2 μm lasers as pump sources for mid-IR ... - The ISLA...
Transcript of 2 μm lasers as pump sources for mid-IR ... - The ISLA...
June 2015 Proprietary and Confidential
2 μm lasers as pump sources for mid-IR
supercontinuum sources
June 2015
Lasse Leick Peter M Moselund
Christian Petersen Laurent Huot
Chris Brooks Carsten L Thomsen
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
Supercontinuum light sources A sun in a box
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
4
Supercontinuum what is it ndash simplified
Supercontinuum Output
Pulsed
laser (ps) Non linear fiber
Supercontinuum is generated when high (peak) power
light enters a nonlinear material
The enabling technology is photonic
crystal fibres (PCFs)
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
5
Supercontinuum - The difference
Merged set of conventional lasers One Single Supercontinuum Source
SuperContinuum Conventional Lasers
5
Continues in spectrum
High power density
Short Pulsed in time
Mode-locked fiber laser
Nonlinear
fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
6
Applications of supercontinuum
Microscopy
BioTech
OCT Ophthalmology
Industrial NDT Life Science
Diagnostics
Nanotechnology
Food sorting
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
7
Extending the spectrum to the Mid-IR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
8
Chasing MID IR ndash Why
Chemical finger printing
Detecting explosives (32-35 um)
Food analysis
Combustion analysis
Medical ndash Spectral Imaging
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
9
Chasing MID IR ndash Why
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
10
NKTs role PCF for 2 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
11
Thermal light source Broad spectral coverage and low cost
Power spectral density in a single mode fiber lt50 dBmnm
OPOs Up to 10 W in a ultra-narrow line tunable over up to 700 nm
High cost system for lab use only
Mid-IR diodes Compact energy efficient wide range of powers
One fixed line w lt10 nm tunability low volume cost of gt10 k$ per diode
External cavity QCLs Compact energy efficient gt50 mW line tunable over eg 600 nm 43 microm
Poor operation lt4 microm high cost gt50 k$
Syncrotron High intensity and covers the full spectrum
Very large and very expensive facility
Current mid-IR light sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
12
Requirements for mid-IR supercontinuum sources
1New fiber material to generate mid-IR light
2Pulsed laser sources (preferable with
wavelengths above 1700 nm)
3Single and multimode components to amplify the
pulsed laser to high ~10 kW power
4Components to collimate and shape mid-IR light
5Proving reliability and mass reducibility
6Building up the market for mid-IR SuperK sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
13
Fiber Material choice
bull Silica is opague above 24 microm
bull Soft glasses necessary
bull Glass choice dependent on several parameters
bull Dispersion loss and nonlinearity is most important
0
1
2
3
4
5
6
7
8
9
10
2 3 4 5 6 7 8 9
Fib
er
los
s [
dB
m]
Wavelength [microm]
ZBLAN AsS AsSe SiO2
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
14
Pump laser for the mid-IR supercontinuum
Possible options
bull 10 microm lasers (Yb)
bull 155 microm lasers (Er)
bull 20 microm laser (Tm)
bull 21 microm laser (TmHo)
bull 29 microm laser
Wavelength too low
Cheap
Good wavelength
Expensive
Good wavelength
Very expensive
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
Supercontinuum light sources A sun in a box
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
4
Supercontinuum what is it ndash simplified
Supercontinuum Output
Pulsed
laser (ps) Non linear fiber
Supercontinuum is generated when high (peak) power
light enters a nonlinear material
The enabling technology is photonic
crystal fibres (PCFs)
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
5
Supercontinuum - The difference
Merged set of conventional lasers One Single Supercontinuum Source
SuperContinuum Conventional Lasers
5
Continues in spectrum
High power density
Short Pulsed in time
Mode-locked fiber laser
Nonlinear
fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
6
Applications of supercontinuum
Microscopy
BioTech
