Homework for Chapter 4 4.1 We wish to fabricate a planar ...

Homework for Chapter 4 4.1 We wish to fabricate a planar ... Homework for Chapter 4 4.1 We wish to fabricate a planar ...

homepage.ntu.edu.tw
from homepage.ntu.edu.tw More from this publisher
29.12.2012 Views

Homework for Chapter 4 4.1 We wish to fabricate a planar waveguide for light of wavelength λ0 = 1.15 μm that will operate in the single (fundamental) mode. If we use the proton bombardment, carrier-concentration-reduction method to form a 3μm thick waveguide in GaAs, what are the minimum and maximum allowable carrier concentrations in the substrate? (Calculate for the two cases of p-type or n-type substrate material if that will result in different answers.) 4.2 If light of λ0 = 1.06 μm is used, what are the answers to Problem 4.1? 4.3 Compare the results of Problems 4.1 and 4.2 with those of Problems 2.1 and 2.2, note the unique wavelength dependence of the characteristics of the carrier-concentration-reduction type waveguide. 4.4 We wish to fabricate a planar waveguide for light of λ0 = 0.9 μm in Ga(1−x)AlxAs. It will be a double layer structure on a GaAs substrate. The top (waveguiding) layer will be 3.0 μm thick with the composition Ga0.9Al0.1As. The lower (confining) layer will be 10 μm thick and have the composition Ga0.17Al0.83As. How many modes will this structure be capable of waveguiding? 4.5 What is the answer to Problem 4.4 if the wavelength is λ0 = 1.15 μm? 4.6 A planar asymmetric waveguide is fabricated by depositing a 2.0 μm thick layer of Ta2O5 (n = 2.09) onto a quartz substrate (n = 1.5). (a) How many modes can this waveguide support for light of 632.8 nm (vacuum wavelength)? (b) Approximately what angle does the ray representing the highest-order mode make with the surface of the waveguide? 4.7 A three-layer planar waveguide structure consists of a 5 μm thick waveguiding layer of GaAs with electron concentration N = 1× 10 14 cm −3 , covered on top with a confining layer of Ga0.75Al0.25As with N = 1× 10 18 cm −3 , and on bottom with a confining layer of GaAs with N = 1× 10 18 cm −3 . If this waveguide is used to guide light of λ0 = 1.06 μm, how many modes can it support? 4.8 For an asymmetric planar waveguide like that of Fig. 3.1 with n1 = 1.0, n2 = 1.65, n3 = 1.52, tg = 1.18 μm, and λ0 = 0.63 μm, find the number of allowed TE modes. Fig. 3.1 Basic three-layer planar waveguide structure 4.9 If the waveguide of Prob. 4.4 were to be modified so as to support one additional mode, would it be practical to produce the required change in n by using the electro-optic effect? (Assume a uniform electric field to be applied over the thickness of the waveguide in the direction normal to the surface, with r41 = 1.4× 10 −12 m/V). 4.10 Explain why the cutoff condition for a carrier-concentration-reduction type waveguide is

<strong>Homework</strong> <strong>for</strong> <strong>Chapter</strong> 4<br />

<strong>4.1</strong> <strong>We</strong> <strong>wish</strong> <strong>to</strong> <strong>fabricate</strong> a <strong>planar</strong> waveguide <strong>for</strong> light of wavelength λ0 = 1.15 μm that will operate in<br />

the single (fundamental) mode. If we use the pro<strong>to</strong>n bombardment,<br />

carrier-concentration-reduction method <strong>to</strong> <strong>for</strong>m a 3μm thick waveguide in GaAs, what are the<br />

minimum and maximum allowable carrier concentrations in the substrate? (Calculate <strong>for</strong> the two<br />

cases of p-type or n-type substrate material if that will result in different answers.)<br />

4.2 If light of λ0 = 1.06 μm is used, what are the answers <strong>to</strong> Problem <strong>4.1</strong>?<br />

4.3 Compare the results of Problems <strong>4.1</strong> and 4.2 with those of Problems 2.1 and 2.2, note the unique<br />

wavelength dependence of the characteristics of the carrier-concentration-reduction type<br />

waveguide.<br />

4.4 <strong>We</strong> <strong>wish</strong> <strong>to</strong> <strong>fabricate</strong> a <strong>planar</strong> waveguide <strong>for</strong> light of λ0 = 0.9 μm in Ga(1−x)AlxAs. It will be a<br />

double layer structure on a GaAs substrate. The <strong>to</strong>p (waveguiding) layer will be 3.0 μm thick<br />

with the composition Ga0.9Al0.1As. The lower (confining) layer will be 10 μm thick and have the<br />

composition Ga0.17Al0.83As. How many modes will this structure be capable of waveguiding?<br />

4.5 What is the answer <strong>to</strong> Problem 4.4 if the wavelength is λ0 = 1.15 μm?<br />

4.6 A <strong>planar</strong> asymmetric waveguide is <strong>fabricate</strong>d by depositing a 2.0 μm thick layer of Ta2O5 (n =<br />

2.09) on<strong>to</strong> a quartz substrate (n = 1.5).<br />

(a) How many modes can this waveguide support <strong>for</strong> light of 632.8 nm (vacuum wavelength)?<br />

(b) Approximately what angle does the ray representing the highest-order mode make with the<br />

surface of the waveguide?<br />

4.7 A three-layer <strong>planar</strong> waveguide structure consists of a 5 μm thick waveguiding layer of GaAs<br />

with electron concentration N = 1× 10 14 cm −3 , covered on <strong>to</strong>p with a confining layer of<br />

Ga0.75Al0.25As with N = 1× 10 18 cm −3 , and on bot<strong>to</strong>m with a confining layer of GaAs with N = 1×<br />

10 18 cm −3 . If this waveguide is used <strong>to</strong> guide light of λ0 = 1.06 μm, how many modes can it<br />

support?<br />

4.8 For an asymmetric <strong>planar</strong> waveguide like that of Fig. 3.1 with n1 = 1.0, n2 = 1.65, n3 = 1.52, tg =<br />

1.18 μm, and λ0 = 0.63 μm, find the number of allowed TE modes.<br />

Fig. 3.1 Basic three-layer <strong>planar</strong> waveguide structure<br />

4.9 If the waveguide of Prob. 4.4 were <strong>to</strong> be modified so as <strong>to</strong> support one additional mode, would it<br />

be practical <strong>to</strong> produce the required change in n by using the electro-optic effect? (Assume a<br />

uni<strong>for</strong>m electric field <strong>to</strong> be applied over the thickness of the waveguide in the direction normal <strong>to</strong><br />

the surface, with r41 = 1.4× 10 −12 m/V).<br />

<strong>4.1</strong>0 Explain why the cu<strong>to</strong>ff condition <strong>for</strong> a carrier-concentration-reduction type waveguide is


independent of wavelength.<br />

<strong>4.1</strong>1 <strong>We</strong> desire an epitaxially-grown double-heterojunction In(1-x)GaxAs(1-y)Py waveguide that will have<br />

a bandgap Eg = 1.1 eV in the waveguiding layer at room temperature.<br />

(a) If lattice-matched layers are desired, what should be the relative concentrations of the<br />

constituent elements? i.e. What are x and y?<br />

(b) What is the shortest wavelength that can be guided in this waveguide without excessive<br />

interband absorption?<br />

<strong>4.1</strong>2 <strong>We</strong> <strong>wish</strong> <strong>to</strong> make an epitaxially grown waveguide in In(1-x)GaxAs(1-y)Py that has a bandgap of 0.9<br />

eV at liquid nitrogen temperature (77 K). Find the values of x and y that are required.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!