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I'm planning on doing an (undergraduate-level) experiment to study Zeeman Splitting in Cadmium.
There's no complete set of instructions for the lab, but after seeing the materials, it appears that I will attempt to use a cylindrical Fabry-Perot Etalon to resolve the wavelength differences between light emitted from certain Cadmium transitions with/without a supplemental magnetic field, and then use that information to estimate the shifts in the energy states.
For preliminary reading, my instructor posted a paper describing a computational method for Fabry-Perot fringe analysis (Least squares algorithm for rapid analysis of Fabry–Perot fringe patterns, by O'Hora, Bowe, and Toal). This leads me to suspect that casting the interference pattern on a piece of graph paper and making measurements this way will not be sufficient to resolve the wavelength difference between light emitted from transitions with vs. without the presence of the external magnetic field. My instructor usually indicates optional readings quite clearly, and I'm aware that the change in the energy levels will be quite small, given the limits to the magnetic fields the equipment can generate. (Though I'm not sure how much the Fabry-Perot patterns can exacerbate small wavelength differences.)
I spent a summer working in an optics lab and worked on image processing and camera testing. There, we had cameras (ThorCam C1285R12M) that would output multipage TIFF files that I could then split and process with Mathematica. (Each individual image was then treated as a 1280x1024 matrix populated with 8-bit grayscale values.) We would frequently shine laser light into the camera sensor (with a filter screwed on) and capture images this way, rather than shining a laser onto a screen and taking a picture of that.
For my current experiment, I have no such specialized cameras, but I saw that Smartphone mounts were available for use with the optical breadboard. I don't think I'll be able to direct light directly into the smartphone camera lens, and I'm also uncertain if the presence of that extra lens of unknown characteristics could distort the image. The alternative would be casting the pattern on a screen and simply using the camera to take a picture of it, but then I'd have to deal with distortion due to the image being taken off of the optical axis. I believe I could use OpenCV to compensate for distortion of the image, but I'd prefer not to rely on that.
I do have my own camera (Sony Alpha 6000) with a removable lens. I'm wondering if I should remove the lens and place the camera in the path of the light (with the room lighting off). I have heard that shining a laser directly into a camera sensor without filtering can cause damage, but this is not a laser. It is a cadmium lamp, and the light will interact with a quartz Fabry-Perot etalon before reaching the camera.
My camera can take RAWs without automatic corrections for vignetting and other such things. I think I should be able to work with these similar to how I did with TIFFs in Mathematica, except these will not be in grayscale.
I'm mainly hoping to get much closer to having the sensor normal to the optical axis. I've also thought about using photosensitive paper and developing it as a photo to scan, but I believe that would take too long.I don't expect to be able to figure out all the answers before I actually get into the experiment, but I'd appreciate any guidance to avoid damaging equipment. Thanks for any advice.
There's no complete set of instructions for the lab, but after seeing the materials, it appears that I will attempt to use a cylindrical Fabry-Perot Etalon to resolve the wavelength differences between light emitted from certain Cadmium transitions with/without a supplemental magnetic field, and then use that information to estimate the shifts in the energy states.
For preliminary reading, my instructor posted a paper describing a computational method for Fabry-Perot fringe analysis (Least squares algorithm for rapid analysis of Fabry–Perot fringe patterns, by O'Hora, Bowe, and Toal). This leads me to suspect that casting the interference pattern on a piece of graph paper and making measurements this way will not be sufficient to resolve the wavelength difference between light emitted from transitions with vs. without the presence of the external magnetic field. My instructor usually indicates optional readings quite clearly, and I'm aware that the change in the energy levels will be quite small, given the limits to the magnetic fields the equipment can generate. (Though I'm not sure how much the Fabry-Perot patterns can exacerbate small wavelength differences.)
I spent a summer working in an optics lab and worked on image processing and camera testing. There, we had cameras (ThorCam C1285R12M) that would output multipage TIFF files that I could then split and process with Mathematica. (Each individual image was then treated as a 1280x1024 matrix populated with 8-bit grayscale values.) We would frequently shine laser light into the camera sensor (with a filter screwed on) and capture images this way, rather than shining a laser onto a screen and taking a picture of that.
For my current experiment, I have no such specialized cameras, but I saw that Smartphone mounts were available for use with the optical breadboard. I don't think I'll be able to direct light directly into the smartphone camera lens, and I'm also uncertain if the presence of that extra lens of unknown characteristics could distort the image. The alternative would be casting the pattern on a screen and simply using the camera to take a picture of it, but then I'd have to deal with distortion due to the image being taken off of the optical axis. I believe I could use OpenCV to compensate for distortion of the image, but I'd prefer not to rely on that.
I do have my own camera (Sony Alpha 6000) with a removable lens. I'm wondering if I should remove the lens and place the camera in the path of the light (with the room lighting off). I have heard that shining a laser directly into a camera sensor without filtering can cause damage, but this is not a laser. It is a cadmium lamp, and the light will interact with a quartz Fabry-Perot etalon before reaching the camera.
My camera can take RAWs without automatic corrections for vignetting and other such things. I think I should be able to work with these similar to how I did with TIFFs in Mathematica, except these will not be in grayscale.
I'm mainly hoping to get much closer to having the sensor normal to the optical axis. I've also thought about using photosensitive paper and developing it as a photo to scan, but I believe that would take too long.I don't expect to be able to figure out all the answers before I actually get into the experiment, but I'd appreciate any guidance to avoid damaging equipment. Thanks for any advice.