Difference between revisions of "Astronomical Spectroscopy"

From Advanced Projects Lab
Jump to: navigation, search
 
(37 intermediate revisions by 2 users not shown)
Line 1: Line 1:
The overall goal of the Astronomical Spectroscopy Project is to be able to collect and reduce data gathered from astronomical objects. This will be done using a Celestron CPC 800 GPS (XLT) telescope and a fiber-fed Ocean Optics USB2000+ spectrometer. The initial setup at the beginning of Fall term consisted of the telescope with a beam splitter and lens tube system attached to the back. The beam splitter attached to an eyepiece on top and a lens tube at the back with a converging lens and the fiber attached at the end of the lens tube. The fiber was attached using a fiber adapter with thumb screws which gave three degrees of freedom for the fiber: 1 along the z axis where the length of the lens tube can be changed on the outside, and 2 and 3 along the x and y axis where the position of the fiber can be adjusted using the two thumb screws.
+
== Astronomical Spectroscopy Project ==
  
The overall goal of the Astronomical Spectroscopy Project is to be able to collect and reduce data gathered from astronomical objects. This will be done using a Celestron CPC 800 GPS (XLT) telescope and a fiber-fed Ocean Optics USB2000+ spectrometer. The initial setup at the beginning of Fall term consisted of the telescope with a beam splitter and lens tube system attached to the back. The beam splitter attached to an eyepiece on top and a lens tube at the back with a converging lens and the fiber attached at the end of the lens tube.
+
[http://hank.uoregon.edu/experiments/Astronomical-Spectroscopy/astro.html Astronomical Spectroscopy Web Page]
The fiber was attached using a fiber adapter with thumb screws which gave three degrees of freedom for the fiber: 1 along the z axis where the length of the lens tube can be changed on the outside, and 2 and 3 along the x and y axis where the position of the fiber can be adjusted using the two thumb screws.
 
  
This term, the current students on the project (Annika Gustafsson, Justin Stockwell, and Gerald Buxton) set goals of working to improve the spectrometer-telescope setup to rule out some of these factors. The first goal was to improve the T-adapter by replacing the beam splitter with a flip mirror. In the first 2 weeks, we ordered a flip mirror, machined an adapter for the lens tube to connect to the flip mirror, and began initial lab table setup. The flip mirror replaced the beam splitter in the fiber adapter, allowing us to retain all of the light coming through the back of the telescope instead of dividing it 50:50 between the fiber and the eyepiece. With the fiber adapter assembled using the newly machined adapter between the lens tube and flip mirror, we were able to begin moving forward and design the lab table setup. We wanted to calculate an efficiency measurement for the simplest system possible, which we would design on a lab table, and compare that to an efficiency measurement of light through our entire telescope system. The purpose of having the simplest lab table setup was to eliminate as many opportunities for light loss as possible and to calculate a maximum efficiency. This number would be equivalent to the efficiency through our telescope system if we had 100% efficiency.  
+
The overall goal of the Astronomical Spectroscopy Project is to be able to collect and reduce data gathered from astronomical objects. Before spectra can be collected, the system needs to be prepared. This preparation involves aligning the telescope-fiber system and calculating the efficiency of the ratio to determine that the project is feasible with the current setup.  
  
Initially, for our lab table setup, we used a red laser with known power and wavelength and aligned it directly down a multimode fiber using a converging lens with the fiber attached directly to the spectrometer. We wanted to calculate the total energy received by the spectrometer using the conversion 61 photons/count at 600 nm given by Ocean Optics. Then, we would compare our calculated energy with the 1mW power given off by the laser to find our efficiency. However, data measurements revealed a loss of light that was about a factor of 10,000 less than that emitted by the laser. We went back and checked the power emitted by the laser, which we confirmed as 1mW. We also checked the numerical aperture of our setup to rule out loss of light due to that reason, however, our focal distance was large enough that it would not have played any effect. Thus, we concluded that the lab table setup had too many places for light loss and there were not enough ways to do fine alignment on the fiber.
 
