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REAL
TIME AMPLIFIER NOISE MEASUREMENT
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| AMPLIFIER
SPECIFICATION TCI P/N 905-A2 |
|
| FREQUENCY RANGE | 9.0 to 11.0 GHz |
| SMALL SIG. GAIN | 24 dB min. 28 dB max. |
| GAIN FLATNESS | ±.5 dB @ 25°C |
| GAIN VARIATION | |
| OVER TEMPERATURE | ±.5 dB |
| NOISE FIGURE | 5 dB max. |
| P1dB (dBm) | 24 dBm min. |
| PM NOISE @ 10 KHz | -165 dBc/Hz max. |
| AM NOISE @ 10 KHz | -153 dBc/Hz max. |
| INPUT POWER HANDLING | +20 dBm max. CW |
| VSWR (:1) | 2/2 i/o |
| OPERATING VOLTAGE | +12 VDC |
| OPERATING CURRENT | < 500 ma |
| SPEC. TEMPERATURE | -20°C to +70°C |
| CONNECTORS | DC
- Solder Pin RF IN - SMA (F) RF OUT - SMA (F) |
The AM noise
was measured to evaluate the performance of the amplifiers. In most cases,
amplifiers are specified for PM noise. The PM noise, however, has been
found to be a direct result of deficient AM noise performance. AM to PM
noise conversion within the amplifier is the primary factor which results
in the lacking performance of the amplifier. Under gain compression, amplifiers
exhibit useful noise signatures, which can be used to determine the causal
effect reducing amplifier performance. Semi-conductor selection, bias
configuration and level, inter stage matching, and voltage regulator noise,
to name a few factors, can all effect amplifier performance. A block diagram
is shown in Figure 1.
AM and PM
REAL TIME NOISE MEASUREMENT
USING THE 3712 SYSTEM ANALYZER

Figure 1—Block Diagram
AM and PM noise can be measured using the 3712 Real Time Noise Measurement System. The noise measurement system provides results with a ±1.5 dB repeatability and accuracy. The incorporation of the TCI model NAL2000 allows rapid calibration of the PM phase discriminator and AM detector. Calibration of the measurement system includes all components of the measurement system unlike other noise measurement systems which exclude the low noise amplifier used to bring the base band noise up to a level which can be measured by a spectrum analyzer.
It is important to understand that several types of noise and several different sources of noise comprise the resulting noise signature of an amplifier. In this case, the term noise signature refers to the AM, PM and spurious noise components. The noise generated within the amplifier is termed its additive or residual noise. If a carrier whose noise signature is higher than that of the amplifiers residual noise, the signal will pass through the amplifier with little or no effect to its noise signature. The noise factors which are involved in the noise signature of a carrier passing through an amplifier are:
| PM Noise of the Carrier | (NOISE SIGNATURE INPUT) |
AM Noise of the Carrier |
|
| Amplifier Residual PM Noise | (AMPLIFIER NOISE) |
Amplifier Residual AM Noise |
|
Amplifier Spurious Components |
|
Resulting PM Noise |
(NOISE SIGNATURE OUTPUT) |
Resulting AM Noise |
|
Resulting Spurious Components |
|
The Input
and Output PM and AM noise to the amplifier are measured using an absolute
noise measurement technique. Where extremely low PM noise is required,
two carrier sources are used to make the PM noise measurement. AM noise
is measured from only one carrier source. If a single carrier source is
used to measure PM noise, such as is shown in Figure 1, a residual noise
measurement will result. The carrier source PM noise is canceled in the
phase discriminator with only the residual noise of the amplifier being
measured. The phase discriminator acts to cancel both carriers which are
fed into it and base band noise from the discriminator results. Using
this process effectively converts the small phase noise fluctuations into
voltage fluctuations which can then be measured with a low frequency spectrum
analyzer.
AM noise is a different issue. Only one carrier source is measured using
a detector diode and therefore carrier cancellation can not be used. As
a result, only absolute AM noise can be measured. Additive or residual
noise can only be determined by subtracting the output AM noise results
from the input AM noise. If a carrier source which has lower noise than
the amplifier residual noise is used as an input signal to the amplifier,
the inherent residual noise of the amplifier can be determined. The AM
noise measurement technique is however, the same.
The 3712 is a Real Time Measurement System which allows very accurate
and rapid measurement of residual PM and absolute AM noise. Amplifiers
can be monitored while changes are made to them. Within a few seconds
of turning an amplifier on for the first time, its performance can be
determined. With signature identification techniques, corrections take
minutes.
Even though each amplifier engineer designs uses different design techniques
and components, there are a limited number of additive noise signature
types. With a sampling of many amplifier manufacturers, it has been found
that the noise personality of each manufacturer is different. Semi-conductor
selection is another critical issue for extremely low noise amplifiers.
Again it has been found that not every semi-conductor is useable, even
from the same lot. The 3712 Real Time Measurement System provides a platform
to select usable semi-conductors very quickly.
Several frequency configurations of the 3712 Real Time Measurement System
are available. The system can be supplied with or without a low frequency
spectrum analyzer.
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