MRC Compact Laser Beam Stabilisation System User Manual
- June 9, 2024
- MRC
Table of Contents
- General
- System components
- Specification
- Optical components
- Installation and operation
- Operation and safety features
- Option: Sample&hold circuit (“ADDA“)
- Option: Serial interface (USB, RS-232 or Ethernet)
- Additional inputs and outputs (Options)
- Drawings
- Cables
- Troubleshooting
- Safety
- References
- Read User Manual Online (PDF format)
- Download This Manual (PDF format)
Laser Beam Stabilisation System
Compact
User Manual
General
The Compact laser beam stabilisation compensates for vibrations, shocks,
thermal drift, or other undesired fluctuations of the laser beam pointing. The
system should be applied whenever laser fluctuations or movements of optical
components occur but a high precision and stability of the beam position and
angle is required.
The desired position of the laser beam is defined by a position detector (4
-quadrant-diode (4-QD) or PSD). For that purpose a small portion of laser
power transmitted through a high-reflective deflection mirror (“leakage”) is
sufficient.
The closed-loop real-time control continuously determines the deviation of the
laser beam from the desired position and drives the fast Piezo actuators in
that way that the steering mirrors stabilise the laser beam in the desired
position.
The 4-axes system combines two pairs of detectors and steering mirrors in
order to stabilise the laser beam in 4 degrees of freedom (4D, position and
angle). The 2-axes system uses only one such pair. It stabilises either the
beam position at exactly one point or – if e.g. the detector is placed into
the focus of a lens – the beam angle.
System components
The laser beam stabilisation utilizes the control electronics and the optoelectronic components (steering mirrors, detectors). The following figures show the standard components. Beyond these, we offer various types of steering mirror mounts with Piezo actuators and detectors. For more details please check the specification in sections 3 and 4.
Figures 2, 3, and 4 (from left to right): Steering mirror with Piezo drive
(version P2S30), detector with position and intensity display (horizontal
orientation), detector (vertical orientation)
The system electronics (controller, amplifiers, power supplies) is fully
integrated into a single compact housing. It is powered by a standard 12 V
wall power supply.
Specification
You can find detailed data sheets of the different components of the beam
stabilisation system on our website. We can also send them to you. The
following table shows an overview:
Optical parameters
Wavelength| 320 to 1100 nm, UV and IR detectors are also available any rate or
cw
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Repetition rate| For lasers with low repetition rates (< 1 kHz), with single
pulses or with laser off-times we offer an additional sample & hold circuit,
see also note 1
Laser beam diameter| < 6-8 mm (1/e²), see also note 2
Height of laser beam| 40 mm for P2S30 and P4S30,
45 mm for PKS, 39.5 mm for PSH
Mirror diameter| P2S30: 1” (standard)
P4S30: 1”, 1.5”, 2” and other mirror diameters
Mirror thickness| 1/4″ or 1/8″ (recommended)
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Controller housing dimensions
w x h x d| 166 x 106 x 56 mm3
Control features
Power level display| LED line with 10 elements on the backside of the detector
Position display| LED cross on the backside of the detector
Variable intensity gain| Continuous, adjustable with potentiometer (1:6)
Low power switch-off| Power level falls below 10% of saturation power
Switch on activity delay| 300 ms
Computer interface
Options | USB, RS-232 or Ethernet |
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Connectors at controller unit
Actuator| LEMO 0S series
Detector| LEMO 0B series
Controller status signal (interlock)| LEMO 00 series
x, y position output| LEMO 00 series
P factor setting and read-out| LEMO 00 series
Power supply| 12 V / DC pin-and-socket connector
Notes:
- A description of the sample & hold circuit is given in section 7 of this user manual.
- If the beam diameter is larger than 8 mm, a lens in front of the detector can be used. Please refer to the description “Optimisation of the setup with lenses” on our website for details.
3.1. Positioning accuracy
The positioning accuracy depends on several parameters:
• Optical distance between steering mirror and detector: The accuracy is
higher for larger distances. Therefore a large distance should be chosen.
• Beam diameter: Having the same absolute change of laser beam position, a
smaller diameter leads to stronger power differences on the quadrants of a
4-QD and therefore a steeper control signal. That is why laser beams with
smaller diameter can be positioned with higher accuracy.
• Intensity: The resolution of the detectors further depends on the intensity
hitting the sensitive area. However, this can be varied by optical filters and
optimised electronically (see section 5.4).
• Repetition rate and pulse duration: The controller bandwidth can be
optimised for different laser parameters. Higher bandwidths lead to a faster
reaction and therefore higher accuracy in case of fast fluctuations.
Note: The system uses the centre of the transversal laser beam profile.
It does not reduce fluctuations of the laser beam profile itself.
The position signals of the detectors can be read out at the front panel of
the controller.
Position outputs x, y
Description| 4 outputs: beam position (stage 1 and stage 2)
Signal| Analog, – 5 V … + 5 V
Connectors| LEMO 00 series
Figure 8 shows the typical resolutions of the 4-quadrant detectors. The example demonstrates that a resolution of better than 100 nm on the detectors can be achieved with an appropriate choice of parameters. The angular resolution can be determined from these data with respect to the respective arm lengths.
Figure 8: Resolution of a 4-quadrant diode irradiated by a red He-Ne laser
with different beam diameters and laser intensities
By the use of the material Invar with a very low coefficient of thermal
expansion the detectors are stabilised against temperature variations which
ensures that the accuracy is maintained over long term.
The actuators are controlled with an analog signal so that the positioning is
not restricted to separate steps. The positioning accuracy of the Piezo
elements is in the range of a few nrads.
3.2. Relation between measured voltage and actual position
The position signals are given as voltages. The following formulas allow to
convert the voltages into actual positions.
