frontières et défis de l'optique non-linéaire nouveaux guides d’ondes, nouvelles non...
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Frontières et défis de l'optique non-linéairenouveaux guides d’ondes, nouvelles non linéarités,
nouvelles directions …
John Dudley
CNRS Institut FEMTO-ST
Université de Franche-Comté
Besançon, France
Mardi 2 décembre 2014Workshop INSIS - Optique électromagnétique
The high power and spatial coherence of laser light enabled the study of the nonlinear response of light to optical fields
(the first evidence of the second harmonic was removed as a speck of dirt)
Nonlinear optics and lasers are natural partners
1960 1961
The high power and spatial coherence of laser light enabled the study of the nonlinear response of light to optical fields
(the first evidence of the second harmonic was removed as a speck of dirt)
Nonlinear optics and lasers are natural partners
1960 1961
The uses of nonlinear optics
Does this mean that nonlinear optics has only very few applications?
E. Garmire, Nonlinear Optics in Daily Life, Optics Express 21 30532 (2013)
Nonlinearity is often embedded within optical systems and applications
Nonlinear Optics
FundamentalScience
Source Development
Applications in Materials
Information Technology etc
New Wavelengths
Ultrafast lasers
Frequency Combs
Machining
Spectroscopy
Analytical Tools
Amplifiers
Soliton-like pulses
Sensors
The uses of nonlinear optics
… … …
…
E. Garmire, Nonlinear Optics in Daily Life, Optics Express 21 30532 (2013)
A selection of topics
• Where is nonlinear optics useful today?
Supercontinuum and applications• Telecommunications
• Source development• Other areas of physics
• Towards true nanoscale nonlinear optics
Nanoscale material processing
Proof of principle results
Challenges
• Reliable techniques for fabricating small-core waveguides allows tailored linear guidance (dispersion) and controlled nonlinear interactions
1960’s saw low-loss optical waveguide development
New optical waveguides
Solution: all-optical integration and functionality
Basic communication system
Opticalresponse
Propagation control
SOURCE MODULATOR DETECTOR
Nonlinear functionalities
A Hype Cycle of Nonlinear Optics
TIMETrigger
Peak of Hype
Depths of Despair
Hard Work, Realism
Low loss waveguides, new materialsNonlinear Solutions to every problem
Limited real world useNonlinearity
RE
SE
AR
CH
Practical sourcesAlternative solutions
…
A Hype Cycle of Nonlinear Optics
TIMETrigger
Peak of Hype
Depths of Despair
Hard Work, Realism
Low loss waveguides, new materialsNonlinear Solutions to every problem
Limited real world useNonlinearity
RE
SE
AR
CH
Practical sourcesAlternative solutions
New Trigger
New waveguides enable other possibilities
Nonlinear effects now observed using a wider range of sources
Match wavelengths of source & waveguide zero dispersion
The mid 1990’s saw the development of micro (then nano) structured waveguides with the ability to engineer nonlinearity and dispersion
(Note on history)
• Russell’s initial idea was to create a photonic bandgap guidance mechanism in contrast to the refractive index guidance mechanism
• The first fibers they tried to make failed to show a photonic bandgap, but they tested them anyway, and discovered the fact that the microstructure provided new possibilities to engineer refractive index guidance
1991
Nonlinear pulse propagation
Polarization contains linear and nonlinear components
In fibres we are concerned with nonlinear polarization from c(3)
Neglecting third harmonic generation yields :
intensity-dependent refractive index n(I) = n0 + n2 I
Modelling the supercontinuum is more complex
Linear dispersion SPM, FWM, RamanSelf-steepening
Three main processes
Soliton ejection
Raman – shift to long l Radiation – shift to short l
Physics: NLSE + perturbations
We use a generalized nonlinear Schrödinger equation (NLSE)
Modelling agrees with experiment !!
Linear dispersion SPM, FWM, RamanSelf-steepening
Three main processes
Soliton ejection
Raman – shift to long l Radiation – shift to short l
Physics: NLSE + perturbations
We use a generalized nonlinear Schrödinger equation (NLSE)
Experiment
Simulation
Wavelength (nm)
Spe
ctru
m (
20 d
B/d
iv)
Output Spectra
Basic description of ultrashort pulses
Ultrafast nonlinear fiber optics
An octave-spanning spectrum allows comb position to be readily stabilized
We can bridge the gap between a knownoptical frequency locked to definition of the second and any optical frequency
Who would have predicted this ?
