Engineering the Mode Coupling in Microrings for Laser and Sensor Applications (Lynford L Goddard)
Zusammenfassung
TLDRIn this talk, the speaker presents the work done by their group on reflective micro ring resonators over eight years at the University of Illinois. They explain the principles of these devices, including the coupling of different modes within the micro ring, and how this engineering leads to applications in laser mirrors and biosensing. The presentation covers experimental results demonstrating single wavelength operation, the simulation and design processes using tools like COMSOL and MATLAB, and the advantages over traditional structures such as linear Bragg reflectors including smaller size and better performance. Applications also include the detection of biomolecules using plasmonics based whispering gallery mode sensors. The speaker concludes by discussing future directions in developing low threshold lasers and optimizing fabrication processes, emphasizing the collaborative efforts that made the work possible.
Mitbringsel
- 🔬 Reflective micro ring resonators improve sensing capabilities.
- 🔄 Mode coupling enhances laser output and minimizes noise.
- ⚙️ Simulation tools like COMSOL and MATLAB aid design processes.
- 🌟 Applications include single wavelength lasers and biosensing.
- 🔍 Plasmonic sensors detect small biomolecules effectively.
- 🔧 Collaboration and funding were key to research success.
- ⚖️ Balancing design for high sensitivity vs. resonance quality factor.
- 📏 Smaller devices reduce fabrication variation sensitivity.
- ♻️ Temperature affects refractive index, changing resonances.
- 📈 Future work includes improving fabrication and developing new designs.
Zeitleiste
- 00:00:00 - 00:05:00
The speaker expresses gratitude to the i optics organizing committee and introduces the topic of micro ring resonators, focusing on mode coupling for applications in sensing. The presentation will cover motivations, simulations, experimental results, and applications.
- 00:05:00 - 00:10:00
The traditional micro ring resonators utilize constructive interference for light coupling, but the speaker's group has innovated with reflective designs that incorporate gratings to enhance reflection spectra. The outline includes motivation, methods, results, and applications.
- 00:10:00 - 00:15:00
The speaker discusses the motivation behind studying reflective micro ring resonators, highlighting the efficiency, size reduction, and benefits over traditional linear Bragg reflectors, particularly in terms of power tuning and elimination of side lobes.
- 00:15:00 - 00:20:00
The design and fabrication of these reflective micro ring resonators are presented, including the use of simulations to understand light behavior and coupling mechanisms. The effective coupling theory guides the device design for optimal resonance properties.
- 00:20:00 - 00:25:00
The speaker discusses experimental results demonstrating high reflection capabilities and precise resonance control using their reflective micro ring designs, showcasing their potential for practical applications in lasers and sensors.
- 00:25:00 - 00:30:00
Applications of the reflective micro ring resonators are explored, emphasizing their use as mirrors for lasers, achieving single wavelength operation through careful design and mode selection in the resonators.
- 00:30:00 - 00:35:00
The speaker introduces integrated devices, such as the single wavelength integrated ring laser, highlighting how mode coupling and engineering can lead to improved performance in lasing operations.
- 00:35:00 - 00:40:00
The summary touches on the development of hybrid sensing platforms, where micro ring resonators interact with plasmonic nanostructures to enable highly sensitive detection of biomolecules through mode coupling effects.
- 00:40:00 - 00:45:00
The presentation concludes with the focus on future advancements, including exploring plasmonic antennas and optimizing laser designs to enhance sensitivity and performance in sensing applications.
- 00:45:00 - 00:54:03
Acknowledgments are given to the research team's efforts and funding sources, with an invitation for questions from the audience.
Mind Map
Video-Fragen und Antworten
What are reflective micro ring resonators used for?
They are used in applications such as sensing and laser technologies.
How has the speaker's group contributed to this field?
They engineered mode coupling in reflective micro ring resonators, leading to several innovative results.
What simulation tools are mentioned in the presentation?
COMSOL and MATLAB were used for simulation and design.
What are the benefits of reflective micro ring resonators over traditional designs?
They offer smaller size, reduced sensitivity to fabrication variations, and less noise in laser output.
What is the significance of mode coupling in these devices?
Mode coupling allows for selective reflection and reduces unwanted resonances, enhancing performance.
What experimental results were discussed?
The results include the demonstration of single wavelength reflectors and laser operations.
What are the applications of plasmonics based whispering gallery mode sensors?
They are used for detecting small biomolecules binding to the sensor surface.
What is the advantage of using a reflective micro ring as a laser mirror?
It allows narrow operating bandwidth and higher efficiency in semiconductor lasers.
How does temperature affect the resonator structure?
Temperature changes affect the refractive index and can shift resonance wavelengths.
What future work is mentioned for the reflective micro rings?
The group is looking at further optimizing fabrication processes and developing new designs for enhanced performance.
Weitere Video-Zusammenfassungen anzeigen
- 00:00:05Thank You Hasan and also thank you to
- 00:00:08the rest of the i optics organizing
- 00:00:10committee for giving me the opportunity
- 00:00:11to share some of the results that my
- 00:00:14group has had in my Kron resonators over
- 00:00:17the past Wow eight eight years I've been
- 00:00:21at Illinois now this is my ninth year
- 00:00:22and very early in our in our development
- 00:00:26as a group we got interested in the
- 00:00:28theory and application of reflective my
- 00:00:30crane resonators and so we'll talk today
- 00:00:32about how we engineer the mode coupling
- 00:00:35between the different modes and the
- 00:00:37micro ring so that we can have
- 00:00:38applications and sensing and amazing so
- 00:00:42brief outline um I'm going to talk about
- 00:00:44some motivation there's the traditional
- 00:00:46my crowing resonator that many of you
- 00:00:48are familiar with basically light
- 00:00:50couples in from a waveguide into a micro
- 00:00:52resonator and based on constructive
- 00:00:54interference the field intensity builds
- 00:00:56up inside the ring so our group started
- 00:00:59looking at reflective micron resonators
- 00:01:01where we put our grading inside the ring
- 00:01:02so that we can generate a reflection
- 00:01:04spectrum I'll talk about some of the
- 00:01:07simulation design tools on basically our
- 00:01:09methods of using comsol to simulate
- 00:01:12two-dimensional cross sections of the
- 00:01:15mode profile using finite element method
- 00:01:17I'll talk about the work that we did to
- 00:01:20develop a cylindrical couple mode theory
- 00:01:22so that we can understand how the
- 00:01:24different modes of the micro ring
- 00:01:26coupled to each other and how we can
- 00:01:28engineer the spectra by doing the
- 00:01:30Selective coupling I'll talk about the
- 00:01:32results that we have four passive
- 00:01:34microwave resonators how we design in
- 00:01:35fabricated structures in silicon nitride
- 00:01:38using silicon dioxide cladding the
- 00:01:40measurement of these devices so that we
- 00:01:43can calculate the spectra of the
- 00:01:45transmitted and also the reflected
- 00:01:48properties of the device and I'll show
- 00:01:51some experimental results where we
- 00:01:52demonstrated single wavelength
- 00:01:53reflectors based on our micro ring
- 00:01:56design next I'll go into some
- 00:01:59applications so the first part of the
- 00:02:01talk will be mostly about the theory of
- 00:02:03these devices and gives some basic
- 00:02:05fabrication results the second part of
- 00:02:07the talk will go into the applications
- 00:02:09so we want to be able to use these
- 00:02:10devices as micro these pet these
- 00:02:13reflective my crowing mirrors as laser
- 00:02:16mirrors so
- 00:02:16replacing the linear bragg reflector
- 00:02:18with this compact micro ring based
- 00:02:21reflector and we show experimental
- 00:02:24results of how we did monolithic active
- 00:02:26and passive integration of a device on a
- 00:02:29gallium arsenide substrate I'll then get
- 00:02:32into our work in single wavelength
- 00:02:34integrated mic releasers it's nice to
- 00:02:38have good acronyms so we call this
- 00:02:40device the swirl single wavelength
- 00:02:42integrated ring laser I'll talk about
