mixers, which often operate up to 50 GHz.

Limitations

• The most evident limitations of Schottky diodes are the relatively low reverse voltage ratings for silicon-metal Schottky diodes, typically 50 V and below, and a relatively high reverse leakage current. Some higher-voltage designs are available; 200V is considered a high reverse voltage.

• Reverse leakage current, because it increases with temperature, leads to a thermal instability issue. This often limits the useful reverse voltage to well below the actual rating.

• While higher reverse voltages are achievable, they would be accompanied by higher forward voltage drops, comparable to other types; such a Schottky diode would have no advantage

Applications

• Voltage clamping• Reverse current and discharge protection• Power supply

7

*Other Two-Terminal Devices

*Schottky Barrier Diodes

Two-Terminal Devices Having A Single p-n Junction

SchottkyTunnelVaractorPhotodiodeSolar Cell

Other Two-Terminal DevicesOf A Different Construction

Photoconductive CellLCD (Liquid-Crystal Display)Thermistor

Schottky-Barrier Diode

*Surface-Barrier/Hot-Carrier Diode

Schottky-Barrier Diode

Areas of Application

Very high frequency rangeLower noise figureLow-voltage or high-current power suppliesAC-to-DC convertersRadar systemsSchottky TTL logic

Fig. 20.1 Passivated hot-carrier diode

Gold leaf metal contact

Anode (+)

MetalSilicon dioxide screen

Metal semiconductor junction

Metal contactCathode (-)

Fig. 20.2 Comparison of characteristics of hot-carrier and p-n junction diodes

ID

VD

p-n junction

diode

Hotcarrierdiode

Hotcarrierdiode

p-n junction

diode

Fig. 20.3 Schottky (hot-carrier) diode: (a) equivalent circuit; (b) symbol

(a)

Fig. 20.4 Approximate equivalent circuit for the Schottky diode

Fig. 20.5 Motorola Schottky barrier devices.(Courtesy Motorola Semiconductor Products, Incorporated

IO Average rectified forward current (amperes)

VRRM

(Volts)

CaseAnode

Cathode

51-02(DO-7)

Glass

59-04Plastic

267Plastic

60Metal

257(DO-4)Metal

257(DO-5)Metal

430-2(DO-21)

Metal

20

MBR020

IN5817

MBR120P

IN5820

MBR320P

MBR320M

IN5823

IN5826

MBR1520

IN5829

MBR2520

IN5832

MBR4020

MBR4020P

F

30

MBR030

IN5818

MBR130P

IN5821

MBR330P

MBR330M

IN5824

IN5827

MBR1530

IN5830

MBR2530

IN5833

MBR4030

MBR4030P

F

35

MBR135P

MBR335P

MBR335M

MBR1535

MBR2535

MBR4035

MBR4035P

F

40

IN5819

MBR140

P

IN5822

MBR340

P

MBR340

M

IN5825

IN5828

MBR154

0

IN5831

MBR253

4

IN5834

MBR404

0

IFSM (Amps) 5.0 100 50 250 200 500 500 500 500 800 800 80

0800 800

TC @ Rated IO (ºC) 85 80 85 80 75 70 50TJ Max 125ºC

Max VF @ IFM = IO

Fig 20.6 Characteristics curves for Hewlett-Packard 5082-2300 series of general-purpose Schottky barrier diodes.

.1

0.1

1

10

100

T = 100ºCT = 25ºC

T = -50ºC0 100 200 300 400 700600500

IF Temperature Coeffiecient10A -2.3mV/ºC100A -1.8mV/ºC1.0mA -1.3mV/ºC10mA -0.7mV/ºC100mA -0.2mV/ºC

Forward voltage (mV)

Forward current (m

A)

I-V Curve Showing Typical Temperature Variation for 5082-2300 Series Schottky Diodes

(a)

50

10

100

500

100

0 5 1510Reverse voltage (V)

Reverse current

(nA)

5082-2300 Series Typical Reverse Current vs. Reverse Voltage at TA = 25ºC

(b)

29002303

2301

23022305

Capacitance

(pF)

VR-Reverse voltage (V)

5082-2300 Series Typical Capacitance vs. Reverse Voltage at TA = 25ºC

(c)

0 8 16124 20

0.2

0.3

0.6

0.8

1.0

1.2

29002303

230123022305

Schottky diode I-V characteristics

Schottky diode is a metal-semiconductor (MS) diodeHistorically, Schottky diodes are the oldest diodesMS diode electrostatics and the general shape of the MS diode I-

V characteristics are similar to p+n diodes, but the details of current flow are different.

Dominant currents in a p+n diode– arise from recombination in the depletion layer under small

forward bias.– arise from hole injection from p+ side under larger forward

bias.Dominant currents in a MS Schottky diodes

– Electron injection from the semiconductor to the metal.

Current components in a p+n and MS Schottky diodes

IR-G

negligible

dominant

p+ n

B

dominant

Ir-g

negligible

M n-Si

I-V characteristics

kT*kTqV

TAIIIBA

ewhere1e 2ss

A

where B is Schottky barrier height, VA is applied voltage, A is area, and A* is Richardson’s constant.

The reverse leakage current for a Schottky diode is generally much larger than that for a p+n diode.

Since MS Schottky diode is a majority carrier devices, the frequency response of the device is much higher than that ofequivalent p+ n diode.