Lecture 21 QCM and Ellipsometry

Slides:



Advertisements
Similar presentations
Today’s summary Polarization Energy / Poynting’s vector
Advertisements

1 General Properties of Electromagnetic Radiation Lecture 1.
In this presentation you will: explore how sound is propagated
Optical sources Lecture 5.
Physics and the Quantum Mechanical Model l OBJECTIVES: - Calculate the wavelength, frequency, or energy of light, given two of these values.
Optical methods for semiconductor characterization Guillaume von Gastrow.
11.7 Properties of Waves – see also lecture notes 11.7
Spectroscopic Ellipsometry University of Texas at El Paso Lynn Santiago Dr. Elizabeth Gardner Chem 5369.
The Quartz Crystal Microbalance and its Applications
Quantum System “ Ion flux fraction measurement system.
Variable Capacitance Transducers The Capacitance of a two plate capacitor is given by A – Overlapping Area x – Gap width k – Dielectric constant Permitivity.
Sound Chapter 15.
Introduction to Light IN THIS LECTURE –Light –Electromagnetic Radiation –Wave Nomenclature –Electromagnetic Spectrum –Speed of Light –Wave front and wave.
Light and Reflection Light and Reflection. Characterization of Light Light has both a wavelike and particle like nature. Light has both a wavelike and.
8. Wave Reflection & Transmission
EE 5340/7340, SMU Electrical Engineering Department, © Carlos E. Davila, Electrical Engineering Dept. Southern Methodist University slides can be.
Ellipsometry and X-ray Reflectivity (XRR)
Chapter 29 Continued-Chapter 31- Chapter EMF Induced in a Moving Conductor Example 29-8: Force on the rod. To make the rod move to the right.
ECE5320 Mechatronics Assignment#01: Literature Survey on Sensore and Actuators Topic: Quartz Crystal Microbalances Prepared by: Jack J Stepan Dept. of.
K L University 1 By G.SUNITA DEPARTMENT OF PHYSICS.
“+” = Silicon “-” = Oxygen By definition: A unit cell is the smallest parallelepiped (6 sided parallelogram) that will describe the molecule.
Interference Diffraction and Lasers
1 Optical Properties of Materials … reflection … refraction (Snell’s law) … index of refraction Index of refraction Absorption.
EE3321 ELECTROMAGNETIC FIELD THEORY
6. Interference by thin films
The tendency to reduce the cost of CVGs results in metallic resonator. In comparison to quartz resonator CVG, it has much lower Q-factor and, as a result,
Waves - I Chapter 16 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
The Hong Kong Polytechnic University Optics II----by Dr.H.Huang, Department of Applied Physics1 Light Waves Nature of Light: Light can be viewed as both.
Superposition of Sinusoidal Waves Let us now apply the principle of superposition to two sinusoidal waves travelling in the same direction in a linear.
GENERAL ULTRASONIC SYSTEM  TRANSMITTER CIRCUIT  ULTRASONIC TRANSDUCERS  RECEIVER CIRCUIT  MEASURING CIRCUIT  ANALYZER CIRCUIT  SIGNAL PROCESSOR 
Level and Pressure Measurement Christopher Foot Patrick Lawlor.
THIS IS Review Your For Simple Harmonic Motion Electro- magnetic Spectrum Light Basics Light Reflection and Refraction Electricity.
1 Acoustic ↔ Electromagnetic Conversion in THz Range Alex Maznev Nelson group meeting 04/01/2010.
GENERAL ULTRASONIC SYSTEM
Creative Research Initiatives Seoul National University Center for Near-field Atom-Photon Technology - Near Field Scanning Optical Microscopy - Electrostatic.
Electronic Structure. Bohr Bohr proposed that the __________ atom has only certain allowable energy states.
1 Investigation of Optical Properties n, k … index of refraction and damping  1,  2 … polarization and absorption Problems: The penetration depth of.
Measurements in Fluid Mechanics 058:180:001 (ME:5180:0001) Time & Location: 2:30P - 3:20P MWF 218 MLH Office Hours: 4:00P – 5:00P MWF 223B-5 HL Instructor:
Maxwell’s microscopic equations (gaussian units): Classical theory: Quantum theory:
Surface Plasmon Resonance
EE 4BD4 Lecture 16 Piezoelectric Transducers and Application 1.
Waves - I Chapter 16 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Introduction to materials physics #4
Chapter 16 Waves-I Types of Waves 1.Mechanical waves. These waves have two central features: They are governed by Newton’s laws, and they can exist.
WAVES. Traveling disturbanceTransfer of energy 2) Mechanical Wave- need a medium 1) Electromagnetic Wave 1) transversetransverse 2) longitudinallongitudinal.
Surface Acoustics Wave Sensors. Outline Introduction Piezoelectricity effect Fabrication of acoustic waves devices Wave propagation modes Bulk Wave sensor.
Modelling and Simulation of Passive Optical Devices João Geraldo P. T. dos Reis and Henrique J. A. da Silva Introduction Integrated Optics is a field of.
Signal Analyzers. Introduction In the first 14 chapters we discussed measurement techniques in the time domain, that is, measurement of parameters that.
Real-time Ellipsometry on Cesium-Telluride Photocathode Formation
Properties of the bakelite used for standard RPC chambers as a function of the operating temperature F. Bruni – G. Hull – S.M. Mari 4 digital thermometers.
CHAPTER 5 DC AND AC BRIDGES.
Damian Luna Yetziel Sandoval – Alberto Gonzales – 80546
6. Interference by thin films t If there is a very thin film of material – a few wavelengths thick – light will reflect from both the bottom and the top.
17. Electromagnetic waves
Lecture 19 Electromagnetic Waves.
Variable Capacitance Transducers
Radio Coverage Prediction in Picocell Indoor Networks
Laser Physics & Nonlinear Optics
Immobilization Of Biomolecules On Biosensors
6. Interference by thin films
BAHIRDAR UNIVERSTY COLLEGE OF SCIENCE DEPARTMENT :MATERIAL SCIENCE AND ENGINNERING PRESENTETON ON: ELLIPSOMETRY INSTRUMENT PREPEARED BY :ZELALEM GETU AMSALE.
Ellipsometry Measures the amplitude and phase of reflected light
Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
N. BRIMHALL, N. HEILMANN, N. HERRICK, D. D. ALLRED, R. S. TURLEY, M
© 2014 John Wiley & Sons, Inc. All rights reserved.
Physics and the Quantum Mechanical Model
SPECTROPHOTOMETRY Applied Chemistry.
6. Interference by thin films
X-Ray Reflection Data Analysis Update
ANTENNA THEORY by Constantine A. Balanis Chapter 2.13 –
Presentation transcript:

Lecture 21 QCM and Ellipsometry

Quartz Crystal Microbalance The Quartz Crystal Microbalance (QCM) is an extremely sensitive mass sensor, capable of measuring mass changes in the nanogram range. QCMs are piezoelectric devices fabricated of a thin plate of quartz with electrodes affixed to each side of the plate. .

Quartz crystal microbalance Quartz crystals have piezoelectric properties, that is they develop an electric potential upon the application of mechanical stress. The frequency of oscillation of the quartz crystal is partially dependent on the thickness of the crystal. During normal operation, all the other influencing variables remain constant; thus a change in thickness correlates directly to a change in frequency. As mass is deposited on the surface of the crystal, the thickness increases; consequently the frequency of oscillation decreases from the initial value. With some simplifying assumptions, this frequency change can be quantified and correlated precisely to the mass change using Sauerbrey's equation.

Sauerbrey equation f0 – Resonant frequency(Hz) Δf – Frequency change (Hz) Δm – Mass change (g) A – Piezoelectrically active crystal area (Area between electrodes, cm2) ρq – Density of quartz (ρq = 2.648 g/cm3) μq – Shear modulus of quartz for AT-cut crystal (μq = 2.947x1011 g/cm.s2) νq – Transverse wave velocity in quartz (m/s)

MODE OF OPERATION In ring-down, one measures the voltage between the electrodes after the exciting voltage has suddenly been turned off. The resonator emits a decaying sine wave, where the resonance parameters are extracted from the period of oscillation and the decay rate. QCMs make use of oscillator circuits, ring-down and impedance analysis.

MODE OF OPERATION In impedance analysis, the electric conductance as a function of driving frequency is determined by means of a network analyzer. By fitting a resonance curve to the conductance curve, one obtains the frequency and bandwidth of the resonance as fit parameters.

Ellipsometry Ellipsometry is a method that enables the determination of the optical properties of surfaces. The principle of this method is based on the change in polarization state of light reflected from the surface of a sample.

Experimental Setup Electromagnetic radiation is emitted by a light source and linearly polarized by a polarizer. After reflection the radiation passes a compensator (optional) and a second polarizer, which is called analyzer, and falls into the detector.

Theory Ellipsometry measures the ratio of rs and rp, which is described by the fundamental equation of ellipsometry: tanΨ is the amplitude ratio upon reflection, and Δ is the phase shift. Ψ and Δ values are calculated using the Fresnel equations.

Advantages of Ellipsometry It measures the ratio of two values so is highly accurate and reproducible, does not need a reference sample, and is not so susceptible to light source fluctutation Since it measures phase, it is highly sensitive to the presence of ultrathin films (down to submonolayer coverage). It provides two pieces of data at each wavelength. More film properties can be determined.

Types of Ellipsometer Ellipsometers may be single wavelength or spectroscopic They may be single- or multiple- angle of incidence They may operate as rotating element or as nulling ellipsometers They may be single point or imaging

Spectroscopic Ellipsometer SOPRA GESP5 SOPRA variable angle spectroscopic ellipsometer GESP5

Rotating polariser ellipsometer