4-quadrant detector
For the calculation, the beam diameter must be determined first. Then the
deviations of the positions in µm can be approximated with the following
formula which is valid as long as the beam is near to the centre of the
4-quadrant diode:
Where x is the x position signal measured in volts or calculated in µm. The
same calculation can be made for y. D is the Gaussian beam diameter (1/e ) and
I is the measured intensity signal. For a more precise calculation or if the
beam is further away from the centre, the following formula can be used. Here
erfinv() is the inverse error function:
In case of non-Gaussian beams or to obtain the exact relation, you have to
perform a calibration by means of a micrometer stage.
PSD detector
In case of PSDs the relation between voltage and position is almost linear.
Here you can use the following ratio (similarly for y):
You can find further information on the calculations in the description “Position and angular accuracy” on our website.
Optical components
In this chapter we summarize some essential properties of the optical
components of the beam stabilisation. More detailed information can be found
in the respective data sheets.
4.1. Steering mirror mounts
Specification | P2S30 | P4S30 |
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Tilting range
Coarse adjustment (manually) Piezo stacks
High resonant frequencies High stabilisation bandwidths
Mirror sizes
Free aperture for beam transmission| 2 mrad (± 1 mrad) mechanical,
4 mrad optical ± 4.5°
2 integrated Piezo stacks up to 1,200 Hz ~ 400 Hz (with 1” mirror) 1 inch 12 x
12 mm2| 4 mrad (± 2 mrad) mechanical,
8 mrad optical ± 4.5°
4 integrated Piezo stacks
1,200 Hz (with 1” mirror)
~ 300 Hz (with 2” mirror)
400 Hz (with 1” mirror)
100 Hz (with 2” mirror)
1, 1.5, 2 and 3 inches
Notes:
- The movable top plate of the Piezo elements is sensitive to mechanical forces. Please avoid the impact of strong forces or torsional moments on it. The Piezo stacks are attached to this plate.
- If you intend to remove a mirror adapter you should be especially careful. We can provide a specific instruction and a tool for this purpose.
4.2. Detectors
4.2.1. 4-quadrant detectors
Specification| vis 4-QD (silicon)| UV 4-QD 3×3 (enhanced
silicon)| IR InGaAs 4-QD| IR Germanium 4-QD
---|---|---|---|---
Wavelength range
Sensitivity range Element gap| 320 – 1.100 nm
10 x 10 mm2
30 µm| 190 – 1.000 nm
3 x 3 mm2 100 µm| 900 – 1.700 nm
Ø = 3 mm 45 µm| 800 – 2.000 nm
5 x 5 mm220 µm
Sensitivity range
Damage threshold| 10–165 μW / 3-55 nJ @ 532 nm cw (adjustable with gain
potentiometer and optical filters) limited by optical filters – typical
values:
Max. absorbed power: 0.05 – 0.1 W for Ø=1mm, 0.2 – 0.4 W for Ø=3mm
Max. absorbed energy: 1-5 µJ for Ø=1mm, 5-20 µJ for Ø=3mm
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Dimensions
Housing (w x h x d)| 40 x 49.5 x 23.9 mm3
Optical filter| 11.9 x 11.9 mm2
Further functions
Power indication| LED line with 10 elements on the backside
Position display| LED cross on the backside
Connectors
x, y, intensity outputs Power supply| MCX
| 12 V / MCX
4.2.2. Wide intensity detector – 4-quadrant diode with wide intensity range
Specification
Dynamics / Intensity range| 3 decades
Bandwidth| < 10 kHz
Signal scaling| 9 mV / µm (typical for 1 mm beam diameter)
Sensitivity range| ~ 5 µW – 5 mW (@ 532 nm, cw)
Reproducibility over the complete intensity range| 10 mV (with 1 mm beam
diameter ~ ± 1 µm)
All other specifications are the same as those of the standard 4-quadrant
detectors.
Notes:
- For the wide intensity detector, the function of the intensity display is unchanged. It can still support the selection of the filters. The potentiometer described in section 5.4, however, is omitted.
- Due to the wide intensity range it is possible to detect even lowest laser powers. That is why, de pending on the selection of the optical filters, the detection can be affected by ambient light.
4.2.3. PSD detector
Specification | VIS PSD |
---|---|
Wavelength range | 320 – 1,100 nm |
Sensitive area | 9 x 9 mm2 |
In contrast to the 4-quadrant diode the PSD has a continuous measurement area.
Notes:
- If we equip the beam stabilisation with PSDs but no further measures, we use the electronic centre (defined by a voltage of 0V for x and y position) as the target position.
- The position vs. voltage characteristics of a PSD is usually not linear. This means that a pincushion distortion occurs when the beam is sweeping the complete sensor area. I.e. the expected position value can deviate minimally from the voltage value. Therefore, we recommend performing a calibration if the target shall be moved along a defined path.The absolute accuracy at a stabilized position is not affected.
4.3. Vacuum adaptions
Both, the detectors and the actuators, can be adapted for use in vacuum. In
case of the actuators, this is possible for vacuum pressures down to 10 mbar.
But this is an extreme value. In case you intend to place some components in
vacuum please let us know the conditions so that we can discuss and suggest
the required measures. Some measures (choice of materials, cables, sealing)
are mainly focussed to avoid degassing and depend on the pressure. Others are
important to protect the components themselves.
Notes:
- The controller itself should not be placed in vacuum.
- The vacuum compatible detector does not have the LED displays on the backside. That is why additional intensity outputs are integrated into the control box.
4.4. Optical filters
We usually integrate a pair of optical filters in front of each sensor. They
have a size of 11.9 x 11.9 mm2 and fit into the provided slot in the detector
housing. The filter which is further inside is optically denser.
Installation and operation
A quick installation guide is part of the scope of delivery. It explains how
to start up the beam stabilisation. If you no longer have this guide, you can
download it from our website or ask us to send it. In the following sections,
we explain individual steps in more detail.