  
With the guidance of Bryan Boggs, we changed the lab table setup to allow for the possibility of doing fine alignment on the fiber. The setup consisted of the laser emitted through an iris to a converging lens, and directed into the fiber using two square mirrors with thumb screws for fine alignment. The focal distance of the lens was large enough to be in agreement with the numerical aperture of our fiber. We were able to track power loss through the system using the hand held power meter and found that the power at the fiber was about 0.7mW. We also took spectra of our data and gathered a bias frame which we would later subtract off of our data.
 
  
Next, we wanted to work on calculating the efficiency of the entire telescope system. However, we first needed to align the system before we could take any measurements. We began our alignment process by first aligning the eyepiece to the finderscope. We did this alignment in the Willamette basement hallway by placing the telescope at one end of the hallway and aligning the telescope on an Oregon O which was over 100 feet away. Once the O was placed directly on the crosshairs in the eyepiece, we adjusted the finderscope so that it was also perfectly aligned in the crosshairs. Then, we needed to align the fiber to the eyepiece. We began with a similar setup in the Willamette basement hallway. We placed the telescope at one end of the hallway and a hydrogen spectral lamp at the other end. Again, we aligned the hydrogen lamp on the optical axis of the telescope so that it was perfectly in the crosshairs of the eyepiece. With the fiber connected to the spectrometer, we had a nice hydrogen spectra to view in SpectraSuite.
+
The current setup for the project involves a Celestron CPC 800 GPS (XLT) telescope and a fiber-fed Ocean Optics USB2000+ spectrometer.
  
We used this spectra to check the alignment of the fiber. By changing the x, y, and z axes we can maximize the number of counts in the main hydrogen spectral peak. When the counts are maximized, we know that our system is perfectly aligned. We began by adjusting the z axis. The distance of the fiber is changed by altering the length of the lens tube. We started with the lens tube completely screwed in and then slowly unscrewed the lens tube, increasing the length. We noticed that each full turn we would get a max counts and they were roughly the same each full turn. We decided to settle on a distance that was close to the focal distance of our converging lens where we had a max counts. Then, we proceeded to adjust the x and y axes by rotating the thumb screws on the fiber adapter. We found that max counts was when the thumb screws were all the way screwed in. However, we noticed that we had a difficult time returning to a specific max counts number. Even if when we were super careful and tedious, there was variance in the max counts number when we would move the fiber and then try to return it to the previous position. We also noticed how the flexure in our fiber system changed the counts by a couple hundred counts just lifting the fiber up and down.
+
[[File:TelescopeSystem.png]]  [[File:TAdapter.png]]
  
We decided to change our procedure after talking with Bryan Boggs. Bryan recommended that we move our setup to a dark room, such as Willamette 100, where we have an LED on one end of the room and our telescope system on the other. We can measure the power given by the LED that has gone through the back of the telescope. Then, we can calculate the power through the entire telescope system out of the end of the fiber. This power should be 70-80% of the power received through just the telescope. We can fine align the fiber setup until we get a power that is 70-80% of the initial power.
 
So, we went forward with the recommended procedure. We first ran into trouble when the power meter would not pick up our LED. After messing around with the power meter and calibrating it a couple of times, we finally got some measurements. We measured a power of 4.8 microwatts through the back of the telescope and 17 nanowatts through the entire telescope system with the fiber as best aligned as we could get. We calculated that we were losing 99% of the light through our telescope system. We were very surprised by this, so we decided to try to determine where the problem was. We took the T-adapter off of the telescope and used a piece of paper to find the focal point of the light. We found the focal point was 14.5cm from the back of the telescope. On our T-adapter, 14.5cm is right after the flip mirror, so the light is being focused way too fast. We then tried to replace our converging lens with one that converged much slower. We chose a 100cm converging lens placed as close to the flip mirror as possible and the light still focused far before the fiber. Next, we tried to use a diverging lens with a converging lens to see if we could get the light to focus slower, but we were unsuccessful, and the light still focused far before the fiber. The best solution to this problem would be to use Optica and determine exactly what the light is doing in our T-adapter because we need to change the setup so that we can have the light focused directly onto the fiber.
 
