An optical ring resonator is a set of waveguides in which at least one is a closed loop coupled to some sort of light input and output. (These can be, but are not limited to being, waveguides.) The concepts behind optical ring resonators are the same as those behind whispering galleries except that they use light and obey the properties behind constructive interference and total internal reflection. When light of the resonant wavelength is passed through the loop from input waveguide, it builds up in intensity over multiple round-trips due to constructive interference and is output to the output bus waveguide which serves as a detector waveguide. Because only a select few wavelengths will be at resonance within the loop, the optical ring resonator functions as a filter. Additionally, as implied earlier, two or more ring waveguides can be coupled to each other to form an add/drop optical filter [1].
Background
Total internal reflection in PMMA
Optical ring resonators work on the principles behind total internal reflection, constructive interference, and optical coupling.
Total internal reflection
Main article: Total internal reflection
The light travelling through the waveguides in an optical ring resonator remain within the waveguides due to the ray optics phenomenon known as total internal reflection (TIR). TIR is an optical phenomenon that occurs when a ray of light strikes the boundary of a medium and fails to refract through the boundary. Given that the angle of incidence is larger than the critical angle (with respect to the normal of the surface) and the refractive index is lower on the other side of the boundary relative to the incident ray, TIR will occur and no light will be able to pass through. For an optical ring resonator to work well, total internal reflection conditions must be met and the light travelling through the waveguides must not be allowed to escape by any means.
Interference
Main article: Interference (wave propagation)
Interference is the process by which two waves superimpose to form a resultant wave of greater or less amplitude. Interference usually refers to the interaction of waves that are correlated or coherent with each other. In constructive interference, the two waves are of the same phase interfere in a way such that the resultant amplitude will be equal to the sum of the individual amplitudes. As the light in an optical ring resonator completes multiple circuits around the ring component, it will interfere with the other light still in the loop. As such, assuming there are no losses in the system such as those due to absorption, evanescence, or imperfect coupling and the resonance condition is met, the intensity of the light emitted from a ring resonator will be equal to the intensity of the light fed into the system.
Optical coupling
A pictoral representation of the coupling coefficients
Important for understanding how an optical ring resonator works, is the concept of how the linear waveguides are coupled to the ring waveguide. When a beam of light passes through a wave guide as shown in the graph on the right, part of light will be coupled into the optical ring resonator. The reason for this is the phenomenon of the evanescent field, which extends outside of the waveguide mode in an exponentially decreasing radial profile. In other words, if the ring and the waveguide are brought closely together, some light from the waveguide can couple into the ring. There are three aspects that affect the optical coupling: the distance, the coupling length and the refractive indices between the waveguide and the optical ring resonator. In order to optimize the coupling, it is usually the case to narrow the distance between the ring resonator and the waveguide. The closer the distance, the easier the optical coupling happens. In addition, the coupling length affects the coupling as well. The coupling length represents the effective curve length of the ring resonator for the coupling phenomenon to happen with the waveguide. It has been studied that as the optical coupling length increases, the difficulty for the coupling to happen decreases. Furthermore, the refractive index of the waveguide material, the ring resonator material and the medium material in between the waveguide and the ring resonator also affect the optical coupling. The medium material is usually the most important feature under study since it has a great effect on the transmission of the light wave. The refractive index of the medium can be either large or small according to various applications and purposes.
One more feature about optical coupling is the critical coupling. The critical coupling shows that no light is passing through the waveguide after the light beam is coupled into the optical ring resonator. The light will be stored and lost inside the resonator thereafter. [2] Lossless coupling is when no light is transmitted all the way through the input waveguide to its own output; instead, all of the light is coupled into the ring waveguide (such as what is depicted in the image at the top of this page).[3] For lossless coupling to occur, the following equation must be satisfied:
\( |\mathrm{K} |^{2}+|t|^{2}={\mathbf {1}} \)
where t is the transmission coefficient through the coupler and \( \Kappa \) is the taper-sphere mode coupling amplitude, also referred to as the coupling coefficient.