The system operation can be described best with reference to figures 5 to 7.
The top panel in figure 5 shows the keyboard and the position signal outputs
for two pairs of detectors and actuators (stage 1 and stage 2). Each stage can
be started and stopped independently by pressing the Start/Stop button. When
the stage is started the small LED in the top right corner of the button is
shining. The Range display shows whether or not the steering mirrors are
within the available capture range. The Active LED is shining whenever the
control stage is active. This is the case whenever the Start/Stop button has
been pressed and the laser power on the detectors has the right level.
The Position outputs on the top panel can be used to read out the current
position of the laser beam on each detector (x and y).
Notes:
- Whenever the Start/Stop button is pressed (and the Active LED is on) the actuators start to move from the zero position and then respond to the controller input.
- If a Range LED is shining red, this does not automatically mean that the beam is not stable. But it indicates that no further tilt of the respective steering mirror is possible although it might be necessary.
- If the power on the detectors is too low the actuators are driven to the zero position (and the Active LED is off). This is due to the low power switch off that was implemented for safety reasons (see section 6.2).
Figures 6 and 7 show both sides of the control box with the connectors, the P
factor adjustment and the switches for the Directions and the Bandwidth
selection. The cables to the actuators are connected on the left side. The
cables coming from the detectors are connected on the right side.
The description of the adjustment and read-out of the P factor is given in
section 5.8. The Directions switches enable a coding of the x and y directions
of each control stage. They are connected with Det1 and Det2, respectively.
The performance is further described in section 5.6. The function of the
bandwidth limitation switch is explained in section 6.5.
The Status signal output can be used as an interlock or to drive a shutter
(see section 6.4).
Note: The Piezo elements have a large electrical capacity. That is why
the cables should not be disconnected as long as the Piezo elements are
charged. I.e. you should always switch off the power of the stabilisation
system on the left side of the panel and then wait for a few seconds before
you disconnect the actuator cables.
5.1. Set-up of optical components
The steering mirrors and detectors can be set up in variable arrangements for
different applications. The detectors can be placed behind high-reflection
mirrors. They are very sensitive and can work with the leakage behind the
mirrors. This has the advantage, that no additional components are required in
the beam path. Alternatively, it is possible to use the reflection of a glass
plate or a beam splitter. The latter can be necessary for lasers with larger
beam sizes where the actuator would constrain the transmission.
In any case, the centres of the detectors should be positioned in that way,
that they define the desired laser beam direction. The target positions on the
PSD detectors can be different from their centres. For further information
please refer to section 4.2.3. The first actuator should be placed close to
the laser or the last source of interference. The last detector should be
placed close to the target.
Note: Take care for a robust mechanical mounting of the optical
components. If possible, the delivered components should be directly tightened
to an optical table without further positioning equipment (like height
adjustment). If there are oscillating components with resonance frequencies
within the control bandwidth in the set-up, such resonances can provoke
oscillations of the system at those frequencies. The following figures 9-13
show a selection of possible arrangements. These examples are demonstrated
with the 4-axes system with two detectors. However, they can be applied in
similar configurations for the 2-axes system with only one actuator and one
detector.
- Figure 9 shows a typical 4-axes set-up of the system where the laser beam hits the optical components in the following sequence: steering mirror, combination of steering mirror and detector, mirror with detector.
- Figure 10 shows a similar set-up where additional lenses are placed in front of the detectors. Further, a beam splitter is integrated in the beam path. This set-up might be better for lasers with large beam diameters.
- In figure 11 a lens is placed in front of detector 2 in order to improve the angular resolution. In this case, the distance between lens and detector should be the focal length of the lens. The focal length itself should be chosen in that way – depending on the beam diameter – that the focal spot is not too small. In case of 4-QDs the beam should still have a diameter on the sensor area of > 50 µm, so that it hits all quadrants of the diode. (The gap between the quadrants is 30 µm for our standard 4-QD, and even more for other 4QDs.)
- Figure 12 shows a variation of 11 where both detectors are placed behind the same mirror. In order to measure both, the beam position and the direction at the same point, a lens is placed in front of detector 2.
- Figure 13 finally shows an arrangement where the 4-axes system is used as two 2-axes systems, i.e. the two stages of the controller are used to separately stabilise two independent beam lines.
Notes:
- In some cases in set-ups where the distance between the actuators 1 and 2 is rather small, a positioning error can occur. This is the case if detector 1 is not placed sufficiently close behind actuator 2. A lens in front of detector 1 can eliminate this positioning error. The lens and the distances should be chosen in a way that the front surface of the mirror is imaged on the detector. The distances and the focal length f of the lens can be calculated with the lens equation 1/f = 1/ b + 1/g. While g is the distance between the mirror’s surface and the lens, b is the distance between the lens and the detector’s surface.
- For setups with lenses, please also refer to the description “Optimisation of the setup with lenses” on our website.
Figure 9: Typical sequence of components for the 4-axes stabilisation:
Detector 1 stabilises the beam position on actuator 2. Detector 2 then defines
the beam position at a separate point and hence the direction.| Figure 10:
Set-up as in 9, with an additional beam splitter and a lens in front of
detector 1 and an additional lens in front of detector 2 (Often used for
lasers with larger beam diameters)
Figure 11: Set-up as in 9, but a lens is used to discriminate the angle by
means of detector 2. This can be of advantage in case of restricted space with
small distances between the optical components. Detector 2 must be placed in
the focal plane of the lens.| Figure 12: This set-up shows a variation of
figure 11. Both detectors are placed behind the same mirror in order to
measure both, the beam position and the direction at the same point. A lens is
placed in front of detector 2 which discriminates for the angle.
Figure 13: Set-up of a 4-axes system used as two 2-axes systems. With
this set-up the position of two independent lasers can be stabilised with one
controller.
