Projects:2019s2-21501 Terahertz Waveplates - Revision history

A1699335 at 15:00, 8 June 2020

2020-06-08T15:00:14Z

A1699335 at 14:51, 8 June 2020

2020-06-08T14:51:10Z

A1699335: This thesis introduces the background of the terahertz technology, wave plate. Based on the background, the equations which are related to the optical parameters used in the wave plate design and data processing are also given. Further details on the stru

2020-06-08T14:46:54Z

This thesis introduces the background of the terahertz technology, wave plate. Based on the background, the equations which are related to the optical parameters used in the wave plate design and data processing are also given. Further details on the stru

A1699335 at 12:26, 8 June 2020

2020-06-08T12:26:59Z

A1699335: /* Supervisors */

2019-09-25T12:00:15Z

‎Supervisors

A1699335: /* Project students */

2019-09-25T12:00:06Z

‎Project students

A1699335: Created page with "Category:Projects Category:Final Year Projects 21501 The project is to learn knowledge of terahertz technology, wave plate, CST software. And in th..."

2019-09-25T11:59:47Z

Created page with "Category:Projects Category:Final Year Projects 21501 The project is to learn knowledge of terahertz technology, wave plate, CST software. And in th..."

New page

[[Category:Projects]]
[[Category:Final Year Projects]]
[[Category:2019s2|21501]]
The project is to learn knowledge of terahertz technology, wave plate, CST software. And in this project we aim to design, simulate and test a wave plate operating at a frequency between 0.1 to 10 THz.
== Introduction ==
The terahertz range spans 0.1 and 10 THz. It defines a transition between the electronics and photonics domains—the frequency range is at the upper bound of electronics and the lower bound of photonics. For this very reason, in the past the band has been perceived as a terahertz gap due to the lack of efficient generation and detection approaches. Over a few decades, a myriad of sources and detectors have become mature to tap into unique opportunities in this frequency range. Much has yet to be done in this area towards integrated high-performance platforms, envisioned for post-5G applications. Core components that underpin any integrated platform are interconnects, i.e., waveguiding structures. A large number of terahertz waveguides have been proposed with different trade-offs related to bandwidth, dispersion, confinement, losses, and fabrication complexity. Here we will investigate a waveguide design that could carry terahertz waves with practical performance. This project will tackle on different waveguide designs and related components. The students will gain experience on full-wave electromagnetic simulation, theoretical analysis of waveguides, and a terahertz measurement system.

=== Project team ===
==== Project students ====
* <Fan Zhang>
* <Yingzhe Guo>

==== Supervisors ====
* <Dr. Withawat Withayachumnankul>
* <Dr. Wendy Suk Ling Lee>

=== Objectives ===
To design, simulate and test a terahertz wave plate. we need to achieve:

* learn the background of terahertz technology and wave plate
* design a wave plate

== Background ==
=== Topic 1 ===

== Method ==

== Results ==

== Conclusion ==

== References ==
[1] Tonouchi, M 2007, Cutting-edge THz technology, Nature Photonics, vol. 1, pp.97–105 .

[2] Ferguson, B & Xi-Cheng Zhang 2002, Materials for terahertz science and technology, Nature Materials, vol. 1, pp.26–33.

[3] P.H. Siegel 2002, Terahertz Technology, IEEE Transactions on Microwave Theory and Techniques, vol. 50, no. 3.

[4] Ornik, J, Gomell, L, Busch, SF, Hermans, M, & Koch, M 2018, High quality terahertz glass wave plates, Optics Express, vol. 26, no. 25, pp. 32631-32639.

@@ Line 43: / Line 43: @@
 '''Experiments in CST'''
-Before the half wave plate and the quarter wave plate are constructed, the dimension of the slab needs to be determined. Note that this dimension is about the widths of the COC bars and air grooves, but not the thickness of the slab. The thickness of the wave plate is determined by the difference between the horizontal and vertical refractive index which is called delta n. As the thickness of the wave plate is unknown, an initial thickness can be assumed as 1 mm. Then, the widths of the COC bars and air grooves are initially set as 0.3 mm periodic which means the COC bars and air grooves are all 0.3 mm in width. The slab of this dimension can be considered as a sample. After the dimension is set, the model of the sample in the CST can be changed into this dimension and simulated. The figure below is the model of the sample in the CST.[[File:CST structure.png|thumb]],
+Before the half wave plate and the quarter wave plate are constructed, the dimension of the slab needs to be determined. Note that this dimension is about the widths of the COC bars and air grooves, but not the thickness of the slab. The thickness of the wave plate is determined by the difference between the horizontal and vertical refractive index which is called delta n. As the thickness of the wave plate is unknown, an initial thickness can be assumed as 1 mm. Then, the widths of the COC bars and air grooves are initially set as 0.3 mm periodic which means the COC bars and air grooves are all 0.3 mm in width. The slab of this dimension can be considered as a sample. After the dimension is set, the model of the sample in the CST can be changed into this dimension and simulated. The figure below is the model of the sample in the CST.
-[[File:Phase diagram.png|thumb]]
+                                          [[File:CST structure.png|thumb]],
@@ Line 51: / Line 52: @@
 After the half wave plate and quarter wave plate are simulated, the S21 parameter data are imported into the MATLAB code and the delta n for the half wave plate and quarter wave plate is  the same with the delta n of the sample. To be more specific, the phase difference of the wave plate is shown has already be verified.For the phase difference of the half wave plate is 179.86 degrees and the phase difference of the quarter wave plate should be 90.15 degrees.
-[[File:Ha.png|thumb]][[File:Qu.png|thumb]]
+                                                       [[File:Ha.png|thumb]]

