birefringence and bragg grating control in femtosecond laser written optical circuits
DESCRIPTION
PhD thesis presented at the University of Porto in December 2012. The full thesis can be found here: http://www.luisfernandes.org/thesis.php http://books.google.pt/books/about/Birefringence_and_Bragg_grating_control.html?hl=pt-PT&id=iZFNRFl90d4CTRANSCRIPT
www.inescporto.ptwww.fc.up.pt
http://photonics.light.utoronto.ca/
Birefringence and Bragg grating control in femtosecond laser written optical circuits
Luís A. Fernandes
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Outline
Nonlinear absorption process
Bragg grating spectral control
Integrated wave plates
Polarization beam splitters
Birefringence control
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The advantages of nonlinear absorption
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Itoh et al. [MRS Bull. 31(8), 620, 2006]
Ultrafast oscillators: ~ 100 fs ~ nJ ~ 100 MHz
Amplified systems: ~ 100 fs ~ μJ to mJ ~ kHz
Nonlinearphotopolymerization
Laser ablationWaveguide writing in insulators
Nonlinear absorption process
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Femtosecond laser writing
Laser ablation 10 μm under the glass surface
Waveguide end facet
Localized refractive index change
10 μm
Green light filtered
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Fiber Laser1044 nm, 300 fs
SHG
Z Position Stage
X Y Position Stages
500 kHz
Pulse Energy = 90 nJ to 160 nJWavelength = 522 nm
Scan Speed = 0.27 mm/s
Femtosecond waveguide writing
Shah et al. [Optics Express 13, 6, 2005]
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Fiber Laser1044 nm, 300 fs
SHG
PSO Control
AOM
X Y Position Stages
500 kHz
500 Hz
Pulse Energy = 90 nJ to 160 nJWavelength = 522 nm
Scan Speed = 0.27 mm/s
Zhang et al. [Opt. Lett. 32, 2559-2561 (2007)]
Bragg Grating Waveguide (BGW) Fabrication
Z Position Stage
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Positive index change provides confinement
SMF28 Fiber Waveguide BGW
Bragg Grating Waveguides (BGWs)Waveguide propagation loss
Waveguide end facet
Typical coupling loss of 0.05 dB/facet
10 μm
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Fabrication of Phase-Shifted BGWsNormal Bragg Grating
Defect in the grating structure
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Spectral shaping applications
Chirped gratings for pulse shapingMultiple phase shifts for spectral shaping
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The intensity controls the light matter interaction
Suspended core fibers
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Bragg grating waveguides summary
Tunable interferometry inscription of gratings in suspended core fibers
With applications in temperature and strain independent sensing
Flexible grating fabrication for prototyping and spectral shaping
Phase control for arbitrary shifts along a grating
With sharp features (22 pm linewidth)
Design of chirped gratings with pulse shaping applications
Becker et al. IEEE Photonics Technology Letters, 21, 1453-1455, 2009Fernandes et al. IEEE Photonics Technology Letters, 24, 7, 554-556, 2012Dolgaleva et al. Optics Letters, 36, 22, pp. 4416-4418, 2011Grenier et al. Optics Letters, 37, 12, pp. 2289-2291, 2012Fernandes et al. Oral presentation OSA Frontiers in Optics, 2009
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Hnatovsky et al. [Appl. Phys. A 84, 47–61, (2006)]
Laser polarization: (formation of nanogratings / form birefringence)
Laser pulse energy / Stress induced anisotropy
Scanning speed, etc
Measured birefringent values ~ [10-5,10-4]
Birefringence in Femtosecond Written Waveguides
Δ n=nV−nH
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Opportunities to use birefringent waveguides
Waveguide birefringence in fused silica:
Bhardwaj et al. [Optics Letters 29, 1312–1314 (2004)]
Yang et al. [J. Appl. Phys. 95, 5280 (2004)]
Bellouard et al. [Optics Express 14, 8360-8366 (2006)]
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Opportunities to use birefringent waveguides
Waveguide birefringence in fused silica:
Bhardwaj et al. [Optics Letters 29, 1312–1314 (2004)]
Yang et al. [J. Appl. Phys. 95, 5280 (2004)]
Bellouard et al. [Optics Express 14, 8360-8366 (2006)]
Nanogratings formation and form birefringence:
Bricchi et al. [Optics Letters 29, 119-121 (2004)]
Hnatovsky et al. [Appl. Phys. A 84, 47–61, (2006)]
Taylor et al. [Optics Letters 32, 2888-2890 (2007)]
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Opportunities to use birefringent waveguides
Waveguide birefringence in fused silica:
Bhardwaj et al. [Optics Letters 29, 1312–1314 (2004)]
Yang et al. [J. Appl. Phys. 95, 5280 (2004)]
Bellouard et al. [Optics Express 14, 8360-8366 (2006)]
Nanogratings formation and form birefringence:
Bricchi et al. [Optics Letters 29, 119-121 (2004)]
Hnatovsky et al. [Appl. Phys. A 84, 47–61, (2006)]
Taylor et al. [Optics Letters 32, 2888-2890 (2007)]
Quantum entanglement measurements:
Marshall et al. [Optics Express 17, 12546–12554 (2009)]
Sansoni et al. [Phys. Rev. Lett. 105, 200503 (2010)]
Lobino and O’Brien [Nature 469, 43-44 (2011)]
Sensor applications:
Polarization sensitive devices
Integrated Lasers
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B
Polarizers
Detector
L
The birefringence splits the Bragg reflectioninto two polarization modes
Δ n=Δλ B
2 Λ
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BGW measurement of birefringence removes the ambiguity of the cross polarizer technique.