Theory
To understand how optical ring resonators work, we must first understand the optical path length difference (OPD) of a ring resonator. This is given as follows for a single-ring ring resonator:
\( {\mathbf {OPD}}=2\pi rn_{{eff}} \)
where r is the radius of the ring resonator and \( n_{{eff}} \) is the effective index of refraction of the waveguide material. Due to the total internal reflection requirement, \(n_{{eff}} \) must be greater than the index of refraction of the surrounding fluid in which the resonator is placed (e.g. air). For resonance to take place, the following resonant condition must be satisfied:
\( {\mathbf {OPD}}=m\lambda _{{m}} \)
where \( \lambda _{{m}} \) is the resonant wavelength and m is the mode number of the ring resonator. This equation means that in order for light to interfere constructively inside the ring resonator, the circumference of the ring must be an integer multiple of the wavelength of the light. As such, the mode number must be a positive integer for resonance to take place. As a result, when the incident light contains multiple wavelengths (such as white light), only the resonant wavelengths will be able to pass through the ring resonator fully.
The quality factor of an optical ring resonator can be quantitatively described using the following formula:
\( {\mathbf {Q}}=m{\mathcal {F}}=m{\frac {\nu _{{f}}}{\delta \nu }} \)
where \( {\mathcal {F}} \) is the finesse of the ring resonator, \( \nu _{{f}} \) is the free spectral range, and \( \delta \nu \) is the full-width half-max of the transmission spectra. The quality factor is useful in determining the spectral range of the resonance condition for any given ring resonator. The quality factor is also useful for quantifying the amount of losses in the resonator as a low Q factor is usually due to large losses.
A transmission spectra depicting multiple resonant modes (m=1, m=2, m=3, ..., m=n) and the free spectral range.
Double ring resonators
A double ring resonator with rings of varying radii in series showing the relative intensities of light passing through on the first cycle. Note that the light passing through a double ring resonator would more often travel in multiple loops around each ring rather than as pictured.
In a double ring resonator, two ring waveguides are used instead of one. They may be arranged in series (as shown on the right) or in parallel. When using two ring waveguides in series, the output of the double ring resonator will be in the same direction as the input (albeit with a lateral shift). When the input light meets the resonance condition of the first ring, it will couple into the ring and travel around inside of it. As subsequent loops around the first ring bring the light to the resonance condition of the second ring, the two rings will be coupled together and the light will be passed into the second ring. By the same method, the light will then eventually be transferred into the bus output waveguide. Therefore, in order to transmit light through a double ring resonator system, we will need to satisfy the resonant condition for both rings as follows:
\( \ 2\pi n_{{1}}R_{{1}}=m_{{1}}\lambda _{{1}} \)
\( \ 2\pi n_{{2}}R_{{2}}=m_{{2}}\lambda _{{2}} \)
where \( m_{{1}} \) and \( m_{{2}} \) are the mode numbers of the first and second ring respectively and they must remain as positive integer numbers. For the light to exit the ring resonator to the output bus waveguide, the wavelength of the light in each ring must be same. That is, \( \lambda _{{1}}=\lambda _{{2}} \) for resonance to occur. As such, we get the following equation governing resonance:
\( \ {\frac {n_{{1}}R_{{1}}}{m_{{1}}}}={\frac {n_{{2}}R_{{2}}}{m_{{2}}}} \)
Note that both \( m_{{1}} \) and \( m_{{2}} \) need to remain integers.
Optical mirror (reflector) made of a double ring system coupled to a single waveguide. Forward propagating waves in the waveguide (green) excite anti-clockwise traveling waves in both rings (green). Due to the inter-resonator coupling, these waves generate clockwise rotating waves (red) in both rings which in turn excite backward propagating (reflected) waves (red) in the waveguide. The reflected wave exists only in the part of the waveguide to the left of the coupling point to the right ring.[4]
A system of two ring resonators coupled to a single waveguide has also been shown to work as a tunable reflective filter (or an optical mirror).[4] Forward propagating waves in the waveguide excite anti-clockwise rotating waves in both rings. Due to the inter-resonator coupling, these waves generate clockwise rotating waves in both rings which are in turn coupled to backward propagating (reflected) waves in the waveguide.
