I frequently get questions from people about the Altera DE2 where the DE2 itself seems to be working (light flashing at about 10 Hz), but they canít read any counts from it in LabView. Here are a list of suggestions:
∑ †The breakout box is not properly wired. Make sure that the signals are properly wired to the correct pins on the DE2.
∑ In the setup instructions it mentions that we had trouble with USB to RS232 adapters, and I suggested to get a real RS2332 board for your compter. Lately we have used USB-RS2323 adapters with no problem.
∑ Make sure that your COM port is properly working, and that you have selected the proper COM port that you are plugged into. (This is probably the most common problem.)
∑ Make sure that you have the official version of NI VISA installed (this is NOT an obvious problem). Hereís a note from a user:
Turns out NI-VISA wasn't installed, but since TekVISA was (for our Tek scope) it didn't complain or warn me... just didn't work. Installed NI-VISA this am and now it looks good.
∑ Weíre still running LabView 2011. I donít THINK there should be any problems running a more recent version, but I have not checked. Iím guessing that if there is a problem, LabView would warn you about it, rather than just not run properly.
∑ Finally, there is an executable version of one of the programs on the LabView page. That should be independent of the version of LabView that you have. Install that and see if it works. If you donít have a NewStep controller, make sure to leave ďNewStep?Ē set to ďNoĒ.
∑ LabVIEW programs updated. Upgraded to LabVIEW 2011. Support for Newport NewStep rotation stages (NSR1). New vi to measure the polarization state of a single photon.
∑ Parts list updated.
∑ Inexpensive detectors are here! See this information.
Thanks to Blu-Ray DVD technology, lasers are finally cheap! I bought some 405 nm laser diodes for about $17 each (!!) from hightechdealz.com. The lasers I bought were model PHR803T, which were surplus from an HD DVD player. I managed to get 40mW of power by driving them with 100mA of current from an ILX Lightwave laser diode current source. I had them in a temperature controlled mount, but I wasnít using the active temperature controlóas long as theyíre well heat-sinked they should work fine. I could easily perform all of the experiments described on this site with this laser.
Only thing about these lasers were that the leads had been cut very short.† To get them to fit into my mount I had to solder longer leads on, but then they worked fine.
††††† I see that now there are even higher power lasers available from the same source.† Theyíll probably work as well.
Weíve developed some virtual laboratories.† Check them out here.
Entanglement with Dispersion Precompensation:
When trying to do experiments with polarization entangled photon pairs it is necessary that the two entangled states be as indistinguishable as possible. For the two crystal geometry that we use in our experiments this means that if one can determine, even in principle, which of the two crystals the photons were produced in, then there is some distinguishing information, and the degree of entanglement is reduced. This leads to a lesser violation of inequalities testing local realism. One in principle means for determining which crystal the photons are produced in is via their arrival time. For example, if photons produced in one crystal take longer to reach the detector than photons produced in the second, it is in principle possible to determine the photon polarization. As long as the time delay between the production times is much less than the temporal duration of the photons, entanglement will be preserved. The effective temporal duration of the downconverted photons is given by their coherence length, which is the inverse of their bandwidth.
One way that photons could be produced at different times in the two crystals would be if the blue pump took different times to reach the two crystals. Even though the pump is continuous, it has a finite bandwidth, and hence it also has a finite coherence length. In some sense this coherence length behaves like a pulse width for the pump. When the pump enters the first crystal it has polarization components in both the horizontal and vertical directions. Since this crystal is birefringent and dispersive, these polarization components will propagate at different speeds through the first crystal. The important velocity here is the group velocity, and what we are most interested in is the difference in group delay times between the two orthogonal polarizations of the pump. As long as the difference in group times is less than the coherence length of the downconverted photons then entanglement is preserved.
The finite bandwidth of the pump means that there is some mismatch in the group delays, but it's not large. It's not difficult to calculate, but I haven't bothered to do this calculation. However, I've found experimentally that while the entanglement in our experiments is degraded somewhat because of this effect, it's not enough to destroy the entanglement. The question is, how pure do you need? We are certainly able to easily violate local realism, even though the entanglement is somewhat degraded.
