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8/6/2019 Design of RF Solid State Switches
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CONTENTS
Page No¶s
Abstract 1Introduction 3
Common Switch Configurations 3
Ideal Vs Practical Switches 4
Types of RF Switches 4
Reflective or Absorptive Switches 4
Advantages 5
PIN Diode Fundamentals 5
RF Switch Considerations and Terminology 7
Classification based on circuit combinations 10(a) Series connected switch 10
(b) Shunt Connected Switch 11
(c) Compound Switch 12
FET Switches 13
(a) Single(Series) FET Switch 13
(b) Series Shunt Switch 14
PIN Vs FET Switches- which one to use? 16
Comparison of PIN Diodes & FET¶s 19
Conclusion 19
Future Scope 20References 20
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Department of Electronics and Communication Engineering,
College of Engineering, Osmania University, Hyderabad-07
DESIGN OF SOLID STATE RF SWITCHES
Switches are widely used in many RF Systems, from low power transmit-receive
switches in time division duplex wireless transreceivers to millimetric wave beam-
forming systems for satellite tracking to high power(often military) phased array
systems. PIN diode operation is reviewed such that the impact of device choice and
characteristics on the design can be understood. This Paper examines basic design
techniques employing PIN diode as switching element and FET switches
concentrates on circuit layout techniques to achieve high isolation. The Paper
concludes with a comparison of PIN and FET based switching components.
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INTRODUCTION
A switch is an electrical component for opening and closing the connection of a
circuit or for changing the connection of a circuit device. An ³Ideal Switch´ exhibitszero resistance to current flow in the ³ON´ state and infinite resistance to current
flow in the ³OFF´ state. A practical switch design exhibits a certain amount of
resistance in the ³ON´ state and a finite resistance in the ³OFF´ state.
The use of PIN diodes as the switching element in microwave circuits is based on
the difference between the PIN diode reverse and forward bias characteristics. At
lower microwave frequencies, f < 2 GHz), the PIN diode (including package
parasitics) appears to be a very small impedance under forward bias and a very large
impedance under reverse bias. It is the difference in performance between forward
and reverse bias states upon which switch operation relies.
Most switch designs to be considered use a difference in reflection, rather than
dissipation, to obtain switch performance. Very little power is dissipated by the
diode itself, thus permitting small devices to control relatively large amounts of
microwave power. Thus, PIN diode switches are reactive networks, where losses are
a second order effect. In subsequent sections, we will see that switch circuits
resemble filter circuits in many ways.
Common Switch Configurations
Switches may be implemented in many configurations. These configurations are
described in terms of the number of poles and the number of throws implemented in
the switch. The number of poles describes the number of signal paths controlled by
the switch. The number of throws indicates the number of potential directions into
which a pole may be placed. For example, the simplest switch configuration is a
single pole, single throw (SPST) switch. This configuration has one signal path
which can either be completed by the switch or interrupted by the switch. A single
pole double throw switch (SPDT or SP2T) can connect a single transmission line to
either of two other transmission lines. The number of poles and throws, and the
combinations thereof, is unlimited in the ideal sense, but has practical limitations
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Ideal vs. Practical Switches
In practical solid state RF/microwave switches, it is not possible to produce neither
perfect open impedance nor a perfect short circuit. Consequently, there is always
some small amount of incident signal that is absorbed by the switch and a bit more
reflected by the switch¶s non-ideal impedance when the switch is in the state inwhich it should ideally pass all incident signal energy. This small reduction in signal
amplitude is known as insertion loss (IL) and is typically described in terms of
decibels (dB). Insertion loss is simply the ratio of the output power to the input
power.
TYPES OF RF SWITCHES
Mechanical
Relays, Rotary Switches, Push Buttons
Electronic Switches
Semiconductor Switches (FET¶s, Diodes)
Reflective or Absorptive Switches?
Reflective Switches
A reflective switch is one in which the incident power at the ³off´ port isreflected back to the source as a result of the impedance mismatch presented by the
PIN diode. In contrast, an absorptive switch is designed to present 50-ohm
impedance in the ³off´ state, and to absorb incident power.
