These are *Kits* of
parts to construct laser interferometer-based displacement measuring
systems from materials about as close to stone blocks and bear skins as
is reasonably possible. ;-)
However, if your goal is to end up with a system that is usable for an actual application like a CNC machine or something similar rather than simply the joy and satisfaction of being able to say you actually built the thing, consider listing 303500535042 instead. While more expensive, it uses a commercial laser, interferometer optics, and optical receiver(s), and thus eliminates many issues of fiddly construction (fragile glass laser tube, high voltage, precision mounting and alignment, etc.). And it in the end will almost certainly be better in terms of reliability.
Note that displacement measuring systems are
NOT rangefinders - they keep
track of the CHANGE in position
between the interferometer and a moving reflector and must be zeroed
to a
reference. The reflector generally needs to be either a good quality cube corner or plane mirror. A diffuse surface will NOT work.
Versions are now available for use with
homodyne and heterodyne
interferometers.
Note: If a kit you are interested in is out of stock,
contact me for availability or
alternative.
The following are the standard
kits:
- Homodyne Kit with Single frequency Laser: Includes HeNe laser tube tested for single frequency operation, heater, power supplies, optics, µSLC1, Quad Decoder, parts for thresholding to Quad A/B, and
µMD2. Native resolution with Linear Interferometer of -80
nm. The path length difference can be up to several meters.
- Homodyne Kit with LP Head: Similar to the one above but replaces the bare laser tube with a Linearly Polarized (NOT Low Power!) HeNe laser head
(minimum power 0.7 mW) with Alden connector and matching power
supply. This eliminates virtually all wiring, is easier to
mount, and no potentially shocking high voltages are involved. ;-) The
resolution is similar to the one
above but the path length difference must be limited to no more than +/- a few cm. It has the same laser as in the Michelson Educational Setups I used to offer. Parts are provided to convert from Quad-Sin-Cos to µMD2, but there is no PCB for that. As a practical matter for a demo or proof-of-conecpt, the lower cost "Minimal Homodyne Kit with LP Head" kit, below, will be just as good.
- Heterodyne Kit with Two frequency Laser: Includes HeNe laser tube tested for two frequency operation, Zeeman magnets, heater, power supplies, optics, µSLC1, and µMD2.
The laser tube has a minimum output power of 0.4 mW. Native resolution with Linear Interferometer is ~158
nm. The path length difference can be up to several meters.
- Heterodyne Kit with High Power Two frequency Laser: Similar to above but the tube has an output power of >0.8 mW.
- Combined Kit for Heterodyne or Homodyne: Parts to construct both type but not at the same time. This really doesn't make sense as the laser had to be significantly modified to switch between types and that's just asking to screw up. This option is currently disabled because it ends up being too confusing for both of us, sorry. ;( ;-)
- Heterodyne Kit with Hewlett Packard Laser Tube Assembly: A complete assembly with glass laser tube in magnet, beam expander or collimator, waveplates, and frame replaces the individual parts of the other options. This has been deleted because the only tubes currently available are very low power - below 0.15 mW
and would be challenging to stabilize and get working in an interferometer. However, if really interested, I can provide one.
The optics included with these kits can be used to construct several types of interferometers. With a Plane Mirror Interferometer, the resolution is
improved by a factor of 2 (e.g., down to 40 nm for the homodyne
interferometer or 80 nm for a heterodyne interferometer) compared to a Linear Interferometer. For those setups that support a large path length difference, a beam expander will be required to prevent the beam divergence from being an issue.
Note that while µMD2 has no practical upper limit on counts per second, the
interface electronics included in the homodyne kits are very limited, so they are recommended only for a proof of concept
or student project unless you are able to construct a pair of high speed
trans-impedance amplifiers whose outputs are thresholded and converted to RS422. A schematic is in the
Quad-Decoder manual or will be provided upon
request. Otherwise, the heterodyne kits are recommended.
And for this reason, the Minimal versions of the homodyne kits are probably perfectly acceptable and less expensive.
While the heterodyne native resolution is only 80 nm with a Plane Mirror Interferometer (PMI), and the homodyne native resolution is only 40 nm, for slowly changing displacement, the actual accuracy can be a few nm or even better with averaging in the GUI.
