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balanced amplification technique using Wilkinson and 90 degrees

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LNA<br />

Article 1 (<strong>Wilkinson</strong>)<br />

An ideal <strong>balanced</strong> configuration provides low input <strong>and</strong> output VSWR in addition to a 3 dB<br />

improvement of the power <strong>and</strong> linearity performance.<br />

The Traveling-Wave Divider/Combiner(1) is a planar structure used to increase output power<br />

by combining parallel amplifier stages. The simplest implementation is a 2-way <strong>Wilkinson</strong> type<br />

divider/combiner with a <strong>90</strong>transmission line in one arm. The <strong>Wilkinson</strong> divider provides an<br />

equal-power, equal-phase power split <strong>and</strong> the transmission line shifts the phase of one path<br />

by <strong>90</strong>° so at the output of the divider we have two equal power signals in quadrature (phase<br />

shifted by <strong>90</strong>°) as shown in Figure 1. Two identical power amplifiers with gain A are placed in<br />

each arm. Any reflected power at the input to the amplifier is terminated in the 100-isolation<br />

resistor, since the reflected power of the two arms at the resistor is 180° out of phase. A<br />

combiner with similar properties is placed at the output to combine both output signals from<br />

the amplifiers, but the extra <strong>90</strong>° line is placed in the opposite arm so that the output signals<br />

add in phase through the combiner. Assuming no loss <strong>and</strong> perfect combining, the 2-way<br />

combiner will increase output power <strong>and</strong> linearity by 3 dB. Given a real life application, the<br />

typical increase is 2.5 dB. Even though this power combiner is comprised of multiple quarterwave<br />

lines, the <strong>Wilkinson</strong> type divider/combiner with a <strong>90</strong>° transmission line has a broad<br />

b<strong>and</strong>width, significantly wider than a branch-line type combiner, <strong>and</strong> has low loss. Since the<br />

combiner is planar, it is much easier to fabricate <strong>using</strong> st<strong>and</strong>ard PCB technology. The<br />

example we show in Figure 1 has a 50-impedance at the amplifier input.<br />

However, lower impedances can be achieved by increasing the transformation ratio in the<br />

quarter wave lines. Unlike branch line or Lange type combiners, the <strong>Wilkinson</strong> type<br />

divider/combiner easily scales to 4-way combining for even higher power. The performance of<br />

the <strong>balanced</strong> stage is 2.5 dB to 2.8 dB better than performance of a single-ended unit under<br />

the same conditions. This novel design approach for combining two power amplifiers offers<br />

simple low-cost implementation, wide b<strong>and</strong>width (approximately 40% versus 15% for a<br />

branch-line approach).


Article 2 (<strong>90</strong>deg)<br />

The absence of S-parameter information in low temperatures precluded the design of a<br />

feedback amplifier, so a <strong>balanced</strong> configuration was adopted. This has the advantage of<br />

providing a good input match even though the amplifiers in the two arms of the <strong>balanced</strong><br />

circuit are poorly matched. However, there are disadvantages. The loss of the input hybrid<br />

degrades the noise temperature <strong>and</strong> coupling errors in the hybrids, <strong>and</strong> differences between<br />

the amplifiers reduce the gain <strong>and</strong> result in a noise contribution from the input load.<br />

Article 3 (Narda <strong>90</strong>° Hybrids)<br />

A <strong>90</strong>° Hybrid (Hybrid Junction) is a network having the<br />

electrical characteristics of a 3 dB directional coupler<br />

whose branch line is not terminated. The four terminal network<br />

can be considered to have two pairs of terminals<br />

called conjugate pairs. In most packages, each conjugate<br />

pair is located on either side of the device (Figure 1). The<br />

two terminals that make up the conjugate pair are isolated<br />

from each other. Therefore, power flowing into one terminal<br />

of the pair does not appear at its conjugate, but is<br />

equally divided between the terminals of the opposite conjugate<br />

pair. When used as a power divider, any one of the<br />

four terminals can be used as the input. With the conjugate<br />

port of the input terminated in 50 ohms, the two outputs<br />

at the opposite conjugate pair will be of equal<br />

amplitude <strong>and</strong> in quadrature (<strong>90</strong>° apart in phase).<br />

