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Simple Multiwavelength Time-Division Multiplexed Light Source for Sensing Applications Thilo Kraetschmer and Scott Sanders Engine Research Center Department of Mechanical Engineering University of Wisconsin 14 th Gordon Research Conference August 12, 2007
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MotivationDesignResultsConclusions 14 th GRC 2007 2 Outline Motivation How this laser works Experimental results Comparison to multiplexed diode lasers
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MotivationDesignResultsConclusions 14 th GRC 2007 3 Sample Light Source Detector Light Source Detector Sample Time Division Multiplexing (TDM)
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MotivationDesignResultsConclusions 14 th GRC 2007 4 Desired optical output 00.511.522.533.544.5 0 0.2 0.4 0.6 0.8 1 Time [ s] Signal [V] 1 2 3...... 17 18 19 A sequence of pulses, each at a unique wavelength
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MotivationDesignResultsConclusions 14 th GRC 2007 5 Understanding the laser design BOA* time p o w e r p o w e r 4-step upgrade from a CW fiber laser to a 2-color TDM source *Booster optical amplifier, a form of semiconductor optical amplifier:
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MotivationDesignResultsConclusions 14 th GRC 2007 6 Step 1: Replace mirrors with Bragg gratings time p o w e r p o w e r Customization of laser wavelength, linewidth BOAFBG
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MotivationDesignResultsConclusions 14 th GRC 2007 7 Step 2: Pulsed operation time p o w e r p o w e r BOAFBG 1 period L R FBG Pulsed operation
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MotivationDesignResultsConclusions 14 th GRC 2007 8 Step 3: Add second grating pair time p o w e r p o w e r BOAFBG 1 period Pulsed operation at an additional wavelength with a modified pulse pattern L R
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MotivationDesignResultsConclusions 14 th GRC 2007 9 Step 4: Use the same gratings on both ends time p o w e r p o w e r BOA FBG 1 period Still a linear cavity laser, enforced within ring arrangement by the pulse pattern
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MotivationDesignResultsConclusions 14 th GRC 2007 10 Animation of 3-color TDM source for animation: right click on the figure, select play
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MotivationDesignResultsConclusions 14 th GRC 2007 11 distance [m] time [s] x-t diagram familiar to gasdynamicists Color-map of density in a shock tube experiment: He-air-CO 2, M = 2.5
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MotivationDesignResultsConclusions 14 th GRC 2007 12 TDM source x-t diagram ASE only, no FBGs
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MotivationDesignResultsConclusions 14 th GRC 2007 13 Main reflections only, 3 FBGs TDM source x-t diagram
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MotivationDesignResultsConclusions 14 th GRC 2007 14 All signals, 3 FBGs TDM source x-t diagram
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MotivationDesignResultsConclusions 14 th GRC 2007 15 Schematic of 19-color realization fiber roundtrip length ~ 3 km repetition rate ~ 66 kHz
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MotivationDesignResultsConclusions 14 th GRC 2007 16 00.511.522.533.544.5 0 0.2 0.4 0.6 0.8 1 Time [ s] Signal [V] 1 2 3...... 17 18 19 Experimental Results Time trace of TDM output 19 pulses of ~ 200 ns duration Optical power is ~ 10 mW during each pulse
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MotivationDesignResultsConclusions 14 th GRC 2007 17 Experimental Results Spectrum of TDM output the gain of each wavelength was adjusted to obtain a flat output spectrum the active linewidth is ~ 5 times narrower than the passive linewidth
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MotivationDesignResultsConclusions 14 th GRC 2007 18 13301335134013451350135513601365137013751380 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Wavelength [nm] Spectral Power [a.u.] Experimental Results Spectrum of TDM output the BOA injection current pulse pattern was customized to form a ramped output spectrum
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MotivationDesignResultsConclusions 14 th GRC 2007 19 Experimental Results High-speed detection strategy
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MotivationDesignResultsConclusions 14 th GRC 2007 20 012345678910 0 0.2 0.4 0.6 0.8 1 Time [ s] Signal [V] Experimental Results Liquid phase Methanol, I and I o
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MotivationDesignResultsConclusions 14 th GRC 2007 21 Experimental Results Measured spectra of Methanol and Isopropanol single shot measurement 66 kHz rep. rate standard deviation of 100 consecutive shots: ~0.0013
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MotivationDesignResultsConclusions 14 th GRC 2007 22 Laser features no moving parts individual tunability of each wavelength (typ: 1 nm) narrow spectral linewidth of each channel (< 1 GHz) small longterm spectral drift of each channel (< 1 GHz) fiber coupled output, typical in 10 – 100 mW range To build this laser you need only: gain medium (preferably with a broad gain bandwidth and fast switching times) custom waveform generator applying modulation (preferably to the gain medium) matched compressor / stretcher (preferably as part of a long laser cavity)
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MotivationDesignResultsConclusions 14 th GRC 2007 23 Comparison to Multiplexed Diode Lasers Advantages of TDM source over multiplexed diode lasers 1.straightforward to reach high wavelength count N: 100s to 1000s 2.single gain medium (for N wavelengths that lie within the gain bandwidth of a single gain medium) 3.modulation decoupled from wavelength-selective element 4.no external couplers / multiplexers needed 5.simple and stable wavelength control 6.broad tunability 7.more options for custom-wavelength lasers 8.opportunities for high-power lasers Advantages of multiplexed diode lasers over TDM source 1.long fiber not required 2.some diode lasers are very inexpensive 3.direct scanning by current modulation Questions?
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MotivationDesignResultsConclusions 14 th GRC 2007 24
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MotivationDesignResultsConclusions 14 th GRC 2007 25 The original 19 wavelengths were chosen to align with H2O peaks – now we choose the N wavelengths differently
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