Refer to Figure 1 below while performing the following steps.
Align the alignment laser to pass through both irises attached to the main board.
Place your group board on the main board.
Set heights of your two iris's to match the height of the alignment beam above your group board.
Visually check level of beamsplitter and adjust it so that the top plate is not tilted relative to the bottom plate. This can be done by eye, using your judgement as to when the top and bottom plates are as parallel as you can get them.
Place beamsplitter as shown in Fig 1 so that the incident alignment beam is reflected in the direction of M2 on on Fig 1.
Check that beam does not hit top, bottom, or sides of the beamsplitter.
Place Mirror M1 as shown.
Check that the beam hits near center of mirror and does not clip the edge.
Place Iris 1 between the beamsplitter and M1 as shown, so that the beam passes through the center of the iris.
Attach the post holder to the table, do not leave it sitting unattached.
The reflected beam from M1 should now be passing through the beamsplitter again, traveling from right to left, with some of the beam being reflected towards the photodetectors. Place Iris 2 on your group table as shown and adjust the beamsplitter so that the reflected beam from M1 goes through it.
Position Photodetector I so that the reflected beam from M1 hits the active area of the photodiode.
Note that the cap with a hole in the center can be helpful here. If the beam goes through the hole in the center of the cap, and the photodetector is pointed back at the beamsplitter, you can be confident that the beam is hitting the active area of the detector.
Place M2 on your group table as shown, and adjust it do that the its reflected beam also passes through the center of Iris 2.
There are internal reflections from within the beamsplitter which will also appear near Iris 2. Using a piece of paper or thin cardboard to block the reflected beams from M1 and M2 will help with ensuring you are aligning the correct beams, and not reflections.
Switch to IR laser.
Trace IR beam front to back, making sure it hits all of the optical components correctly.
It is unlikely that the IR beam will follow the exact same path as the alignment beam. You will almost certainly need to realign some of the optics at least a little bit, but they should all be close.
Connect photodiode I to the scope and trigger on the sync output of the electronics. Adjust the scope settings to show approximately one full frequency sweep of the laser. If you have performed the above steps carefully you should observe a small sinusoidal interference pattern on the photodetector signal.
You may have to add some neutral density filters to the beam path to avoid saturating the photodetector.
If you see what you suspect is an interference pattern, do a simple sanity check to ensure that the signal you see is in fact due to the combined beams from the interferometer. Other things which can create signals that look like an interference pattern include:
Having the incandescent lights on in the room. Note that the fluorescent lights will not cause this effect, only the incandescents.
Having unwanted reflections entering the photodetector.
Having the beams only partially hitting the active area of the photodetector, resulting in a noisy signal that has to be zoomed in on a lot.
Once you are convinced that you are able to see at least a hint of an interference pattern, make very small adjustments to M1 and M2 to try and maximize the amplitude of the interference by improving the overlap of the beams:
Start by making small adjustments to both axes of M2. Note that your finger pressure on the mirror adjustment screws will be enough to alter the path length of the interferometer. So you need to make an adjustment then let go of the screw to see the effect. With a bit of practice this is not as difficult as it sounds.
Once you have made the interference signal as large as you can by adjusting M2, repeat the same procedure on M1.
Alternate back and forth between M2 and M1, making small adjustments to each until you are no longer able to make the interference pattern larger in amplitude.