5.2. Connecting the cables
The first steering mirror is connected to the Actuator 1 output. The second
steering mirror is connected to Actuator 2.
The detectors are connected to the control box with a LEMO cable with a length
of 4 m and an adapter cable that splits the LEMO cable into four separate
cables. These cables are connected to the detectors according to the following
rules: The x and y lines have to be connected in accordance to the orientation
of the detector housing. If the detector is oriented in vertical orientation
as shown in figure 4, the x line has to be connected to the x output and the y
line to the y output. If the detector is turned by 90° to za horizontal
orientation as shown in figure 3, the x line has to be connected to the y
output and the y line to the x output. At the other end, the LEMO cables of
the detectors are connected to the respective detector inputs at the
controller module.
Note: In case of the 2-axes system you can either use the first or the
second stage for stabilisation.
5.3. Power supply
The power supply is provided by the delivered plug-in power supply. The system
is switched on via the switch on the left side of the housing.
Note: The power supply is specified with 12V and 3.8A. The 3.8A is not
needed during the operation. However, due to the loading of the buffer
capacitors and the ramp-up of the high voltage module, the peak currents are
quite high when the system is switched on. If at least 3A are not available
during the switch-on phase, the high-voltage modules do not reach their rated
voltage and there is a risk of damage.
5.4. Intensity adjustment
5.4.1. Adjustment of sensitivity with 4-QDs
To make sure that the detectors operate in the linear range, the power level
can be adjusted by tuning the potentiometer for intensity variation (see
figure 14). For that purpose, switch on the system (Power on) and inactivate
the closed-loop control (Start/Stop button switched off, green Active-LED and
LED on button off). Then adjust the laser beam onto the detectors in that way
that at least 3 but not more than 9 elements of the power level display are
shining. The amplification increases by counter-clockwise rotation. If the
intensity on a detector is too high the sensor gets saturated. In this case
all LEDs of the power level display are blinking.
If you do not find an appropriate adjustment you have to exchange the optical
filters in front of the 4QDs (see section 5.4.3). If the required filters are
not available please contact us.
Notes:
- In a standard delivery we integrate two optical filters in front of the sensor. These are filters with a high and a low density for coarse and fine adjustment, respectively. Usually the filter which is the first to be reached is the low density one.
- Please be aware that the sensor is quite sensitive. If you want to clean it you should do this carefully with a lint-free cloth.
Figure 14: 4-quadrant-diode. The arrow points to the potentiometer for
intensity variation (Please use a screwdriver)
5.4.2. Adjustment of sensitivity with PSDs
The PSDs have small push-buttons instead of the potentiometer. The adjustment
of this digital potentiometer can be carried out with the delivered metal pin
by means of soft pushing. There is a small push-button for each direction
behind the bores in the housing (see the arrows in figure 15). With the upper
push-button you can increase the gain step by step, with the lower push-button
you can decrease it. There are 64 steps between the highest and the lowest
gain. This corresponds to a change of the
sensitivity by a factor of 20.
If you do not find a fitting adjustment, you can exchange the optical filters
in front of the PSD sensors.
Figure 15: PSD detector. The arrows point to the push-buttons of the
digital potentiometers for the gain adjustment (which can be carried out with
the delivered metal pin)
5.4.3. How to replace the optical filters in the detector housing
In some cases it can be necessary to exchange the optical filters. The filters
are fixed to the housing with two plastic screws. To replace the filters
carefully open the plastic screws. You can use forceps to hold the screws
during the fixation. Usually, the filter with the higher optical density is
the one which is deeper in the slot.
5.5. Pre-alignment
For pre-alignment of the laser onto the detectors you should at first not
activate the control (Active-LEDs off). However, the electronics must be
switched on (supplied with power) so that the Piezo actuators drive into their
zero positions. The laser should be aligned onto the detectors so that only
the green LEDs in the centre of the LED position display are shining. If you
use the software, you can also observe the positions there.
5.6. Direction coding of detector outputs
Each control stage makes use of a steering mirror and a detector as described
in sections 5.1. For any deviation of the laser beam position on a detector
the respective steering mirror is tilted in that way that it aligns the laser
beam back to the desired position. The components that are working together
are identically coloured in figures 9-13. The direction in which the steering
mirror must be tilted depends on the arrangement of detector and steering
mirror. It can be changed during the adjustment process
described in section 5.7 in the following way:
There are four switches on the right side of the controller module (see figure
7). These switches stand for the x and y directions of the control stages
Stage 1 and Stage 2. To turn them into the correct position just activate the
respective stage. If the laser beam is then deflected into an extreme x
(horizontal) and/or y (vertical) position instead of the centre of the
detector, you have to toggle the belonging switch.
5.7. Fine-adjustment
The fine-adjustment should also be performed with inactivated control stages.
The better the correlation of desired position and zero position of the Piezo
actuators, the smaller the position shift once the closedloop control is
started.
Adjust the laser beam by means of manually tilting the steering mirrors or any
other mirrors in the setup in that way, that it hits the centres of the
detectors. This can be done by observing the displays in the software or by
reading out the x and y position outputs of the controller which deliver
voltages that directly depend on the deviation from the target position. You
can easily display these signals on an oscilloscope.
A helpful indication for a good adjustment are also the Piezo voltages. If you
use the software, you can continue to manually adjust the laser beam onto the
detectors with the control-loop activated ( Start button switched on, green
Active-LED and LED on button shining) for a final adjustment until all four
Range displays in the software are close to 0 V. Now the steering mirrors are
operating in their linear range.
After these adjustments the system should show no fluctuations of the laser
beam position after the last mirror with detector when the controller is
activated.