Applications
Due to the nature of the optical ring resonator and how it "filters" certain wavelengths of light passing through, it is possible to create high-order optical filters by cascading many optical ring resonators in series. This would allow for "small size, low losses, and integrability into [existing] optical networks." [5] Additionally, since the resonance wavelengths can be changed by simply increasing or decreasing the radius of each ring, the filters can be considered tunable. This basic property can be used to create a sort of mechanical sensor. If an optical fiber experiences mechanical strain, the dimensions of the fiber will be altered, thus resulting in a change in the resonant wavelength of light emitted. This can be used to monitor fibers or waveguides for changes in their dimensions.[6] The tuning process can be effected also by a change of refractive index using various means including thermo-optic,[7] electro-optic [8] or all-optical [9] effects. Electro-optic and all-optical tuning is faster than thermal and mechanical means, and hence find various applications including in optical communication. Optical modulators with a high-Q microring are reported to yield outstandingly small power of modulation at a speed of > 50 Gbit/s at cost of a tuning power to match wavelength of the light source. A ring modulator placed in a Fabry-Perot laser cavity was reported to eliminate the tuning power by automatic matching of the laser wavelength with that of the ring modulator while maintaining high-speed ultralow-power modulation of a Si microring modulator.
Optical ring, cylindrical, and spherical resonators have also been proven useful in the field of biosensing.,[10][11][12][13][14] and a crucial research focus is the enhancement of biosensing performance [15][16][17] One of the main benefits of using ring resonators in biosensing is the small volume of sample specimen required to obtain a given spectroscopy results in greatly reduced background Raman and fluorescence signals from the solvent and other impurities. Resonators have also been used to characterize a variety of absorption spectra for the purposes of chemical identification, particularly in the gaseous phase.[18]
Another potential application for optical ring resonators are in the form of whispering gallery mode switches. "[Whispering Gallery Resonator] microdisk lasers are stable and switch reliably and hence, are suitable as switching elements in all-optical networks." An all-optical switch based on a high Quality factor cylindrical resonator has been proposed that allows for fast binary switching at low power. material.[5]
Many researchers are interested in creating three-dimensional ring resonators with very high quality factors. These dielectric spheres, also called microsphere resonators, "were proposed as low-loss optical resonators with which to study cavity quantum electrodynamics with laser-cooled atoms or as ultrasensitive detectors for the detection of single trapped atoms.”[19]
Ring resonators have also proved useful as single photon sources for quantum information experiments.[20] Many materials used to fabricate ring resonator circuits have non-linear responses to light at high enough intensities. This non-linearity allows for frequency modulation processes such as four-wave mixing and Spontaneous parametric down-conversion which generate photon pairs. Ring resonators amplify the efficiency of these processes as they allow the light to circulate around the ring.
See also
Resonator
Ring laser
Total internal reflection
Coupling
Filter (optics)
Optical switch
Coupled mode theory
References
Chremmos, Ioannis; Schwelb, Otto; Uzunoglu, Nikolaos, eds. (2010). Photonic Microresonator Research and Applications. Springer Series in Optical Sciences. 156. Boston, MA: Springer US. doi:10.1007/978-1-4419-1744-7. ISBN 9781441917430.
Xiao, Min; Jiang, Dong & Yang. Coupling Whispering-Gallery-Mode Microcavities With Modal Coupling Mechanism. IEEE Journal of Quantum Electronics (44.11, November 2008).
Cai; Painter & Vahala. Observation of Critical Coupling in a Fiber Taper to a Silica-Microsphere Whispering-Gallery Mode System. Physical Review Letters (85.1, July 2000).
Chremmos, I.; Uzunoglu, N. (2010). "Reflective properties of double-ring resonator system coupled to a waveguide". IEEE Photonics Technology Letters. 17 (10): 2110–2112. doi:10.1109/LPT.2005.854346. ISSN 1041-1135.
Ilchenko & Matsko. Optical Resonators With Whispering-Gallery Modes — Part II: Applications. IEEE Journal of Selected Topics in Quantum Electronics (12.1, January 2006).
Westerveld, W.J.; Leinders, S.M.; Muilwijk, P.M.; Pozo, J.; van den Dool, T.C.; Verweij, M.D.; Yousefi, M.; Urbach, H.P. (10 January 2014). "Characterization of Integrated Optical Strain Sensors Based on Silicon Waveguides". IEEE Journal of Selected Topics in Quantum Electronics. 20 (4): 101. Bibcode:2014IJSTQ..20..101W. doi:10.1109/JSTQE.2013.2289992.