The operating bandwidth of the switch is determined by the blocking capacitors
selected, the bias circuitry, and the diode¶s reverse-bias capacitance. Reducing the
diode¶s shunt resistance increases isolation in this type of switch. This reduction is
achieved either by increasing the current or decreasing the diode¶s overall resistance.
Absorptive Switches Multi-throw absorptive switches typically employ the series-shunt approach.
The required 50-ohm terminating impedance is achieved by the series combination
of the diode and terminating resistance to ground. This type of termination has good
high-frequency characteristics, but power-handling ability is limited by the ability of
the diodes and resistors to dissipate RF power. In addition, absorptive switches
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typically exhibit somewhat slower switching speeds. These types of switches are
usually not absorptive at their common port (in the ³all-off´ state) but can be made
absorptive for special applications.
Advantages of Electronic Switches over Mechanical Switches are as follows:
High Switching Speed
Small in Size
More efficient and reliable
Cost effective
The PIN diode finds wide usage in RF, UHF and microwave circuits. It is
fundamentally a device whose impedance, at these frequencies, is controlled by its
DC excitation. A unique feature of the PIN diode is its ability to control largeamounts of RF power with much lower levels of DC.
PIN Diode Fundamentals:
The PIN diode is a current controlled resistor at radio and microwave frequencies. It
is a silicon semiconductor diode in which a high-resistivity intrinsic I region is
sandwiched between a P-type and N-type region. When the PIN diode is forward
biased, holes and electrons are injected into the I region. These charges do not
immediately annihilate each other; instead they stay alive for an average time, calledthe carrier lifetime, t. This results in an average stored charge, Q, which lowers the
effective resistance of I region to a value R S.
When the PIN diode is at zero or reverse bias there is no stored charge in I region
and the diode appears as a capacitor, CT, shunted by a parallel resistance R S.
PIN DIODE
PIN diodes are specified for the following parameters:
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R S : Series resistance under forward bias
CT : Total capacitance at zero or reverse bias
R D : Parallel resistance at zero or reverse bias
VR : Maximum allowable DC reverse bias voltage
: Carrier lifetimeAV : Average thermal resistance
PD : Maximum average power dissipation
Pulse : Pulse thermal impedance
PP : Maximum peak power dissipation
In simplest form the capacitance of a PIN is determined by the area and width of the
I region and the dielectric constant of silicon. This minimum capacitance is obtained
by the application of a reverse bias in excess of VPT, the voltage at which the
depletion region occupies the entire I layer.
Equivalent Circuit of
I-region before punch
Through
Simplified Equivalent Circuit, series
A good way to understand the effects of series resistance is to observe the insertion
loss of a PIN chip series mounted in a 50 � line.
Simplified Equivalent
Circuit, shunt
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RF switch considerations and terminology
Frequency and Bandwidth
Although most of the switching systems do not have a limit on the lowest
frequency of operation, they do have an upper limit. For semiconductor devicesthis is due to the ¿nite time in carrier mobility. The losses incurred from
resistance and parasitic reactances are the main cause limiting the performance of
electromechanical switches at higher frequencies.
Insertion loss
The insertion loss of an RF device is a measure of its efficiency for signal
transmission. In the case of a switch, the insertion loss is speci¿ed only when its
state is such that signal is transmitting or when the switch is in the on-state. This
is speci¿ed in terms of the transmission coefficient, S21, in decibels, between the
input and output terminals of the switched circuit. Usually speci¿ed in decibels,
one of the design goals for most of the RF switches is to minimize the insertion
loss. The insertion loss tends to degrade with increase in frequency for most of
the solid-state switching systems. Compared with these, RF MEMS switches can
be designed to operate with a small insertion loss at several gigahertz. Resistive
losses at lower frequencies and skin-depth effects at higher frequencies are the
major causes for losses.