OCT Ophthalmology
Industrial NDT Life Science
Diagnostics
Nanotechnology
Food sorting
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
7
Extending the spectrum to the Mid-IR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
8
Chasing MID IR ndash Why
Chemical finger printing
Detecting explosives (32-35 um)
Food analysis
Combustion analysis
Medical ndash Spectral Imaging
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
9
Chasing MID IR ndash Why
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
10
NKTs role PCF for 2 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
11
Thermal light source Broad spectral coverage and low cost
Power spectral density in a single mode fiber lt50 dBmnm
OPOs Up to 10 W in a ultra-narrow line tunable over up to 700 nm
High cost system for lab use only
Mid-IR diodes Compact energy efficient wide range of powers
One fixed line w lt10 nm tunability low volume cost of gt10 k$ per diode
External cavity QCLs Compact energy efficient gt50 mW line tunable over eg 600 nm 43 microm
Poor operation lt4 microm high cost gt50 k$
Syncrotron High intensity and covers the full spectrum
Very large and very expensive facility
Current mid-IR light sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
12
Requirements for mid-IR supercontinuum sources
1New fiber material to generate mid-IR light
2Pulsed laser sources (preferable with
wavelengths above 1700 nm)
3Single and multimode components to amplify the
pulsed laser to high ~10 kW power
4Components to collimate and shape mid-IR light
5Proving reliability and mass reducibility
6Building up the market for mid-IR SuperK sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
13
Fiber Material choice
bull Silica is opague above 24 microm
bull Soft glasses necessary
bull Glass choice dependent on several parameters
bull Dispersion loss and nonlinearity is most important
0
1
2
3
4
5
6
7
8
9
10
2 3 4 5 6 7 8 9
Fib
er
los
s [
dB
m]
Wavelength [microm]
ZBLAN AsS AsSe SiO2
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
14
Pump laser for the mid-IR supercontinuum
Possible options
bull 10 microm lasers (Yb)
bull 155 microm lasers (Er)
bull 20 microm laser (Tm)
bull 21 microm laser (TmHo)
bull 29 microm laser
Wavelength too low
Cheap
Good wavelength
Expensive
Good wavelength
Very expensive
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
4
Supercontinuum what is it ndash simplified
Supercontinuum Output
Pulsed
laser (ps) Non linear fiber
Supercontinuum is generated when high (peak) power
light enters a nonlinear material
The enabling technology is photonic
crystal fibres (PCFs)
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
5
Supercontinuum - The difference
Merged set of conventional lasers One Single Supercontinuum Source
SuperContinuum Conventional Lasers
5
Continues in spectrum
High power density
Short Pulsed in time
Mode-locked fiber laser
Nonlinear
fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
6
Applications of supercontinuum
Microscopy
BioTech
OCT Ophthalmology
Industrial NDT Life Science
Diagnostics
Nanotechnology
Food sorting
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
7
Extending the spectrum to the Mid-IR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
8
Chasing MID IR ndash Why
Chemical finger printing
Detecting explosives (32-35 um)
Food analysis
Combustion analysis
Medical ndash Spectral Imaging
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
9
Chasing MID IR ndash Why
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
10
NKTs role PCF for 2 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
11
Thermal light source Broad spectral coverage and low cost
Power spectral density in a single mode fiber lt50 dBmnm
OPOs Up to 10 W in a ultra-narrow line tunable over up to 700 nm
High cost system for lab use only
Mid-IR diodes Compact energy efficient wide range of powers
One fixed line w lt10 nm tunability low volume cost of gt10 k$ per diode
External cavity QCLs Compact energy efficient gt50 mW line tunable over eg 600 nm 43 microm
Poor operation lt4 microm high cost gt50 k$
Syncrotron High intensity and covers the full spectrum
Very large and very expensive facility
Current mid-IR light sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
