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NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
HsinChu, Taiwan
Presenter : Wan-Cheng Chiu (邱萬誠)
Instructor : Cheng-Hsien Liu (劉承賢)
Midterm Project Presentation
-Presentation I-
April 22, 2014
NATIONAL TSING HUA UNIVERSITY
Capacitive Silicon Resonator Structure with Movable
Electrodes to Reduce Capacitive Gap Widths Based on
Electrostatic Parallel Plate Actuation
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
2
• Introduction & Motivation
• Principle
• Purpose
• Method
• Design
• Experiment Results
• Conclusion
Outline
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
3
•Resonator is a fundamental component in many MEMS devices.
•Small electromechanical structure that vibrate at high frequencies
Introduction
Mode Shape Mode Shape
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
4
•These devices can be used as timing references, filters, sensors, and
so on.
•It has the possibility to replace quartz due to the capability for further
miniaturization.
Introduction & Motivation
Medical Ultrasonography
GPS
Smartphone
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
5
•For two parallel plate:
Principle
+
V
-
g
Capacitance = εA/g
If one of the plate is free to move up
and down, then the capacitance can
vary.
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
6
•For a single beam capacitive resonator, we can measure the response
of the device.
Principle
When a small signal vi
is applied, we will get a
frequency response.
Resonant
frequency
vi
Rm im
Vp
vo
Driving
electrode
Sensing
electrode
Resonator
body
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
7
Principle
•Electrical System• Mechanical System
Lm = mr / ηe
2
Rm = cr / ηe
2
Cm = ηe
2 /kr
mr
kr = ωn
2mr
cr = (√krmr)/Q
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
8
Principle
• Pull-In Effect
g0
2/3g0
•Spring Force:
Fspring = kδ
•Electrostatic Force:
Fe = εAV2/2(g- δ)2
Fnet = εAV2/2(g- δ)2 - kδ
•Pull-In Voltage:
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
9
Purpose
•Electrical System
Lm = mr / ηe
2
Rm = cr / ηe
2
Cm = ηe
2 /kr
Rm is also known as motional impedance,
a low Rm device has a low insertion loss
and lower phase noise.
In this paper, the author focus on reducing
gap width to reduce the motional
impedance.
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
10
Method
By making the electrodes movable,
when voltage is applied the electrodes
will move towards the resonator body
due to electrostatic force. Thus the gap
widths become smaller.
d Rm
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
11
Design
•The electrodes are attached to spring,
which will make the electrodes movable.
•In the design stoppers are added to
prevent pull-in effect from occurring.
•The new gap width is equal to:
greduced = gB-B’ – gA-A’
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
12
Experiment Results
•The image below is a SEM image of silicon resonator with movable electrodes.
A-A’ is the stopper gap = 400nm
B-B’ is the capacitive gap = 500nm
Final gap = 100nm
*A same version of the silicon resonator without movable electrodes is also fabricated
for measurement comparison.
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
13
Experiment Results
•The measurement was done inside a vacuum chamber with pressure of 0.01 Pa.
The resonator with movable
electrode shows lower insertion loss
and Rm.
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
14
Experiment Results
• Loading Effect Qloaded:
Originally, the Q of the device can be calculated by:
However, when we measure a device, other resistances needs to be included:
Rm
R1 R2
Since the Rm of the movable electrode resonator is
smaller, the loading effect affects the Q more than
the other resonator.
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
15
Experiment Results
•By applying different bias voltage, VDC, to the resonator we can observe the frequency
shift.
•The resonator with movable
electrode has a better tuning
capability than the other.
•This is an advantage because
due to fabrication process or
operation temperature the
resonant frequency may shift
from our desired frequency.
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
16
Conclusion
• In this paper, capacitive silicon resonators with
movable electrodes was designed, fabricated,
and evaluated.
• The insertion loss increased by 21 dB, and the
motional impedance was reduced.
• The frequency tuning capability is also 7 times
better.
