Radius of Curvature: 900 micron Fig. 1 a.) Snell’s Law b.) Total Internal Reflection a. b....

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Radius of Curvatur e: 900 micron Fig. 1 a.) Snell’s Law b.) Total Internal Reflection a. b. Modeling & Fabrication of Ridge Waveguides and their Comparison to Photonic Bandgap Structures Kathleen Beddow, Meron Tekeste, Senthil Rajagopal, Jan M. Yarrison-Rice, Physics Department, Miami University Total Internal Reflection •Total Internal Reflection occurs as light travels from a higher to a lower index of refraction when the refracted angle is equal to 90 o or greater, which depends on the angle of incidence. Introduction Optoelectronics is a field of technology involving the study and fabrication of microelectronic devices that interact with light (photons). An optoelectronic device either contains or acts as a transducer, a device that converts between electrical and optical signals. This technology provides the capacity to generate, transport, and manipulate data at exceptional rates. Our study focuses upon the characterization of both waveguides, specifically the Ridge Waveguide, and Photonic Bandgap Structures with a goal to be able to fabricate the waveguides in house. Optical Waveguide Waveguide: Structural component of integrated optical circuits having the ability to guide high frequency electromagnetic waves due to different indices of refraction. Ridge Waveguide: A slab waveguide with a “Ridge” etched into the upper substrate, changing the effective indices of refraction on either side, creating conditions for Total Internal Reflection within the ridge area allowing for guidance of light. MIAMI UNIVERSITY CENTER FOR NANOTECHNOLOGY Summary •We are studying the field of optoelectronics in an effort to model both ridge waveguides and photonic bandgap structures. •In examining the properties of these waveguides and PBG structures, their ability to guide and contain light will be examined and compared. •In addition to modeling ridge waveguides, the goal is to be able to fabricate these structures within our facilities. This will be done through an wet etching process with HF. •Once fabricated our waveguides will be characterized through a series of measurements to show their effectiveness in containing light. Photonic Bandgap Structures (PBG) •Photonic Bandgap Structure: Substrate (e.g. Silicon Nitride) etched with periodic array of air pores is used to create a photonic lattice. Fabrication of Ridge Waveguide •The fabrication of the Ridge Waveguide will be done through UV photolithography followed by immersion of a slab waveguide in a dilute hydrofluoric acid (HF) solution for wet etching. Although the HF solution will etch both the Si 3 N 4 and SiO 2 , selectivity for the Si 3 N 4 can be increased by increasing the dilution of the HF solution. In doing this however, the etch rate is sacrificed, some of which may be regained through elevation of temperature. •PBG structure will be fabricated via e-beam lithography and plasma etching. Experimental Characterization of Waveguide • Once fabrication has occurred, the waveguide will be characterized by measuring the input and output power. This will allow us to determine the amount of light escaping as it travels down the waveguide. Fig. 3 a.) Triangular Lattice of PBG b.) Dispersion Graph a. ) b. ) Modeling: Waveguides Modeling: PBG a.) 0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5 0 0.5 1 1.5 2 2.5 x (micron) y (micron) 0.5 1 1.5 -3 -2 -1 0 1 2 3 0 0.5 1 1.5 2 s (micron) Amplitude Si 3 N 4 (n=2.02) SiO 2 (n=1.46) Fig. 2 a.) Slab Waveguide b.) Ridge Waveguide 1.Wafer Cut to Size 2. Coat with Negative Photoresis t 3. Add Glass Slide with Ridge Pattern in Chromium 4. Expose to UV light 5. Develop the Resist 6. Add HF to Wet Etch Wafer 7. Remove Resist Fig. 6 a.) Selectivity and Etch Rate of HF solution at various Dilutions (Knotter, D. Martin et.al. "Selective Si3N4 etch in Single Wafer Application" Solid State Phenomena ” Vol.103- 104 (2005): 103-106.) b.) Etching Process b.) Fig. 4 Waveguide Modeling at 632.8nm wavelength: a.) Straight Slab Waveguide: Light Propagation with High Power Loss b.)Straight Ridge Waveguide (1.3 micron Ridge): Light Propagation with Minimal Power Loss c.)S-Ridge Waveguide, Curve of Radius 900 micron: Light Guidance d.) S-Ridge Waveguide, Curve of Radius 13 micron: Light Loss Radius of Curvature : 13 micron 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Frequency ( a/2 c) X M a = 257nm R = 75nm R a a Silicon Nitride n=2.02 Air holes n=1 b Fig. 5 Triangular Lattice PBG Modeling at 632.8nm wavelength: a.) Triangular Lattice Straight PBG Structure: Minimal Light Loss, 92% Transmission b.) Triangular Lattice Curved PBG Structure: Minimal Light Loss, 94% Transmission 0.5 1 1.5 2 2.5 3 3.5 4 4.5 0.5 1 1.5 2 2.5 3 3.5 x (micron) y (micron) 0.5 1 1.5 2 435nm 435nm 440nm Fig. 7 Setup for Measuring Light Transmission through Waveguide
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Transcript of Radius of Curvature: 900 micron Fig. 1 a.) Snell’s Law b.) Total Internal Reflection a. b....

