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Stress effects on the performance of optical waveguides

M. Huang
- 01 Apr 2003 - 
- Vol. 40, Iss: 7, pp 1615-1632
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TLDR
In this paper, the photo-elastic relation and wave equations for inhomogeneous and anisotropic waveguides are reviewed and the effective refractive indexes and mode shapes of planar waveguide under different stress states are obtained analytically.
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This article is published in International Journal of Solids and Structures.The article was published on 2003-04-01 and is currently open access. It has received 198 citations till now. The article focuses on the topics: Birefringence & Photoelasticity.

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Citations
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Polarization management for silicon photonic integrated circuits

TL;DR: Polarization management is very important for photonic integrated circuits (PICs) and their applications as mentioned in this paper, however, due to geometrical anisotropy and fabrication inaccuracies, the characteristics of the guided transverseelectrical (TE) and transverse-magnetic (TM) modes are generally different.
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The Emergence of Silicon Photonics as a Flexible Technology Platform

TL;DR: This paper will concentrate on the key technological milestones that were crucial in demonstrating the capability of silicon photonics as both a successful technical platform, as well as indicating the potential for commercial success.
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Birefringence control using stress engineering in silicon-on-insulator (SOI) waveguides

TL;DR: In this article, the authors demonstrate that stress engineering is an effective tool to modify or eliminate polarization dispersion in silicon-on-insulator (SOI) waveguide devices, for a wide range of waveguide cross-section shapes and dimensions.
Journal ArticleDOI

Stress in femtosecond-laser-written waveguides in fused silica.

TL;DR: By annealing the sample, this work reduces the losses by approximately 30% (at 633 nm) and decreases the birefringence by a factor of 4 in fused silica.
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Rethinking Optical Fiber: New Demands, Old Glasses

TL;DR: In this paper, the authors focused on the use of the molten core approach to optical fiber fabrication and the novel yet practical fibers that can be produced, with stimulated Brillouin scattering being the primary exemplar.
References
More filters
Journal ArticleDOI

Tunable mechanically induced long-period fiber gratings.

TL;DR: This filter, which is simple and inexpensive, exhibits transmission spectra and temperature stability similar to those of photoinduced LPFG's and offers the unique advantages of being tunable, erasable, and reconfigurable.
Book

Acousto-optic devices: principles, design, and applications

Jeiping Xu, +1 more
TL;DR: In this paper, the piezoelectric effect and the piezelectric transducers of thin-film Acousto-Optic devices are discussed. But they do not consider the effect of the Bragg cells.
Book

Inhomogeneous optical waveguides

TL;DR: In this article, the authors present a method for the fabrication of planar waveguides with continuous dielectric constant variation. But they do not consider the propagation of the waveguide through thin films.
Journal ArticleDOI

Birefringence control of silica waveguides on Si and its application to a polarization-beam splitter/switch

TL;DR: In this article, a polarization-beam splitter/switch with a Mach-Zehnder interferometer configuration was fabricated using a silica-based planar lightwave circuit (PLC) on a silicon substrate.
Related Papers (5)
Frequently Asked Questions (20)
Q1. What contributions have the authors mentioned in the paper "Stress effects on the performance of optical waveguides" ?

In this paper, the photo-elastic relation and wave equations for inhomogeneous and anisotropic waveguides are reviewed. 

For buried waveguides, which have rectangular core shape and embedded in other cladding materials, and straight optical fibers, their stress states are similar to the hydrostatic stress state, where stresses will not cause too much loss and birefringence, but may induce multimode. 

For the planar waveguides, the light propagates in the z direction, is confined in the x direction within the central core region, and has no variation in the y direction. 

Stress-induced refractive index non-uniformity and anisotropy may exist simultaneously, so many problems may be induced by stresses. 

Optical waveguides are basic components in many optical systems, such as arrayed waveguide gratings (AWGs), lasers and tunable filters. 

Because the waveguide considered here is symmetric, the field of the first mode is zero at the center of the core, where the stress concentration happens. 

These layers are fabricated at high temperatures (e.g., 300 C for Al interconnect and 1000 C for silica cladding), and cooled down to room temperature. 

In modern optical systems, more and more components are integrated (or hybrid-packaged) in a single chip, where optical waveguides serve as interconnects for photonic components. 

In order to study the stress magnitude effect, the core is assumed to be under hydrostatic stress state, i.e., rxx ¼ ryy ¼ rzz ¼ r and rxy ¼ 0. 

The reason is that stress concentration causes the non-uniform distribution of the refractive index, and the light trends to propagate in the higher refractive index region. 

Although most practical optical waveguides are channel waveguides, where the light is also confined in the y direction, planar waveguides are used to provide a basic understanding since analytical solutions may be obtained for this kind of structure. 

stresses could also cause problems, such as the increments of polarization dependent loss (PDL) and polarization shift (PS) (Min et al., 2000; Yan et al., 2002). 

As shown in this paper, this small index change, aided by non-uniformity and anisotropy, causes unacceptable optical performance degradation and different stress states play different roles: high stress value may induce multimode; in-plane stresses may induce PS and PDL; stress concentration may induce large transition loss; and pure shear stress has little effects on the effective refractive index. 

Many efforts have been made to improve the optical performance by taking advantage of photo-elastic effect, such as stress release grooves to1616 M. Huang / International Journal of Solids and Structures 40 (2003) 1615–1632minimize the polarization shift (Nadler et al., 1999), thermal stress to control the temperature sensitivity of central wavelength (Cohen et al., 1996, 2000; Ooba et al., 2000; Huang and Yan, 2002), stress-induced optical waveguides and filters (Saitoh et al., 1999; Lea andWeiss, 1996; Almashary andKim, 1996; Rho and Jackson, 1999; Savin et al., 2000), stress effects on laser (Maciejko et al., 1989, 1993), and stress-induced birefringence behavior of the waveguides and fibers (Kilian et al., 2000; Okuno et al., 1994; Chowdhury andWilcox, 2000; Buda et al., 2000). 

Although this study is performed on the planar waveguides under four simple stress states, the qualitative picture obtained in this paper should be generic to other waveguide structures and under more complicated stress states. 

These stresses can change the refractive indexes of the waveguide by the acousto-optic (elasto-optic or photoelastic) effect (Xu and Stroud, 1992; Sapriel, 1979), which may affect the optical performance. 

The stresses in microstructures are usually on the order of 108 Pa, and the C values in Table 1 are on the order of 10 11 Pa 1; so the refractive index change caused by stress is normally between 0.01. 

The solutions of the mode equations are listed in Table 4.M. Huang / International Journal of Solids and Structures 40 (2003) 1615–1632 1625Applying interface boundary conditions similar as the hydrostatic stress state, and solving these eigenvalue equations, the authors can obtain the effective refractive index and normalized mode shape. 

The number of modes allowed in a three-layer symmetric planar waveguide is (Boyd, 1994)M ffi 2t kffiffiffiffiffiffiffiffiffiffiffiffiffiffi n2 n21 q : ð34ÞStress can change the refractive index, which may change the number of modes in the waveguide. 

In Section 3, the effect index and mode shape for a planar waveguide are solved analytically under four stress states: hydrostatic, in-plane, stress concentration, and pure shear.