rotation induced super structure in slow-light waveguides w mode degeneracy ben z. steinberg adi...
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![Page 1: Rotation Induced Super Structure in Slow-Light Waveguides w Mode Degeneracy Ben Z. Steinberg Adi Shamir Jacob Scheuer Amir Boag School of EE, Tel-Aviv](https://reader035.vdocuments.mx/reader035/viewer/2022062318/5517ac595503463e368b5e31/html5/thumbnails/1.jpg)
Rotation Induced Super Structure in Slow-Light Waveguides
w Mode Degeneracy
Ben Z. Steinberg
Adi Shamir
Jacob Scheuer
Amir Boag
School of EE, Tel-Aviv University
![Page 2: Rotation Induced Super Structure in Slow-Light Waveguides w Mode Degeneracy Ben Z. Steinberg Adi Shamir Jacob Scheuer Amir Boag School of EE, Tel-Aviv](https://reader035.vdocuments.mx/reader035/viewer/2022062318/5517ac595503463e368b5e31/html5/thumbnails/2.jpg)
Presentation Overview
• The effect of mechanical rotation on Slow-Light Structures– Previous studies: [1]
• Array of weakly coupled “conventional” resonators• New manifestation of Sagnac Effect
• Present work:– What happens if the micro-resonators support mode-degeneracy ?
Interesting NEW physical effects in Slow-Light Structures
– Micro-resonators with mode degeneracy: two stages study• Single resonator w mode-degeneracy: the smallest gyroscope in nature.
[3,4]• Set of coupled resonators: Emergence of rotation-induced superstructure
No mode degeneracy
[1] Steinberg B.Z., “Rotating Photonic Crystals: A medium for compact optical gyroscopes,” PRE 71 056621 (2005).[2] Scheuer J., Yariv A., “Sagnac effect in coupled resonator slow light waveguide structure,” PRL 96 053901 (2006).[3] Steinberg B.Z., Boag A., “Splitting of micro-cavity degenerate modes in rotating PhC… ” submitted.[4] Steinberg B.Z., Shamir A., Boag A., CLEO 2006, Long Beach
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Two waves having the same resonant frequency :
• Two different standing waves
Or: (any linear combination of degenerate modes is a degenerate mode!)
• CW and CCW propagations
Under rotation: (as seen in the rotating system rest frame!)
• Mode shapes are preserved
• Eigenvalues (resonant frequencies) SPLIT: classical Sagnac
effect
The single resonator with mode degeneracy
• The most simple and familiar example: A ring resonator
Rotation eigenmodes:
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The single resonator with mode degeneracy (Cont.)
• Degenerate modes in a Photonic Crystal Micro-Cavity (example, not limited to)
Local defect:
TM
How rotation affects this system ? It turns out that: (slow rotation)
The same general picture holds for ANY resonator w mode degeneracy: [3,4]
Orthogonal Real
Rotation eigenmodes:
[3] Steinberg B.Z., Boag A., “Splitting of micro-cavity degenerate modes in rotating PhC… ” submitted.[4] Steinberg B.Z., Shamir A., Boag A., CLEO 2006, Long Beach
Rotation eigenmodes: specific LC of the degenerate modes
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Rotation Eigenmodes
Rotation eigenmodes:
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… and the resonant frequency splits
For the specific PhC under study:
Full numerical simulationUsing rotating medium Green’s function theory
Extracting the peaks
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Interaction between micro-resonators w degenerate modes
• The basic principle:
A CW rotating mode couples only to CCW rotating neighbor
Mechanically Stationary system: • Both modes resonate at• Prescribed coupling
A new concept: the miniature Sagnac Switch
Mechanically Rotating system: • Resonances split• Coupling reduces
PhC defects, Rings, Disks, etc..
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cascade many of them…
• Periodic modulation of local relevant resonant frequency
• Periodic modulation of the CROW difference equation
• Mathematically rigorous derivation of the above physics by: – tight binding theory– applied to the wave equation in the rotating CROW rest frame!
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Theory
• The wave equation in the rotating CROW rest frame: [1,5]
[1] Steinberg B.Z., “Rotating Photonic Crystals: A medium for compact optical gyroscopes,” PRE 71 056621 (2005).[5] T. Shiozawa, “Phenomenological and Electron-Theoretical Study of the Electrodynamics of Rotating Systems,” Proc. IEEE 61 1694 (1973).
• Express the rotating system total field as a sum of the isolated resonator rotation eigenmodes
Rotation operator: lost of self-adjointness
• Substitute into the wave equation, apply Galerkin method
Tight-binding theory, adapted to mode degeneracy + rotation.
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Theory (Cont.)
• The result is the difference (or matrix) equation for the CROW’s excitation coefficients :
• Let and solve for
• An -dependent gap in the CROW transmission curve
• Size of gap:
Periodic modulation of the CROW, byCoincides w the splitting of degenerate modes !!!
Stationary CROW bandwidth
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Example
• Micro-Ring based CROW:Transmission vs. , 29 resonators
Transmission at , vs
Exponential decay rate as a function of , increases linearly with the number of resonators
(splitting)
Rotation induced stop-bandBandWidth =
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Conclusions
• Rotating crystals and SWS = Fun !
• Rotation of degenerate modes CROW – new physical effects
• The added flexibility and the new physical effects offered by
micro-cavities and slow-light structures a potential for
– New generation of Gyroscopes
– Exponential type sensitivity to rotation.
Thank You !