The primary advantage of the hybrid junction is its power<br />

h<strong>and</strong>ling capability. Since the isolated port (conjugate of<br />

the input port) is terminated externally, the only limitations<br />

to power h<strong>and</strong>ling are heat generated by the internal dissipation<br />

losses <strong>and</strong> the power h<strong>and</strong>ling capability of the external<br />

termination. As stripline losses are typically low,<br />

hybrid junctions can be designed to h<strong>and</strong>le up to 500<br />

Watts average power in special versions. Another advantage<br />

of the hybrid junction is that it maintains its quadrature<br />

relationship over the full operating frequency range of<br />

the device. This characteristic is highly desirable in Polar<br />

Frequency Discrimination <strong>and</strong> Circularly Polarized antenna<br />

circuits.<br />

Article 3<br />

The <strong>90</strong>o Balanced Hybrid<br />

Coupler consists of two 50 strip lines<br />

arranged to be mutually coupled. The strip<br />

lines are made in various ways including PC<br />

board traces, copper or brass strips placed<br />

between high dielectric insulation materials.<br />

A signal applied to the Port 1 & 2 line will be<br />

coupled to Ports 3 & 4. Since the lines are<br />

electrically ¼ wavelength long the currents <strong>and</strong><br />

voltages are changed in phase between Ports<br />

1 & 2 <strong>and</strong> Ports 3 & 4. Forward loss is 3 dB<br />

plus incidental conducted losses.<br />

Note that this places Ports 1 & 3 <strong>and</strong> Ports 2<br />

& 4 at 180o in phase relationship. If a signal is<br />

applied to port 1 <strong>and</strong> Port 4 is terminated with<br />

a 50 load termination the applied power will


e equally split between Ports 2 & 3.<br />

Conversely, power applied to Ports 2 & 3 will<br />

be split between Port 1 <strong>and</strong> the termination at<br />

Port 4.<br />

With this device two transmitters can be<br />

coupled to a common antenna. All<br />

impedances will be matched <strong>and</strong> a high order<br />

of isolation is provided between the transmitter<br />

P.A. circuits, at least 30 dB for the hybrid<br />

coupler alone.<br />

The strip lines are transposed at one end to<br />

facilitate the best chassis layout for a Hybrid –<br />

Ferrite transmitter combiner. Note that the T1<br />

<strong>and</strong> T2 input connectors are on the same side<br />

of the hybrid ho<strong>using</strong>. We have also included<br />

a network at the antenna port that when<br />

properly adjusted, will produce more than 65<br />

dB of isolation between the T1 <strong>and</strong> T2 input<br />

ports.<br />

The <strong>Wilkinson</strong> Splitter employs two 70 <br />

sections of line, each ¼ wave length. Each<br />

line will produce a phase change of <strong>90</strong>o<br />

resulting in a 180o phase relationship between<br />

Ports 1 <strong>and</strong> 2. The 100 terminating resistor<br />

provides an effective match at the isolated<br />

ports <strong>and</strong> the conjunctive impedance of the<br />

two 70 lines in parallel is 50 at Port 1.<br />

<strong>Wilkinson</strong> Splitters are mostly used for dividing<br />

signal power to feed a number of devices from<br />

one source. One example (Figure 3) is an 8-<br />

way signal power divider for receiver<br />

multicoupling service. Of course, it works in<br />

reverse, to combine low power transmitters,<br />

provided that the 100 termination resistors<br />

<strong>and</strong> related heat sinks are capable of<br />

dissipating ½ of all power applied to the inputs.<br />

Insertion loss is 3 dB plus conducted circuit<br />

losses <strong>and</strong> isolation is usually 25 dB or better<br />

between ports.<br />

Article 4 (wikipedia)<br />

<strong>90</strong> deg. The phase difference between the two output ports of a hybrid coupler should be 0,<br />

<strong>90</strong>, or 180 <strong>degrees</strong> depending on the type used. However, like amplitude balance, the phase<br />

difference is sensitive to the input frequency <strong>and</strong> typically will vary a few <strong>degrees</strong>.