- 00:02:44how we can engineer the loss of the
- 00:02:47different modes based on mode coupling
- 00:02:51and then show some fabrication results
- 00:02:53and experimental results about how we
- 00:02:55can choose the specific resonance the
- 00:02:57specific as a middle order of the
- 00:02:59resonant for lazing finally I'll go into
- 00:03:04the application and sensing on so our
- 00:03:06group is interested in making a
- 00:03:09plasmonics based whispering gallery mode
- 00:03:11based micro ring sensors so this hybrid
- 00:03:15sensor allows us to detect small
- 00:03:18biomolecules as it binds to the surface
- 00:03:21so the structure consists of this
- 00:03:24silicon microsphere surrounded by these
- 00:03:27gold nanoparticles which we call
- 00:03:29epitopes and based on the design of the
- 00:03:32dimensions of the epitopes relative to
- 00:03:34the design of the whispering gallery
- 00:03:36mode we can engineer coupling between
- 00:03:38the isolated my crowing resonator on
- 00:03:41formed by the whispering gallery mode
- 00:03:43and the plasmonics chain ring resonator
- 00:03:45formed by these epitopes and will show
- 00:03:47that based on the device dimensions we
- 00:03:50essentially get something like mode anti
- 00:03:53crossing or abandoned I crossing where
- 00:03:55we generate the symmetric and
- 00:03:56anti-symmetric modes and in this very
- 00:03:59small variation in the radius we can get
- 00:04:03significantly significant changes in the
- 00:04:06resonance on shift due to binding events
- 00:04:10okay so let's talk about the motivation
- 00:04:12so why do we want to study reflective my
- 00:04:15crowing resonators so when you look at a
- 00:04:17semiconductor laser on typically the end
- 00:04:19facets are made by linear Bragg
- 00:04:21reflectors so alternating high and low
- 00:04:23refractive index materials and you make
- 00:04:26these quarter wavelength long for each
- 00:04:28section
- 00:04:29and this is a well-known reflection
- 00:04:31spectrum profile which has a maximum in
- 00:04:33the reflection when the wavelength is
- 00:04:36exactly such that the thicknesses lab
- 00:04:38Dover for for each layer so you can
- 00:04:40design these high reflective mirrors on
- 00:04:42some of the disadvantages of the linear
- 00:04:45dbr is that it's very long in order to
- 00:04:48get a high reflectivity and narrow line
- 00:04:50with you have to make it longer so the
- 00:04:52width in frequency is inversely
- 00:04:55proportional to the length of the dbr so
- 00:04:57if you want to improve the narrowness of
- 00:05:01this reflection spectrum by a factor of
- 00:05:0210 you need it to be 10 times as long
- 00:05:05there's also an issue when you start
- 00:05:07making these gratings to the millimeter
- 00:05:09to centimeter size in that you get
- 00:05:11fabrication non-uniformities so across
- 00:05:13the wafer on the pitch that you're able
- 00:05:16to achieve the refractive index the
- 00:05:18device dimensions when you fabricate
- 00:05:20these devices it becomes less uniform as
- 00:05:23it spreads out there is also the issue
- 00:05:26of these side lobes so the side lobes
- 00:05:28are actually additional modes that can
- 00:05:30lays in your spectrum they add noise in
- 00:05:33the overall laserperformance and so
- 00:05:35although you get the main output power
- 00:05:37at the peak of the reflection spectrum
- 00:05:39you also generate light at these other
- 00:05:41unwanted wavelengths which produces
- 00:05:44laser noise so our group had a very
- 00:05:47simple idea our idea was just take the
- 00:05:49linear dbr and roll it into itself and
- 00:05:52make a ring dbr and we didn't really
- 00:05:54fully understand all the great benefits
- 00:05:57that you can have just by doing this our
- 00:05:59main motivation was we wanted to make a
- 00:06:01smaller device so after we started
- 00:06:03simulating these structures we found
- 00:06:05some really nice properties so the main
- 00:06:07goal was we wanted to make it smaller
- 00:06:09but in addition to this because it's
- 00:06:12smaller it's less sensitive to way for
- 00:06:14scale variations so I'm only patterning
- 00:06:16a grating over a 60 or 70 micron
- 00:06:19diameter ring instead of a few
- 00:06:22millimeters two centimeters long and I
- 00:06:24can achieve the same amount of
- 00:06:26reflection power from my very compact
- 00:06:29structure that I could from this very
- 00:06:30long device so if I want to tune the
- 00:06:33structure if I do something like
- 00:06:35temperature tuning in the first case I
- 00:06:37have to temperature tune the entire
- 00:06:38length of the dbr whereas in this case I
- 00:06:41only have two temperature to in a very
- 00:06:42small micro
- 00:06:43resonator so there's less power required
- 00:06:45for tuning probably the biggest benefit
- 00:06:48of the structure is that there are no
- 00:06:50side lobes so these side lobes exist
- 00:06:53because of the fact that the linear
- 00:06:56grading has a finite length and so this
- 00:06:59finite length introduces zeros into the
- 00:07:02summation that you would get from adding
- 00:07:04up the reflectivities because this ring
- 00:07:07is periodic when you add up the
- 00:07:08reflections from multiple passes around
- 00:07:11the ring it becomes an infinite sum and
- 00:07:15this infinite sum does not have zeros so
- 00:07:17as a results there are no side lobes in
- 00:07:19the reflection profile and you'll get a
- 00:07:21much cleaner laser output if you use
- 00:07:25this as a reflective mirror so um let's
- 00:07:29look at how we discuss these things on
- 00:07:33so we have lights in a waveguide that
- 00:07:35couples to a ring on we form the ring
- 00:07:37just by bending the waveguide into ring
- 00:07:39shape we can easily fabricate one
- 00:07:41dimensional or two dimensional arrays of
- 00:07:43these ring resonators on chip through
- 00:07:45standard even lithography a single micro
- 00:07:48ring resonator will have equally spaced
- 00:07:50resonant modes at each one of these
- 00:07:52wavelengths that's resonant essentially
- 00:07:54you have an integer multiple of
- 00:07:56wavelengths fitting inside the
- 00:07:58circumference of the ring so when this
- 00:08:00has a constructive interference such
- 00:08:02that i have an integer multiple on the
- 00:08:04power in the ring will build up and all
- 00:08:07the power gets lost in the ring instead
- 00:08:09of being transmitted so when I'm off
- 00:08:10resonance the light goes into the ring
- 00:08:12and then it destructively interferes and
- 00:08:14the light couples back out when I'm on
- 00:08:16resonance the light couples into the
- 00:08:18ring and it keeps circulating until it
- 00:08:20builds up in strength and eventually
- 00:08:22it's absorbed inside the ring so add a
- 00:08:26single resonance there's actually two
- 00:08:28degenerate modes the two degenerate
- 00:08:30modes are the counter propagating modes
- 00:08:31so there's one that's going clockwise
- 00:08:33one that's going counterclockwise and
- 00:08:35these have the exact same resonance
- 00:08:37frequency it's the key that we're going
- 00:08:39to do with our engineered mode coupling
- 00:08:40is we're going to couple the clockwise
- 00:08:43and the counterclockwise propagating
- 00:08:44modes to be able to form standing wave
- 00:08:47modes so the standing wave modes are
- 00:08:49going to allow us to have high
- 00:08:50reflection in our device so we study the
- 00:08:53reflective micro ring resonators using s
- 00:08:55parameters
- 00:08:56we do the simple calculation in matlab
- 00:08:58we model our system as we have power
- 00:09:01coming in and there's a certain amount
- 00:09:02or electric field coming in we have a
- 00:09:04certain amount of electric field
- 00:09:06circulating in the ring there's a
- 00:09:07reflective element which you can write
- 00:09:09in terms of a scattering matrix with
- 00:09:11reflection and transmission coefficients
- 00:09:13and what you can calculate is as a
- 00:09:15function of the wavelength normalized by
- 00:09:17the free spectral range of the device
- 00:09:19what is the overall reflection of this
- 00:09:22structure as a function of the
- 00:09:25reflection that you put the reflection
- 00:09:28coefficient of the element that you put
- 00:09:30inside this ring so we get a profile
- 00:09:33that looks like this so this is a plot
- 00:09:35so for a fixed amount of coupling into
- 00:09:37the ring for a fixed amount of loss we
- 00:09:39generate one of these plots and this
- 00:09:41plot allows us to design the type of
- 00:09:43reflective element that we put in the
- 00:09:45ring so that we get an overall
- 00:09:47reflection spectrum that's useful for a
- 00:09:49device so as an example if I wanted to
- 00:09:52design a structure that reflects exactly
- 00:09:54at this one wavelength and doesn't
- 00:09:57reflect it any of the other resonances
- 00:09:59what I need to do is I need to construct
- 00:10:01a wavelength dependent reflector inside
- 00:10:04the ring that goes through the maximum
- 00:10:06in this curve here and goes through