NATIONAL TSING HUA UNIVERSITY
National Tsing Hua University
17
~Thank you for your attention~

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Sensing and Actuation in Miniaturized Systems _ Midterm Presentation

  • 1. 按一下以編輯母片標題樣式 NATIONAL TSING HUA UNIVERSITY National Tsing Hua University HsinChu, Taiwan Presenter : Wan-Cheng Chiu (邱萬誠) Instructor : Cheng-Hsien Liu (劉承賢) Midterm Project Presentation -Presentation I- April 22, 2014 NATIONAL TSING HUA UNIVERSITY Capacitive Silicon Resonator Structure with Movable Electrodes to Reduce Capacitive Gap Widths Based on Electrostatic Parallel Plate Actuation
  • 2. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 2 • Introduction & Motivation • Principle • Purpose • Method • Design • Experiment Results • Conclusion Outline
  • 3. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 3 •Resonator is a fundamental component in many MEMS devices. •Small electromechanical structure that vibrate at high frequencies Introduction Mode Shape Mode Shape
  • 4. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 4 •These devices can be used as timing references, filters, sensors, and so on. •It has the possibility to replace quartz due to the capability for further miniaturization. Introduction & Motivation Medical Ultrasonography GPS Smartphone
  • 5. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 5 •For two parallel plate: Principle + V - g Capacitance = εA/g If one of the plate is free to move up and down, then the capacitance can vary.
  • 6. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 6 •For a single beam capacitive resonator, we can measure the response of the device. Principle When a small signal vi is applied, we will get a frequency response. Resonant frequency vi Rm im Vp vo Driving electrode Sensing electrode Resonator body
  • 7. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 7 Principle •Electrical System• Mechanical System Lm = mr / ηe 2 Rm = cr / ηe 2 Cm = ηe 2 /kr mr kr = ωn 2mr cr = (√krmr)/Q
  • 8. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 8 Principle • Pull-In Effect g0 2/3g0 •Spring Force: Fspring = kδ •Electrostatic Force: Fe = εAV2/2(g- δ)2 Fnet = εAV2/2(g- δ)2 - kδ •Pull-In Voltage:
  • 9. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 9 Purpose •Electrical System Lm = mr / ηe 2 Rm = cr / ηe 2 Cm = ηe 2 /kr Rm is also known as motional impedance, a low Rm device has a low insertion loss and lower phase noise. In this paper, the author focus on reducing gap width to reduce the motional impedance.
  • 10. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 10 Method By making the electrodes movable, when voltage is applied the electrodes will move towards the resonator body due to electrostatic force. Thus the gap widths become smaller. d Rm
  • 11. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 11 Design •The electrodes are attached to spring, which will make the electrodes movable. •In the design stoppers are added to prevent pull-in effect from occurring. •The new gap width is equal to: greduced = gB-B’ – gA-A’
  • 12. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 12 Experiment Results •The image below is a SEM image of silicon resonator with movable electrodes. A-A’ is the stopper gap = 400nm B-B’ is the capacitive gap = 500nm Final gap = 100nm *A same version of the silicon resonator without movable electrodes is also fabricated for measurement comparison.
  • 13. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 13 Experiment Results •The measurement was done inside a vacuum chamber with pressure of 0.01 Pa. The resonator with movable electrode shows lower insertion loss and Rm.
  • 14. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 14 Experiment Results • Loading Effect Qloaded: Originally, the Q of the device can be calculated by: However, when we measure a device, other resistances needs to be included: Rm R1 R2 Since the Rm of the movable electrode resonator is smaller, the loading effect affects the Q more than the other resonator.
  • 15. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 15 Experiment Results •By applying different bias voltage, VDC, to the resonator we can observe the frequency shift. •The resonator with movable electrode has a better tuning capability than the other. •This is an advantage because due to fabrication process or operation temperature the resonant frequency may shift from our desired frequency.
  • 16. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 16 Conclusion • In this paper, capacitive silicon resonators with movable electrodes was designed, fabricated, and evaluated. • The insertion loss increased by 21 dB, and the motional impedance was reduced. • The frequency tuning capability is also 7 times better.
  • 17. NATIONAL TSING HUA UNIVERSITY National Tsing Hua University 17 ~Thank you for your attention~