The phase properties of a <strong>90</strong>-degree hybrid coupler can be used to great advantage in<br />

microwave circuits. For example in a <strong>balanced</strong> microwave amplifier the two input stages are<br />

fed through a hybrid coupler. The FET device normally has a very poor match <strong>and</strong> reflects<br />

much of the incident energy. However, since the devices are essentially identical the<br />

reflection coefficients from each device are equal. The reflected voltage from the FETs are in<br />

phase at the isolated port <strong>and</strong> are 180 <strong>degrees</strong> different at the input port. Therefore, all of the<br />

reflected power from the FETs goes to the load at the isolated port <strong>and</strong> no power goes to the<br />

input port. This results in a good input match (low VSWR).<br />

<strong>Wilkinson</strong>. The <strong>Wilkinson</strong> power divider has low VSWR at all ports <strong>and</strong> high isolation<br />

between output ports. The input <strong>and</strong> output impedances at each port are designed to be<br />

equal to the characteristic impedance of the microwave system.<br />

Article 5<br />

A <strong>balanced</strong> amplifier design is defined by two amplifiers of equal gain, 1dB compression point<br />

(P1dB) <strong>and</strong> Third-Order Intercept (IP3), arranged in the configuration shown to the right. The<br />

couplers are 3 dB hybrids, where the input power is split equally between a 0°<strong>and</strong> a <strong>90</strong>° port.<br />

The unused ports are terminated in the system impedance – typically 50 Ω. Reflections from<br />

the input <strong>and</strong> output ports of the amplifiers are shunted to the unused port of each coupler,<br />

giving the entire arrangement a matched impedance.


Article 6<br />

The <strong>Wilkinson</strong> power divider<br />

At higher frequencies (above 500 Mhz) these devices are usually<br />

realized as a microstrip or stripline <strong>Wilkinson</strong> design. All<br />

Browadwave reactive power dividers are <strong>Wilkinson</strong> types. Figure<br />

5 shows a simple 2-Way <strong>Wilkinson</strong> power divider. Being a<br />

lossless reciprocal three port network, it inherits all its properties<br />

which state that this type of network cannot have all the<br />

ports simultaneously matched. To solve this an isolating resistor<br />

is placed between the two output ports, since no current<br />

flows through the resistor (there is no potential difference between<br />

the output ports), this resistor does not contribute to any<br />

resistive loss. This makes an ideal <strong>Wilkinson</strong> a 100% efficient<br />

device. This resistor also provides excellent isolation even<br />

when the device is used as a combiner. Another property of<br />

the <strong>Wilkinson</strong> divider is that it is broken down into quater wavelength<br />

(l/4) sections. This device is useful for limited b<strong>and</strong>width<br />

applications, but to achieve a wider b<strong>and</strong>width a multi<br />

section <strong>Wilkinson</strong> design is used as shown in Figure 6. As a<br />

general rule, the greater the b<strong>and</strong>width the more sections<br />

added to the design. But by doing so, makes devices become<br />

larger <strong>and</strong> more importantly lossy. These devices can be designed<br />

for octave b<strong>and</strong>widths <strong>and</strong> are sometimes cascaded to<br />

form higher order devices.


Article 7<br />

Balanced amplifier


Article 8<br />

For the distributed <strong>90</strong>-deg. hybrid, there are basically four quarter-wavelength distributed<br />

transmission lines connected in a "square" arrangement (Fig. 2). Two opposite transmission<br />

lines have an impedance of 50 Ω(assuming a characteristic impedance of 50 Ω) <strong>and</strong> the other<br />

two lines have an impedance of 35.35 Ω[(50 Ω) 0.5 ]. It is very important to get the orientation of<br />

the coupler input <strong>and</strong> isolated port correct (see ref. 2).<br />

As noted previously, there are two simple lumped-element equivalent circuits in a pi or tee<br />

arrangement. Either arrangement will work, although the choice may depend on other factors:<br />

for example, MMIC inductors tend to have more loss than MMIC capacitors. By choosing the<br />

pi arrangement to reduce the number of inductors, the lumped-element circuit of Fig. 3<br />

results. Note the combining of capacitors at the "corners" of the 35- <strong>and</strong> 50-Ω branches.<br />

