Maria Bayard Dühring - Solid Mechanics
Maria Bayard Dühring - Solid Mechanics Maria Bayard Dühring - Solid Mechanics
26 Chapter 4 Design of sound barriers by topology optimization [P1]
Chapter 5 Design of photonic-crystal fibers by topology optimization [P2] The second type of wave problem is studied in this chapter and is about optical waves propagating in hollow core photonic-crystal fibers. The method of topology optimization is used to maximize the energy flow by redistributing air and silica material around the core, such that the overlap of the magnetic field in the lossy silica cladding is decreased. The chapter is a summary of publication [P2]. One- or two-dimensional photonic crystals are employed to confine optical waves in the core region of photonic-crystal fibers, which were first studied in the 1990s [75, 76]. A holey fiber consists of a hollow core, which is surrounded by a two dimensional periodic pattern of air holes that confine the wave by the band-gap effect [17]. Thus, a part of the optical wave propagates in air for this type of fiber, and therefore losses as well as unwanted dispersion and nonlinear effects from the cladding material can be reduced. Another part of the wave propagates in the cladding, which is usually silica. For optical wavelengths in general, silica is a lossy material and will absorb a part of the energy. For most wavelengths holey fibers will therefore not be convenient for long fiber links, but rather for short distance applications as for instance in laser surgery. Compared to conventional laser surgery with reflecting mirrors fibers gives the possibility to do operations inside the body without the need to open it. A first application of photonic-crystal fibers for medical purposes is found in [77] where a fiber is employed successfully in laryngeal and airway surgery. In order to get a high energy flow in the fiber it is important to design the cross section such that the overlap between the optical mode and the cladding is as small as possible. This problem is considered in a number of papers [78, 79, 80], where geometry parameters such as the core size, the thickness and the shape of a solid core boundary as well as the size of the fingers pointing towards the core have been varied. In this chapter topology optimization, which has already been applied to design photonic crystals [50, 53, 54, 56], is employed to increase the energy flow in a holey fiber. First the method is presented and then an example of its performance is shown for an optical wavelength relevant for medical purposes. 5.1 Method The purpose of the presented method is to distribute air and silica material in the design domain Ωd around the fiber core such that the energy flow in the core region Ωc is maximized. The initial design of the holey fiber is given in figure 5.1. The pitch is Λ = 3.1 µm, the hole diameter over the pitch ratio is d/Λ = 0.92 and the 27
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Chapter 5<br />
Design of photonic-crystal fibers by topology<br />
optimization [P2]<br />
The second type of wave problem is studied in this chapter and is about optical<br />
waves propagating in hollow core photonic-crystal fibers. The method of topology<br />
optimization is used to maximize the energy flow by redistributing air and silica<br />
material around the core, such that the overlap of the magnetic field in the lossy<br />
silica cladding is decreased. The chapter is a summary of publication [P2].<br />
One- or two-dimensional photonic crystals are employed to confine optical waves<br />
in the core region of photonic-crystal fibers, which were first studied in the 1990s<br />
[75, 76]. A holey fiber consists of a hollow core, which is surrounded by a two<br />
dimensional periodic pattern of air holes that confine the wave by the band-gap<br />
effect [17]. Thus, a part of the optical wave propagates in air for this type of fiber,<br />
and therefore losses as well as unwanted dispersion and nonlinear effects from the<br />
cladding material can be reduced. Another part of the wave propagates in the<br />
cladding, which is usually silica. For optical wavelengths in general, silica is a lossy<br />
material and will absorb a part of the energy. For most wavelengths holey fibers<br />
will therefore not be convenient for long fiber links, but rather for short distance<br />
applications as for instance in laser surgery. Compared to conventional laser surgery<br />
with reflecting mirrors fibers gives the possibility to do operations inside the body<br />
without the need to open it. A first application of photonic-crystal fibers for medical<br />
purposes is found in [77] where a fiber is employed successfully in laryngeal and<br />
airway surgery. In order to get a high energy flow in the fiber it is important to<br />
design the cross section such that the overlap between the optical mode and the<br />
cladding is as small as possible. This problem is considered in a number of papers<br />
[78, 79, 80], where geometry parameters such as the core size, the thickness and the<br />
shape of a solid core boundary as well as the size of the fingers pointing towards<br />
the core have been varied. In this chapter topology optimization, which has already<br />
been applied to design photonic crystals [50, 53, 54, 56], is employed to increase the<br />
energy flow in a holey fiber. First the method is presented and then an example of<br />
its performance is shown for an optical wavelength relevant for medical purposes.<br />
5.1 Method<br />
The purpose of the presented method is to distribute air and silica material in the<br />
design domain Ωd around the fiber core such that the energy flow in the core region<br />
Ωc is maximized. The initial design of the holey fiber is given in figure 5.1. The<br />
pitch is Λ = 3.1 µm, the hole diameter over the pitch ratio is d/Λ = 0.92 and the<br />
27