- 00:10:08nulls at all these other resonances if I
- 00:10:11can construct such a device then the
- 00:10:14overall structure will have one
- 00:10:15reflection peak in it and all the other
- 00:10:18resonances will be non reflective so I
- 00:10:21want to construct a device that has this
- 00:10:23particular reflection profile it's
- 00:10:25reflective in this case it's like five
- 00:10:28percent reflection on at this one
- 00:10:31wavelength and then it has no reflection
- 00:10:33at these other wavelengths and so if I
- 00:10:37can construct such a device than the can
- 00:10:39the combined response of the overall
- 00:10:41ring plus reflector will have high
- 00:10:43reflectivity at my design wavelength and
- 00:10:45then i'll have the suppressed
- 00:10:47reflectivity at the other resonances so
- 00:10:50at these other residences the field
- 00:10:52wants to build up and become stronger
- 00:10:54because it's a resonant condition but at
- 00:10:56the same time this element is becoming
- 00:10:58non-reflective so as a result the
- 00:11:00overall reflection will be very small so
- 00:11:03how do i construct something that has
- 00:11:05this profile it turns out that if i put
- 00:11:07exactly half the grade
- 00:11:10filled with this linear dbr then I get
- 00:11:12these reflection nodes so in the linear
- 00:11:15DVR it's a bad thing but when I combine
- 00:11:17it into the ring I get the exact
- 00:11:19spectrum that I want and it turns out
- 00:11:21that if this is exactly half then I get
- 00:11:23the nulls at exactly the resonance
- 00:11:25wavelength of the other residences so
- 00:11:28this combined structure gives us high
- 00:11:30reflectivity at the design wavelength
- 00:11:31and no reflection or in this case minus
- 00:11:3440 DB in terms of reflection at the
- 00:11:36other resonances so if i zoom in I can
- 00:11:40see I have a nice reflection at that one
- 00:11:42wavelength the transmission goes down
- 00:11:44and then at the other residences the
- 00:11:46reflection is zero so this will form the
- 00:11:49basis of a single wave length mirror so
- 00:11:51if I want to make a laser and I want it
- 00:11:53to be operating at a single wavelength
- 00:11:54if I put this device as the output or as
- 00:11:58the awe as the high reflectivity mirror
- 00:12:01in my laser cavity then this structure
- 00:12:03will reflect and give me lazing
- 00:12:05condition at this one resonant
- 00:12:08wavelength and all the other wavelengths
- 00:12:10will be not able to laze because the
- 00:12:12loss going from the mirror is going to
- 00:12:14be very high because it has very low
- 00:12:17reflectivity overall so now let's shift
- 00:12:21into on the simulation and design tools
- 00:12:23that we use so our group does quite a
- 00:12:26bit of modeling depending on what
- 00:12:28program we use we combine comsol
- 00:12:30modeling we also do modeling and matlab
- 00:12:32we're collaborating with professor Jim
- 00:12:35scroop to do a computational fe m so we
- 00:12:38have all these different simulation and
- 00:12:40design tools so I'll talk about our
- 00:12:42simplified versions of the of the tools
- 00:12:45so in order to design a general my
- 00:12:49crowing reflector on we want fast and
- 00:12:52accurate simulations the challenge was
- 00:12:54simulating a micro ring resonator is
- 00:12:56that since the dimensions are very large
- 00:12:58compared to the wavelength and since the
- 00:13:01dimensions are it's a three-dimensional
- 00:13:03structure you need a lot of memory and
- 00:13:05you need a lot of computational power to
- 00:13:07be able to accurately simulate it with a
- 00:13:09brute force method so one of the
- 00:13:11quickest things that you can do is
- 00:13:13notice that the modes have it as a
- 00:13:15mutual dependence of the form e to the j
- 00:13:18nu five so taking off this azimuthal
- 00:13:20dependence allows you to reduce the
- 00:13:23problem
- 00:13:23from a three-dimensional problem into a
- 00:13:25two-dimensional problem and so typically
- 00:13:27we simulate the mood profile in this
- 00:13:29two-dimensional constant five plane
- 00:13:31where we plot as a function of radius
- 00:13:33and a function of Z the mode profile so
- 00:13:36this tiny blocks here is the core
- 00:13:39surrounded by some cladding material and
- 00:13:41then based on the way that we fabricate
- 00:13:43it we actually have some more unwanted
- 00:13:45material at the side so in order to
- 00:13:49study the effect of the gratings that
- 00:13:51we're putting on our structure what we
- 00:13:53wanted to do is developed a develop a
- 00:13:56cylindrical coordinate coupled mode
- 00:13:58theory so a couple mode theory is well
- 00:14:00known in a Cartesian coordinates is very
- 00:14:02easy to write down on well I should say
- 00:14:04very easy in the sense that you have to
- 00:14:06look up a bunch of papers and then it
- 00:14:07becomes very easy to write down but what
- 00:14:10we wanted to do is we wanted to study
- 00:14:11the coupling between the clockwise and
- 00:14:14the counterclockwise amplitudes of the
- 00:14:18mode so what we developed well we write
- 00:14:21out Maxwell's equations we do a whole
- 00:14:22bunch of algebra we simplify it using
- 00:14:24these approximations and we get a
- 00:14:26differential equation that talks about
- 00:14:28the coupling of the forward and the
- 00:14:29backward propagating modes this coupling
- 00:14:32matrix on what you have to do is you
- 00:14:34have to calculate the electric and
- 00:14:35magnetic fields and then compute various
- 00:14:37integrals of the electric and magnetic
- 00:14:39field tangential and parallel components
- 00:14:42/ cross sectional areas so in this paper
- 00:14:45you can figure out what these integrals
- 00:14:47you have to compute is but basically all
- 00:14:49you need to do is simulate the
- 00:14:50two-dimensional cross sectional profile
- 00:14:52for electrical magnetic fields and then
- 00:14:53calculate a bunch of integrals based on
- 00:14:56that and this allows you to figure out
- 00:14:57how do the forward and the backward
- 00:14:58waves a couple to each other so we
- 00:15:03verified this with fim simulations so
- 00:15:06the FM simulation that we did was a two
- 00:15:08dimensional simulation so the method
- 00:15:10that we developed is good to run in 3d
- 00:15:13however the commercial software we're
- 00:15:15validating it against doesn't have
- 00:15:16enough memory to simulate in 3d so we do
- 00:15:18the simulation in 2d where this is the
- 00:15:21same structure in the out-of-plane
- 00:15:24directions so a two-dimensional
- 00:15:26simulation of this reflective micro ring
- 00:15:29and you can see that we have these nice
- 00:15:30standing wave generated from sending
- 00:15:34light in and then having it highly
- 00:15:36ected and we get very good agreement
- 00:15:38between the finite element method in
- 00:15:40comsol and our cylindrical coupled
- 00:15:41million theory next we wanted to look at
- 00:15:45some nonlinear effects so we wanted to
- 00:15:47study the self-heating dynamics that
- 00:15:49occur in micro resonators so basically
- 00:15:52as you send power into this micro ring
- 00:15:55the amplitude builds up in strength
- 00:15:56because we have constructive
- 00:15:58interference and this increase in power
- 00:16:00that's circulating inside the ring
- 00:16:01there's this tiny bit of absorption that
- 00:16:04causes heating of the ring which changes
- 00:16:06the refractive index which therefore
- 00:16:08shifts the resonances so we wanted to
- 00:16:10study the time domain evolution of the
- 00:16:13optical properties of the Ring so we
- 00:16:16developed time domain coupled mode
- 00:16:17theory plus a lump thermal circuit model
- 00:16:20so we have these equations which are
- 00:16:22just the standard coupled mode theory in
- 00:16:25the time domain plus there's this
- 00:16:27thermal model where we consider that the
- 00:16:29core is the source of heat so when the
- 00:16:32light is propagating in the core of the
- 00:16:34waveguide if there's absorption there's
- 00:16:36a certain amount of heat generated given
- 00:16:38by alpha Q there's a certain amount of
- 00:16:40heat that's generated in the cladding
- 00:16:42which is oxide given by 1 minus alpha Q
- 00:16:44and then there's thermal resistance
- 00:16:46between the core and the cladding
- 00:16:48between the cladding and the substrate
- 00:16:49and these are also heat sick these are
- 00:16:52also heat storage materials so there's a
- 00:16:55thermal capacitance from the core to the
- 00:16:57substrate and from the cladding to the
- 00:16:59substrate and we get an equivalent
- 00:17:00circuit model that looks like this so
- 00:17:02there are heat sources and there are
- 00:17:04compassed ences and resistances in the
- 00:17:06structure and you can calculate the
- 00:17:08temperature at different parts of the
- 00:17:10device based on this model you can then
- 00:17:12predict what happens if I sit at a
- 00:17:15specific wavelength relative to the