5.8. Adjustment of the proportional element (P factor)
Usually the factory settings of the proportional and integral elements of the
control loop lead to a very stable performance of the beam stabilisation
system with desired bandwidths. That is why no user interactions are required
to adjust the control loop. However, in specific cases the user might wish to
adjust the control loop for his application. Such cases can e.g. be setups
with rather long arm lengths.
Since the control loop is mainly influenced by the proportional element, the
system offers a direct access to the P factors of both control stages by means
of potentiometers or via the (optional) serial interface. The potentiometers
P1 and P2 are located at the side panel of the control box (figure 7). The
adjustment can be done separately for each stage. An increase of the P factor
usually leads to an increase of the overall bandwidth. In order to optimize
the performance, we recommend to start with a small P factor
and operate the system in this stable configuration. Then you can increase the
P factor by simply turning the potentiometer in clockwise direction or by
increasing the values in the software, until the system reaches its
stabilisation limits and starts to oscillate. The potentiometers or values
should then be turned back to a level, where an operation without oscillations
is guaranteed.
Notes:
- The optimal P factors of stages 1 and 2 can differ.
- If the distances of the optical components, the beam diameter, the laser intensity, or other laser data change, the P factor of the overall system might also change.
The system is also equipped with analog inputs for a remote setting of the P factors. The remote adjustment connectors are integrated into the control box in addition to the potentiometers. They are labelled with P1-Sig and P2-Sig (figure 7). Whenever a voltage signal is applied to the remote adjustment, the potentiometers are ineffective. The input voltages can be set between 0 and 5 V. The interface can also be used to read out the current voltages as set by the potentiometers.
Specification
Input/output voltage range| 0 … +5 V
Connector| LEMO 00 series
Cable (optional)| LEMO 00 → BNC for each stage, length 2 m, 2 units
Note: The remote adjustment has to be driven with a low impedance voltage source (≤ 1 kOhm), whereas the read-out drives only high impedance terminations (≥ 1 MOhm).
Operation and safety features
6.1. Power level and position display
The total power on each connected detector is displayed by means of a LED line
on the backside of the detector housing. Furthermore, a LED cross on the
detector housing displays the current laser beam position. If the laser beam
hits the centre of the detector only the green LED of the position display
will shine. In other cases also yellow and red LEDs will shine according to
the examples in figure 16.
Figure 16: Examples for laser beams hitting the detector (orange spots)
and the corresponding position display. The left pictures are shown in a view
from the rear side of the housing to the sensor area.
If only green and yellow LEDs are shining the sensor electronics is in the
linear range where a direct correlation between measured signal and position
exists. If a red LED is shining too, the correlation is no more possible due
to the principle of 4-QDs. In case of the PSDs, if a red LED is shining, the
beam probably hits an edge of the sensor. Please check if the full diameter of
the beam hits the sensor area.
6.2. Low power switch-off
If the total power falls below 10% of the saturation power (only two LEDs of
the LED line are on) the controller automatically drives the mirrors into
their zero positions. This leads to the advantage that the closed-loop control
can start from the zero position even if the laser was switched off or
blocked.
6.3. Switch-on activity delay
The integrated switch-on activity delay starts the control only some time
after sufficient intensity hits the detector again. This ensures that the
control does not start until a reliable control signal is present and the
steering mirrors have reached the zero positions. The Active LED will not
shine during this delay.
6.4. Controller status signal (interlock)
If the system is completely switched off (power off), the Piezo actuators of
the P2S30 tilt the steering mirror into an extreme position. This is about 1
mrad from the zero position. (The P4S30 does not show this behaviour due to
its design with 4 Piezo stacks.) However, the system is equipped with a TTL
output that can be used to block or electronically switch off the laser in
order to avoid damage by the misaligned beam. The level is HIGH when the
controller is active and the steering mirrors are in the
correct range or in zero position. It is LOW if the controller is active and
one of the actuators is out of range. (If the controller is not active, the
level is always HIGH.)
Note: The criterion for the actuators being “out of range” is that the
Piezo voltage reaches 95% of its maximum or minimum value.
Status signal
Description| 1 output for both stages
Signal| TTL, LOW if Piezo is out of range
Connector| LEMO 00
Cable (optional)| LEMO 00 → BNC, length 2 m
6.5. Bandwidth limitation switch
The controller bandwidth directly influences the quality of the stabilisation.
The system can be operated with two different controller bandwidths. The
default setting is the high bandwidth. However, especially in case of unstable
mechanical set-ups or if a mutual interference of the control stages occurs it
can be of advantage to choose the low bandwidth. Therefore a bandwidth
limitation switch is integrated in the controller module (Bandwidth, see
figure 7, H = HIGH, L = LOW bandwidth). The bandwidth can be chosen
independently for both stages.
Option: Sample&hold circuit (“ADDA“)
The additional circuit is used to fix the laser beam in the last position
during laser off times. With this add-on, which is integrated into the control
box, the positions of the steering mirrors can be fixed for an arbitrarily
long time interval without control signal or laser intensity on the detectors.
In that way it is possible to start the control-loop after switching on the
laser not from the zero position but from that latest stabilised position. You
can find the detailed description “Sample&Hold circuit (“ADDA”)” on our
website which explains the various applications of this add-on.
The name “ADDA” is derived from the functional aspect that the actuators’
drive signals are first AD converted and digitally stored before they are
subsequently DA converted again and fed to the amplifiers of the mirror
actuators.
