Model 5209
High Performance Single Phase Analog Lock-in Amplifier

The SIGNAL RECOVERY model 5209 is the
benchmark single-phase lock-in amplifier against which others are judged.
It is widely referenced in technical publications describing a diverse
range of research applications including optical, electrochemical,
electronic, mechanical and fundamental physical studies. We also offer a
dual-phase version, the model 5210.
Although the introduction of instruments using digital signal
processing has brought advances in phase sensitive detection techniques,
units using analog demodulators are still the first choice for many
experiments. These include those requiring a true analog output, for
example in some feedback control loops, or where the instrument is used to
recover the envelope modulation of a "carrier" frequency. Of
course, they are also chosen for compatibility with previous experimental
setups.
Voltage or current inputs...
The instrument includes a current preamplifier with two
transimpedance settings and so can directly measure signals from current
sources such as photodiodes. With an input impedance of down to typically
only 25 Ω the resulting voltage generated across the source by the
signal current is minimized for the very best performance.
Continuous full-scale sensitivity control...
As with all lock-ins the model 5209 has a range of calibrated full-scale
sensitivity settings. However, unlike other units it also has a
sensitivity vernier control, allowing the full-scale sensitivity to be set
to any value between the calibrated values. Suppose you are performing an
optical transmission experiment and you want to measure transmission in
terms of a percentage relative to that of a "reference" sample.
All you need to do is put the reference sample in the optical path and
press the auto vernier control on the lock-in. It will then adjust the
sensitivity so that the display reads 100%. Now replace the reference
sample with the test sample and read the percentage transmission directly.
Unique Walsh Function Demodulators...
The simplest method of implementing the phase sensitive detector
at the heart of an analog lock-in is with a reversing switch driven at the
reference frequency, giving excellent linearity, dynamic range and
stability. This is known as a "squarewave" demodulator since the
instrument responds to signals not only at the reference frequency but
also at its odd harmonics. It offers much better performance than can be
achieved by using a true analog multiplier, which requires the synthesis
of a very pure reference sinusoid and is very non-linear when handling
large levels of interfering signal.
Squarewave demodulation is ideal for many applications, such as
experiments using chopped light beams where the signal being detected is a
square-wave, since the odd harmonics contain useful information. However
in other cases the requirement is for "sinewave" or
"fundamental" response where only signals at the reference
frequency are measured.
In theory, a squarewave can be modified to a sinewave response by
inserting a low-pass or bandpass filter in the signal channel ahead of the
demodulator. However this requires a highly selective filter in order to
reject signals at the third harmonic without at the same time causing
significant phase and magnitude errors for signals at the reference
frequency.
The model 5209 uses a modified form of switching demodulator, known as
the Walsh demodulator, which multiplies the applied signal by a stepped
approximation to the reference sinusoidal waveform. This gives a
demodulator that does not respond to signals at the third and fifth
harmonics, although it does respond to higher harmonics. A fourth-order
signal channel filter is therefore included to reject these harmonics,
giving a overall sinewave response. The advantages of the switching
demodulator are thereby retained without the phase and magnitude errors
associated with the use of highly selective filters.
The instrument can be switched to operate in either sinewave or
squarewave mode, giving you the choice of the optimum detection method for
your experiment. Only SIGNAL RECOVERY gives you
this flexibility.
Choice of signal channel filter modes…
In the usual sinewave response mode, the filter is set to the
bandpass or low-pass modes. But what if you are trying to measure a signal
at twice the reference frequency in the presence of a strong signal at the
reference frequency? In this case, the filter can be set to a notch
(band-stop) mode and tuned to the reference frequency, leaving the signal
at 2F unattenuated and easy to measure.
In addition to the main signal channel filter, a line-frequency
rejection filter operating at 50/60 Hz and/or 100/120 Hz is also
included, for elimination of troublesome line pickup.
High dynamic reserve...
The combination of the Walsh demodulator(s) and the signal
channel filter gives the instruments a dynamic reserve of up to 130 dB
- implying that you can, for example, measure a signal of 1 µV in
the presence of an interfering signal of more than 1 V. No other
analog lock-ins deliver this performance.
