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- Authors : Ashwini.H
- Paper ID : IJERTCONV2IS13039
- Volume & Issue : NCRTS – 2014 (Volume 2 – Issue 13)
- Published (First Online): 30-07-2018
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
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Integrated Optic Ring Resonator Based Pressure Sensor
Department of IT
M. Tech, 4th Semester, Dayananda Sagar College of Engineering
AbstractIntegrated Silicon Photonics has emerged as a powerful platform in the last two decades amongst high- bandwidth technologies, particularly since the adoption of CMOS compatible silicon-on-insulator(SOI) substrates. Micro- ring resonators are one of the fundamental blocks on a photonic integrated circuit chip oering versatility in varied applications like sensing, optical buering, ltering, loss measurements, lasing, nonlinear eects, understanding cavity opt mechanics etc. we propose and analyze an optical MEMS pressure sensor consisting of a ring resonator located over the edge of a circular silicon diaphragm. As the diaphragm deects due to the applied pressure, stress induced refractive index change in the waveguide leads to change in phase of the light propagating through resonator. Shift in the resonance frequency due to this phase change gives the measure of the applied pressure. The phase response of the sensor is found to be about 19Âµrad/Pa for 1mm radius 65Âµm thick circular diaphragm. The wavelength shift of 0.78pm/kPa is obtained for this sensor and can be used up to a range of 300kPa. Since the wavelength of operation is around 1.55Âµm, hybrid integration of source and detector is possible on the same substrate. This type of sensor can be used for blood pressure monitoring, precession instrumentation, aerospace propulsion application and other harsh environments with suitable design.
Keywords micro-ring resonator, silicon-on-insulator, CMOS, MEMS
Micro-opto-electro-mechanical (MOEM) devices and systems, based on the principles of integrated optics and micromachining technology on silicon have immense potential for sensor applications . Optical MEMS sensors have the advantages of immune to EMI, larger bandwidth and higher sensitivity compared to electronic counter parts. Many types of optical MEMS pressure sensors using Mach- Zehnder interferometer(MZI) [2, 3], Fabry-Perot interferometer  have been reported. Phase change in the sensing arm of MZI due to applied pressure is read out as intensity change in case of MZI based sensor. In Fabry- Perot interferometer based pressure sensor, the variation of cavity length because of displacement of the diaphragm due to applied pressure is readout as intensity changes. Brabander et.al  have considered ring resonator based pressure sensor whose straight arms are over the long edge
of a micro machined rectangular diaphragm. But here we consider a circular silicon diaphragm and consider the resonant wavelength shift of the ring resonator as a measure of applied pressure.
Figure 1. Schematic of the proposed Optical MEMS Pressure Sensor.
When pressure is applied on the diaphragm, due to the stress in the waveguide located over the diaphragm, the refractive index changes (due to elasto-optic effect) and hence the phase of the light propagating through it. This phase change is read out as resonant wavelength shift of the ring resonator located over the diaphragm. Since the waveguide is along the edge of the diaphragm where maximum stress occurs, phase change in the waveguide due to cumulative photo elastic effect is more.
The ring resonator is located over the edge of the diaphragm as shown in gure 1. Light is coupled into and out of the ring from the straight waveguide placed adjacent to it over the substrate . The ring is made up of oxinitride (SiO2/SiON/SiO2) waveguide single moded at 1.55Âµm. The ratio of the output and input field (It) is given by It= (1)
where, k is the coupling co-efficient, T = L is the total propagation loss in the ring, = 2/*neff L and L =2r, where r is the radius of the ring.
Figure 2. Output Characteristics of the Ring Resonator.
Figure 2 shows the intensity variations at the output with the variation in the input wavelength with periodic dips at resonant wavelengths. Here r=1mm and neff =1 .48789 at 1550nm is taken for the desired waveguide structure with k=0.1% and very low loss ( 0). As seen from the graph, the free spectral range (FSR) is about 257pm.
Mechanical Design and Opto-mechanical Coupling
The deection w of a circular diaphragm of radius a and thickness h due to pressure P is given by
D 4 W(r) = P (2)
where D = Ep/ 12(12) is the exural rigidity and E is the Youngs modulus and is the Poissons ratio along with the boundary conditions
w(a)=0 w'(a)=0 w'(0) = 0 (3)
The radial and transverse stress along the thickness of the diaphragm are given by
where r and t indicate radial and transverse direction. Hence the radial and tangential stresses at the surface of the circular diaphragm (z = h/2) are given by
Figure 3 shows the normalized stress(Pa2 / p ) variation along the diagonal of the diaphragm. The maximum radial stress occurs at the edge of the circular diaphragm and is 3a2/ 4p P. Hence the waveguide is placed at the edge to get the maximum refractive index change due to photoelastic effect. Larger radius and thinner diaphragm will have more stress for a given applied pressure. The radius of the diaphragm is chosen considering the ring radius which dictates the resonant wavelengths.
Figure 3. Normalized stress (Pa2 /p ) along the diagonal of the diaphragm.
Due to the stress, the refractive index of the waveguide changes. Refractive index change is related to the stress through a fourth rank tensor called photo-elastic tensor. There are only two nonzero co-efcients C1 and C2 for the oxynitride core waveguide. The refractive index change is more for TM modes since the radial stress is more and is given by
nTM = C2r (6)
where C2 =4 .22Ã—1012/Pa is the photo-elastic co-efcient of the core silicon oxynitride. Figure 4 shows the index change along the diameter for TM modes
Figure 4. Normalized refractive index change (Pa2h/ D ) along the diagonal of the diaphragm.
The cumulative phase change along the edge of the diaphragm is given by
=2/*n/neff*n(2a) (7) Substituting for n, we get
= (2/)(n/neff) c (3a2/4p)((2a) P (8)
Figure 5 shows the cumulative phase change for 1mm radius ring for various applied pressure. The phase sensitivity here is about 19Âµrad/Pa for diaphragm thickness of 65Âµm. Since maximum allowable phase change can be 2, about 300kPa can be detected.
Figure 5. Phase change in the resonator due to applied pressure. The free spectral range (FSR) in terms of wavelength is
FSR = /2neffa (9)
Hence the wavelength shift due to applied pressure can be written as
Shift = FSR (P)/2 (10)
Figure 6. Intensity vs Wavelength for 0 and 100kPa.
Figure 6 shows the variation of the intensity versus input wavelength for an applied pressure of 100kPa. The dotted curve shows the variations without any applied pressure. It is observed from the graph that there is a resonant wavelength shift of 78pm for 100kPa.
Figure 7. Resonant wavelength Shift vs Pressure.
Figure 7 shows the plot of wavelength shift with pressure up to 300kPa which is the maximum detectable range for the proposed design. The plot shows linear variation in the shift with pressure which is desirable for sensor applications. In the present design, the diaphragm thickness is taken to be 65Âµm. However by reducing the thikness (eg. 10Âµm), one can achieve better sensitivity (32pm/k Pa), for low pressure (7.5kPa) sensing applications.
We have proposed and analyzed a novel optical MEMS pressure sensor using integrated optical ring resonator over a micro-machined silicon circular diaphragm. Because the frequency of operation is around 1.55Âµm, hybrid integration of source and detector is possible on the same substrate. Since the detection of pressure is in frequency domain, it is less amenable to noise. We have designed the sensor for 300kPa range. But with suitable modication in the design parameters, this sensor can be used for blood pressure monitoring, precession instrumentation, aerospace propulsion application and other harsh enviroments.
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