12
Requirements for mid-IR supercontinuum sources
1New fiber material to generate mid-IR light
2Pulsed laser sources (preferable with
wavelengths above 1700 nm)
3Single and multimode components to amplify the
pulsed laser to high ~10 kW power
4Components to collimate and shape mid-IR light
5Proving reliability and mass reducibility
6Building up the market for mid-IR SuperK sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
13
Fiber Material choice
bull Silica is opague above 24 microm
bull Soft glasses necessary
bull Glass choice dependent on several parameters
bull Dispersion loss and nonlinearity is most important
0
1
2
3
4
5
6
7
8
9
10
2 3 4 5 6 7 8 9
Fib
er
los
s [
dB
m]
Wavelength [microm]
ZBLAN AsS AsSe SiO2
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
14
Pump laser for the mid-IR supercontinuum
Possible options
bull 10 microm lasers (Yb)
bull 155 microm lasers (Er)
bull 20 microm laser (Tm)
bull 21 microm laser (TmHo)
bull 29 microm laser
Wavelength too low
Cheap
Good wavelength
Expensive
Good wavelength
Very expensive
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
5
Supercontinuum - The difference
Merged set of conventional lasers One Single Supercontinuum Source
SuperContinuum Conventional Lasers
5
Continues in spectrum
High power density
Short Pulsed in time
Mode-locked fiber laser
Nonlinear
fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
6
Applications of supercontinuum
Microscopy
BioTech
OCT Ophthalmology
Industrial NDT Life Science
Diagnostics
Nanotechnology
Food sorting
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
7
Extending the spectrum to the Mid-IR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
8
Chasing MID IR ndash Why
Chemical finger printing
Detecting explosives (32-35 um)
Food analysis
Combustion analysis
Medical ndash Spectral Imaging
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
9
Chasing MID IR ndash Why
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
10
NKTs role PCF for 2 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
11
Thermal light source Broad spectral coverage and low cost
Power spectral density in a single mode fiber lt50 dBmnm
OPOs Up to 10 W in a ultra-narrow line tunable over up to 700 nm
High cost system for lab use only
Mid-IR diodes Compact energy efficient wide range of powers
One fixed line w lt10 nm tunability low volume cost of gt10 k$ per diode
External cavity QCLs Compact energy efficient gt50 mW line tunable over eg 600 nm 43 microm
Poor operation lt4 microm high cost gt50 k$
Syncrotron High intensity and covers the full spectrum
Very large and very expensive facility
Current mid-IR light sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
12
Requirements for mid-IR supercontinuum sources
1New fiber material to generate mid-IR light
2Pulsed laser sources (preferable with
wavelengths above 1700 nm)
3Single and multimode components to amplify the
pulsed laser to high ~10 kW power
4Components to collimate and shape mid-IR light
5Proving reliability and mass reducibility
6Building up the market for mid-IR SuperK sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
13
Fiber Material choice
bull Silica is opague above 24 microm
bull Soft glasses necessary
bull Glass choice dependent on several parameters
bull Dispersion loss and nonlinearity is most important
0
1
2
3
4
5
6
7
8
9
10
2 3 4 5 6 7 8 9
Fib
er
los
s [
dB
m]
Wavelength [microm]
ZBLAN AsS AsSe SiO2
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
14
Pump laser for the mid-IR supercontinuum
Possible options
bull 10 microm lasers (Yb)
bull 155 microm lasers (Er)
bull 20 microm laser (Tm)
bull 21 microm laser (TmHo)
bull 29 microm laser
Wavelength too low
Cheap
Good wavelength
Expensive
Good wavelength
Very expensive
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
6
Applications of supercontinuum
Microscopy
BioTech
OCT Ophthalmology
Industrial NDT Life Science
Diagnostics
Nanotechnology
Food sorting
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
7
Extending the spectrum to the Mid-IR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
8
Chasing MID IR ndash Why
Chemical finger printing
Detecting explosives (32-35 um)