The branchline or <strong>90</strong>-deg. hybrid can be used for many functions. Some of these include<br />

image-reject mixers, attenuators, phase shifters, modulators, <strong>and</strong> power combiners/dividers.<br />

This is true of both the lumped element <strong>and</strong> distributed implementations of the branchline<br />

hybrid. However, the distributed equivalent will repeat at three times the fundamental<br />

frequency. Also, the b<strong>and</strong>widths of the two implementations are different near the<br />

fundamental frequency, F 0 . The input match of the hybrid is good provided the terminations at<br />

the direct <strong>and</strong> coupled ports are nearly identical. Mismatches at the direct <strong>and</strong> coupled ports<br />

reflect to the isolated port. By adding a switch or variable resistor to the direct <strong>and</strong> coupled<br />

ports of the branchline hybrid, one can create a switched or variable attenuator <strong>using</strong> the<br />

input <strong>and</strong> isolated ports. Likewise, a switch or variable capacitor can be used to build an<br />

analog or digital phase shifter or phase modulator. In an image-reject mixer, one branchline<br />

hybrid at RF helps distinguish between the upper sideb<strong>and</strong> <strong>and</strong> the lower sideb<strong>and</strong> of the<br />

signal. An additional <strong>90</strong>-deg. hybrid at the intermediate frequency (IF) combines or cancels<br />

the two mixed signals to select just the upper or lower sideb<strong>and</strong>.<br />

The hybrid can also be used as a combiner or power splitter with the properties that the input<br />

match is good provided that the loads at the coupled <strong>and</strong> direct ports are matched. As a<br />

combiner, reflections from the coupled <strong>and</strong> direct port are absorbed by a resistor at the<br />

isolated port. The difficulty with the hybrid as a combiner/divider is controlling the impedances<br />

<strong>and</strong> lengths of the 35- <strong>and</strong> 50-Ω transmission lines to obtain an equal 3-dB split at the two<br />

ports.<br />

The <strong>Wilkinson</strong> coupler is often used as a power combiner or splitter. It divides an input signal<br />

equally between two outputs, or can be used to create unequal split or an n-port divider. In a<br />

<strong>Wilkinson</strong>, two quarter-wavelength 70.7-Ω lines—assuming a 50-Ω characteristic<br />

impedance—split the input to two output ports (Fig. 4). A 100-Ω resistor is tied between the<br />

two output ports to provide isolation in the odd-mode case. Placing this resistor can be much<br />

easier in a MMIC lumped-element layout than in a distributed layout (Fig. 5). For this<br />

example, a pi arrangement was chosen to reduce the number of lossy inductors. The input<br />

shunt capacitors combine into a single capacitor yielding two inductors, one shunt capacitor at<br />

each port, <strong>and</strong> the 100-Ω isolation resistor plus interconnect for the MMIC <strong>Wilkinson</strong>.<br />

As a splitter, the input is divided into two equal in-phase outputs, ideally at −3-dB levels from<br />

the input signal level. When fed at the outputs by two signals in phase <strong>and</strong> of comparable<br />

signal level, the <strong>Wilkinson</strong> acts as a power combiner. The major differences between <strong>using</strong> a<br />

<strong>Wilkinson</strong> as a divider/combiner versus the branchline hybrid is that the input match now<br />

depends on the match at the other two ports. However, it is much easier to get an equalphase,<br />

equal-power split, as well as wider b<strong>and</strong>width, with the <strong>Wilkinson</strong> than with a hybrid<br />

combiner.<br />

A <strong>90</strong>-deg. lumped-element MMIC hybrid coupler is a useful for a variety of designs, such as a<br />

phase modulator MMIC developed by a student in the Johns Hopkins University MMIC<br />

