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8/14/2019 Cathy 25th Nov Imperial Vf
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25th November 200925th November 2009
Physical & Theoretical Chemistry
Cathy Rushworth
Supervisor: Dr. Claire Vallance
Direct absorption measurementsusing fibre-loop cavity ring-downspectroscopy
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Page 2Page 2
Outline
Absorption spectroscopy
Results so far
Challenges ahead
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Page 3
Absorption spectroscopy
Beer-Lambert Law: eI
I=
0
cl
Usually the path length is ~ 1 cm, but in a chip it can be 1000 times smaller How can we make absorption measurements on sample volumes this
small?
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CRDS with mirrors
)1( clRcd
+
=
In
tens
ity
Time
OKeefe and Deacon 1988
No absorberAbsorber present
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CRDS with fibres
Loock 2002
Fiberguide Industries, Inc.
1
2
n1sin1 =n2sin2Core RI = 1.457Cladding RI = 1.439
)( clLc
d
+
=
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Fibre signal
Light travels in the core and the cladding
In
tens
i ty
Time
Cladding
Cladding modes
Core modes
Start recording signalafter this point
Core
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Sample measurements
Direct absorption
Evanescent wave absorption
HF etching
Taper
CladdingCladding
CoreCore
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Optical set-up
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Sample introduction
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Fibre-loop ring-downs
Water = 224 ns
R6G 0.1125 mM =181 ns
50 um core diameter fibre, l = 24 um,
0.5 pL sample volume!
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End separation in water
200 um
105 um
100 um50 um
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SFS100
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Finding optimum l and d for SFS100
Waechter 2009
For a given abs C,
optimise l and d tomaximise sensitivity
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Lensing
100 um
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Preliminary results SFS50, l = 24 um, d = 4 m
Probed volume ~ 0.5 pL50 uM R6G: Detect ~ 2 fmoles, ~ 1 billion molecules
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Improvements
Minimize loop losses
Separate core and cladding modes
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Contact HF etching in situ
Non contact
Remembering Fibre alignment, Limit to end separation, RI (core) = 1.457
Page 17
Options for fibre chip coupling
Fibre ends
Chip
Chip
Uncleaved fibre
Chip
Fibre ends
Fibre ends
Fibre end
Chip Observationwindows
Plan view
Channel HFflow
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Important considerations
Fibre chip coupling parameters
End separation tolerances
Systems to study
Data acquisition rate?
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Acknowledgements
Thank you for listening
Thank you to Claire, Joao, Bobby and Joanna
Questions?