Page 1: Radius of Curvature: 900 micron Fig. 1 a.) Snell’s Law b.) Total Internal Reflection a. b. Modeling & Fabrication of Ridge Waveguides and their Comparison.

Radius of Curvature: 900 micron

Fig. 1 a.) Snell’s Law b.) Total Internal Reflection

a. b.

Modeling & Fabrication of Ridge Waveguides and their Comparison to Photonic Bandgap StructuresKathleen Beddow, Meron Tekeste, Senthil Rajagopal, Jan M. Yarrison-Rice, Physics Department, Miami University

Total Internal Reflection•Total Internal Reflection occurs as light travels from a higher to a lower index of refraction when the refracted angle is equal to 90o or greater, which depends on the angle of incidence.

IntroductionOptoelectronics is a field of technology involving the study and fabrication of microelectronic devices that interact with light (photons). An optoelectronic device either contains or acts as a transducer, a device that converts between electrical and optical signals. This technology provides the capacity to generate, transport, and manipulate data at exceptional rates. Our study focuses upon the characterization of both waveguides, specifically the Ridge Waveguide, and Photonic Bandgap Structures with a goal to be able to fabricate the waveguides in house.

Optical Waveguide• Waveguide: Structural component of integrated optical circuits having the ability to guide high frequency electromagnetic waves due to different indices of refraction.

• Ridge Waveguide: A slab waveguide with a “Ridge” etched into the upper substrate, changing the effective indices of refraction on either side, creating conditions for Total Internal Reflection within the ridge area allowing for guidance of light.

MIAMI UNIVERSITY CENTER FOR NANOTECHNOLOGY

Summary•We are studying the field of optoelectronics in an effort to model both ridge waveguides and photonic bandgap structures.

•In examining the properties of these waveguides and PBG structures, their ability to guide and contain light will be examined and compared.

•In addition to modeling ridge waveguides, the goal is to be able to fabricate these structures within our facilities. This will be done through an wet etching process with HF.

•Once fabricated our waveguides will be characterized through a series of measurements to show their effectiveness in containing light.

Photonic Bandgap Structures (PBG)•Photonic Bandgap Structure: Substrate (e.g. Silicon Nitride) etched with periodic array of air pores is used to create a photonic lattice.

Fabrication of Ridge Waveguide •The fabrication of the Ridge Waveguide will be done through UV photolithography followed by immersion of a slab waveguide in a dilute hydrofluoric acid (HF) solution for wet etching.

•Although the HF solution will etch both the Si3N4 and SiO2, selectivity for the Si3N4 can be increased by increasing the dilution of the HF solution. In doing this however, the etch rate is sacrificed, some of which may be regained through elevation of temperature.

•PBG structure will be fabricated via e-beam lithography and plasma etching.

Experimental Characterization of Waveguide• Once fabrication has occurred, the waveguide will be characterized by measuring the input and output power. This will allow us to determine the amount of light escaping as it travels down the waveguide.

Fig. 3 a.) Triangular Lattice of PBG b.) Dispersion Graph

a.) b.)

Modeling: Waveguides

Modeling: PBG

a.)

0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 50

0.5

1

1.5

2

2.5

x (micron)

y (m

icro

n)

0.5

1

1.5

-3 -2 -1 0 1 2 30

0.5

1

1.5

2

s (micron)

Am

plit

ude

Si3N4 (n=2.02)

SiO2 (n=1.46)

Fig. 2 a.) Slab Waveguide

b.) Ridge Waveguide

1. Wafer Cut to Size

2. Coat with Negative Photoresist

3. Add Glass Slide with Ridge Pattern in Chromium

4. Expose to UV light

5. Develop the Resist

6. Add HF to Wet Etch Wafer

7. Remove Resist

Fig. 6

a.) Selectivity and Etch Rate of HF solution at various Dilutions (Knotter, D. Martin et.al. "Selective Si3N4 etch in Single Wafer Application" Solid State Phenomena” Vol.103-104 (2005): 103-106.)

b.) Etching Process

b.)

Fig. 4 Waveguide Modeling at 632.8nm wavelength:

a.) Straight Slab Waveguide: Light Propagation with High Power Loss

b.)Straight Ridge Waveguide (1.3 micron Ridge): Light Propagation with Minimal Power Loss

c.)S-Ridge Waveguide, Curve of Radius 900 micron: Light Guidance

d.) S-Ridge Waveguide, Curve of Radius 13 micron: Light Loss

Radius of Curvature: 13 micron

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

Fre

quen

cy (

a/

2

c)

X M

a = 257nm

R = 75nm

R

a

a

Silicon Nitriden=2.02

Air holesn=1

b

Fig. 5 Triangular Lattice PBG Modeling at 632.8nm wavelength:

a.) Triangular Lattice Straight PBG Structure: Minimal Light Loss, 92% Transmission

b.) Triangular Lattice Curved PBG Structure: Minimal Light Loss, 94% Transmission

0.5 1 1.5 2 2.5 3 3.5 4 4.5

0.5

1

1.5

2

2.5

3

3.5

x (micron)

y (m

icro

n)

0.5

1

1.5

2

435nm

435nm 440nm

Fig. 7

Setup for Measuring Light Transmission through Waveguide