  
Going forward next term, we propose that Optica should be the first goal. Once we have a visual of what is going on in the T-adapter, we can get the light to focus on the fiber. Then, we can return to our previous procedure where we want to align the fiber to the eyepiece using the power meter. Once the system has been successfully aligned, we can calculate an efficiency ratio of the entire telescope system and continue to characterize the spectrometer. The overall goal of the project at this point in time is to determine if it is feasible to use this spectrometer for astronomical purposes.
+
Efficiency of the more basic system is calculated using a lab table procedure. An efficiency of the entire telescope system can be used in comparison to create an efficiency ratio of the system.
 +
 
 +
[[File:LabTableSetup.png]]
 +
 
 +
 
 +
All of the telescope alignment takes place at long distances greater than the focal distance of the telescope, like the Willamette Basement Hallways. Here, the finderscope is being aligned to the eyepiece.
 +
 
 +
[[File:AligningTelescope.png]]
 +
 
 +
 
 +
The fiber alignment process, which involves aligning the fiber to the eyepiece, is the most difficult part of the preparation. This is done in large areas as well, including the Willamette Basement Hallways, but dark rooms like Willamette 100 have given the best results.
 +
 
 +
[[File:AligningFiber.png]]
 +
 
 +
 
 +
Data is collected during the alignment process to track the max number of counts read by the spectrometer.
 +
 
 +
[[File:AlignmentData.png]]
 +
 
 +
 
 +
 
 +
The furthest progress that has been made on the project is successfully getting a spectra of Vega using the SpectraSuite software. However, the integration time used to get the spectra was 60 seconds with a scans to average of 10, and box car smoothing of 10.
 +
 
 +
[[File:Vega.png]]
 +
 
 +
 
 +
'''Winter 2014'''
 +
During the winter term of 2014 the Astronomical Spectroscopy group, comprised of Gerald Buxton, William McNichols, and Justin Stockwell, made some good headway in determining how best to rebuild the fiber setup.  To do so we focused on precisely determining the visual spot size of a calibrated beam coming out of the telescope.  This was done through the use of a calibrated light source placed across the room and a beam profiler. Our results form this test are shown below.
 +
 
 +
              [[File:Beam Profile Winter 2014.jpg|750px]]
 +
 
 +
The key measurement needed to determine the feasibility of our setup is the Effective Beam Diameter.  This measurement measures the number of pixels above a Clip Level of 1%.  This effectively means that 99% of the light is focused into a spot with a precise diameter of 656nm. Our fiber size is 600nm so we are able to capture almost the entire amount of light from a calibrated light source. 
 +
 
 +
We also were able to effectively determine the focal distance of our telescope.  This will allow us to build a new fiber adapter to place the fiber mount at the focal distance of the telescope.  With this information we no longer need a focusing mirror, instead we can use the telescope itself to focus the light into our fiber/spectrometer setup
 +
 
 +
Next term we plan on using the information gleaned from the beam profiler to rebuild our fiber adapter setup. This should allow us to couple at least 80% of the incoming light into our fiber, which is far better than the 1.1% we were coupling during the Fall term.  We need to machine a new adapter that directly attaches the flip mirror to the telescope, as well adapter that couples the fiber with the flip mirror at an approximate distance of 11.88cm from the back of the telescope.  With these adapters built, we should be able to take advantage of the nicer weather and get some better spectra of some astronomical objects.
 +
 
 +
'''Spring 2014'''
 +
This term we focused once again on using the beam profiler to determine minimum spot size coming through our telescope.  But this time we wanted to see how the back focus knob affected the the focal distance of our telescope.  We set up the profiler setup exactly as we had done it during Winter term with a calibrated L.E.D light source across the room, and the beam profiler set on the stands behind the telescope. This time, however, we placed the profiler on a sliding base that way we could see how the spot size changed as we adjusted the focus knob. Using this setup we discovered that our minimum spot size was 177um which is far better than the 656um we were able to achieve last term, and is well within the 600um core size of our fiber.  Therefore with proper alignment we should be able to couple 100% of the incoming light through our telescope.  We also discovered that were able to change the back focal distance substantially by turning the focus knob.  Just 12 full turns increased the back focal distance to 48.5cm. 
 +
                                          [[File:Beam Profile Near Screenshot Spring 2014.png|750px]]   
 +
 