The only downside of SG-µMD2 had been that it didn't support sub-wavelength interpolation. However, V2.61.XX SG-µMD2 interpolation firmware now exists hot off the presses that will work for one axis, and probably for up to 3 axes. It implements phase-based interpolation with nm-scale resolution for slowly changing displacement, but now over a millisecond time scale - a thousand times faster than using GUI averaging. For higher slew rates, the resolution should be similar to the way it was before. So while one cannot achieve such high precision if slewing rapidly, end-point resolution and accuracy will be stellar. Three axes are implemented but only Axis 1 has been tested so far. Be the first on your block to try this! But be warned, making sense out of such precision requires a special setup with immunity from vibrations and with ultra-low thermal expansion that may change the relative path lengths. Otherwise the display will be nonsense due to the Laws of Physics. ;-) V2.61.xx is also usable without interpolation as well as for its frequency counter function. But to be safe, stick with the default V2.20.
These are basically a combination of an unstabilized HeNe laser tube or head kit, a stabilized
HeNe laser kit, or the stabilized HeNe Zeeman laser kit along with DIY
interferometer optics, and the µMD0 of µMD2 Micro Measurement Display
to implement a complete displacement measuring system with nanometer
resolution using parts about as close to stone blocks and bear skins as
is reasonably possible. :-) The diagrams show schematic
representations of typical systems as well as some of the interferometer
configurations.
The following minimal systems are lower performance but still more than adequate for tracking the
movement of a micrometer stage as noted. Only a Linear Interferometer may be constructed with the parts included in the Minimal Kits. The native resolution
is the same as that of the Standard
kits. Here are the options:
- Minimal Homodyne Kit with SF laser:
Single frequency HeNe laser with µMD0. Very limited slew
rate but capable of a large path length difference.
- Minimal Homodyne Kit with MLM laser:
Unstabilized HeNe laser with µMD0. The path length difference
for this random polarized laser must be 1/2 the tube cavity length +/- up to a few cm. This one would be great for a student
project on precision measurement using the wavelength of light as a
"yardstick". One can do a lot in a few cm. ;-)
- Minimal Homodyne Kit with LP Head:
Replaces the bare laser tube with a Linearly Polarized laser head
(minimum power 0.7 mW) with Alden connector and matching power
supply. This eliminates virtually all wiring, is easier to
mount, and no potentially shocking high voltages are involved. ;-) . This also includes µMD0 and the performance is similar to the one
above except that the path length difference must be zero +/- up to a few cm. It has the same laser as was in the Michelson Educational Setups I used to sell. This is the easiest of all these kits to construct with the conversion from Quad-Sin-Cos to µMD0 done on the µMD0 PCB.
- Laser Doppler Displacement Meter: This is very similar to the basic Heterodyne Kit with Two frequency Laser but the only optics it has are for the Linear Interferometer, which is intended to mount inside the laser enclosure along with both the REF and MEAS optical receivers. Then the only external optic is a 1/2 inch retro-reflector for the moving target.
The accuracy with any of the kits, even the minimal ones, will be similar to that of a $20,000 interferometer-based metrology
system and the entire experience could be quite rewarding.
And to put that resolution in perspective, 80 nm is approximately
1/90th the diameter of a human red blood cell, and 1/600th diameter of
an average human
hair. (The commercial systems do go lower, but for many practical purposes, it is almost impossible to tell the difference.)
As general
recommendations:
- The Heterodyne Kits have the highest
performance and are easiest to
align.
- The Homodyne Kits with the LP Head are simplest to
construct. The Standard homodyne kits will NOT have substantially higher performance than the Minimal kits without additional high speed front-end electronics (not included) and they are more complex to construct.
If this doesn't make sense, ask!
None of these
undertakings are for the lazy, even the Minimal ones. For
someone who has little or no experience with lasers and electronics, it
may take several months to a year or more. For a
tinkerer-scrounger type with some basic experience, it could be as
little as a few hours. Construction will require the
fabrication of some mechanical parts, wiring up of electronics, and
testing of the laser with the
µMD0
or µMD2 Micro Measurement Display. But any of these could
make nice college-level Senior Projects especially if combined with some
real application for precision
measurement.