- 00:17:17resonance and i put in a pulse of
- 00:17:19optical energy so this pulse of optical
- 00:17:22energy essentially in this graph on we
- 00:17:25have this turning off and so there's a
- 00:17:28certain time constant in which this
- 00:17:30decays so we get a certain time response
- 00:17:33that we measured experimentally and
- 00:17:34validated with our simulation ok so now
- 00:17:39let's talk about the structures that we
- 00:17:41fabricate and how we test them so on our
- 00:17:44general setup we have a tunable laser
- 00:17:46isolator polarization controller so we
- 00:17:48can control the
- 00:17:49zation whether we launch te or TM
- 00:17:51polarized light into our device under
- 00:17:53test this polarizer ensures that the
- 00:17:55polarization is lined to the direction
- 00:17:57that we want we have a reference arm
- 00:18:00that measures the power that we're
- 00:18:01putting in a circulator so that we can
- 00:18:03send the light to the device under test
- 00:18:05and the reflective power gets measured
- 00:18:06by the reflection detector and then the
- 00:18:09transmitted power goes to the
- 00:18:10transmitted detector and on each of
- 00:18:12these fibers are lens tips so that we
- 00:18:15can focus light from the fiber into this
- 00:18:17mic rowing resonator chip and I'll
- 00:18:19explain how we were able to achieve
- 00:18:21these measurement results of having a
- 00:18:23single reflection peak so our structure
- 00:18:27consists of silicon nitride core on a
- 00:18:30grown thermal oxide of of sio2 on a
- 00:18:35silicon substrate and so we designed
- 00:18:37this using the simulation methods I
- 00:18:40previously described we fabricated these
- 00:18:42structures with ebm lithography so
- 00:18:44thanks to Edmond and some of the others
- 00:18:46in the MNT all clean room for helping us
- 00:18:48with the fabrication so you can see the
- 00:18:50microwave resonator the scale bar is
- 00:18:52about 15 microns and we made different
- 00:18:54types of indentations to form our
- 00:18:56reflectors so in this case we made 50
- 00:18:59nanometer indentations in the waveguide
- 00:19:01with in this case we have a waveguide
- 00:19:03that's here and then we have a separate
- 00:19:05grading structure so the evanescent tale
- 00:19:08of the mode in this waveguide couples
- 00:19:11with the grading that's on the separate
- 00:19:13region and then we measure the
- 00:19:15reflection and transmission setup or
- 00:19:17spectra with our setup so the design
- 00:19:20wavelength so when we did the first run
- 00:19:23of devices on we didn't have accurate
- 00:19:25numbers for the refractive index of
- 00:19:27silicon nitride or for silicon dioxide
- 00:19:29that we were depositing so our first
- 00:19:32design we wanted to get wavelengths
- 00:19:34being 1550 because that's the center
- 00:19:36wavelength for the c-band which is the
- 00:19:38wavelength that has the minimum loss in
- 00:19:40optical fiber but our first set of
- 00:19:43devices came out at 1,500 instead of
- 00:19:461550 and the main source of error was
- 00:19:48the refractive indices that we assume so
- 00:19:51we were assumed that the value of the
- 00:19:52refractive index of silicon nitride was
- 00:19:54too it turns out that it's 1.98 and that
- 00:19:57very small change of one percent is
- 00:20:02enough to shift some
- 00:20:03portion of the spectrum there are some
- 00:20:04other errors in the dimensions and the
- 00:20:06values of the refractive index of the
- 00:20:08core of the cladding that also
- 00:20:10contributed to the shift so what we did
- 00:20:13was ok so the wavelength that we wanted
- 00:20:16was incorrect so how can we accurately
- 00:20:18measure the wavelength or the refractive
- 00:20:21indices of our devices well one thing to
- 00:20:23notice is that the resonance wavelengths
- 00:20:26depend very critically on whether it's
- 00:20:28te or TM polarized light so you get
- 00:20:31different effective indices for
- 00:20:33different modes of propagation and based
- 00:20:35on these resonance locations the
- 00:20:38difference between te and TM and also
- 00:20:41the geometry the free spectral range
- 00:20:42which is the separation between adjacent
- 00:20:46resonances the free spectral range plus
- 00:20:49the te and TM dependencies these
- 00:20:51determine where these resonances lined
- 00:20:54up so we measure for a single micron
- 00:20:56resonator the positions of these
- 00:20:58resonances and from this we can infer
- 00:21:01the refractive index attractive indices
- 00:21:03of the core in the cladding material so
- 00:21:05we get a measurement of 34 resonance
- 00:21:07wavelengths we form it into a vector and
- 00:21:10then we have to somehow resolve the
- 00:21:13ambiguity that occurs in micro
- 00:21:15resonators so there's no way to tell
- 00:21:17from the spectrum whether this is the
- 00:21:19200th mode or the 200 first as a methyl
- 00:21:21mode but with a reflective structure we
- 00:21:24know that this particular resonance
- 00:21:26corresponds to the 200th mode so by
- 00:21:28using the reflection peak we're able to
- 00:21:31resolve the mode ambiguity and based on
- 00:21:33that we can then say okay this is the
- 00:21:35200 both this is the 199 this 198 197
- 00:21:39and so forth and we can uniquely
- 00:21:40identify each mode so in order to
- 00:21:44calculate the parameters in our model
- 00:21:48what we did was we linearize the
- 00:21:50relationship between what we measured
- 00:21:52and what our initial guesses based on
- 00:21:54the model we calculated based on the
- 00:21:56model the sensitivity matrix the
- 00:21:58sensitivity matrix tells us how much
- 00:22:00does the predicted wavelength change
- 00:22:02when I change a parameter such as the
- 00:22:04width of the ring or the refractive
- 00:22:06index of the core or the refractive
- 00:22:08index of the cladding so based on our
- 00:22:10measured values of the wavelength our
- 00:22:12initial simulation based on our initial
- 00:22:15guesses for the parameter
- 00:22:16this allows us to solve for how much we
- 00:22:18have to adjust the parameters so that we
- 00:22:21get an agreement between our measured
- 00:22:23data and our predicted simulation so we
- 00:22:26want to minimize this so we minimize the
- 00:22:29difference of this equaling zero so we
- 00:22:32do a singular value decomposition to
- 00:22:34find the parameters it turns out that
- 00:22:36although we have 34 measured parameters
- 00:22:38there are only four the rank of this
- 00:22:42matrix s is only four so we can only
- 00:22:45accurately determine four parameters in
- 00:22:47our model and the key parameters are the
- 00:22:49refractive indices of the quorum of the
- 00:22:51cladding the thickness of the core and
- 00:22:53also the chromatic dispersion so the
- 00:22:55reason that we only have a rank of four
- 00:22:57is that when you look at the spectrum
- 00:22:59it's pretty much determined by te versus
- 00:23:02TM and also the free spectral range all
- 00:23:04these other resonances all agree with if
- 00:23:07I give you those four quantities like
- 00:23:09the resonance location of one of the
- 00:23:11residences for TE plus the free spectral
- 00:23:13range for TE the resonance wavelength
- 00:23:15for TM plus a free spectral range for TM
- 00:23:17those four parameters pretty much
- 00:23:18determine these entire spectra so the
- 00:23:21rank of our measured or of our singular
- 00:23:25matrix s is only four so we're able to
- 00:23:28achieve very accurate results for our
- 00:23:31model parameters for four parameters so
- 00:23:33we determine refractive index of the
- 00:23:35core with a precision of of essentially
- 00:23:39four decimal places the cladding to
- 00:23:41three decimal places and then the core
- 00:23:43thickness to it looks like one decimal
- 00:23:45place and the dispersion to essentially
- 00:23:48hundred percent it's not very well it's
- 00:23:51not very accurate we also measured these
- 00:23:55resonances as we change the temperature
- 00:23:56so when you change the temperature
- 00:23:58there's a change in the refractive index
- 00:23:59due to the thermal optic effect so these
- 00:24:02resonances we tracked as a function of
- 00:24:04temperature and by measuring a best-fit
- 00:24:06slope and also modeling the effect of te
- 00:24:09and TM we're able to extract the thermal
- 00:24:12optic coefficients of silicon nitride
- 00:24:14and silicon dioxide so this is a method
- 00:24:16that allows us to figure out what's
- 00:24:19going on in our device geometry and our
- 00:24:22device parameters from observations of
- 00:24:24the resonances of the ring the reason
- 00:24:26that this method is very accurate is
- 00:24:28because we can determine the resin
- 00:24:30wavelength of the Ring two on the order
- 00:24:32of like one picometer in a measurement
- 00:24:35that has 15 50 nanometers so it's
- 00:24:37essentially about six or seven digits of
- 00:24:39precision that we can measure these
- 00:24:41residents wavelengths lambda so then the