Design Course. 3 Students in that course learn to develop practical MMIC layouts that are then


fabricated at the TriQuint Semiconductor foundry. Those students developed several lumpedelement<br />

hybrid layouts, planned around a central substrate via shared by four capacitors <strong>and</strong><br />

four spiral inductors to make up the four transmission lines of the lumped element equivalent<br />

hybrid (Fig. 6). Using the pi arrangement for the lumped-element branches <strong>and</strong> combining the<br />

capacitors at the ends, the layout has a single capacitance value <strong>and</strong> two inductance values<br />

that can be tuned for performance. Arranging the layout allows performance trade-offs by<br />

tuning the single capacitance <strong>and</strong> the size of the two inductors. Careful use of symmetry<br />

makes it easier to tune the circuit without "breaking" the layout. A 2.1-GHz hybrid coupler<br />

fabricated on a 34 × 54 mil die is an example of the several hybrid couplers fabricated with<br />

the TriQuint process (Fig. 6). Hybrid couplers for other frequency ranges can use the same<br />

topology by changing the capacitor <strong>and</strong> two inductor values (plus interconnect).<br />

The performance of the hybrid coupler was simulated (Fig. 7) with the Advanced Design<br />

System (ADS) software from Agilent Technologies <strong>and</strong> the TriQuint TQTRX device library, as<br />

well as with EM simulation software from Sonnet Software (Liverpool, NY). Only the "core" of<br />

the hybrids were simulated <strong>and</strong> assumptions were made that the effects of the ground-signalground<br />

probe pads <strong>and</strong> off-chip wire bonds were minimal at these frequencies. Given<br />

additional time, the matches can be tuned to offset the off-chip wire bond inductance <strong>and</strong><br />

provide a better 50-Ω termination.<br />

A 7.5-GHz <strong>Wilkinson</strong> divider/combiner was also fabricated with the MMIC process. It consists<br />

of two 71-Ω transmission lines <strong>and</strong> a 100-Ω resistor to provide isolation for the coupled ports.<br />

Symmetry was used to ensure proper equal phase <strong>and</strong> equal amplitude split. The hybrid pi<br />

lumped-element equivalent was chosen for the MMIC implementation since it has the least<br />

number of lossy inductors. Capacitors on the input side can be combined resulting in one<br />

value for the two inductors <strong>and</strong> two values for the three capacitors—the first capacitor is twice<br />

the value of the other two. Optimizing the simulation is done by tuning the one inductor value<br />

<strong>and</strong> "one" or "two" capacitor values. A single shared substrate via was used for the shunt<br />

capacitor to ground connections. The <strong>Wilkinson</strong> was also computer simulated, although the<br />

ADS simulations did not include the isolation resistor in the layout because its effect was<br />

considered to be minimal. The layout for the 7.5-GHz X-b<strong>and</strong> <strong>Wilkinson</strong> looks similar to half of<br />

the hybrid coupler layout (Fig. 8). The 100-Ω isolation resistor was added to the layout along<br />

with the ground-signal-ground probe pads in the final layout <strong>using</strong> the ICED layout software.<br />

The 7.5-GHz <strong>Wilkinson</strong> measures 34 × 29 mils, <strong>and</strong> measured performance compared<br />

closely with ADS <strong>and</strong> EM simulations (Fig. 9). Various branchline hybrids from 2.1 to 8.4 GHz<br />

were all fabricated on a 34 × 54 mil MMIC tile with room to spare. The higher-frequency<br />

hybrids had some additional room for test circuits. Of course, the great advantage of MMICs<br />

over MICs is size, <strong>and</strong> a quarter wavelength on an alumina substrate (dielectric constant of<br />

9.8), for example, is almost 600 mils. If one needs to incorporate additional circuits such as<br />

switches, varactors, diodes, FETs, etc., the size, weight, <strong>and</strong> power savings of a MMIC over<br />

an MIC circuit can be substantially higher, although for small volumes, MICs still offer cost<br />

advantages compared to the high price of a MMIC wafer run.

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