← Older revision		Revision as of 14:51, 8 June 2020
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	'''Simulation results for the half wave plate and quarter wave plate'''		'''Simulation results for the half wave plate and quarter wave plate'''

−	After the half wave plate and quarter wave plate are simulated, the S21 parameter data are imported into the MATLAB code and the delta n for the half wave plate and quarter wave plate is the same with the delta n of the sample. To be more specific, the phase difference of the wave plate is shown has already be verified.For the phase difference of the half wave plate is 179.86 degrees and the phase difference of the quarter wave plate should be 90.15 degrees.	+	After the half wave plate and quarter wave plate are simulated, the S21 parameter data are imported into the MATLAB code and the delta n for the half wave plate and quarter wave plate is the same with the delta n of the sample. To be more specific, the phase difference of the wave plate is shown has already be verified.For the phase difference of the half wave plate is 179.86 degrees and the phase difference of the quarter wave plate should be 90.15 degrees.
		+	[[File:Ha.png\|thumb]][[File:Qu.png\|thumb]]
		+

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 [[Category:Projects]]
 [[Category:Final Year Projects]]
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 == Background ==
 '''Terahertz technology'''
-The terahertz range spans from 100 GHz to 10 THz which is between microwaves and infrared waves.The Photon energy is  from 1.2 meV to12.4meV.The advantage of the terahertz technology is non-ionisation.The limitation of the terahertz is hardly penetrate fog and clouds, and it is cannot penetrate water or metal ,so the terahertz technology can only use indoor.The property the terahertz is Far-infrared, sub-millimetre wave,Penetrate conventionally opaque materials and high chemical sensitivity.Some of the applications are used in Information and communication technology areas,Biological; medical and pharmaceutical sciences areas; security areas;Earth and space science.
 '''Wave plates'''
 Wave plate is a optical device that changes the polarisation state of the transmitted wave.Wave plate can be divided into two types: half-wave plate and quarter-wave plate. In Lee’s (2018) study, as for the half-wave plate, a 45 degrees linearly polarized light going through the wave plate will be resolved into a vertical component and a horizontal component. And there will be a phase difference of  radian between these two components, then the two components will compose a linearly polarized light but being rotated by 90 degrees than the original light. As for the quarter-wave plate, if a 45 degrees linearly polarized light goes through the wave plate, it will also be resolved into a vertical component and a horizontal component.There will be a phase difference of pi/2 radian between these two components. And the two components will compose a circularly polarized light.
 == Design ==
-Experiments in MATLAB
+'''Experiments in MATLAB'''
-Experiments in CST
+Before the half wave plate and the quarter wave plate are constructed, the dimension of the slab needs to be determined. Note that this dimension is about the widths of the COC bars and air grooves, but not the thickness of the slab. The thickness of the wave plate is determined by the difference between the horizontal and vertical refractive index which is called delta n. As the thickness of the wave plate is unknown, an initial thickness can be assumed as 1 mm. Then, the widths of the COC bars and air grooves are initially set as 0.3 mm periodic which means the COC bars and air grooves are all 0.3 mm in width. The slab of this dimension can be considered as a sample. After the dimension is set, the model of the sample in the CST can be changed into this dimension and simulated. The figure below is the model of the sample in the CST.[[File:CST structure.png|thumb]],
-Before the half wave plate and the quarter wave plate are constructed, the dimension of the slab needs to be determined. Note that this dimension is about the widths of the COC bars and air grooves, but not the thickness of the slab. The thickness of the wave plate is determined by the difference between the horizontal and vertical refractive index which is called delta n. As the thickness of the wave plate is unknown, an initial thickness can be assumed as 1mm. Then, the widths of the COC bars and air grooves are initially set as 0.5mm periodic which means the COC bars and air grooves are all 0.5mm in width. The slab of this dimension can be considered as a sample. After the dimension is set, the model of the sample in the CST can be changed into this dimension and simulated. The figure below is the model of the sample in the CST.
+[[File:Phase diagram.png|thumb]]
 == Results ==
 == Conclusion ==
 == References ==
@@ Line 49: / Line 67: @@
 [4] Ornik, J, Gomell, L, Busch, SF, Hermans, M, & Koch, M 2018, High quality terahertz glass wave plates, Optics Express, vol. 26, no. 25, pp. 32631-32639.

@@ Line 19: / Line 19: @@
 * learn the background of terahertz technology and wave plate
-* design a wave plate
+* design a half-wave plate and a quarter-wave plate
 == Background ==
-=== Topic 1 ===
+'''Terahertz technology'''
 == Results ==

@@ Line 12: / Line 12: @@
 ==== Supervisors ====
-* <Dr. Withawat Withayachumnankul>
+* Dr. Withawat Withayachumnankul
-* <Dr. Wendy Suk Ling Lee>
+* Dr. Wendy Suk Ling Lee
 === Objectives ===

@@ Line 8: / Line 8: @@
 === Project team ===
 ==== Project students ====
-* <Fan Zhang>
+* Fan Zhang
-* <Yingzhe Guo>
+* Yingzhe Guo
 ==== Supervisors ====