Food analysis
Combustion analysis
Medical ndash Spectral Imaging
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
9
Chasing MID IR ndash Why
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
10
NKTs role PCF for 2 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
11
Thermal light source Broad spectral coverage and low cost
Power spectral density in a single mode fiber lt50 dBmnm
OPOs Up to 10 W in a ultra-narrow line tunable over up to 700 nm
High cost system for lab use only
Mid-IR diodes Compact energy efficient wide range of powers
One fixed line w lt10 nm tunability low volume cost of gt10 k$ per diode
External cavity QCLs Compact energy efficient gt50 mW line tunable over eg 600 nm 43 microm
Poor operation lt4 microm high cost gt50 k$
Syncrotron High intensity and covers the full spectrum
Very large and very expensive facility
Current mid-IR light sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
12
Requirements for mid-IR supercontinuum sources
1New fiber material to generate mid-IR light
2Pulsed laser sources (preferable with
wavelengths above 1700 nm)
3Single and multimode components to amplify the
pulsed laser to high ~10 kW power
4Components to collimate and shape mid-IR light
5Proving reliability and mass reducibility
6Building up the market for mid-IR SuperK sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
13
Fiber Material choice
bull Silica is opague above 24 microm
bull Soft glasses necessary
bull Glass choice dependent on several parameters
bull Dispersion loss and nonlinearity is most important
0
1
2
3
4
5
6
7
8
9
10
2 3 4 5 6 7 8 9
Fib
er
los
s [
dB
m]
Wavelength [microm]
ZBLAN AsS AsSe SiO2
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
14
Pump laser for the mid-IR supercontinuum
Possible options
bull 10 microm lasers (Yb)
bull 155 microm lasers (Er)
bull 20 microm laser (Tm)
bull 21 microm laser (TmHo)
bull 29 microm laser
Wavelength too low
Cheap
Good wavelength
Expensive
Good wavelength
Very expensive
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
7
Extending the spectrum to the Mid-IR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
8
Chasing MID IR ndash Why
Chemical finger printing
Detecting explosives (32-35 um)
Food analysis
Combustion analysis
Medical ndash Spectral Imaging
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
9
Chasing MID IR ndash Why
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
10
NKTs role PCF for 2 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
11
Thermal light source Broad spectral coverage and low cost
Power spectral density in a single mode fiber lt50 dBmnm
OPOs Up to 10 W in a ultra-narrow line tunable over up to 700 nm
High cost system for lab use only
Mid-IR diodes Compact energy efficient wide range of powers
One fixed line w lt10 nm tunability low volume cost of gt10 k$ per diode
External cavity QCLs Compact energy efficient gt50 mW line tunable over eg 600 nm 43 microm
Poor operation lt4 microm high cost gt50 k$
Syncrotron High intensity and covers the full spectrum
Very large and very expensive facility
Current mid-IR light sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
12
Requirements for mid-IR supercontinuum sources
1New fiber material to generate mid-IR light
2Pulsed laser sources (preferable with
wavelengths above 1700 nm)
3Single and multimode components to amplify the
pulsed laser to high ~10 kW power
4Components to collimate and shape mid-IR light
5Proving reliability and mass reducibility
6Building up the market for mid-IR SuperK sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
13
Fiber Material choice
bull Silica is opague above 24 microm
bull Soft glasses necessary
bull Glass choice dependent on several parameters
bull Dispersion loss and nonlinearity is most important
0
1
2
3
4
5
6
7
8
9
10
2 3 4 5 6 7 8 9
Fib
er
los
s [
dB
m]
Wavelength [microm]
ZBLAN AsS AsSe SiO2
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
14
Pump laser for the mid-IR supercontinuum
Possible options
bull 10 microm lasers (Yb)
bull 155 microm lasers (Er)
bull 20 microm laser (Tm)
bull 21 microm laser (TmHo)
bull 29 microm laser
Wavelength too low
Cheap
Good wavelength
Expensive
Good wavelength
Very expensive