- 00:24:43question is how precisely can we model
- 00:24:46the structures and it turns out that we
- 00:24:47can extract several digits of precision
- 00:24:49in our parameters both for the
- 00:24:51parameters at room temperature and also
- 00:24:54their dependency on temperature so based
- 00:24:58on these new values we fixed all the
- 00:24:59designs so now that we know the actual
- 00:25:01refractive indices we constructed a
- 00:25:04second generation of devices and we hit
- 00:25:06exactly the wavelength that we want so
- 00:25:08we were targeting 1549 we got 1549 or
- 00:25:11retargeting 1550 we got 15 49.6 so
- 00:25:15within point for nanometers of our
- 00:25:16target wavelength by having very
- 00:25:19accurate model parameters on these
- 00:25:22ripples these are due to the end effects
- 00:25:25from the fiber and also from the facet
- 00:25:27of the of the chip so by doing a
- 00:25:30model-based data interpretation so
- 00:25:32basically you have a measurement you
- 00:25:33model the entire system not just the
- 00:25:36micro ring but also the end facets and
- 00:25:38so forth you can extract the effective
- 00:25:41reflection of just the ring itself and
- 00:25:44you get this red dotted line and if you
- 00:25:47compare this DVR structure that's in a
- 00:25:50ring to what you get from the linear DVR
- 00:25:52you can see two things one we've gotten
- 00:25:54rid of the ripples so there aren't these
- 00:25:56these ripples in the spectrum but also
- 00:25:59the roll-off is much faster so this
- 00:26:02device will be better for single mode
- 00:26:04operation so we achieved 93% reflection
- 00:26:08point for nanometer full with half max
- 00:26:09and the overall structure is 70 times
- 00:26:12smaller than the conventional dbr
- 00:26:14structures that you find in the
- 00:26:16semiconductor laser we got rid of the
- 00:26:18side lobes and we also have a faster
- 00:26:19roll off ok so now I'm going to move
- 00:26:23into the applications so the first
- 00:26:25application they'll talk about is how we
- 00:26:27make a single wave well how do we
- 00:26:29integrate an active laser with a passive
- 00:26:31microwave mirror so what we want to
- 00:26:34achieve is a device that has a single
- 00:26:36wavelength of lazing and lazing being
- 00:26:38determined by the passive section which
- 00:26:40has the micronian grading
- 00:26:43late mirror so the advantage of this
- 00:26:47micro ring reflector is that it has a
- 00:26:49very narrow reflection bandwidth this
- 00:26:51narrow reflection bandwidth means that
- 00:26:52the device will lays in a very specific
- 00:26:54wavelength and this specific wavelength
- 00:26:57allows us to use this reflective micron
- 00:26:59resonator as the mirror for a single
- 00:27:02mode laser device so we're trying to
- 00:27:04make a compact replacement for the
- 00:27:06linear distributed bragg reflectors that
- 00:27:08you find in conventional semiconductor
- 00:27:10diode lasers there's another advantage
- 00:27:14of using passive mirrors so this is if
- 00:27:17you look at the theory shallow towns
- 00:27:19theory and also study on the henry line
- 00:27:23with enhancement factor there is a
- 00:27:25benefit of having a wavelength dependent
- 00:27:27mirror if you lock your laser to the
- 00:27:30right side of the resonance peak and you
- 00:27:32have this wavelength dependent mirror
- 00:27:34you can reduce the line width by this
- 00:27:36factor f c squared compared to a plain
- 00:27:38laser and so if you want to make a laser
- 00:27:41that's useful for spectroscopy so that
- 00:27:43you can have precise wavelengths in your
- 00:27:45measurement then the line width becomes
- 00:27:47a limiting factor and so being able to
- 00:27:49reduce the line width is a very
- 00:27:50important goal of making the
- 00:27:53semiconductor laser diodes so having a
- 00:27:57wavelength dependent mirror which is
- 00:27:58what we have from our reflective micro
- 00:28:00ring so we have this nice wavelength
- 00:28:03dependent mirror so there's a very sharp
- 00:28:05change in the reflection as I very the
- 00:28:07wavelength this will make a light a nice
- 00:28:09mirror that locks the wavelength of the
- 00:28:11laser so this laser that we constructed
- 00:28:14it has a amplification section so
- 00:28:17there's a gain section there's this
- 00:28:18optional phase section and then you have
- 00:28:20this passive section where on you're not
- 00:28:23injecting current and so there's going
- 00:28:24to be less noise because this mirror is
- 00:28:27going to serve as a wavelength lock for
- 00:28:29your laser so the goal is to achieve a
- 00:28:31single a single wavelength out of our
- 00:28:34device now there's another application
- 00:28:37which is if you put these two structures
- 00:28:39instead of having a single wavelength in
- 00:28:41the reflection spectrum if you can
- 00:28:43generate a coma of reflection peaks and
- 00:28:45you can do that by putting a single
- 00:28:46notch then you can have two different
- 00:28:49free spectral range for the mirror
- 00:28:51reflective atif and by aligning these up
- 00:28:54using the vernier effects essentially
- 00:28:56if I have a set of resonances here and I
- 00:28:58have a different spacing when I get one
- 00:29:01of these to align then that's going to
- 00:29:02be the wavelength that lazes and then I
- 00:29:05just need to make a very small shift in
- 00:29:07one of the mirrors to line up a
- 00:29:09different resonance and that gives me a
- 00:29:11large tuning so I can get quasi
- 00:29:14continuous tuning over a large
- 00:29:15wavelength range by using the vernier
- 00:29:17effect if I can get the free spectral
- 00:29:19range to be different for the two
- 00:29:21different mirrors so this is one
- 00:29:23application we're interested in we
- 00:29:24haven't fabricating these devices I'll
- 00:29:26talk about this device because we have
- 00:29:29that fabricated so in order to integrate
- 00:29:32active sections with passive sections on
- 00:29:35we have to do a bit of work in the
- 00:29:37device design and fabrication so we have
- 00:29:39these two we have this material which
- 00:29:41has grown for us by epitaxial growth
- 00:29:44MOCVD growth by a company called epi
- 00:29:47works in champaign on so we have the
- 00:29:49conventional gallium arsenide core
- 00:29:52surrounding indium gallium arsenide
- 00:29:54quantum well and then we have this
- 00:29:56indium gallium phosphide etch stop layer
- 00:29:57in these two locations we have this
- 00:30:00undoped aluminum gallium arsenide bottom
- 00:30:02plotting and then we have n-type and
- 00:30:04p-type aluminum gallium arsenide to form
- 00:30:07the separate confinement hetero
- 00:30:09structure so that we can separately
- 00:30:10confine electrons and optical fields and
- 00:30:14then what we're going to do is normally
- 00:30:17this quantum well we'll be in the very
- 00:30:18center of the core we're going to shift
- 00:30:20it up slightly so that in one section of
- 00:30:22the Vice we keep the full length so that
- 00:30:24this is the active section in this other
- 00:30:27section of the device we're going to
- 00:30:28etch away all this material including
- 00:30:30the quantum well and so without the
- 00:30:32quantum well this section becomes a
- 00:30:33passive section so it works as a
- 00:30:36transparent waveguide that's made of
- 00:30:38just gallium arsenide so what we need to
- 00:30:41do is we need to go from this active
- 00:30:43section which has the quantum well and
- 00:30:44has the mode sitting way up here to this
- 00:30:47passive section where the mode is going
- 00:30:49to sit much lower down in the gallium
- 00:30:51arsenide core so we formed this
- 00:30:53adiabatic horizontal taper where we
- 00:30:55taper the ridge waveguide etch and we
- 00:30:57also taper underneath so that we can
- 00:30:59confine the mode and transition it from
- 00:31:02being centered in the quantum wall
- 00:31:04region to be centered in the core /
- 00:31:07bottom clotting so the mode is going to
- 00:31:09Tran
- 00:31:09position downwards from this active
- 00:31:11region into the passive region and then
- 00:31:14it's going to couple into the reflective
- 00:31:15my crowing resonator which is going to
- 00:31:17serve as a release or mirror so we
- 00:31:20fabricated these structures this is a
- 00:31:21picture of it on where we have the
- 00:31:24active section we have our taper we go
- 00:31:26into the passive section we have our
- 00:31:27reflective my crowing resonator and
- 00:31:29because we don't want any light
- 00:31:30reflecting back from an end facet we
- 00:31:33split out the power so it just
- 00:31:34dissipates into the substrate so our
- 00:31:37output facet is going to be to the side
- 00:31:39this side is just serving as a high
- 00:31:41reflectivity mirror from the structure
- 00:31:43we achieve single mode operations so we
- 00:31:46get lazing at a threshold of about 30
- 00:31:48milliamps for a device that's 1,100 by I
- 00:31:51think this was one micron wide and you
