Noise parameter
extraction using source pull
Updated
August 27, 2005
New for September 2005!
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Here is an index to the page
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Definitions
of load pull versus source pull
Types
of microwave tuners (separate page)
Why source-pull
a low noise device?
Noise
parameters: Gamma Opt, Fmin and RN
Source pull bench block diagram
(coming soon)
Definitions
of load pull versus source pull
Microwaves101 convention:
When we're talking about the process of load pull or source pull
as nouns (or adjectives like "load pull bench") we won't
hyphenate. When we're telling you to load-pull or source-pull something
(verbs), we'll hyphenate. Just so you know.
Load pull: the process
of varying the impedance seen by the output of an active
device to other than 50 ohms in order to measure performance parameters,
in the simplest case, gain. In the case of a power device, a load
pull power bench is used to evaluate large signal parameters such
as compression characteristics, saturated power, efficiency and
linearity as the output load is varied across the Smith chart.
Harmonic
load pull: the process of varying the impedance at the output
of a device, with separate control of the impedances at F0, 2F0,
3F0, etc. A very tricky measurement!
Source pull: the process
of varying the impedance seen by the input of an active device
to other than 50 ohms in order to measure performance parameters.
In the case of a low noise device, source pull is used in a noise
parameter extraction setup to evaluate how signal-to-noise ratio
(noise figure) varies with source impedance.
In practice, power benches employ
both load and source pull, and noise parameter setups employ both
as well, but the emphasis is on one or the other. In power measurements,
the input is source-pulled to a single location that provides good
power gain, while the output is swept all over the Smith chart.
In noise parameter extraction, the output is load-pulled to an impedance
that provides good gain, then the input is swept all over the Smith
chart.
Microwave
impedance tuners are the "engines" that let you drive
all over the Smith Chart.
Why source-pull
a low noise device?
The performance of a low noise
device is a function of many things:
- Frequency
- Bias point
- Temperature
- Source impedance
- Device geometry (number gates,
gate width, etc.)
When you measure noise figure
on a noise figure meter or noise parameter analyzer, you typically
evaluate signal-to-noise ratio (noise figure) while restricted to
a fifty-ohm system. At the device level, your low noise transistor
is not going to give you the best response at fifty ohms. Measuring
noise parameters using source pull is what is used to empirically
gather all of the data you need to design a low noise amplifier,
starting from the device level.
Noise
parameters
It turns out that signal-to-noise
ratio of a device is one of those "magic parameters" that
are exactly described by circles of constant value on the Smith
chart (much like small-signal gain). Contrast this with power amplifier
responses such as contours of constant maximum efficiency, which
are more generally described as "potatoes".
Once you have the noise parameters
in hand using linear CAD software you
can mathematically calculate the signal-to-noise response if the
device sees impedances other than fifty ohms. Noise parameters are
can be very accurate, if they are measured carefully.
There are three things that you
are after when you measure noise parameters (four if you consider
that gamma opt is a vector and has a real and imaginary part). Remember,
the three noise parameters are functions of bias point, frequency
and temperature, and of course, device geometry.
Gamma
Opt
Gamma opt is the optimum impedance that must be presented to
a low noise device to achieve its lowest possible noise figure.
Fmin
Fmin is the minimum noise figure of a device, and it is only achieved
at gamma opt.
RN (equivalent
noise resistance)
RN gives an indication of how fast the noise figure of a device
degrades when it's input is matched to other impedances beside gamma
opt. Lower RN is always desirable, it is a measure of the slope
of noise figure versus impedance.
More to come!
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