As you did for the start of day 2, reinstall your group table on the main table and restore and realign the optics as necessary.
Since the same photodetectors and the wedge beam splitter are used by all groups, you will have to reposition them for your setup. Regardless, you should be able to get the whole apparatus set back up to where it was at the end of Day 1 in under 30 minutes, including turning the IR laser on and tuning it to resonance.
Once you have aligned the interferometer and obtained a clean interference pattern on the scope, use the cursor feature of the scope to measure the locations of the interference maxima (including an estimate on the uncertainty of these measured values) and record them in your lab notebook. You should also transfer a screenshot and the digitized data to the lab computer for inclusion in your out of lab assignment.
You will be expected to be able to articulate clearly and concisely how you performed this measurement, and how you estimated the uncertainties in the measured values.
Do not forget to measure and record the dimensions of the interferometer.
(DFSAS) Doppler-Free Saturated Absorption Spectroscopy
Your goal is to setup the optics to perform DFSAS measurements of the hyperfine splitting in ${}^{87}$Rb(F=2) and ${}^{85}$Rb(F=3).
Over the first two days of this lab you will have built and aligned virtually all of the optical setup needed for the DFSAS measurement. If this work is still intact on your personal optical table, you can proceed straight to the next section on creating and aligning a pump beam. If this is not the case you first need to reestablish the optical setup from day 2 before continuing.
The final optical component which needs to be positioned and aligned is the 50/50 beam splitter as shown in Figure X. This beam splitter must be positioned so that the beam labeled “Probe” from the wedge beam splitter passes through it and into photodetector #1. The second reflected beam from the beam splitter is not used.
The 50/50 beam splitter must be positioned such that the beam traveling right to left in the figure is reflected into the vaporcell overlapping the Probe Beam. This new beam will function as the Pump beam.
Getting this last optical component in the proper location and aligned is a little tricky. Before you begin you should consult with an instructor who will give you some tips on how to proceed.
Once you have the pump beam in place and aligned with the probe beam, obtain the signal from the probe beam PD on the scope. The output of this PD should show the doppler broadened spectra but with dips now superimposed on each transition peak. These dips are the doppler free features associated with the individual hyperfine states and their cross overs. Each of the four transitions, two for each isotope, should in principle show 6 of these doppler free dips. However it is likely that you will need to spend a bit of time fine tuning the alignment and intensities of the probe and pump beams to see all of them.
From this point forward you will want to focus on the first two doppler broadened features, the 87Rb(F=2) and 85Rb(F=3) transitions. For each of these two peaks you need to record and save a scope trace which has been zoomed in enough to see all 6 doppler free dips clearly. You should also use the cursor feature to carefully measure the locations of these dips, with estimated uncertainties.
You will need to spend some time adjusting the overlap and power of the probe and pump beam in order to see all 6 of the expected doppler free features on each of the doppler broadened peaks. The optimal beam powers for the 87Rb(F=2) and 85Rb(F=3) transitions are different enough that you will need to optimize and record them separately.
The following figure shows the full doppler broadened spectrum for Rb, with the two peaks of interested annotated by the red box.
(The above figure was taken from the manufactures user manual for this apparatus. TeachSpin Diode Laser Spectroscopy User's Manual, p2-8, Rev 2.0 11/09.)