Polarizers
Detector
±45º
45º
L
I p=I i2
1cos I c=I i2
1−cos n=
2
L
δ=±cos−1( I p−I cI i )+ m2πm=0,1,2, ...
Waveguide retardance:
Parallel polarizers Crossed polarizers
Measuring birefringence with crossed polarizers
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160 nJ
=±cos−1I p− I cI i
m2 with m=0,1,2, ...
25.4 mm long waveguide
Dependence on writing energy and wavelength
n=
2
L
Energy dependence for parallel writing
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λ/2 - 35 dB polarization contrast(linear polarized output)
λ/4 - 5% variation(circular polarized output)
Zero-order half-wave plate (m = 0)
Parallel polarization writingWaveguide length = 25.4 mmPulse Energy = 160 nJ
Integrated wave plates demonstration
45º
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Integrated wave plates summary
Birefringence measured with BGWs and with crossed polarizers provided accurate and unambiguous values
Successfully demonstrated integrated wave plates:
Less than 5% output variation in a quarter-wave plate
35 dB linearity contrast for a half-wave plate
Broadband (66 nm) wave plates
As small as 4 mm with as low as 0.8 dB loss
Fernandes et al. Optics Express, 19, 19, 18294-18301, (2011)Fernandes et al. Oral presentation in CLEO, 2011Fernandes et al. Oral presentation in Frontiers in Ultrafast Optics, SPIE Photonics West, 2012
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r=P2
P1+P2
P1
P2
r (λ )=Asin2[ κ(λ)L+ϕ(λ )]
Using directional couplers to design polarization beam splitters
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Coupling is polarization dependent
Δ r=sin [(K V−K H )L+ϕV−ϕH ]×sin [(K V+K H )L+ϕV+ϕH ]
Polarization splitting contrast ratio: Δ r=∣rV−rH∣
Separation = 8 μm
r (λ )=Asin2[ κ(λ)L+ϕ(λ )]
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Definition of a more convenient parameter
Δ r=sin [(KV−K H )L+ ϕV−ϕH ]×sin [(KV+ K H )L+ ϕV+ ϕH ]
Δ r=∣r V−rH∣Polarization splitting contrast ratio:
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19 dB and 24 dB extinction ratio polarization splitting
Polarization beam splitters
Parallel polarization writingInteraction length = 19.2 mmSeparation = 8 μmS-Bends radius = 100 mm
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Polarization beam splitters summary
Birefringence provided polarization dependent coupling in directional couplers
Successfully demonstrated integrated polarization beam splitters:
19 dB to 24 dB of polarization contrast splitting
Relatively large devices (19 mm), but higher birefringence can reduce this value
Fernandes et al. Optics Express, 19, 13, 11992-11999, (2011)Fernandes et al. Oral presentation SPIE LASE, Photonics West, 2010
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Controlling the birefringence with stress
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The stress fields are dependent on the geometry
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Independent birefringence control is possible with the strength of the stress fields and with the writing polarization
Strength of thestress fields
Writing polarization
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Birefringence control summary
Birefringence is controllable over a range of < 4 x 10-6 to 4.35 x 10-4 with laser induced stress and writing polarization
Distinction between form birefringence (nanogratings) and stress birefringence
This birefringence control can reduce the size and total loss of wave plates
Minimum of 2 mm with 0.2 dB loss
Ability to design low and high birefringence elements with one step fabrications
Fernandes et al. Optics Express, 20, 22, 24103-24114, (2012)
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Conclusions
Improved Bragg grating fabrication control:
Demonstrated Bragg gratings in pure silica suspended core fibers
Improvements towards flexible spectral shaping and fast prototyping
Demonstrated pulse shaping applications
Demonstrated control and definitive birefringence determination:
From 10-6 to 10-4 birefringence control measured as a function of wavelength, pulse energy and
writing laser polarization
Integrated wave plate demonstration:
λ/2 with 35 dB polarization contrast and λ/4 with 5% variation; Possible broadband operation
Polarization beam splitters with 19.2 mm:
From 19 dB to 24 dB extinction ratios
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Polarization beam splitter
Wave plates
Millimeter length devices with[10-6 to 10-4] birefringence low loss
Future Work
Spectral control:
BGWs for pulse shaping and rapid prototyping
Polarization Control:
Smaller polarization splitters and wave plates
Applications in quantum photonics
Single step fabrication and prototyping
Integration of devices for quantum measurements
Optical circuits in fiber cladding
Implementation of polarization devices
Distributed sensing
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Fundação para a Ciência e Tecnologia (FCT)
Canadian Institute for Photonic Innovations
Natural Sciences and Engineering Research Council of Canada
Acknowledgments
www.inescporto.ptwww.fc.up.pt
http://photonics.light.utoronto.ca/
Thank you
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List of publications
Bragg gratings in suspended core fibers
● ''Inscription of Fiber Bragg Grating Arrays in Pure Silica Suspended Core Fibers''
Becker, Fernandes, et al. [IEEE Photonics Technology Letters, 21, 1453-1455, 2009]
● ''Temperature and Strain Sensing With Femtosecond Laser Written Bragg Gratings in Defect and Non-Defect Suspended-Silica-Core Fibers,''
Fernandes et al. [IEEE Photonics Technology Letters, Vol. 24, Issue 7, pp. 554-556, 2012]
BGW spectral control (phase shifts, chirps) and application in pulse shaping
● ''Femtosecond Laser Fabrication of Phase-Shifted Bragg Grating Waveguides in Fused Silica,''
Grenier, Fernandes et al. [Optics Letters, Vol. 37, Issue 12, pp. 2289-2291, 2012]
● ''Integrated Optical Temporal Fourier Transformer Based on Chirped Bragg Grating Waveguide,''
Dolgaleva, Fernandes et al. [Optics Letters, Vol. 36, Issue 22, pp. 4416-4418, 2011]
Birefringence measurements, control and applications
● ''Stress induced birefringence tuning in femtosecond laser fabricated waveguides in fused silica,''
Fernandes et al. [Optics Express, Vol. 20, Issue 22, pp. 24103-24114, 2012]
● ''Femtosecond laser writing of waveguide retarders in fused silica for polarization control in optical circuits,''
Fernandes et al. [Optics Express, Vol. 19, Issue 19, pp. 18294-18301, 2011]
● ''Femtosecond laser fabrication of birefringent directional couplers as polarization beam splitters in fused silica,''
Fernandes et al. [Optics Express, Vol. 19, Issue 13, pp. 11992-11999, 2011]
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List of communications● ''Femtosecond laser writing of polarization devices for optical circuits in glass,''
Fernandes et al. Proc. SPIE, 82470M, SPIE LASE: Frontiers in Ultrafast Optics, Photonics West, 2012
● ''Femtosecond laser direct fabrication of integrated optical wave plates in fused silica,''
Fernandes et al. Oral presentation in CLEO:2011 - Laser Applications to Photonic Applications, paper CWO6, 2011
● ''Integrated Temporal Fourier Transformer Based on Chirped Bragg Grating Waveguides,''
Dolgaleva et al. Oral presentation in CLEO:2011 - Laser Applications to Photonic Applications, paper CThHH6, 2011
● ''Femtosecond laser fabrication of birefringent directional couplers in fused silica,''
Fernandes et al. 7584-22, SPIE LASE: Laser Applications in Microelectronic and Optoelectronic Manufacturing XV, Photonics West, 2010
[Received Student Award for best oral presentations]
● ''Flexible tailoring of femtosecond laser-written Bragg grating waveguides,''
Grenier et al. SPIE MOEMS-MEMS: Advanced Fabrication Technologies for Micro/Nano Optics and Photonics III, Photonics West, 2010
● ''Femtosecond Laser Writing of Phase-Shifted Bragg Grating Waveguides in Fused Silica,''
Fernandes et al. OSA Frontiers in Optics, paper LMTuC5, 2009
● ''Temperature and strain characterization of Bragg gratings impressed with femtosecond laser radiation in suspended-silica-core fibers,''
Fernandes et al. Proc. SPIE, 73861N, Photonics North, 2009
● ''Fiber Bragg grating inscription with DUV femtosecond exposure and two beam interference,''
Becker et al. Proc. SPIE, 73862Y, Photonics North, 2009