 +
We also wanted to determine the overall efficiency our our spectrometer.  That is, we wanted to determine a photons/count number at a particular wavelength.  To do this we used a laser setup that consisted of a laser, a converging lens, two focusing aluminum plates, three neutral density filters and then our fiber fed spectrometer. This set up looks like this.
 +
                                          [[File:Laser Setup 2 Fall 2013.jpg|350px]]
 +
Through the use of a power meter we were able to a power meter we were able to accurately determine the laser thruput coming out of our fiber.  Then by converting that power into number of photons/second we were able to compare that with the number of counts recorded by our spectrometer. The math for this is shown below.
 +
                                          [[File:20140612_161231.jpg|350px]]
 +
This showed that it was taking nearly 1850 photons at 634nm to record one count.  This poor result may be an indication that the spectrometer we're using is not suitable for the high signal=to=noise, low signal that we get from observing stars.
 +
 
 +
The last thing we did was actually take the telescope out to observe. This allowed us to get a functional understanding of observation, and allowed us to figure out how to couple our telescope with the computer program Stellarium. This process is fully detailed in the new Observational Astronomy wiki under the advanced Projects tab.  A couple of our results are shown below.
 +
                        [[File:20140612_000609.jpg|350px]][[File:Saturn Spring 2014.jpg|350px]]
 +
 
 +
'''Presentations:'''
 +
 
 +
[https://docs.google.com/presentation/d/12X-PH-YWL5QNGBpAwOIU7EYMS1AtcNG7aff_62sN-rE/edit#slide=id.p Spring2013]
 +
 
 +
[https://docs.google.com/presentation/d/1IBA_8ghSto6H9ivADDnq0qd3YHWw_VMEhpLkqUiVbXs/edit#slide=id.p9 Fall2013]
 +
 
 +
 
 +
 
 +
 
 +
'''Links:'''
 +
 
 +
[http://www.oceanoptics.com/products/usb2000+.asp Ocean Optics Spectrometer]
 +
 
 +
[http://www.celestron.com/astronomy/celestron-cpc-800-gps-xlt.html Celestron Telescope]
 +
 
 +
[http://en.wikipedia.org/wiki/Spectrometer Wiki- Spectrometer]
 +
 
 +
[http://en.wikipedia.org/wiki/Astronomical_spectroscopy Wiki-Astronomical Spectroscopy]

Latest revision as of 10:27, 24 November 2014

Astronomical Spectroscopy Project

Astronomical Spectroscopy Web Page

The overall goal of the Astronomical Spectroscopy Project is to be able to collect and reduce data gathered from astronomical objects. Before spectra can be collected, the system needs to be prepared. This preparation involves aligning the telescope-fiber system and calculating the efficiency of the ratio to determine that the project is feasible with the current setup.


The current setup for the project involves a Celestron CPC 800 GPS (XLT) telescope and a fiber-fed Ocean Optics USB2000+ spectrometer.

TelescopeSystem.png TAdapter.png


Efficiency of the more basic system is calculated using a lab table procedure. An efficiency of the entire telescope system can be used in comparison to create an efficiency ratio of the system.

LabTableSetup.png


All of the telescope alignment takes place at long distances greater than the focal distance of the telescope, like the Willamette Basement Hallways. Here, the finderscope is being aligned to the eyepiece.

AligningTelescope.png


The fiber alignment process, which involves aligning the fiber to the eyepiece, is the most difficult part of the preparation. This is done in large areas as well, including the Willamette Basement Hallways, but dark rooms like Willamette 100 have given the best results.