However, where enthusiasm is lacking, a
halfhearted attempt will result in the parts ending up dumped in a box in
your attic next to the unfinished telescope mirror. :( Trust
me, I know about unfinished telescope mirrors.
:)
And these are NOT Heathkits™ - there is no
complete step-by-step assembly manual for the entire system (though
there are manuals with
Heathkit™-style
assembly instructions for
the SG-µMD2,
SG-OR3, and SG-AB2
PCBs.)
While there is extensive information on all the subsystems, creativity
will be required to scrounge and assemble or fabricate mechanical and
electrical parts not in the
kit.
Having given fair warning, here is the
description. Differences between the heterodyne and homodyne
kits will be
noted.
HeNe laser (upper left
of main photos):
For all except the kits using a linearly polarized laser head, the laser itself consists
of:
- Well behaved 4.75 or 6 inch bare HeNe laser
tube.
- DC-input HeNe laser power supply
brick with ballast
resistor, tube mounting brackets, and DC wall adapter.
The single and two frequency lasers also
include:
- Thin-film Kapton
heater that attaches to the tube.
- Tiny PCB to mount a PBS cube and two photodiodes for
stabilization
feedback.
The two frequency laser further
includes:
- Set of rare earth magnets to place surrounding the tube which should be
sufficient for a 1 MHz or greater split frequency when locked.
- Quarter Wave Plate (QWP) to convert
circular to linear
polarization.
- Linear polarizer and photodiodes for
detecting REF and MEAS during
testing.
Assembly of the lasers differ
slightly:
- The basic laser is similar for all consisting of the
laser tube, HeNe laser power supply, and DC power
pack.
- For a stabilized single frequency laser, the
thin-film heater is attached to the HeNe laser tube and the polarizing
beam-splitter and photodiodes are used to provide optical feedback to
control the power to the heater so the amplitude of the X and Y
components are
equal.
- For a stabilized two-frequency HeNe Zeeman laser, in
addition to the heater, a series of magnets are configured to surround
the tube and provide an axial magnetic field. Some
experimentation will be required to optimize the configuration of the
small rare-earth magnets. 7 strips of 7 magnets all pointing the same way should be
sufficient to provide a locked split frequency of at least around 1 MHz
but your mileage by vary. Additional magnets can be added to
boost it somewhat (but there is a limit). The QWP then converts the circular
polarization from the tube inside the magnet to linear polarization in X
and Y.
- A beam sampler (included) can be used to divert a portion of the
beam for use for normal 2 mode stabilization. When the
amplitude of the X and Y components are equal, the laser will be locked correctly. For the Zeeman laser, the two frequency components will be present in the output. A pair of beam samplers will generally be used to provide the feedback and REF signal. For some lasers, the waste beam out the back can be used for feedback and/REF but it may be very weak.
µSLC1 using Arduino (stabilized single
and two frequency lasers ONLY, upper right of main
photos):
- Atmega 328 Nano 3.0 Arduino compatible microprocessor PCB
with µSLC1 firmware preloaded.
- A BLANK PCB Rev 1.1 or higher. The completed controller
using the PCB is shown in the sixth
photo.
- Most other
parts to construct a digital controller - socket, LEDs, resistors,
connectors, etc.
- 12 VDC wall adapter for heater and optical receivers -
styles may vary (not shown). OR3 will run on 12-15 V.
- Links to µSLC1 GUI, firmware, and assembly and operation
manual.
µSLC1 is also available by itself.
Interferometer (all except Minimal Kits, lower right of main
photos):
- 1/2 inch Polarizing Beam-Splitter (PBS)
cube.
- 2 each 1/2 inch retro-reflector (cube-corner)
prism.
- 1 small
planar (dielectric or aluminum coated)
mirror, generally intended to divert the beam from the interferometer to the detector.
- 1 "large"
(1/2") planar aluminum coated mirror on cheesy but usable kinematic
mount, may be removed. This would be the remote reflector for the Plane Mirror Interferometer or High Stability Plane Mirror Interferometer, not for the Linear Interferometer. Not in minimal kits.
- 2 each Quarter Wave Plates
(QWPs). Not in minimal kits.