Isolation
The isolation of a switching system is speci¿ed when there is no signal
transmission. This is also measured as S21 between the input and output
terminals of the switched circuit, under the no-transmission state or when the
switch is in the off condition. A large value (in decibels) indicates very small
coupling between input and output terminals. Thus the design goal is to
maximize the isolation. In RF MEMS switches isolation may degrade as a result
of proximity coupling between the moving part and the stationary transmissionline as a result of leakage currents.
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RF Power handling
RF power handling is a measure of how efficiently a switch passes the RF signal.
This is commonly speci¿ed in terms of a 1 dB compression point, which is
adopted from the ampli¿er characterization industry. It is commonly assumed
that the output power level follows the input power with a linear ratio. But inmany devices there is a maximum power above which this linearity does not
hold. The 1 dB compression point is de¿ned as the maximum input power level
at which the output power differs by 1 dB with respect to linearity. The 1 dB
compression points and the power handling of many devices such as PIN diodes
and MMIC switches are functions of frequency.
Switching time (Rise time & Fall time)
These parameters, fundamental too many designs, are actually composed of several subsets, each one defining the time required for switching to take place
between two states in the switch response (Figure 3a). Rise time is defined as the
period between full ³off´ and full ³on," specifically from 10 percent of this
condition to 90 percent of the square-law-detected RF power. Conversely, fall
time is the period between 90 percent of full ³on´ to 10 percent of full ³off." Rise
time and fall time do not include driver propagation delays.
On time and Off time
The time lapse between 50 per cent of full input control signals from the driver to
90 percent of the square-law-detected RF power when the device is switched
from full ³off´ to full ³on´ is called the ³on´ time. The ³off´ time begins when
the 50 percent point of control signal occurs, to the point when it achieves 10
percent of its square-law detected RF power and the unit is switched from full
³on´ to full ³off." On and off times include driver propagation delays. This is
sometimes referred to as "Modulation Time."
Switching Transients
Switching transients are the exponentially decaying voltage spikes at the input,
output or both of an RF signal path, due to a change in the control voltage. These
switching transients are often called sidebands due to switching, and it shows
important indications of the performance of a switching system. It is often
required to monitor the output RF spectrum during the design of an RF system,
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and hence components of the RF chain, such as ampli¿ers and switches, must be
tested with a known stimulus. Both electromechanical and electromagnetic
transients exist during the switching process. While the electromechanical
transient is due to mechanical motion (wherever present) of the switch element,
the electromagnetic transient is due to energy exchange between electric ¿eldsand magnetic ¿elds of the electric equipment in the network.
It may be noted that these transients arise from nonlinearities in the
network. The switching transients in PIN diode switches are due to the stored
charge in the intrinsic region being quickly discharged by the control voltage. In
balanced Schottky barrier designs, the charge stored by the diode is very small
and the majority of the transients are caused by the mismatch within the drive
circuits. However, the switching transient mechanism of the gallium arsenide
¿eld effect transistor (GaAs FET) MMIC circuits results when the rapidlychanging gate voltage is coupled to the switch output through the gate-to-channel
capacitance of the FET, thus experiencing a greater feed through because of its
faster switching speed.
Classification based on the circuit combination:
Series Combination
Shunt Combination
Compound Combination (Series-Shunt)
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Series Connected Switch:
Figures below show two basic types of PIN diode series switches, (SPST and
SPDT), commonly used in broadband designs.
Principal operating parameters of switch are calculated as follows:
(A) Insertion Loss (dB) =
(B) Isolation (dB) =
(C) Power Dissipation (Forward Bias)
For , this becomes
(D) Peak Current
(E) Peak RF Voltage
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Shunt Connected Switch:
Figure below shows two typical shunt connected PIN diode Switches.
The Principal equations describing the operating parameters of shunt switches are
given by
(A) Insertion Loss
(B) Switch Isolation
(C) Power Dissipation (Forward Bias)
(D) Power Dissipation
(E) Peak RF Current
(F) Peak RF Voltage
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Compound Combination (Series-Shunt):
Compound Switches are series-shunt switches used in combinations to improve
overall switch performance. The broad band Insertion Loss of the series switch is
combined with the broad band Isolation of the shunt switch in a number of
combinations to follow. Here are few combinations:
FET Switches:
FET Switches
The control field effect transistor (FET) or switching FET functions as a three port
device, where the channel between source and drain ports forms a conduction path
for the RF signal and the gate port, controls whether an RF signal is blocked or may pass. A DC control voltage applied between the gate and channel is required to
create this function. Most control FETs use a depletion mode configuration, which
means that the channel is normally in its low impedance state with no control
voltage applied and in its high impedance, pinched off state when a negative voltage
with respect to the channel is applied (thus the term ³pinch off voltage´).