N. Li, E. Timurdogan, C. V. Poulton, M. Byrd, E. S. Magden, Z. Su, G. Leake, D Coolbaugh, D. Vermeulen, M. R. Watts (2016) “C-band swept wavelength erbium-doped fiber laser with a high-Q tunable interior-ridge silicon microring cavity”, Optics Express, Vol. 24, Issue 20, pp.22741-22748
Sadasivan, Viswas (2014). "QCSE Tuned Embedded Ring Modulator". Journal of Lightwave Technology. 32 (1): 107–114. Bibcode:2014JLwT...32..107S. doi:10.1109/JLT.2013.2289324.
Ibrahim,and, Tarek A.; Grover, Rohit; Kuo, Li-Chiang; Kanakaraju, Subramaniam; Calhoun, Lynn C.; Ho, Ping-Tong (2003). All-optical switching using a critically coupled InP micro-racetrack resonator. OSA Trends in Optics and Photonics (Optical Society of America, 2003). p. ITuE4. doi:10.1364/IPR.2003.ITuE4. ISBN 978-1-55752-751-6.
A. Ksendzov & Y. Lin (2005). "Integrated optics ring-resonator sensors for protein detection". Opt. Lett. 30 (24): 3344–3346. Bibcode:2005OptL...30.3344K. doi:10.1364/ol.30.003344.
Fard, S. T., Grist, S. M., Donzella, V., Schmidt, S. A., Flueckiger, J., Wang, X., ... & Cheung, K. C. (2013, March). Label-free silicon photonic biosensors for use in clinical diagnostics. In SPIE OPTO (pp. 862909-862909). International Society for Optics and Photonics.
K. D. Vos; I. Bartolozzi; E. Schacht; P. Bienstman & R. Baets (2007). "Silicon-on-Insulator microring resonator for sensitive and label-free biosensing". Opt. Express. 15 (12). pp. 7610–7615.
Witzens, J.; Hochberg, M. (2011). "Optical detection of target molecule induced aggregation of nanoparticles by means of high-Q resonators". Optics Express. 19 (8): 7034–7061. Bibcode:2011OExpr..19.7034W. doi:10.1364/OE.19.007034. PMID 21503017.
Lin S.; K. B. Crozier (2013). "Trapping-Assisted Sensing of Particles and Proteins Using On-Chip Optical Microcavities". ACS Nano. 7 (2): 1725–1730. doi:10.1021/nn305826j. PMID 23311448.
Donzella, V., Sherwali, A., Flueckiger, J., Grist, S. M., Fard, S. T., & Chrostowski, L. (2015). Design and fabrication of SOI micro-ring resonators based on sub-wavelength grating waveguides. Optics Express, 23(4), 4791-4803.
Fard, S. T., Donzella, V., Schmidt, S. A., Flueckiger, J., Grist, S. M., Fard, P. T., ... & Ratner, D. M. (2014). Performance of ultra-thin SOI-based resonators for sensing applications. Optics Express, 22(12), 14166-14179.
Flueckiger, J., Schmidt, S., Donzella, V., Sherwali, A., Ratner, D. M., Chrostowski, L., & Cheung, K. C. (2016). Sub-wavelength grating for enhanced ring resonator biosensor. Optics Express, 24(14), 15672-15686.
Blair & Chen. Resonant-Enhanced Evanescent-Wave Fluorescence Biosensing with Cylindrical Optical Cavities. Applied Optics (40.4, February 2001).
Götzinger; Benson & Sandoghdar. Influence of a Sharp Fiber Tip on High-Q Modes of a Microsphere Resonator. Optics Letters (27.2, January 2002).
E. Engin; D. Bonneau; C. Natarajan; A. Clark; M. Tanner; R. Hadfield; S. Dorenbos; V. Zwiller; K. Ohira; N. Suzuki; H. Yoshida; N. Iizuka; M. Ezaki; J. O?Brien & M. Thompson (2013). "Photon pair generation in a silicon micro-ring resonator with reverse bias enhancement". Opt. Lett. 21 (23): 27826–27834. arXiv:1204.4922. Bibcode:2013OExpr..2127826E. doi:10.1364/OE.21.027826. PMID 24514299.
Hellenica World - Scientific Library
Retrieved from "http://en.wikipedia.org/"
All text is available under the terms of the GNU Free Documentation License