These parts can be used to
construct a Linear Interferometer, Plane Mirror Interferometer, Single
Beam Interferometer, Angular Interferometer, Straightness
interferometer, and more. (But not at the same
time!) If you would prefer to skip building the
interferometers and use HP / Agilent / Keysight optics cheating just a
bit :), that can be arranged with an adjustment in cost using parts from
me or elsewhere. Inquire if interested. The
interferometer is probably the most dicey assembly in terms of
construction and alignment. But then you won't be able to
claim you built this thing from
scratch if that is just bought!
Only a
Linear Interferometer may be constructed using the Minimal
kits.
Detectors:
If you are the lazy type
and don't want to construct OR3, I may have a limited number of HP or
Excel optical receivers available at extra cost. You can also
hunt for them elsewhere on eBay. But if you are the lazy type,
the entire DIY Interferometer Displacement Measurement System Kit is
definitely NOT for you! :(
:)
- Homodyne: Parts for quadrature
sin-cos decoder includes variable attenuator plate to be used as a Non-Polarizing Beam-Splitter (NPBS), a piece of circular polarizer sheet (LP+QWP), a piece of LP sheet, two photodiodes, two 1M trim-pots as a adjustable loads, and two 100K ohm resistors as fixed loads. Its output will be Quad Sin/Cos with a p-p voltage of up to a few V for a typical 0.5-1 mW laser. for conversion to Quad A/B (TTL) order the version with µMD0 since it has the thresholding or use your own parts for that. Note that
additional electronic components will be required for a high speed
interface including a dual trans-impedance op-amp circuit with gain and
offset adjustments. Parts for this are NOT included but a
schematic to get you started is available in the
manual.
- (A high quality 10
mm Non-Polarizing Beam-Splitter Cube (NPBSC) is available in place of
the variable attenuator plate for an additional $25. This mounts on the
same PCB and is slightly easier to align and virtually guarantees
nearly equal amplitude Sin/Cos signals. Inquire if interested and I
will create a Special Option in the listing which includes it. Less expensive NPBSs tend to not be very "Non-Polarizing". ;-) But as a practical matter, this luxury really isn't needed.)
- The QAB2 design is available including a blank PCB, but it is NOT included in the standard Hom
and Het+Hom kits. (A populated QAB PCB is shown in the photo.) QAB2 has a bandwidth exceeding 3 MHz so it should
suffice
for any DIY application. QAB2 consists of a 1.6 x 2.25 inch
PCB and runs on 12 to 15 VDC. It has the photodiodes
for input and RS422 outputs compatible
with µMD2. Heathkit™-style assembly instructions
will be
provided. However, it may not be that stable thermally so some fiddling may be required. That is why the complete kit is not included as an option. There is a link
to QAB2 on "Sam's Electronics and Laser Kit Information and Manuals"
page. Google will find
it. The kits in this listing ONLY include the basic parts to convert to TTL.
Measurement Displays (lower left of
main photo):
The µMD2 display portion for the Standard kits
contains:
- SG-µMD2 PCB and all electronic
components.
- USB A male to USB B Micro male
cable.
- Headers or
screw terminal blocks for 1
axis.
- OLED
display. This may be useful for testing but does NOT provide
anything like the µMD GUI.
- Links to µMD2 and µMD0 Installation and operation manuals. These
include full specifications, assembly and wiring instructions, Windows
GUI operation, and links to the latest firmware and GUI
software.
The "Minimal Homodyne"
systems include parts for µMD0 including the SG-µMD0 PCB.
Documentation including
construction guidelines, and friendly lifetime tech support will be
provided. "Lifetime" is defined as either yours or however
long you remain interested in this stuff, but is assumed to
terminate sometime shortly after the Universe
ends.
One of the short Scanning Fabry-Perot Interferometer (SFPI)
kits (#s 1-8 in listing 303543775362) would permit the longitudinal
modes of the laser to be displayed in real-time. While the
resolution using one of these short SFPIs will NOT be sufficient to see
the individual frequencies of the two-frequency laser, it can be used to
confirm that there are no rogue modes present, and with other lasers as
a general purpose laser spectrum analyzer for wavelengths in the
yellow-red range. Some of the long SFPIs can resolve the two
frequencies if that's what you'd really like to see but they can really only be justified for true SFPI junkies.