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Single FET Switch
Figure below shows a single FET configured as a simplified single pole, single
throw (SPST) switch. The first challenge in fabricating a switch using a GaAs FET
is to isolate the DC gate control from the RF path. This is done by using a 5 k� to 10
k� resistor in series with the gate of the FET. This is a very simple bias network thathas many advantages which will be discussed later. The next step is to DC block the
RF source and drain ports using a capacitor with adequately low capacitive reactance
at the desired frequency of operation. This creates an SPST switch. The insertion
loss of the ³ON´ path of the switch will be affected by the channel resistance.
Likewise the isolation of the ³OFF´ path is limited by the capacitance created by the
source and drain spacing as well as FET physical size (periphery). Hence a balance
of channel resistance (RS) and off capacitance (Coff ) must be met. The following
equations show the relationship of the RS and Coff as expressed in insertion loss (dB)and isolation loss (dB) for a single series FET SPST switch.
Assume the FET has the following characteristics:
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Series-Shunt Switch:
To improve the isolation at higher frequencies, a shunt FET can be used following
the series FET. In this position the FET must be ³ON´ in order to increase isolation
and ³OFF´ to put it in the insertion loss state.
This requires two separate control voltages for the switch. Shunt FET has no
appreciable reactive component when it is biased to its ³ON´ state, isolation will
stay relatively unchanged over frequency. The negative gate voltage required for this
switch can be viewed as a drawback, since in most applications only positive voltage
supplies are available. Also in this series/shunt configuration one FET must be ³ON´
while the other FET is ³OFF´. A solution to this problem is the addition of two
capacitors applied to the shunt FET which provide DC blocks to the RF path and
allow the gate port of the shunt FET to be grounded. An additional reference voltage
port must also be added. This technique also allows for a single positive voltage to
be applied to the switch. The selection of the capacitor value is critical to insure
proper frequency operation and bandwidth. The values can be quite small (5 to 15
pF), since the series FET can provide most of the isolation at the lower frequencies.
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This SPST switch is reflective, which means that the output when in the isolation
state will have a substantial VSWR. A class of switches, known as ³matched´ or
³absorptive´ will terminate the output into a 50 � load when switched to the
isolation state.
PIN vs. FET Switches ± Which One to Use?
PIN diodes and FETs have relative advantages and disadvantages to each other for
use in switching applications. The performance attributes which should be compared
when the selection of one of these technologies is undertaken are more numerous
than one might think at first glance. Table below lists the foremost of these
attributes, but is by no means intended to be complete.
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Attribute PIN Diode FET
³Integratability´ with
other componentsPoor Excellent
Power HandlingVery High
(greater than 1KW CW)
Moderate
(10 Watts or Less)
Switching Time
A few tens of
nanoseconds to several
microseconds
Tens to a few
hundred of
nanoseconds
Control Current Up to 100 milliampsLess than 100
micro amps
Distortion PerformanceI/P IP3 are in the range of
+45dBm or higher
I/P IP3 are in the
range of +30dBm
Integratability:
The wafer processing required for modern FET structures such as pHEMTs is
largely lateral with respect to the top surface of the wafer; it lends itself quite well to
the inclusion of passive component structures -- such as metal-insulator-metal
(MIM) capacitors, spiral inductors, and thin film resistors -- all of which can be
formed on or near the topmost layer of the wafer. The bottom-most layer of a FET
wafer is semi-insulating material, which inherently isolates one FET structure fromanother. In comparison, PIN diode wafer processing is vertical with respect to the
top surface of the wafer; the majority of the physical thickness of a PIN diode wafer
is the cathode of the diode. It is very difficult to isolate the cathodes of PIN diodes
that are on the same die. Consequently, with the exception of common-cathode pairs
of PIN diodes, they are inherently discrete devices.
