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Automation of Swept
Wavelength Spectroscopy
using Python
Trishul Nagenalli
Background
Measurement of Optical Frequencies
 A NIST - oriented objective to my program
 Optical Signals cannot be measured directly because they are
of extremely high frequency
Frequency Combs
 Present a way to measure optical frequencies by creating an “optical
ruler”, a precise spectrum of light
 𝑓0  Offset Frequency
 𝑓𝑟  Interval between
adjacent frequencies
 𝑣 𝑛  Arbitrary wave in
a frequency comb
Optical Microresonators
 Optical microresonators are micrometer scale devices capable
of confining light to the scale of a cubic wavelength
 They can be used to create frequency combs if a resonant
wavelength is used.
Resonance
 In small containers, light
can only exist if the
container’s length is an
integer multiple of the
light’s wavelength.
 The container is a
“resonator” and can only
contain very specific
wavelengths of light.
Optical Microresonators
 Optical microresonators are micrometer scale devices capable
of confining light to the scale of a cubic wavelength
 They can be used to create frequency combs if a resonant
wavelength is used.
Resonance in Microresonators
 If light exists within the ring,
the ring’s circumference
must be evenly divisible
by the light’s wavelength.
 We are using ring-resonators
 If the above condition is
met, light forms a closed
loop within the ring
 If not, the light bypasses
the ring altogether.
Finding Resonance
1. Use a laser to test a specific wavelength on a resonator
2. If the wavelength is not in resonance, it cannot exist within the
resonator, and the photodetector signal will be full strength
3. If the wavelength is in resonance, light will enter the resonator,
and the photodetector signal will drop
Finding Resonance With Computers
1. A Data Acquisition (DAQ) Card sends a signal to the laser forcing it
to a specific wavelength.
2. The DAQ Card reads the photodetector signal and displays a graph
Objectives of Final Application
1. Conduct sweeps over broad wavelength ranges (tens
of nanometers)
2. Allow researcher to manually adjust laser position into
resonance
3. Conduct fine sweeps in the neighborhood of the
resonance (tens of picometers)
Methods
Current Methods: LabVIEW
 A visual programming
language
 Designed for scientific
experiments by
National Instruments
 Required to use
interface of controls
given by LabVIEW
Benefits of Using Python
 A text-based programming language that is more familiar to the
researchers
 Allows direct interfacing with laser motor, is more versatile
 Fully customizable interface
 Continually updatable and open-source
Components of Experiment
 Tunable DC Motor Laser
 Internal DC motor must be directly
programmable using voltage signals
 Photodetector
Sends voltage signals to DAQ Card
 Data Acquisition Card (DAQ Card)
Device to send and receive voltage
signals
DAQ CARD Abilities
 Change voltage of output pins with following parameters
Array of points to send
Rate to move from point to point
 Sample voltage on input pins and save data into an array
Array must be passed as a parameter
Rate of sampling must be specified
DAQ Card Limitations
 DAQ Card cannot synchronize sending and receiving signals to
the same clock
Poses a challenge that must be solved by the program
Algorithm
 This is a graph of the outgoing voltage signal as given by the
LOOPBACK CHANNEL
Algorithm
 The DAQ Card will be listening to the photodetector signal in
between the green lines
Algorithm
 The orange line is the photodetector signal. The two dips represent
resonances (one time passing it forward, one time backwards)
Algorithm
 Using the loopback
channel, we
determine the start
of the sweep by
checking the
difference between
two consecutive
outgoing values.
 Then we pair it with
the corresponding
point in the
photodetector
signal
Algorithm
 The orange line is the photodetector signal. The two dips represent
resonances (one time passing it forward, one time backwards)
Final Application
Conclusions
 All initial objectives have been met
1. Conduct sweeps over broad wavelength ranges (tens of
nanometers)
2. Allow researcher to manually adjust laser position into
resonance
3. Conduct fine sweeps in the neighborhood of the resonance
(tens of picometers)
 Also able to save data in csv files
Future Work
 Resonance shifts to the
right when working with
high intensity light
 Very difficult to land on
backside of resonance
 Must experiment with
different wavelength
approach speeds and
patterns to stop on
backside of resonance
Acknowledgements
 Dr. Kartik Srinivasan, my mentor
 Dr. Miller & Mr. Lee, my SRP Teachers
 My friends and family
Thank You!