Output filters...
The output low-pass filters offer time constants in the range 1 ms
to 3 ks, with all settings available at slopes of both 6 and 12 dB/octave.
In addition, the units include a rear-panel output giving the signal at
the output of the demodulator with a time constant of typically only 100 µs,
for use in those applications such as tandem demodulation where the
largest output bandwidth is required.
Synchronous ADC trigger...
The analog outputs from the demodulator, after filtering by
the output low-pass filter, needs to be digitized by an analog to digital
converter (ADC) for display or for transfer to the controlling computer.
If this conversion is carried out asynchronously then the resulting values
can display significant jitter. This is because the demodulator output
contains not only the required DC level, but also signals at twice the
reference frequency. When the output is sampled for conversion, this 2F
signal means that some samples will be smaller and some larger than the
mean.
Of course, the 2F component can be reduced to any arbitrarily small
value by increasing the time constant, but this reduces the response time
to changes in input signal, slowing down data throughput. The model 5209
therefore offers a unique reference synchronous ADC trigger mode, which
guarantees that the output is sampled at the same point relative to the
reference waveform and thereby removes this source of error.
Internal oscillator...
With the model 5209 there is no need to buy a separate oscillator to use
as an excitation source for your experiment, since it includes one capable
of generating a low distortion sinewave output signal over a frequency
range of 0.5 Hz to 120 kHz. Although in most lock-ins the
frequency of the internal oscillator can be adjusted, in this instrument
the amplitude can also be controlled over the range 1 mV to 2 V
rms.
Manual or computer control...
In manual operation the backlit control setting indicators, the
two digital displays and the analog panel meter makes the instrument very
easy to use, with the settings of all the important controls being
instantly visible. Six auto functions further simplify control adjustment,
while red overload and reference unlock LEDs warn of conditions which will
result in measurement errors. All the front panel indicators can be turned
off for use in blackout conditions.
The instrument includes GPIB (IEEE-488) and RS232 computer interfaces,
allowing virtually all the controls to be operated, and all the outputs
that can be displayed to be read, via simple ASCII mnemonic-type commands.
The communications interface parameters, such as baud rate and GPIB
address are set by front-panel controls, with no difficult DIP switches to
adjust.
Compatible LabVIEW drivers are available for those researchers working
in that environment while the unit is also supported by the SRInstComms
ActiveX control and SDK. It can also be used with our Acquire™ data
acquisition software package, which allows non-programmers an easy way to
log the instrument outputs to a PC file. The
LabVIEW driver and a demonstration version of the software, DemoAcquire,
are available for download from this site.
Specifications
| Input |
|
|
| Mode |
|
|
|
Voltage |
Single-ended or true
differential |
|
Current |
Virtual ground |
| Sensitivity |
|
|
|
Voltage |
10 nV to 3 V (with output
expand) |
|
Current |
10-6 A/V, 10-8
A/V conversion |
| Impedance |
|
|
|
Voltage |
100 MΩ // 25 pF |
|
Current |
25 W (10-6 A/V) |
| Noise |
|
|
|
Voltage |
5 nV/√Hz at 1 kHz |
|
Current |
13 fA/√Hz (10-8
A/V) at 1 kHz |
| C.M.R.R. |
|
120 dB at 1 kHz |
| Frequency
Response |
0.5 Hz to 120 kHz |
| Dynamic
Reserve |
130 dB (max) |
| Detection |
|
|
|
Phases |
1 |
|
Modes |
F, 2F |
| Output |
|
|
|
Modes |
X (%): X (V): Noise |
|
Time constant |
100 µs, 1 ms to 3000 s |
|
Roll-off |
6 or 12 dB/octave |
|
Voltage |
10 V FS |
|
Impedance |
1 kΩ |
| Oscillator |
|
|
|
Voltage |
0 to 2 V rms (1 mV steps)
0 to 5 V rms (software only) |
|
Frequency |
0.5 Hz to 100 kHz |
|
Impedance |
1 kΩ |
| Auxiliary
Control |
4 ADC, 2 DAC |
| Interface |
|
RS232, GPIB (IEEE-488) |
|