If you really need a very high purity source, then the best way to achieve this is to use a single-mode pump laser.
It's also possible to precompensate for the temporal walkoff by inserting a birefringent material in front of the downconversion crystal pair. I've tried this by using a piece of BBO that's the same thickness as each of the other crystals. It's oriented perpendicular to the first crystal of the pair. Thus, in the precompensating crystal the pump polarizations temporally walkoff. This crystal is well in front of the pair, so any photons produced here are not collected. In the first crystal of the pair the two pump polarizations come back together in time, so that they overlap at the interface between the two crystals of the pair, giving maximal entanglement. By precompensating in this way the entanglement is definitely improved. You can use this precompensation crystal in place of the quartz plate that adjusts the relative phase-- it can play both roles.
So, if you want better entanglement and have extra money you can buy a single BBO crystal that's as thick as one of your other crystals.
Lastly, I should note that I borrowed the idea for precompensation from Morgan Mitchell and Paul Kwiat.
Iíve had several people ask me about lasers. If
I were buying a laser now I'd probably go with one of the blue laser diodes
I know someone who has used the 60mW laser with success. The cost is about $2.2k for a bare laser. You'd need to get a separate current source (and I'd think about a temp controlled head and temp controller), probably from Thorlabs or ILX Lightwave (make sure you get a current source with a large enough compliance voltage for blue lasers). Despite this I think you'd save a thousand dollars or more over the Power Technology lasers I use, and you'd get a slightly more versatile system. Just be careful with static!
Updated LabView viís to use our new FPGA-based
Counting Unit page to reflect our new FPGA-based CCU.
Added course lecture notes and updated lab
Updated Labview viís.
The coincidence circuit is ready: email beckmk
at whitman.edu (replace "at" with @) to get the details.
Updated the LabView viís.† Now there are versions for LV 7 and LV 8.2.
Added an updated parts list to the main page.
∑ The coincidence circuit should be ready for general release by the end of the month.
Weíve tried the Power Technology 185mw
laser.† WOW!† LOTS of coincidences!† However, the jury is still out on the
achievable level of entanglement you can generate with this laser.† In tests of Bellís Inequality we are able to
get larger S values with the 50mW laser than the 185mW laser (although the
error is less with the 185mW laser, because we get more counts and thus better
statistics).† Weíre not sure if this is
just because itís a new laser to us, and we havenít spent much time working on
the alignment, or if itís something more fundamental with the laser
itself.† This 185mW laser does have
multiple spatial modes, and the beam is larger and more elliptical than our
circularized 50mw laser.
Our coincidence circuit is coming along.† Weíve done two prototypes which work quite
well.† Weíre currently working on a
version with improved time resolution.
Iíve added some new presentations on the entry page.
Iíve updated the LabView viís.
∑ Iíve made available a copy of the Lab Manual for the lab portion of our QM course.† This lab is being taught for the first time in the fall of 2006.
Weíre working on a circuit that makes
coincidence counting cheaper, and hope to have more to say about this in the
next few months.
Power Technology http://www.powertechnology.com/
now has 185mw, 405 nm laser diode modules available!†
The Bell inequality and Hardy test experiments
require making measurements at several different waveplate settings.† While itís not necessary to use a motorized
rotation stage for this, it does make things nicer.† Newport has recently released a relatively
low-cost motorized rotation stage, the NSR1.†
It uses the same Newstep controller that we use for the linear stepper
motor in the single-photon interference experiment.† Total cost to automate the waveplate movement
for these experiments would be about $2,600.†
I should note that I have never used these stages, so I canít personally
vouch for them.† They only have a
resolution of 1o, but thatís probably sufficient for these
∑ Iíve just released updated LabView viís for these experiments.† Included is a vi that allows one to mimic the behavior of a multichannel analyzer using an A/D board.
webpage updated 9/11/2015
†beckmk at whitman.edu (replace "at" with @)