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NIST_Presentation

  • 1. Automation of Swept Wavelength Spectroscopy using Python Trishul Nagenalli
  • 3. Measurement of Optical Frequencies  A NIST - oriented objective to my program  Optical Signals cannot be measured directly because they are of extremely high frequency
  • 4. Frequency Combs  Present a way to measure optical frequencies by creating an “optical ruler”, a precise spectrum of light  𝑓0  Offset Frequency  𝑓𝑟  Interval between adjacent frequencies  𝑣 𝑛  Arbitrary wave in a frequency comb
  • 5. Optical Microresonators  Optical microresonators are micrometer scale devices capable of confining light to the scale of a cubic wavelength  They can be used to create frequency combs if a resonant wavelength is used.
  • 6. Resonance  In small containers, light can only exist if the container’s length is an integer multiple of the light’s wavelength.  The container is a “resonator” and can only contain very specific wavelengths of light.
  • 7. Optical Microresonators  Optical microresonators are micrometer scale devices capable of confining light to the scale of a cubic wavelength  They can be used to create frequency combs if a resonant wavelength is used.
  • 8. Resonance in Microresonators  If light exists within the ring, the ring’s circumference must be evenly divisible by the light’s wavelength.  We are using ring-resonators  If the above condition is met, light forms a closed loop within the ring  If not, the light bypasses the ring altogether.
  • 9. Finding Resonance 1. Use a laser to test a specific wavelength on a resonator 2. If the wavelength is not in resonance, it cannot exist within the resonator, and the photodetector signal will be full strength 3. If the wavelength is in resonance, light will enter the resonator, and the photodetector signal will drop
  • 10. Finding Resonance With Computers 1. A Data Acquisition (DAQ) Card sends a signal to the laser forcing it to a specific wavelength. 2. The DAQ Card reads the photodetector signal and displays a graph
  • 11. Objectives of Final Application 1. Conduct sweeps over broad wavelength ranges (tens of nanometers) 2. Allow researcher to manually adjust laser position into resonance 3. Conduct fine sweeps in the neighborhood of the resonance (tens of picometers)
  • 13. Current Methods: LabVIEW  A visual programming language  Designed for scientific experiments by National Instruments  Required to use interface of controls given by LabVIEW
  • 14. Benefits of Using Python  A text-based programming language that is more familiar to the researchers  Allows direct interfacing with laser motor, is more versatile  Fully customizable interface  Continually updatable and open-source
  • 15. Components of Experiment  Tunable DC Motor Laser  Internal DC motor must be directly programmable using voltage signals  Photodetector Sends voltage signals to DAQ Card  Data Acquisition Card (DAQ Card) Device to send and receive voltage signals
  • 16. DAQ CARD Abilities  Change voltage of output pins with following parameters Array of points to send Rate to move from point to point  Sample voltage on input pins and save data into an array Array must be passed as a parameter Rate of sampling must be specified
  • 17. DAQ Card Limitations  DAQ Card cannot synchronize sending and receiving signals to the same clock Poses a challenge that must be solved by the program
  • 18. Algorithm  This is a graph of the outgoing voltage signal as given by the LOOPBACK CHANNEL
  • 19. Algorithm  The DAQ Card will be listening to the photodetector signal in between the green lines
  • 20. Algorithm  The orange line is the photodetector signal. The two dips represent resonances (one time passing it forward, one time backwards)
  • 21. Algorithm  Using the loopback channel, we determine the start of the sweep by checking the difference between two consecutive outgoing values.  Then we pair it with the corresponding point in the photodetector signal
  • 22. Algorithm  The orange line is the photodetector signal. The two dips represent resonances (one time passing it forward, one time backwards)
  • 24.
  • 25. Conclusions  All initial objectives have been met 1. Conduct sweeps over broad wavelength ranges (tens of nanometers) 2. Allow researcher to manually adjust laser position into resonance 3. Conduct fine sweeps in the neighborhood of the resonance (tens of picometers)  Also able to save data in csv files
  • 26. Future Work  Resonance shifts to the right when working with high intensity light  Very difficult to land on backside of resonance  Must experiment with different wavelength approach speeds and patterns to stop on backside of resonance
  • 27. Acknowledgements  Dr. Kartik Srinivasan, my mentor  Dr. Miller & Mr. Lee, my SRP Teachers  My friends and family