7.1. Technical specification
Sample & Hold circuit
Storage principle| Digital storage of position data
Sampling time| 64 µs per event
Freezing interval| unlimited
Requirement for automatic triggering| Minimal laser on time: > 100 ms
External triggering
Signal levels| TTL, HIGH for laser on, LOW for laser off
Inputs| 1 input for each stage
Connector| 2x LEMO 00, separate connectors for stage 1 and stage 2
Cable (optional)| LEMO 00 → BNC for each stage, length 2 m, 2 units
Minimal length of trigger signal “high“| tmin ≥ 10 µs
Trigger start| 10 µs before until 50 µs after start of laser pulse
Trigger end| max. 1 ms after laser pulse end
Trigger (digital)
via serial interface| Commands: “SetTriggerFreeze”, “ClearTriggerFreeze“
7.2. Modes of operation
Automatic control of sample & hold elements
The beam stabilisation with additional S&H circuit includes an automatic
recognition of laser on and off states. This is done by sampling the intensity
on the position detectors. The automatic operation controls the S&H elements
in order to store the signals during laser on times and fix the position of
the steering mirrors during intervals with no intensity.
For this mode of operation the laser on intervals or the respective duration
of pulse packages must be longer than 100 ms. In case of the automatic control
you do not need to provide any trigger signals.
Note: When using WID detectors (see section 4.2.2), the automatic control
does on principle not work.
External triggering of the sample & hold elements
For single laser pulses or lasers with very low repetition rates, modulated cw
lasers or pulse trains < 100 ms the automatic control can not release the
stored beam position in due time. In such cases it is necessary to control the
S&H elements by means of external triggering. The requirements for the trigger
signals are described in section 7.3.
7.3. Configuration and start of operation
Cabling
In the operation mode of automatic control there is no need for additional
cabling. For external triggering the trigger signals have to be fed into the
control box via the respective LEMO connectors marked with “Trig” (see figure
17). The left connector controls the S&H function for stage 1 / steering
mirror 1. The right connector controls it for stage 2 / steering mirror 2.
External triggering
The external triggering enables an accurate timely assignment when the system
shall store the position of the steering mirrors and when the position shall
be fixed. This assignment is especially important in case of single laser
pulses. For an optimal function of the S&H circuit there are time restrictions
for the trigger signal which should be met. Figure 18 illustrates the
respective tolerances of the trigger signal.
Start of operation
Whenever the stabilisation is de-activated (i.e. the Start/Stop button is in
off-state) the stored position of the steering mirrors is reset. In this state
the steering mirrors are in their zero position. In this way it is guaranteed
that the system can be adjusted as described in this user manual.
Note: Please note that the last position of the steering mirrors is lost
whenever the stabilisation is deactivated. As soon as the system is started
again it starts from the zero position of the steering mirrors. In case of
large distances between steering mirrors and detectors there is a risk that
the beam will not hit the detector without a prior re-adjustment.
7.4. Performance
The performance of the additional S&H circuit shall be explained in the
following sections with the help of some examples. In figure 19 a sequence of
pulse trains with a repetition rate of 1 kHz and a duration of about 300 ms
was applied. The pulse trains are displayed with green colour. The violet
curve shows the position signal of the laser on the detector.
During the first pulse train the stabilisation was de-activated. You can see
that the pulse does not hit the detector in the centre. During the second
pulse train the stabilisation was started. You can see an initial spike of the
position (enlarged view is shown in figure 20) and then a stable position
signal which is also stable during the third and fourth pulse train. Without
the S&H circuit the spiking of the steering mirror would occur again and again
in the second and all following pulse trains.
At the time the beam stabilisation is started the steering mirrors are in
their zero position. Since this position usually differs from the desired
position the system recognises a strong control amplitude immediately after
its activation. This leads to the described spike. In normal use cases where
the laser provides a continuous control signal this is not a problem since the
controller always gets a signal. However, in case of some applications, there
are time intervals without a control signal. In these cases the additional S&H
circuit becomes effective: After time intervals without laser intensity the
stabilised operation is re-activated for the next pulse train without a larger
spike. This will be demonstrated in the following sections “Automatic control”
and “Operation with external trigger”. Without the S&H circuit it would have
started from the upper position and would have produced a spike.
Only for the first pulse train the S&H circuit has no influence since at this
time there are no valid position data for the desired position in the S&H
elements. After that the control signals for the steering mirrors are stored
continuously and for arbitrarily long time intervals where there is no
intensity (or for trigger “low” periods). This is true as long as the
stabilisation system is switched on and activated.
Note: During the operation, the laser intensity should not be modulated
by means of a mechanical laser shutter or another blocking element. Due to
their functional principle, the detectors would determine a wrong position for
the short period of the partially covered beam. Therefore the position signal
would be distorted.
Automatic control
The operation mode of automatic control is especially suited for long
switching periods of the laser light or long trains of single laser pulses.
In figures 21 and 22 an example with pulse trains of a laser with a repetition
rate of 1 kHz is illustrated.
Again, the green curve shows the laser signal and the violet curve shows the
position signals. In figure 21 the laser is running without stabilisation. In
figure 22 it is running with the automatic control. In the latter case the
position of the steering mirrors is freezed during the laser off times whereby
it is refreshed by each signal on the detectors.
Note: For technical reasons, in the operation mode with automatic control
the timing for the position freeze and the re-start of the stabilisation is
slightly delayed to the on and off times of the laser intensity. This can lead
to slight deviations of the stored positions.
Operation with external triggering
In case a trigger signal for the laser on and off times is available, we
recommend to choose the operation mode with external triggering. The improved
timely correlation with the laser intensity usually leads to a better
performance.
Figure 23 shows the example, now with external triggering. In addition to the
curves described above you can see now the trigger signal as a blue curve.
As shown in this example, in case of pulse trains there is an advantage not to
trigger on each single pulse but on the start and the end of the pulse train.
This is recommended for pulse repetition rates of about 300 Hz and higher.
Operation with single laser pulses and external trigger
The use of an external trigger signal also enables the stabilisation of
single or irregularly occurring laser pulses or lasers with very low
repetition rates.
The performance in such cases is illustrated with an example in figure 24.