;-)
General info on home-built stabilized HeNe lasers including
complete schematics for analog controllers may be found in the Sam's
Laser FAQ chapter: Home-Built HeNe laser. (Google will find it
- eBay is anal about including off-site links.) Only basic
mechanical and electronic skills are required to complete the
laser. As noted, construction guidelines and email tech
support will be provided. However, this is NOT a turnkey
system. Some assembly is definitely
required. How many times have I said that? ;-)
The
HeNe laser tube and its power suppply are used but tested and guaranteed to be healthy be
and suitable for the type(s) of interferometer(s) in the
kit. All other parts are new.
The diagrams above show the hookup for powering
the tube itself and the general scheme used for stabilization
. Detailed instructions may be found by going to
repairfaq.org/sam/manuals. Of critical importance is that the
tube be installed as shown in the diagram. However, the beam
may exit from either end depending on the particular tube that in the
kit. The tube may light and appear to work even if installed
backwards, but it is likely to fail quickly. Failure of the
tube due to incorrect wiring is easily detected via forensic analysis
and not covered by the 30 day warranty.
For
international buyers, the wall adapters will run on 100-240 VAC but will
either have US plugs or a socket for a detachable
cord.
Specific models of parts may vary depending on
availability and may not match the photos precisely. They are fully tested prior to
shipping.
The Micro
Measurement Displays (µMD0 or µMD2) provide most of the capabilities of
an HP-5508A and more. The firmware requires a PC with USB port
running Windows XP or later and .NET 4.0 or later for the custom µMD
application (which is the same for all). The PC is NOT
included but most systems (desktops, laptops, or netbooks) more recent
than the Jurassic period should be satisfactory. :) So dust
off that old computer and put it to good use! Sorry, µMD does
not run on a phone - yet! The Graphical User Interface (GUI)
provides real-time displacement and velocity measurements using common
interferometer optics on up to three independent axes, as well as
optional frequency analysis of the displacement data. µMD also
supports straightness and angle measurements with appropriate optics
and allows for their parameters to be entered if non-standard.
Environmental compensation parameters (temperature, pressure, humidity)
may be entered manually. See the photos for examples of the
typical display. Other features include logging so that data
can be exported to a data analysis application like Matlab or Excel; and
Test Mode which has it's own function generator for simulated data
which can be displayed and processed just like real data for verifying
behavior or just checking out operation. And for custom
applications, the GUI can be bypassed entirely with data input directly
to your custom software. The µMD0 and µMD2 PCBs run from USB 5
VDC.
If you are interested in actually using these parts in a
metrology application (as opposed to simply for the pleasure of
perpetual construction, testing, and adjusting), I recommend one of the
Heterodyne Kits as they are more capable, easier to align, and generally
more useful. For just dipping your feet into interferometery, one
of the Minimum Homodyne Kits would probably
suffice.
Much
more information on homodyne and heterodyne interferometry, stabilized
HeNe lasers, and other related topics may be found in "Sam's Laser
FAQ".
Details on the kits may be found at "Sam's Electronics and
Laser Kit Information and
Manuals", which also have links to the above.
Google will find
these.
And there is a lot to digest here, so please feel free to contact me directly via eBay or the
Manuals page with
questions.
If
you have no idea what this stuff is, you probably don't need any!
:)
Returns will be accepted only if everything is in
identical condition to how it was received, or if incorrect parts were
sent by mistake. Where parts are damaged (like the PCB due to using a
butane torch instead of a proper soldering iron), a partial refund may
be considered. But please understand that the PCB in that case would be scrapped and significant time and effort may be required to retest other parts like the laser.
eBay International Shipping is
likely to be the least expensive reliable shipping method for overseas buyers. However, it may not support your
country and/or lists "lasers" as prohibited items. But
since this is a kit, there have so far been no problems shipping similar
sets of parts. I can also use the shipper of your choice if
you do all the "paperwork" and send me the shipping
documents. Or the kit can be sent to a USA address and accepted there. Then you do the overseas shipping. ;-)
Thanks for looking!
---
sam