- 00:31:54can see that lazing exists and that we
- 00:31:56have single wavelength operation these
- 00:31:58other notches these are from the
- 00:32:01higher-order resonances of the ring and
- 00:32:04we've effectively suppress them compared
- 00:32:06to the dominant mode that we wanted to
- 00:32:07achieve so the second type of device and
- 00:32:11I should mention on with this structure
- 00:32:13what we do is we have these gratings
- 00:32:15that form a first-order grading so a
- 00:32:18first-order grading the length of the
- 00:32:20section is lamb Dover for long the
- 00:32:22period is lambda over to first order
- 00:32:24grading is designed to reflect light in
- 00:32:27the opposite direction so it if I send
- 00:32:29light in the four direction a lamp first
- 00:32:32order grading will directly couple to
- 00:32:34light in the counter propagating
- 00:32:36direction there's also the second order
- 00:32:39draining and a second or degrading what
- 00:32:41it does is it couples light not only to
- 00:32:43the four direction but it also couples
- 00:32:46light out of the out of the plane of the
- 00:32:49of the direction of the plane and so you
- 00:32:52can generate lossy mirrors if you
- 00:32:56pattern a second order grading so we
- 00:32:58have the swirl device single wavelength
- 00:33:00integrated ring laser and the idea is
- 00:33:02that ordinarily all these modes that
- 00:33:05have different azimuthal mode numbers
- 00:33:07and that are degenerate because they're
- 00:33:10clockwise and counterclockwise
- 00:33:11propagating modes they all had
- 00:33:14degenerate loss so they're all the same
- 00:33:15we increase the loss of all the modes
- 00:33:18except for one and that one mode is the
- 00:33:20one that's going to laze so we can show
- 00:33:22that we can get
- 00:33:23single wavelength operation for a
- 00:33:25specific azimuthal motor and if we
- 00:33:27change the azimuthal mode order of the
- 00:33:29grading we can get a different mode to
- 00:33:31laze so the microcavity laser we want a
- 00:33:35small footprint low threshold off for
- 00:33:37applications like vuitton i agreed and
- 00:33:39grade circuits on ship optical
- 00:33:41interconnects and short distance optical
- 00:33:43communication the micro ring and micro
- 00:33:45disk lasers can be good candidates on
- 00:33:47their small but one of the biggest
- 00:33:50issues with the micro ring in the micro
- 00:33:51disk is that they have many modes so all
- 00:33:54the different azimuthal motors like m is
- 00:33:56equal to 200 201 they all have the same
- 00:33:59amount of loss moreover at a single
- 00:34:02resonance they have to counter
- 00:34:04propagating modes that have the same
- 00:34:05loss so the question is can we engineer
- 00:34:08the mode coupling to select a specific
- 00:34:11lazing mode can we do this by putting a
- 00:34:14grading on our structure to increase the
- 00:34:15loss of all the modes except for one the
- 00:34:18answer is yes and so the way that you do
- 00:34:21this is you form a grading with
- 00:34:23azimuthal mode order m and so that puts
- 00:34:26a perturbation on the cavity of the form
- 00:34:28sign of M Phi what this does is if I
- 00:34:31have the ordinary mode on n for the ring
- 00:34:35and i have the grading with mode m i
- 00:34:37scatter in two modes n plus m and n
- 00:34:40minus m so when you think about what
- 00:34:42happens when i multiply sine of n phi x
- 00:34:45sine of m phi i get the sum and
- 00:34:47difference frequencies and so i generate
- 00:34:49things that radiate into these
- 00:34:51higher-order modes so if i have a
- 00:34:53difference of n minus M equals two what
- 00:34:56I'm going to do is I'm going to couple
- 00:34:57the light from the azimuthal mode n with
- 00:35:00the grading of order m into a mode n
- 00:35:03minus M equals two and since this has
- 00:35:05low azimuthal mode order it's going to
- 00:35:07radiate in all directions and so you can
- 00:35:09see that this is a set this is a this
- 00:35:12corresponds to rotational symmetry to on
- 00:35:15so it radiates and so it has higher loss
- 00:35:17so the radiation modes of small as
- 00:35:20methyl of small azimuthal orders have
- 00:35:22small quality factors so by putting the
- 00:35:25second order grading on the structure i
- 00:35:27can select a specific lazing mode i'm
- 00:35:30going to set m is equal to n and i'm
- 00:35:32going to reduce all the quality factors
- 00:35:33of all the modes except for one mode
- 00:35:36so there's one exception and I keep
- 00:35:39bringing this up but the one exception
- 00:35:41occurs when n is equal to M and the
- 00:35:43electric field is shifted by exactly
- 00:35:45one-quarter wavelength relative to the
- 00:35:47grading so if I have a cosine M Phi
- 00:35:49dependence on Phi and have assigned n
- 00:35:52Phi dependence of the grading when I
- 00:35:54multiply these two together the sine
- 00:35:57times the cosine gives me the sign of
- 00:35:59the double angle I don't get a DC
- 00:36:01component I don't get a low frequency
- 00:36:03component and the low frequency
- 00:36:05component is precisely the component
- 00:36:06that radiates so this one particular
- 00:36:08exception gives me something that
- 00:36:11doesn't radiate and therefore the
- 00:36:12quality factor of this mode is not
- 00:36:14reduced by the presence of the grading
- 00:36:16so I can generate something that doesn't
- 00:36:18radiate it propagates as a or it's a
- 00:36:21standing wave inside the cavity and
- 00:36:23instead if I have the sign fi then sign
- 00:36:26fi x sine and my I get the sum and the
- 00:36:31difference and that radiates so to
- 00:36:34confirm this we did fe m simulations and
- 00:36:37we can see that we have this one
- 00:36:39resonant mode that doesn't radiate this
- 00:36:41one ready radiates like the spherical
- 00:36:43harmonic y 0 0 these ones radiate like
- 00:36:46why LM where L is minus 1 or plus 1 and
- 00:36:50so all the other modes starts radiate
- 00:36:53and so as a function of how deep or how
- 00:36:56strong I make this grading I can see
- 00:36:58that this one mode which is non
- 00:37:00radiating the loss does not change no
- 00:37:02matter how I change the grading whereas
- 00:37:04these other modes the losses increase as
- 00:37:06I increase the strength of the grading
- 00:37:08and so if I have a specific indentation
- 00:37:10sighs I can select this mode compared to
- 00:37:13the other modes so for the device design
- 00:37:16we have a similar structure as before
- 00:37:18except it's has fewer layers than what
- 00:37:21we did for active passive and one of the
- 00:37:23key parameters in terms of this design
- 00:37:25because the light is circulating
- 00:37:27radially is how deep I h24 my ridge
- 00:37:30waveguide if I etch too deep and I etch
- 00:37:33into the quantum well region then i
- 00:37:35create surface defects which is going to
- 00:37:37increase the threshold because i have
- 00:37:39high non-radiative recombination if I
- 00:37:42etch too shallow then the light that's
- 00:37:44propagating the ring can radiate
- 00:37:45radially outwards because there isn't
- 00:37:48tidy
- 00:37:48confinement to guide the mode inside the
- 00:37:51ring so there's a function as a function
- 00:37:53of to how deep I H into the core so the
- 00:37:56core the quantum well is 80 nanometers
- 00:37:58into the core if I etch very close to
- 00:38:01that 80 nanometers then what i get is I
- 00:38:03get very low bending loss and I have
- 00:38:05high quality factor if I don't itch deep
- 00:38:08enough so I'm sitting here then I have
- 00:38:10very high bending loss so 10 inverse
- 00:38:11centimeters is pretty high for a laser
- 00:38:13to operate and so what I want to do is I
- 00:38:16need to edge somewhere between 40 and 80
- 00:38:19nanometers into the core if I edge too
- 00:38:21far I get high threshold because I've
- 00:38:23non-radiative recombination fih too
- 00:38:25shallow i also get high threshold
- 00:38:26because i have a poor optical
- 00:38:30confinement and i have high bending loss
- 00:38:32so we design and pattern these with even
- 00:38:35lithography you can see the grading
- 00:38:37formed in gallium arsenide so this is
- 00:38:39three-five material the passive
- 00:38:41structures were in silicon nitride so
- 00:38:43this is a completely different etch
- 00:38:45process compared to the passive
- 00:38:46structures we put metal on top of it and
- 00:38:49we transfer the pattern with ICP rie on
- 00:38:53we then planarize it with BCB so that we
- 00:38:56can make metal contacts and we have
- 00:38:58separate contacts for the bus waveguide
- 00:39:00and also for the bus waveguide and also
- 00:39:03for the ring section so the left 450
- 00:39:07micron section was pumped so that we can
- 00:39:09get to transparency the center part is
- 00:39:12the part that's lazing the right part is
- 00:39:13unpub so our laser cavity is formed just
- 00:39:17by this section alone it's a circulating
- 00:39:20ring configuration for our laser the bus
- 00:39:23waveguide allows light to couple out