Power handling
The vertical structure of a PIN diode is a relative advantage for power handling. The
heat that is generated by Joule heating within the I layer of the diode can easily beconducted downwards through the diode¶s cathode layer to the system heat sink. RF
FET structures such as pHEMTs and MESFETs are typically fabricated from III-V
materials, such as GaAs, that has lower thermal conductivity than Si, which is the
material utilized for most switching PIN diodes.
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Switching Time
The FET is a majority carrier device whose drain-source impedance is controlled by
the thickness of a depletion layer that extends into the channel from the gate-source
interface. The thickness of this depletion layer can be modulated very rapidly in
response to a change in the gate-source control voltage. By contrast, a PIN diode
stores minority carriers in its I layer when it is under forward bias. These charge
carriers must be primarily conducted out of the I layer to change its impedance from
low to high. This process is inherently slower than the change in drain-source
impedance for a pHEMT or MESFET device.
Control Current
The FET is a voltage-controlled device. In a practical pHEMT or MESFET, the only
current that flows into the control port of the transistor is the reverse leakage current
of the gate-source junction, which is very small, typically less than 10 micro amps.
On the other hand, a PIN diode can require a significant injection of charge carriersinto its I layer to lower its impedance to the required level. The typical bias current
for a PIN diode in a switch is 10 to 20 milliamps.
Distortion Performance
The PIN diodes produce nearly ideal, very linear series resistance when the amount
of charge in its I layer -- as a result of DC forward bias current -- is at least ten times
that of the charge that is alternately injected and removed by the RF signal. When
the diode is nonconducting, it presents a very high resistance in parallel with its
junction capacitance. This junction capacitance is independent of applied voltage for
signals with sufficiently high frequency (typically greater than 100 MHz).Consequently, the PIN diode produces excellent distortion performance.
An FET structure responds very quickly to the magnitude of its applied gate-
source voltage, because the gate-source junction in a MESFET and a pHEMT
structure is a Schottky diode. The Schottky diode¶s very nonlinear impedance with
respect to applied bias conditions can be a comparatively efficient distortion
generation mechanism, which results in input third order intercept for a FET switch
that is roughly an order of magnitude or more lower than that of a PIN diode switch.
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Comparison of PIN Diode and FET Characteristics:
FEATURE PIN SWITCH FET SWITCH
Insertion Loss
(typ. 1GHz)
Very Low (0.4-
0.6dB)
Very Low
(0.4-0.6dB)
Isolation
(typ. 1GHz)
Excellent
(typ. 50dB)
Very Good
(typ. 45dB)
Current
consumptionHigh (typ. mA)
Very Low
(typ. Micro Amps)
Switching speed Fast (typ. 100ns) Very Fast (3-10ns)
Operation DC No Yes
Power Handling Excellent Good(typ. +25dBm)
Circuit Size Small-Moderate Very Small
Design
FlexibilityYes N/A
Conclusion:
(1) RF switches may comprise PIN diodes or FET structures such as MESFETs
and pHEMTs. These two approaches to the design of the switch offer advantages
and disadvantages.
(2) A PIN diode switch typically can handle greater power and produce less
distortion, at the expense of longer switching time and much larger control current
requirements.
(3) The very low bias current needs of MESFET and pHEMT switches makes
them very well suited for battery powered applications. These devices can also be
integrated into complex, multi-throw integrated circuit switches.
Future Scope:
Devices with more operating life span and extremely small in size can be fabricated
such as, MEMS based switches and in near future NEMS based switches.
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References:
1. ³Design with PIN Diodes´, Skyworks Solutions application note.
2. ³PIN Diode Circuit Designers Handbook´ Micro-semi Corporation.
3. A.M.Street ³Designing with PIN Diodes´, Practical RF/Microwave Design
Course, university of oxford, International Electronics and CommunicationsProfessional Development course programme, Jan 2000.