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
8
Chasing MID IR ndash Why
Chemical finger printing
Detecting explosives (32-35 um)
Food analysis
Combustion analysis
Medical ndash Spectral Imaging
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
9
Chasing MID IR ndash Why
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
10
NKTs role PCF for 2 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
11
Thermal light source Broad spectral coverage and low cost
Power spectral density in a single mode fiber lt50 dBmnm
OPOs Up to 10 W in a ultra-narrow line tunable over up to 700 nm
High cost system for lab use only
Mid-IR diodes Compact energy efficient wide range of powers
One fixed line w lt10 nm tunability low volume cost of gt10 k$ per diode
External cavity QCLs Compact energy efficient gt50 mW line tunable over eg 600 nm 43 microm
Poor operation lt4 microm high cost gt50 k$
Syncrotron High intensity and covers the full spectrum
Very large and very expensive facility
Current mid-IR light sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
12
Requirements for mid-IR supercontinuum sources
1New fiber material to generate mid-IR light
2Pulsed laser sources (preferable with
wavelengths above 1700 nm)
3Single and multimode components to amplify the
pulsed laser to high ~10 kW power
4Components to collimate and shape mid-IR light
5Proving reliability and mass reducibility
6Building up the market for mid-IR SuperK sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
13
Fiber Material choice
bull Silica is opague above 24 microm
bull Soft glasses necessary
bull Glass choice dependent on several parameters
bull Dispersion loss and nonlinearity is most important
0
1
2
3
4
5
6
7
8
9
10
2 3 4 5 6 7 8 9
Fib
er
los
s [
dB
m]
Wavelength [microm]
ZBLAN AsS AsSe SiO2
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
14
Pump laser for the mid-IR supercontinuum
Possible options
bull 10 microm lasers (Yb)
bull 155 microm lasers (Er)
bull 20 microm laser (Tm)
bull 21 microm laser (TmHo)
bull 29 microm laser
Wavelength too low
Cheap
Good wavelength
Expensive
Good wavelength
Very expensive
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
9
Chasing MID IR ndash Why
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
10
NKTs role PCF for 2 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
11
Thermal light source Broad spectral coverage and low cost
Power spectral density in a single mode fiber lt50 dBmnm
OPOs Up to 10 W in a ultra-narrow line tunable over up to 700 nm
High cost system for lab use only
Mid-IR diodes Compact energy efficient wide range of powers
One fixed line w lt10 nm tunability low volume cost of gt10 k$ per diode
External cavity QCLs Compact energy efficient gt50 mW line tunable over eg 600 nm 43 microm
Poor operation lt4 microm high cost gt50 k$
Syncrotron High intensity and covers the full spectrum
Very large and very expensive facility
Current mid-IR light sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
12
Requirements for mid-IR supercontinuum sources
1New fiber material to generate mid-IR light
2Pulsed laser sources (preferable with
wavelengths above 1700 nm)
3Single and multimode components to amplify the
pulsed laser to high ~10 kW power
4Components to collimate and shape mid-IR light
5Proving reliability and mass reducibility
6Building up the market for mid-IR SuperK sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
13
Fiber Material choice
bull Silica is opague above 24 microm
bull Soft glasses necessary
bull Glass choice dependent on several parameters
bull Dispersion loss and nonlinearity is most important
0
1
2
3
4
5
6
7
8
9
10
2 3 4 5 6 7 8 9
Fib
er
los
s [
dB
m]
Wavelength [microm]
ZBLAN AsS AsSe SiO2
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
14
Pump laser for the mid-IR supercontinuum
Possible options
bull 10 microm lasers (Yb)
bull 155 microm lasers (Er)
bull 20 microm laser (Tm)
bull 21 microm laser (TmHo)
bull 29 microm laser
Wavelength too low
Cheap
Good wavelength
Expensive
Good wavelength
Very expensive
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
10
NKTs role PCF for 2 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
11
Thermal light source Broad spectral coverage and low cost