- 00:39:25from the ring into the waveguide and
- 00:39:27this is at transparency so we let light
- 00:39:29come out the left side so as a function
- 00:39:31of the current we can see that we get an
- 00:39:33increase in power and so we have lazing
- 00:39:34threshold at about twenty six milliamps
- 00:39:37when we set n is equal to M equals 7 24
- 00:39:40we get this one resonance as the lazing
- 00:39:43operation when we change the azimuthal
- 00:39:45mode order so that we can see whether
- 00:39:48it's the grating that determines the
- 00:39:50lazing we can see that it shifts exactly
- 00:39:52four orders on to the fourth resonance
- 00:39:55to the right and so we have precise
- 00:39:57control over the wavelength that lazes
- 00:39:59in the structure by defining the
- 00:40:01azimuthal
- 00:40:02getting so the key to getting single
- 00:40:04mode operation we've made structures
- 00:40:06that looked identical to this but
- 00:40:08without the grading without the grading
- 00:40:10you get resonances you get all these
- 00:40:12resonances competing for lazing and it's
- 00:40:14a multi-mode structure but with the
- 00:40:16grading we get single wavelength
- 00:40:18operation so for the final part of the
- 00:40:22talk I'll talk about our work on hybrid
- 00:40:24whispering gallery mode plasmonics n
- 00:40:26ring resonator sensors the ideas I
- 00:40:28mentioned before we have the silicon
- 00:40:30microsphere which is about 30 microns in
- 00:40:32diameter around the perimeter or the
- 00:40:35circumference of it we put these gold
- 00:40:36epitopes which are going to serve as
- 00:40:38plasmonics ain and the gold epitopes
- 00:40:42allow tight field confinement in the
- 00:40:44vicinity and so we're going to try to
- 00:40:47detect the presence of a thyroid
- 00:40:50globulin cancer marker protein attaching
- 00:40:54to these gold epitopes and we see that
- 00:40:57based on the design of the epitopes we
- 00:41:00can couple effectively between the
- 00:41:01whispering gallery mode resonances and
- 00:41:03the plasmonics chainring resonances and
- 00:41:05get the sharp increase in the creation
- 00:41:07of symmetric and anti-symmetric modes
- 00:41:09and this is a result of mode coupling
- 00:41:11between the plasmonics chain and the
- 00:41:13whispering gallery mode resonator so as
- 00:41:17I mentioned we're looking at the TG
- 00:41:18cancer marker protein and so we have
- 00:41:21these gold epitopes which are basically
- 00:41:23gold nanoshells surrounding silicon nano
- 00:41:27scooters and we place these around the
- 00:41:29equator of a whispering gallery mode
- 00:41:30resonator don't ask me how we're going
- 00:41:33to do this experimental II this is a
- 00:41:34simulation work there's a group that we
- 00:41:37collaborated with at NYU and they have
- 00:41:40methods to use optical gradient force to
- 00:41:42trap particles around the perimeter of
- 00:41:44these spheres whether they can get it
- 00:41:46exactly the way that we simulate or not
- 00:41:48is still open question but the point is
- 00:41:52that we're going to trap or place these
- 00:41:54epitopes at these anti nodes of the
- 00:41:57field and in order to simulate the
- 00:41:59structure very efficiently so this
- 00:42:01structure is about 30 micron radius we
- 00:42:06want to simulate using the symmetry that
- 00:42:08exists in the problem so we're going to
- 00:42:10put perfect electric conductors at the
- 00:42:13at the nodes
- 00:42:15perfect magnetic conductors at the
- 00:42:16antinodes and use periodic boundary
- 00:42:18conditions to essentially solve for the
- 00:42:20entire structure so the field is
- 00:42:23localized near the epitope if I change
- 00:42:25the epitope radius slightly then i can
- 00:42:27get distinct coupling regions in this
- 00:42:29hybrid resonator system as I mentioned
- 00:42:32we model this in 3d using periodic
- 00:42:34boundary conditions with pcs at the
- 00:42:36nodes and pmcs at the anti nodes so this
- 00:42:40is what the field distribution looks
- 00:42:41like as I vary the radius so there's a
- 00:42:44lot of parameters in this model so
- 00:42:46there's like the radius of the
- 00:42:47microsphere there's the radius of the
- 00:42:49epitope there's the thickness of the
- 00:42:50gold coating there's the spacing do i
- 00:42:52put these at every single node or every
- 00:42:54other node there's a lot of parameters
- 00:42:56involved so we fix the thickness of the
- 00:42:58epitope at 10 nanometers we also fix the
- 00:43:02position of the epitopes at the anti
- 00:43:04node so that it has the strongest effect
- 00:43:06and we looked at two different cases of
- 00:43:08the radii so when the radius is small 30
- 00:43:10nanometers and when the radius is large
- 00:43:12there's a very small perturbation in the
- 00:43:15mode profile due to the epitope so this
- 00:43:17is the cross sectional view and xion are
- 00:43:19of this section of the field and you can
- 00:43:23see that we have the field polarized in
- 00:43:25Z and the epitope has a very small
- 00:43:27effect on the overall field shape when I
- 00:43:30have radius of 50 I get slight bending
- 00:43:32in the angles of the vectors near the
- 00:43:34epitopes but there isn't a huge change
- 00:43:36in the overall electric field profile
- 00:43:39this however is completely different if
- 00:43:41I tune the radius of the epitope to the
- 00:43:44resonance of the whispering gallery mode
- 00:43:46so when the radius is 40 nanometers the
- 00:43:48plasma McShane ring resonator and the
- 00:43:50whispering gallery mode resonator these
- 00:43:53modes coupled to each other so the
- 00:43:55hybrid wgm pcr are I generate a
- 00:43:58symmetric mode and an anti symmetric
- 00:44:00mode so compared the previous case where
- 00:44:02the electric field profile for the
- 00:44:04microsphere extends very far in Z and is
- 00:44:07spread out in our to this case where
- 00:44:10it's very tightly confined in Z pretty
- 00:44:12much at the locations of the epitopes
- 00:44:15and so the symmetric mode very tightly
- 00:44:17confined the field at that location the
- 00:44:20anti symmetric mode i end up with the
- 00:44:22fields pointing in the opposite
- 00:44:23direction at this location but again i
- 00:44:25have a significant enhancement of the
- 00:44:26field strength at the
- 00:44:27plasmonics chain epitope location
- 00:44:30compared to this diagram so there's a
- 00:44:32significant increase in the optical
- 00:44:34confinement at that location so we
- 00:44:37wanted to understand this behavior on it
- 00:44:39turns out that this is a very simply
- 00:44:41explained as the coupling of two
- 00:44:43separate resonator systems so one is the
- 00:44:46whispering gallery mode the other is the
- 00:44:48plasmonics Ain ring resonator so if you
- 00:44:50model the plasma exchange I itself you
- 00:44:53can see that it has certain field
- 00:44:54localization properties that basically
- 00:44:57confine the field very tightly near the
- 00:44:59plasmonics chain and so when we look at
- 00:45:01modal dispersion what we can plot is as
- 00:45:04a function of the size of this epitope
- 00:45:07on what are the resonance wavelengths of
- 00:45:10the whispering gallery mode and of the
- 00:45:13plasma exchange so the whispering
- 00:45:15gallery mode microsphere it doesn't
- 00:45:16matter what the plasmonics chain is
- 00:45:18doing it has the same resonance
- 00:45:20wavelength so that's this green curve
- 00:45:21here if you look at the plasmonics chain
- 00:45:24ring resonator by itself it has a sharp
- 00:45:26dependence on the radius and so this is
- 00:45:29this black curve here and so initially
- 00:45:32we're expecting the coupling between the
- 00:45:34screen mode and this black mode however
- 00:45:36there's a perturbation and the
- 00:45:37perturbation is very important these
- 00:45:39epitopes from the plasmonics chain ring
- 00:45:42resonator are not isolated they're
- 00:45:44perturbed by the silicon microsphere
- 00:45:46that's sitting in the center so if you
- 00:45:48do a corrected calculation of the plasma
- 00:45:50etching chain ring resonator in the
- 00:45:53presence of the silicon microsphere you
- 00:45:55get this black dotted line and then when
- 00:45:57i look at the mode coupling between the
- 00:45:59black dotted line and the green line i
- 00:46:01generate the symmetric mode which is in
- 00:46:03red and the anti-symmetric mode which is
- 00:46:05in blue and i can understand the
- 00:46:07existence of these two separate curves
- 00:46:09as simply mode coupling between the
- 00:46:12plasmonics ain and the whispering
- 00:46:13gallery mode so the localization of the
- 00:46:17field at this epitopes is stronger when
- 00:46:20we're in the strong coupling regime
- 00:46:22where the radius is close to 40 so when
- 00:46:25I have a TG binding event on one of the
- 00:46:28epitopes I'll get a resonance wavelength
- 00:46:30shift and this is how i'm going to sense
- 00:46:32the TG cancer markers i'm going to look
- 00:46:34at the resonance of the micro ring and