Here, the position signal of a laser pulsed at 10 Hz is shown as a violet
curve. The green curve shows the trigger signal for single laser pulses. At
the beginning, the laser beam is at an arbitrary position. The beam
stabilisation is started at the time of the fourth laser pulse (counted from
the left). In the following course you can see very well that the beam gets
closer to the desired position with each pulse until it finally stays in the
desired position in a stable manner.
In this example only four additional pulses are required to reach the stable
position. Depending on the set-up of the optical system, the pulse duration
and the duration of the external trigger signal the number of required pulses
can be different.
Note: The time interval for the stabilisation is very short in case of
short trigger intervals. Since the Active LED on the front panel of the beam
stabilisation system is directly connected to this time interval, it can
happen that you will not recognise the shining of the LED due to the short
time.
Option: Serial interface (USB, RS-232 or Ethernet)
The optional serial interface allows, amongst others, the following actions:
- the read-out of positions, intensities and Piezo voltages
- the read-out of the status
- switching on and off of the control loop
- the set & hold functionality for current positions. Here, a current position of the laser beam on the detectors is saved and used as the target position for the further stabilisation. This function is especially used in combination with the PSDs as detectors.
- the setting and read-out of parameters as the P factor, the offsets for the Adjust-in target positions on PSDs, the voltages for the Drive actuator function, etc.
- parameter settings for data streams
Only those functions are available, which are also realized in the hardware,
i.e. where e.g. the additional electronic circuits are integrated into the
control box.
The option includes a software for visualization and communication. You can
find detailed information about the software in the separate software manual
on our website. For integration of the system with your own software you can
further find the description of the communication protocol there. You can also
ask us to provide the documents.
Additional inputs and outputs (Options)
Beside the inputs for the detectors and the outputs to the actuators the basic configuration of the Compact beam stabilisation provides the following outputs:
- Position signals x and y of each detector (analog voltage signal -5 to +5 V)
- Adjustment and read-out of the proportional element (P factor) (see section 5.8)
- Status signal (see section 6.4)
Other optional signal outputs or inputs are described in the following
sections.
Note: In some cases the arrangement of the connectors on the side panels
are changed.
9.1. Voltage offset inputs to move the target position on PSDs (“Adjust-
in”)
As described in section 4.2.3 the measurement principle of PSDs allows to move
the target position on the detector by means of a voltage offset. The offset
values can be applied via the optional serial interface and the software. You
can enter values in the voltage range of -5 V … +5 V. Alternatively, we can
implement additional analog inputs for the x and y axes of both stages, 1 and
2. These inputs can be used to change the still stabilised beam position by an
external source. Figure 25 shows the modified side
panel of the control box with additional inputs Adj1 and Adj2.
Specification
Description| 2 analog inputs LEMO 3-pin, one for each actuator (x, y) or
serial interface
Signal| – 5 V … + 5 V
Connector, analog| LEMO 0S
Cable, analog| LEMO 3-pin → 2x BNC, for each stage, length 2 m, 2 units
Note: The position vs. voltage characteristics of a PSD is usually not
linear. Therefore, a calibration should be performed if the target shall be
moved on a desired path.
9.2. Direct drive of Piezo actuators („Drive Actuator“)
As an option for the direct drive of the Piezo actuators (i.e. without
feedback from the detectors) we can implement additional input channels to the
controller. It is then possible to drive the actuators with an external
voltage signal. This option makes use of the integrated 4-channel high-voltage
amplifier of the system. The input signal will be converted to a high-voltage
signal which is fed to the Piezos.
Specification
Inputs| 2 inputs LEMO 3-pin, one for each actuator (x, y), – 5 V … + 5 V
Outputs / to Piezo actuators| 2 actuator connectors on side panel, LEMO 0S
series, 0 V to 130 V
Output impedance| 110 Ohm@1 kHz, designed for high capacitive load
Notes:
- The voltage range of the Piezo actuators is specified as – 45 V to + 180 V.
- We have specified the voltages for the valid range of the green Range LEDs on the control box to values of 9 V to 120 V (max. range 0 – 130 V).
- There is a non-linearity in both, the characteristics of the Piezos and the amplifiers. Therefore the signal will not be fully proportional to the input signal. If you need a precise and absolute position of the steering mirrors (without the control-loop which usually gives the position feedback) you should carry out a calibration of the angles versus voltages.
- It is also possible that the x and y axes of the same Piezo actuator vary strongly.
9.3. Option: External activation
The external activation enables the change of the operation state of the beam
stabilisation system with an external signal. The external activation can be
independently applied for stage 1 and stage 2 of the stabilisation system. For
this purpose, two LEMO connector plugs (series 00) are embedded on the left
panel of the control box. The inputs are marked as Ext1 and Ext2.
There are three operation states. The specification of the control signal is
as follows:
Signal (Level: 5V TTL)| Voltage range| Controller status|
Reaction of Start/Stop LED
---|---|---|---
H (high)| 2.4 – 5.0 V| Start| on
L (low)| 0.0 – 0.8 V| Stop| off
Z (high impedance or| | Manual mode according to| on/off
not connected)| | selection on front panel|
9.4. Intensity outputs at controller
We can add additional intensity voltage outputs at the control box. These
outputs are marked with Int1 and Int2 on the side panel of the control box.
Specification
Description| 2 outputs for laser intensities of detector 1 and 2
Signal| Analog, 0 – 8 V
Connector| LEMO 00
Cable (optional)| LEMO 00 → BNC, for each stage, length 2 m, 2 units
9.5. Range outputs for monitoring applied Piezo voltages
In some applications it can be helpful to know the applied voltage ranges of
the Piezos, e.g. to see whether or not the tilting range of the Piezos (and
therefore the voltage range) is at its limits. If the Piezo actuators are
combined with additional motorized mounts in order to enlarge the overall
tilting range, the Piezo voltage can be used as a trigger to drive the motors.
