+ All Categories
Home > Documents > Simple Multiwavelength Time-Division Multiplexed Light Source for Sensing Applications Thilo...

Simple Multiwavelength Time-Division Multiplexed Light Source for Sensing Applications Thilo...

Date post: 04-Jan-2016
Category:
Upload: antony-riley
View: 214 times
Download: 0 times
Share this document with a friend
25
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
Transcript

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

14th Gordon Research Conference

August 12, 2007

ConclusionsResultsDesignMotivation 214th GRC 2007

Outline

Motivation

How this laser works

Experimental results

Comparison to multiplexed diode lasers

ConclusionsResultsDesignMotivation 314th GRC 2007

SampleLight Source

Detector

Light Source

Detector

Sample

Time Division Multiplexing (TDM)

ConclusionsResultsDesignMotivation 414th GRC 2007

Desired optical output

1330 1340 1350 1360 1370 138010

-11

10-10

10-9

10-8

10-7

10-6

Wavelength [nm]

Spe

ctra

l Pow

er [a

.u.]

1 2 3 ... ... 17 18 19

0 0.5 1 1.5 2 2.5 3 3.5 4 4.5

0

0.2

0.4

0.6

0.8

1

Time [ s]

Sig

nal [

V]

1 2 3 ... ... 17 18 19

A sequence of pulses, each at a unique wavelength

ConclusionsResultsDesignMotivation 514th GRC 2007

Understanding the laser design

BOA*

time

pow

er

pow

er

4-step upgrade from a CW fiber laser to a 2-color TDM source

*Booster optical amplifier, a form of semiconductor optical amplifier:

ConclusionsResultsDesignMotivation 614th GRC 2007

Step 1: Replace mirrors with Bragg gratings

time

pow

er

pow

er

Customization of laser wavelength, linewidth

BOAFBG FBG

ConclusionsResultsDesignMotivation 714th GRC 2007

Step 2: Pulsed operation

time

pow

er

pow

er

BOAFBG

1 period

L R L R L R

FBG

Pulsed operation

ConclusionsResultsDesignMotivation 814th GRC 2007

Step 3: Add second grating pair

time

pow

er

pow

er

BOAFBGFBG

1 period 1 period

1 period

Pulsed operation at an additional wavelength with a modified pulse pattern

L R L R L R L R L R L R

ConclusionsResultsDesignMotivation 914th GRC 2007

Step 4: Use the same gratings on both ends

time

pow

er

pow

er

BOA

FBGFBG

1 period

Still a linear cavity laser, enforced within ring arrangement by the pulse pattern

ConclusionsResultsDesignMotivation 10

14th GRC 2007

Animation of 3-color TDM sourcefo

r an

imat

ion:

rig

ht c

lick

on t

he f

igur

e, s

elec

t pl

ay

ConclusionsResultsDesignMotivation 11

14th GRC 2007

distance [m]

time

[s]

x-t diagram familiar to gasdynamicists

Color-map of density in a shock tube experiment: He-air-CO2, M = 2.5

ConclusionsResultsDesignMotivation 12

14th GRC 2007

TDM source x-t diagram

ASE only, no FBGs

ConclusionsResultsDesignMotivation 13

14th GRC 2007

Main reflections only, 3 FBGs

TDM source x-t diagram

ConclusionsResultsDesignMotivation 14

14th GRC 2007

All signals, 3 FBGs

TDM source x-t diagram

ConclusionsResultsDesignMotivation 15

14th GRC 2007

Schematic of 19-color realization

fiber roundtrip length ~ 3 km

repetition rate ~ 66 kHz

ConclusionsResultsDesignMotivation 16

14th GRC 2007

0 0.5 1 1.5 2 2.5 3 3.5 4 4.5

0

0.2

0.4

0.6

0.8

1

Time [s]

Sig

nal [

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

ConclusionsResultsDesignMotivation 17

14th GRC 2007

1330 1335 1340 1345 1350 1355 1360 1365 1370 1375 138010

-11

10-10

10-9

10-8

10-7

10-6

Wavelength [nm]

Spe

ctra

l Pow

er [a

.u.]

1 2 3 ... ... 17 18 19

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

ConclusionsResultsDesignMotivation 18

14th GRC 2007

1330 1335 1340 1345 1350 1355 1360 1365 1370 1375 13800

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

Wavelength [nm]

Spe

ctra

l Pow

er [a

.u.]

Experimental Results

Spectrum of TDM output the BOA injection current pulse pattern was customized to form a ramped output spectrum

ConclusionsResultsDesignMotivation 19

14th GRC 2007

Experimental Results

High-speed detection strategy

ConclusionsResultsDesignMotivation 20

14th GRC 2007

0 1 2 3 4 5 6 7 8 9 10

0

0.2

0.4

0.6

0.8

1

Time [s]

Sig

nal [

V]

Experimental Results

Liquid phase Methanol, I and Io

ConclusionsResultsDesignMotivation 21

14th GRC 2007

1330 1335 1340 1345 1350 1355 1360 1365 1370 1375 13800

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

Wavelength [nm]

Abs

orba

nce

[a.u

.]

Methanol Measurement

Methanol ReferenceIsopropanol Measurement

Isopropanol Reference

Experimental Results

Measured spectra of Methanol and Isopropanol

single shot measurement

66 kHz rep. rate

standard deviation of 100

consecutive shots: ~0.0013

ConclusionsResultsDesignMotivation 22

14th GRC 2007

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)

ConclusionsResultsDesignMotivation 23

14th GRC 2007

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?

ConclusionsResultsDesignMotivation 24

14th GRC 2007

ConclusionsResultsDesignMotivation 25

14th GRC 2007

The original 19 wavelengths were chosen to align with H2O peaks – now we choose the

N wavelengths differently


Recommended