AligningFiber.png


Data is collected during the alignment process to track the max number of counts read by the spectrometer.

AlignmentData.png


The furthest progress that has been made on the project is successfully getting a spectra of Vega using the SpectraSuite software. However, the integration time used to get the spectra was 60 seconds with a scans to average of 10, and box car smoothing of 10.

Vega.png


Winter 2014 During the winter term of 2014 the Astronomical Spectroscopy group, comprised of Gerald Buxton, William McNichols, and Justin Stockwell, made some good headway in determining how best to rebuild the fiber setup. To do so we focused on precisely determining the visual spot size of a calibrated beam coming out of the telescope. This was done through the use of a calibrated light source placed across the room and a beam profiler. Our results form this test are shown below.

              Beam Profile Winter 2014.jpg

The key measurement needed to determine the feasibility of our setup is the Effective Beam Diameter. This measurement measures the number of pixels above a Clip Level of 1%. This effectively means that 99% of the light is focused into a spot with a precise diameter of 656nm. Our fiber size is 600nm so we are able to capture almost the entire amount of light from a calibrated light source.

We also were able to effectively determine the focal distance of our telescope. This will allow us to build a new fiber adapter to place the fiber mount at the focal distance of the telescope. With this information we no longer need a focusing mirror, instead we can use the telescope itself to focus the light into our fiber/spectrometer setup

Next term we plan on using the information gleaned from the beam profiler to rebuild our fiber adapter setup. This should allow us to couple at least 80% of the incoming light into our fiber, which is far better than the 1.1% we were coupling during the Fall term. We need to machine a new adapter that directly attaches the flip mirror to the telescope, as well adapter that couples the fiber with the flip mirror at an approximate distance of 11.88cm from the back of the telescope. With these adapters built, we should be able to take advantage of the nicer weather and get some better spectra of some astronomical objects.

Spring 2014 This term we focused once again on using the beam profiler to determine minimum spot size coming through our telescope. But this time we wanted to see how the back focus knob affected the the focal distance of our telescope. We set up the profiler setup exactly as we had done it during Winter term with a calibrated L.E.D light source across the room, and the beam profiler set on the stands behind the telescope. This time, however, we placed the profiler on a sliding base that way we could see how the spot size changed as we adjusted the focus knob. Using this setup we discovered that our minimum spot size was 177um which is far better than the 656um we were able to achieve last term, and is well within the 600um core size of our fiber. Therefore with proper alignment we should be able to couple 100% of the incoming light through our telescope. We also discovered that were able to change the back focal distance substantially by turning the focus knob. Just 12 full turns increased the back focal distance to 48.5cm.

                                         Beam Profile Near Screenshot Spring 2014.png    

We also wanted to determine the overall efficiency our our spectrometer. That is, we wanted to determine a photons/count number at a particular wavelength. To do this we used a laser setup that consisted of a laser, a converging lens, two focusing aluminum plates, three neutral density filters and then our fiber fed spectrometer. This set up looks like this.

                                         Laser Setup 2 Fall 2013.jpg

Through the use of a power meter we were able to a power meter we were able to accurately determine the laser thruput coming out of our fiber. Then by converting that power into number of photons/second we were able to compare that with the number of counts recorded by our spectrometer. The math for this is shown below.

                                         20140612 161231.jpg

This showed that it was taking nearly 1850 photons at 634nm to record one count. This poor result may be an indication that the spectrometer we're using is not suitable for the high signal=to=noise, low signal that we get from observing stars.

The last thing we did was actually take the telescope out to observe. This allowed us to get a functional understanding of observation, and allowed us to figure out how to couple our telescope with the computer program Stellarium. This process is fully detailed in the new Observational Astronomy wiki under the advanced Projects tab. A couple of our results are shown below.

                        20140612 000609.jpgSaturn Spring 2014.jpg

Presentations:

Spring2013

Fall2013



Links:

Ocean Optics Spectrometer

Celestron Telescope

Wiki- Spectrometer

Wiki-Astronomical Spectroscopy