Specification
Description| 2 outputs LEMO 3-pin, one for each actuator (x, y)
Signal| Analog, 0-10 V
Connector| LEMO 0S
Cable| LEMO 3-pin → 2x BNC, for each stage, length 2 m, 2 units
Drawings
Drawings of all main components can be found in the respective data sheets. On request, we are pleased to send you the corresponding STEP files.
Cables
11.1. Standard cables
The standard delivery of a Compact laser beam stabilisation system includes
all required cables to set up the system and to read out the positions. These
are:
Cable set for a 4-axes system (included in standard delivery)| quantity|
length
---|---|---
Detector → Controller| 2| 4 m (including the 4x MCX → LEMO adapter cable)
Actuator → Controller| 2| 2 m (directly mounted to Piezo element)
Actuator → Controller (extension)| 1| 10 m
x, y position cable (LEMO → BNC)| 2| 2 m
11.2. Additional cables
In addition to these cables we can also offer additional cables or cables with
other lengths. The following table shows some examples.
Other available cables and/or lengths (examples) | Typical lengths |
---|---|
Extension cables for detectors (LEMO → LEMO) | 1 m … 25 m |
Extension cables for actuators (LEMO → LEMO) | 1 m … 25 m |
Cables for external activation (LEMO → BNC) | 2 m |
Cables to connect the intensity output (LEMO → BNC) | 2 m |
Cable for P factor (LEMO → BNC) | 2 m |
Cables for adjust-in, range output, drive actuator | 2 m |
(LEMO (3-pin)→ 2x BNC) | |
Cable for sample&hold circuit “ADDA” (LEMO → BNC) | 2 m |
USB cable (USB A → micro USB) | 2 m |
If you do not find the cable you need please do not hesitate to contact us.
Troubleshooting
12.1. No signals on display
Please check if the power line chord is connected to a conducting power plug
and if the power switch at the controller unit is activated. If everything is
okay with the power line, please contact us or your distributor.
12.2. No signals on detector
Please follow the instructions in section 5.4 and check if an aperture or edge
is blocking the laser. If the laser beam hits the sensitive area of the
detector another reason can be that the chosen filters are too strong. In that
case the filters should be exchanged.
12.3. The laser beam is not correctly positioned
Please check the following issues:
i. Is the laser power in the allowed range?
ii. If red Range-LEDs are on:
a. Are all cables connected as described in section 5.2?
b. Is the initial position of the laser beam in an acceptable position? If the
initial position has changed strongly the closed-loop control does not work in
the linear range any more. Please refer then to section 5.7.
c. Is the direction coding correct?
12.4. The steering mirrors make exceptional noise
Please immediately switch off the system. Irreparable damage to the steering
mirrors can occur. Then check the laser power on the detectors and adjust it
as described in section 5.4. Make sure that the initial laser beam has not
changed strongly and that it hits the detectors. Take care that the beam is
not blocked by an aperture or an edge anywhere in the beam path. This could be
the case at the cut-out of the Piezo actuator. If a red Range-LED is on, the
closed-loop control does not work in the linear range any more. Please refer
to section 5.4 then.
12.5. Laser position is not stable
If the automated stabilisation of the laser beam does not work although the
controller is active this might be due to a wrong direction coding of the
detector inputs (see section 5.6). Please check the direction coding.
Another reason might be an unstable mechanical set-up leading to oscillations
of the system. Usually this phenomenon is accompanied by an exceptional
humming noise. E.g. high positions of components (especially of those carrying
the Piezo elements) can lead to mechanical instabilities. In this case a
better stabilisation can be achieved with a lower controller bandwidth. Please
activate the bandwidth limitation switch (see section 6.5).
12.6. Permanently red “Range” signal
A “Range” signal that is permanently shining red on the top of the control box
may indicate a problem with a high-voltage channel. “Permanently” primarily
means that the red LEDs are also shining when the control loop is not
activated. This behaviour may be caused by a short circuit in a Piezo element.
Usually this has caused the fuse to blow and prevents the further use of the
beam stabilisation. Please get in touch with us. We will then clarify in more
detail which tests you can perform to determine the cause of the error.
12.7. “Range” signals jump back and forth when switching the direction
coding
If a “Range” indicator of a control stage jumps from one extreme to the other
(from red to red) when the direction coding is switched (see section 5.6),
this indicates that the associated detector is rotated by 90°. In this case,
swap the cable connections of x and y at the detector as described in section
5.2.
12.8. System steers the beam away from the centre
If the system keeps trying to steer the beam away from the centre of a
detector when the control loop is activated, this could be due to a remaining
setting of values for Adjust-in in the software. In this case, delete the
corresponding values or switch to “external” in the software.
Safety
The system has left our factory in a faultless state. Please store and operate
the system in dry environments in order to maintain this state.
The device fulfills the requirements of the European EMC Directive 2014/30/EU.
Labels
SN: 100208BA123
Model: Compact
1kHz cw
Supply: 12VDC 2A MRC Systems GmbH Hans-Bunte-Str. 10 D-69123 Heidelberg
Germany| SN: 100208DBA4567
Model: XY4QD 1kHz
Supply: 12VDC 0,2A
MRC Systems GmbH
Germany| SN: KBA890
Model: P2S30
---|---|---
Figure 26: Labels on the controller electronics (left), the detectors
(middle) and the actuators (right)
Contact
MRC Systems GmbH
Hans-Bunte-Strasse 10
D-69123 Heidelberg
Germany
Phone: +49 (0)6221/13803-00
Fax: +49 (0)6221/13803-01
Website: www.mrc-systems.de
E-mail: info@mrc-systems.de
https://www.mrc-systems.de/en/products/laser-beam-stabilization
Manual – Beam Stabilisation System Compact
version 14 – 14-March-2022
www.optoscience.com
TEL: I 03-3356-1064
E-MAIL: info@optoscience.com
References
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