Power spectral density in a single mode fiber lt50 dBmnm
OPOs Up to 10 W in a ultra-narrow line tunable over up to 700 nm
High cost system for lab use only
Mid-IR diodes Compact energy efficient wide range of powers
One fixed line w lt10 nm tunability low volume cost of gt10 k$ per diode
External cavity QCLs Compact energy efficient gt50 mW line tunable over eg 600 nm 43 microm
Poor operation lt4 microm high cost gt50 k$
Syncrotron High intensity and covers the full spectrum
Very large and very expensive facility
Current mid-IR light sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
12
Requirements for mid-IR supercontinuum sources
1New fiber material to generate mid-IR light
2Pulsed laser sources (preferable with
wavelengths above 1700 nm)
3Single and multimode components to amplify the
pulsed laser to high ~10 kW power
4Components to collimate and shape mid-IR light
5Proving reliability and mass reducibility
6Building up the market for mid-IR SuperK sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
13
Fiber Material choice
bull Silica is opague above 24 microm
bull Soft glasses necessary
bull Glass choice dependent on several parameters
bull Dispersion loss and nonlinearity is most important
0
1
2
3
4
5
6
7
8
9
10
2 3 4 5 6 7 8 9
Fib
er
los
s [
dB
m]
Wavelength [microm]
ZBLAN AsS AsSe SiO2
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
14
Pump laser for the mid-IR supercontinuum
Possible options
bull 10 microm lasers (Yb)
bull 155 microm lasers (Er)
bull 20 microm laser (Tm)
bull 21 microm laser (TmHo)
bull 29 microm laser
Wavelength too low
Cheap
Good wavelength
Expensive
Good wavelength
Very expensive
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
11
Thermal light source Broad spectral coverage and low cost
Power spectral density in a single mode fiber lt50 dBmnm
OPOs Up to 10 W in a ultra-narrow line tunable over up to 700 nm
High cost system for lab use only
Mid-IR diodes Compact energy efficient wide range of powers
One fixed line w lt10 nm tunability low volume cost of gt10 k$ per diode
External cavity QCLs Compact energy efficient gt50 mW line tunable over eg 600 nm 43 microm
Poor operation lt4 microm high cost gt50 k$
Syncrotron High intensity and covers the full spectrum
Very large and very expensive facility
Current mid-IR light sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
12
Requirements for mid-IR supercontinuum sources
1New fiber material to generate mid-IR light
2Pulsed laser sources (preferable with
wavelengths above 1700 nm)
3Single and multimode components to amplify the
pulsed laser to high ~10 kW power
4Components to collimate and shape mid-IR light
5Proving reliability and mass reducibility
6Building up the market for mid-IR SuperK sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
13
Fiber Material choice
bull Silica is opague above 24 microm
bull Soft glasses necessary
bull Glass choice dependent on several parameters
bull Dispersion loss and nonlinearity is most important
0
1
2
3
4
5
6
7
8
9
10
2 3 4 5 6 7 8 9
Fib
er
los
s [
dB
m]
Wavelength [microm]
ZBLAN AsS AsSe SiO2
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
14
Pump laser for the mid-IR supercontinuum
Possible options
bull 10 microm lasers (Yb)
bull 155 microm lasers (Er)
bull 20 microm laser (Tm)
bull 21 microm laser (TmHo)
bull 29 microm laser
Wavelength too low
Cheap
Good wavelength
Expensive
Good wavelength
Very expensive
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
12
Requirements for mid-IR supercontinuum sources
1New fiber material to generate mid-IR light
2Pulsed laser sources (preferable with
wavelengths above 1700 nm)
3Single and multimode components to amplify the
pulsed laser to high ~10 kW power
4Components to collimate and shape mid-IR light
5Proving reliability and mass reducibility
6Building up the market for mid-IR SuperK sources
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
13
Fiber Material choice
bull Silica is opague above 24 microm
bull Soft glasses necessary
bull Glass choice dependent on several parameters
bull Dispersion loss and nonlinearity is most important
0
1
2
3
4
5
6
7
8
9
10
2 3 4 5 6 7 8 9
Fib
er
los
s [
dB
m]
Wavelength [microm]
ZBLAN AsS AsSe SiO2