- 00:46:36figure out or of the microsphere and
- 00:46:38figure out has it shifted so at this
- 00:46:41you're 40 nanometers I get a 20
- 00:46:43femtometer shift now you say to yourself
- 00:46:4520 50 meters seems incredibly difficult
- 00:46:47to measure experimentally but it turns
- 00:46:50out that this marker is so small that
- 00:46:52there aren't any other good techniques
- 00:46:54to detect it it's a few nanometers it's
- 00:46:57basically an ellipsoid that's like 10 or
- 00:47:0012 nanometers and one to mention in five
- 00:47:02nanometers in the other dimension and
- 00:47:03the refractive index is pretty much the
- 00:47:05same as a refractive index of the fluid
- 00:47:07that it's in and so as a result any
- 00:47:09other method is not really going to be
- 00:47:10sensitive to the subwavelength type
- 00:47:12structure so this method we get a 20
- 00:47:15femtometer shift for the symmetric mode
- 00:47:17unfortunately when you're looking at a
- 00:47:19micro ring based sensor what's important
- 00:47:21is not only how much of a wavelength
- 00:47:23shift you generate but how narrow are
- 00:47:26the resonances that you're measuring
- 00:47:27because the narrowness of the resonance
- 00:47:29that you're measuring determines the
- 00:47:31error that you can make in determining
- 00:47:33the resonance wavelength so when we
- 00:47:35start increasing the shell radius
- 00:47:37unfortunately the quality factor of the
- 00:47:38ring decreases significantly and so as a
- 00:47:41result it becomes difficult to measure
- 00:47:43the smaller the small shift so there may
- 00:47:46be an optimal point in here depending on
- 00:47:49the instrumentation that you have
- 00:47:50whether you're limited in terms of the
- 00:47:52measurement accuracy of the tunable
- 00:47:56laser of G have where you can trade off
- 00:47:58a larger resonance shift for having a
- 00:48:01wider resonance or you can have a
- 00:48:03smaller residence shift for having a
- 00:48:05narrower resonance so there are a bunch
- 00:48:08of trade-offs in this design and so if
- 00:48:10you look at the case where you place an
- 00:48:13epitope at every single anti node we
- 00:48:15call this the amount of shift you get
- 00:48:17for one epitope per one wavelength or
- 00:48:20one anti node and so that's the largest
- 00:48:22case so you get the biggest resonance
- 00:48:24shift unfortunately you get the smallest
- 00:48:26quality factor if you space them further
- 00:48:28apart and so you put one epitope every
- 00:48:31other anti node then you get a smaller
- 00:48:33resonance shift but you have a higher
- 00:48:35quality factor so if you have just a
- 00:48:37single isolated epitope by itself this
- 00:48:40has a high Q micro ring resonator so the
- 00:48:43advantages that is easy to measure
- 00:48:45wavelength shift the disadvantage is you
- 00:48:47only have one binding site so the
- 00:48:49probability that the TG marker is going
- 00:48:51to attach to that one specific epitope
- 00:48:53that you place is
- 00:48:54very very small and so you have to wait
- 00:48:56a long time to be able to detect this TG
- 00:48:59biomarker if instead you have a certain
- 00:49:02number of coupled epitopes you have a
- 00:49:03lower Q but now you have n times the
- 00:49:06detection frequency because you have
- 00:49:08essentially n sensors distributed around
- 00:49:11your microwave so you wait less time to
- 00:49:13detect this biomarker and so if you
- 00:49:16place them at every single anti node
- 00:49:18then you get the most frequent detection
- 00:49:21and you can still trade off the coupling
- 00:49:24by balancing the effects of sensitivity
- 00:49:27so if I place them at every single node
- 00:49:29or anti node I mean I get very high
- 00:49:32sensitivity but I have low Q if I place
- 00:49:34them every other I have lower
- 00:49:35sensitivity but I have better q so I can
- 00:49:37trade off those two parameters while
- 00:49:40still reducing the detection time
- 00:49:41compared to just having a single
- 00:49:43isolated epitope so in summary we
- 00:49:47presented our work on the development of
- 00:49:49new types of devices that operate based
- 00:49:51on selective mode coupling on this mode
- 00:49:54coupling is sort of an emerging theme
- 00:49:56that's in a lot of our groups research
- 00:49:58basically looking at the existence of
- 00:50:02many different modes and how to engineer
- 00:50:03the coupling between these modes to
- 00:50:05generate the type of devices that you're
- 00:50:07interested in we preserve two types of
- 00:50:10approach one is to couple the modes for
- 00:50:12achieving reflection so first order
- 00:50:14grading gives us nice reflection to a
- 00:50:16second order braiding modifies the
- 00:50:18radiation losses and allows us to
- 00:50:20generate a single wavelength laser we
- 00:50:23developed simulation models the
- 00:50:24cylindrical coupled mode theory on we
- 00:50:26designed and fabricated passive devices
- 00:50:28and we demonstrated single wavelength
- 00:50:30operation this device is also useful for
- 00:50:32allowing us to measure the refractive
- 00:50:34index because it allowed us to determine
- 00:50:36the azimuthal mode order without
- 00:50:39ambiguity on from the symmetry we also
- 00:50:43developed a monolithic integration
- 00:50:45platform so we have active laser devices
- 00:50:47passive microwave reflectors and we show
- 00:50:50that we can integrate these two things
- 00:50:51together we fabricated lasers that have
- 00:50:54these mirrors and showed single
- 00:50:56wavelength lazing single mode lazing we
- 00:50:58also proposed and demonstrated
- 00:51:00engineering the radiation quality factor
- 00:51:02using a second-order grading so that we
- 00:51:04get one particular mode that lazes and
- 00:51:07the other modes are radiated
- 00:51:08radiating we verified this
- 00:51:10experimentally and showed that you can
- 00:51:12control which mode lazes by controlling
- 00:51:14the azimuthal mode order of the grading
- 00:51:16and then in terms of our sensor we
- 00:51:19looked at the distinct coupling regions
- 00:51:21between the whispering gallery mode
- 00:51:22resonator and the plasma McShane ring
- 00:51:24resonator and we showed that you can
- 00:51:26make trade-offs in the sensitivity and
- 00:51:28the detection time and the measurement
- 00:51:30limitations of the quality factor
- 00:51:32there's very strong mode field
- 00:51:35localization and mode splitting that
- 00:51:37occurs if the size of the plasmonics
- 00:51:39chain ring resonator epitopes exactly
- 00:51:42lines up the resonances with the
- 00:51:43residences of the whispering gallery
- 00:51:45mode and we showed the existence of the
- 00:51:47symmetric and the anti-symmetric modes
- 00:51:49at that critical value our future
- 00:51:52outlook on so the reflective micro rings
- 00:51:54with small footprints are going to be
- 00:51:56very useful for semiconductor lasers we
- 00:52:00really want to expand our work in terms
- 00:52:03of making these low threshold laser
- 00:52:05devices and especially for applications
- 00:52:08in sensing and spectroscopy there are
- 00:52:11new designs that our group is studying
- 00:52:12so one example is to have a instead of
- 00:52:15having these epitopes sitting around the
- 00:52:17perimeter of a whispering gallery mode
- 00:52:20structure instead make plasmonics
- 00:52:22antennas on top the surface of our micro
- 00:52:26resonator and so we may be able to
- 00:52:28localize the field very strongly so this
- 00:52:30is the gold plasmonics bowtie structure
- 00:52:33on top of a microwave resonator we may
- 00:52:36be able to tightly confined the optical
- 00:52:38mode in this plasmonics and then if we
- 00:52:42have binding events will have very
- 00:52:43strong shifts in the resonance
- 00:52:45wavelength of the structure and so we
- 00:52:47may be able to enable field localization
- 00:52:50without a huge penalty in the quality
- 00:52:52factor and finally we're also looking at
- 00:52:55practical single mode low threshold
- 00:52:57lasers on with further optimization of
- 00:53:00our fabrication processes there's a lot
- 00:53:02that goes into fabricating a device and
- 00:53:05there's a lot of work in terms of
- 00:53:07developing processing recipes to achieve
- 00:53:09high performance and so we're still
- 00:53:12working on that so for acknowledgments
- 00:53:15none of this work would be possible
- 00:53:17without the excellent effort of the
- 00:53:19graduate students a lot of this work
- 00:53:21was led by a mirror Bobby and young moe
- 00:53:23Kang with contributions from Josephine
- 00:53:25masa and ass on the funding was from
- 00:53:28National Science Foundation the Career
- 00:53:30Award and also matching funds from the
- 00:53:33universally University of Illinois so
- 00:53:36thank you for your attention and I'm
- 00:53:37open for questions
- 00:53:53you
- micro ring resonators
- laser technology
- sensing
- mode coupling
- simulation
- fabrication
- biomolecule detection
- plasmonics
- semiconductor lasers
- research development