Example: planetary discovery
Periodic Doppler shift of stellar spectral lines is perturbed by planetary motion
Astrocombs measure radial velocity changes of ~ 10 cm/s
Example: broadband light source
Molecular fingerprinting S. Diddams et al. Nature 445, 627 (2007) Human breath analysis M. J. Thorpe et al. Opt. Express 16, 2387 (2008)
Supercontinuum applied in Terabit/s telecommunications
D. Hillerkuss et al.
Here, the nonlinear optics is enabling but the real breakthrough is the system
Supercontinuum is used for broad spectrum for spectral slicing and OFDM
New materials enable progress to-mid infrared
Organic fingerprint region – gas sensing, medicine, food analysis etc
The ability to pressure-tune dispersion in hollow core fibres enables gas-phase nonlinear optics
Nonlinear optics in gas-filled fibres enables UV
Hollow-core photonic crystal fibres for gas-based nonlinear optics, Nat Photon 8, 278–286 (2014)
Exploiting and managing nonlinearity is critical in the design of a wide range of femtosecond sources in many different application regimes
Nonlinear optics is central to fs source development
W Sibbett et al. The development and application of femtosecond laser systemsOptics Express Focus Issue on Modular Ultrafast Lasers 20 6989-7001 (2012)
Nonlinear saturable absorption is a key component of pulsed lasers
Nonlinear optics is central to fs source development
Optical “toy models” for other physical systems
Nonlinear wave evolution in fiber and on deep water are described by the same nonlinear propagation model
Rogue Waves are extreme events appearing seemingly from nowhere
• Ocean Waves
1974
1995
Kherif et al. Rogue Waves in the Ocean, Springer (2009)
Rogue waves – rare and extreme surface waves
• Optics
Dudley et al. Nature Photonics 8, 755-764 (2014)
Rogue Waves in a Water Tank Chabchoub et al. Phys. Rev. Lett. 106 204502 (2011)
Now influencing research in fluid mechanics
Gatass, R. and Mazur, E. Nature Photonics 2,219 (2008)
Nonlinear optics of permanent material modification
Tradeoff between interaction length and intensity
Gaussian beams cannot penetrate deeply in materials
Gaussian beams have an unavoidabletradeoff between interaction lengthand focal spotsize and power density
White,Y. et al, Opt. Express 16,14411 (2008)
Femtosecond ablation for machiningextended channels is a difficult technology
Enhanced interaction lengths also possible in free space
The spatial phase of femtosecond Gaussian beams can be tailored toyield important classes of non-diffracting and accelerating beams
Non-diffracting Bessel Beams
Accelerating Airy Beams M. V. Berry and N. L. BalazsAm. J. Phys. 47 264 (1979)
G. A. Siviloglou et al. Phys. Rev. Lett. 99 213901 (2007)
J. Durnin et al. Phys. Rev. Lett. 58 1499 (1987)
New possibilities for micro and nano structuring
High aspect ratio channels using Bessel beams
Advanced surface machining using accelerating and vortex beams
Expt10 mm
High aspect ratio nanochannels M. Bhuyan et al. Appl. Phys. Lett. 97 081102 (2010)Sending fs pulses in circles F. Courvoiser et al. Opt. Lett. (April 2012)Machining diamond and silicon A. Mathis et al. Appl. Phys. Lett. 101, 071110 (2012)Vortex Bessel beams in graphene B. Wetzel et al. Appl. Phys. Lett. 103, 241111 (2013)
Graphene
Theoretical challenges
1. Input pulse is a high-order soliton
2. Perturbation due to proximity to ZDW
3. Break up into fundamental solitons
4. Soliton dynamics - Raman self-frequency shift (RED)
5. Soliton dynamics - Dispersive wave generation (BLUE)
Linear dispersion SPM, FWM, Raman
Major Minor
Metamaterials, plasmonics
Enhanced SHGNonlinear phase modulation Fano resonancesBistability
Metamaterial NLSEAllan Boardman Opt. Commun. 283 1585 (2010)
SolitonsParametric amplificationRaman scattering Phase conjugationWavelength conversion