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
14
Pump laser for the mid-IR supercontinuum
Possible options
bull 10 microm lasers (Yb)
bull 155 microm lasers (Er)
bull 20 microm laser (Tm)
bull 21 microm laser (TmHo)
bull 29 microm laser
Wavelength too low
Cheap
Good wavelength
Expensive
Good wavelength
Very expensive
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
13
Fiber Material choice
bull Silica is opague above 24 microm
bull Soft glasses necessary
bull Glass choice dependent on several parameters
bull Dispersion loss and nonlinearity is most important
0
1
2
3
4
5
6
7
8
9
10
2 3 4 5 6 7 8 9
Fib
er
los
s [
dB
m]
Wavelength [microm]
ZBLAN AsS AsSe SiO2
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
14
Pump laser for the mid-IR supercontinuum
Possible options
bull 10 microm lasers (Yb)
bull 155 microm lasers (Er)
bull 20 microm laser (Tm)
bull 21 microm laser (TmHo)
bull 29 microm laser
Wavelength too low
Cheap
Good wavelength
Expensive
Good wavelength
Very expensive
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
14
Pump laser for the mid-IR supercontinuum
Possible options
bull 10 microm lasers (Yb)
bull 155 microm lasers (Er)
bull 20 microm laser (Tm)
bull 21 microm laser (TmHo)
bull 29 microm laser
Wavelength too low
Cheap
Good wavelength
Expensive
Good wavelength
Very expensive
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
15
2 microm lasers mode-locked and MOPA
Jiang Liu Opt Exp Vol
20 pp 22442-22447 2012
Single mode components at 2 microm are 5 -
10 times more expensive than at 15 microm
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
16
Wavelength shifted lasers
ZBLAN Thulium Amp
Er-fiber based mode-locked
Laser
Wavelength
shift in fiber
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
17
Spectrum before the ZBLAN fiber
0
05
1
15
2
25
1500 1700 1900 2100 2300 2500
Po
wer
[Au
]
Wavelength [nm]
Spectrum consists of many short solitons with high peak power
Bandwidth not so important for pumping supercontinuum
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
18
By tailoring the design of the nonlinear fiber one can
control the output spectrum
00
05
10
15
20
25
30
1 15 2 25 3 35 4 45 5
Po
we
r [m
Wn
m]
Wavelength [microm]
Spectral Tailoring
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
20
Different mid-IR prototypes from NKT
-45
-40
-35
-30
-25
-20
-15
-10
-5
0
13 17 21 25 29 33 37 41 45
Po
wer
[dB
mn
m]
Wavelength [microm]
ps system ns system
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
21
Mid-IR SuperK has brightness as a synchrotron
Syncrotron
Glow bar
ps Mid-IR SuperK
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
22
Mid-IR spectroscopy
Lab-data from June 2014
bull Detection limit as FTIR
but faster
bull Acquisition of full
spectrum
bull in milliseconds
bull 30 sec for FTIR
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
23
Mid-IR Microscopy
Test sample
Water Oil and Air
Soslashren Keiding et al
Opt Exp Vol 20 p 4887 (2012)
Water
Oil Air
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
24
MIR microscopy ndash Cancer diagnostics
bullInfrared hyperspectral imaging is simpler
than traditional staining methods
bullThe infrared data is less ambiguous and
thus requires less training to interpret
27 - 38 microm
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy
for Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
25
Brain cancer diagnostics on rats
27 - 38 microm
333-357 microm
304 351 microm
322 348 microm
Traditional FTIR used
Spatial resolution 25 microm
Spectral resolution 4-6 nm
MIR microscopy ndash Cancer diagnostics
Beljebbar A et al rdquoFourier Transform Infrared Microspectroscopy for
Cancer Diagnostic of C6 Glioma on Animal Modelrdquo
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
26
Mid-IR SuperK in Nature Photonics
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
27
Conclusions
bull NKT wants to commercialize mid-IR supercontinuum
bull Requires soft-glass fibers
bull Requires pulsed lasers with wavelengths gt1700 nm
bull 2 microm lasers are very interesting but expensive
bull Hopefully this will change in the future
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28
Crystal Fibre bull aeroLASE bull Koheras bull SuperK
28