
Applications and Metrology at Nanometer-Scale 2
Description
Alles über E-Books | Antworten auf Fragen rund um E-Books, Kopierschutz und Dateiformate finden Sie in unserem Info- & Hilfebereich.
sources of disruptive innovation that open up new fields of application.
Quantum engineering enables the development of very sensitive
materials, sensor measurement systems and computers. Quantum
computing, which is based on two-level systems, makes it possible to
manufacture computers with high computational power.
This book provides essential knowledge and culminates with an industrial
application of quantum engineering and nanotechnologies. It presents
optical systems for measuring at the nanoscale, as well as quantum
physics models that describe how a two-state system interacts with its
environment. The concept of spin and its derivation from the Dirac
equation is also explored, while theoretical foundations and example
applications aid in understanding how a quantum gate works. Application
of the reliability-based design optimization (RBDO) method of mechanical
structures is implemented, in order to ensure reliability of estimates from
the measurement of mechanical properties of carbon nanotube
structures.
This book provides valuable support for teachers and researchers but is
also intended for engineering students, working engineers and Master s
students.
More details
Other editions
Additional editions

Persons
Simulation and Engineering at the University of Versailles Saint-Quentin
in France. He is Director of Institut des Sciences et Techniques des
Yvelines and a specialist in modeling and spectroscopy at the LATMOS
laboratory of the CNRS.
Philippe Pougnet is a former expert in reliability and the technologyproduct-process of embedded mechatronic systems. He graduated from
Universite Grenoble Alpes and Grenoble INP in France.
Abdelkhalak El Hami is Professor at the Institut National des Sciences
Appliquees (INSA-Rouen Normandie) in France and is in charge of the
Normandy Conservatoire National des Arts et Metiers (CNAM) Chair of
Mechanics, as well as several European pedagogical projects.
Content
Introduction xiii
Chapter 1. Measurement Systems Using Polarized Light 1
1.1. Introduction 1
1.2. Matrix optics 2
1.3. Photon emission and detection 12
1.4. Application exercises on interferometry 16
1.4.1. Propagation of electromagnetic waves in a Fabry-Pérot cavity 18
1.4.2. Propagation of electromagnetic waves in a material 19
1.4.3. Interferometry and optical lambda meter 21
1.4.4. The homodyne interferometer and refractometer 34
1.4.5. The heterodyne interferometer 40
1.4.6. Application exercises on ellipsometry 51
1.5. Appendices 56
1.5.1. Conventions used for Jones vectors and Jones ABCD matrices 56
1.5.2. 2×2 transfer dies 59
1.5.3. 2×2 matrix multiplication 59
1.5.4. Trigonometric forms 60
1.5.5. Solution by MATLAB (exercises 1.4.3, 1.4.4 and 1.4.5) 61
1.6. Conclusion 66
Chapter 2. Quantum-scale Interaction 67
2.1. Introduction 67
2.2. The spin through the Dirac equation 69
2.2.1. Theoretical background 69
2.2.2. Application: the Dirac equation and Pauli matrices 74
2.3. The density matrix for a two-level laser system 105
2.3.1. Definition of the density matrix 106
2.3.2. Density matrix properties 110
2.3.3. Equation of motion of the density matrix 113
2.3.4. Application to a two-level system 116
2.4. Ising's phenomenological model for cooperative effects 123
2.4.1. The Ising 1D model 124
Chapter 3. Quantum Optics and Quantum Computers 135
3.1. Introduction 135
3.2. Polarized light in quantum mechanics 136
3.3. Introduction to quantum computers 140
3.4. Preparing a qubit 158
3.4.1. Application of the Bloch sphere 158
3.5. Application: interaction of a qubit with a classical field 172
3.5.1. Answer to question 1 173
3.5.2. Answer to question 2 176
3.6. Applying Ramsey fringes to evaluate the duration of phase coherence 181
3.6.1. Answer to question 1 181
3.6.2. Answer to question 2 183
Chapter 4. Reliability-based Design Optimization of Structures 185
4.1. Introduction 185
4.2. Deterministic optimization 186
4.3. Reliability analysis 187
4.3.1. Optimal conditions 189
4.4. Reliability-based design optimization 191
4.4.1. The objective function 192
4.4.2. Taking into account the total cost 192
4.4.3. Design variables 193
4.4.4. Response of a system by RBDO 193
4.4.5. Limit states 194
4.4.6. Solving methods 194
4.5. Applications 194
4.5.1. Application on a bending beam 194
4.5.2. Application on a circular plate with different thicknesses 196
4.5.3. Application: hook A 201
4.5.4. Application: optimization of the materials of an electronic board 211
4.6. Reliability-based design optimization in nanotechnology 222
4.6.1. Thin-film SWCNT structures 222
4.6.2. Digital model of thin-film SWCNT structures 224
4.6.3. Numerical results 225
4.7. Conclusion 231
Appendix 233
References 237
Index 245
Introduction
The scientific study of measurement is known as metrology. Any measure is based on a universally accepted standard and any measuring process is prone to uncertainty. In engineering science, measurement concerns various types of parameters. Legal metrology is imposed by a regulatory framework that the manufactured product must respect. Technical or scientific metrology involves the methods used to measure the technical characteristics of the manufactured product. In engineering sciences, measurement concerns various types of parameters. In a more general context of a systemic approach, metrology should also be considered in connection with other indicators of the production system. These measures enable the follow-up and development of the processes implemented for ensuring and optimizing product quality or reducing failure so that it meets client expectations. The ability of a product to meet quality and reliability expectations can be addressed in the design stage, according to a RBDO (Reliability-Based Design Optimization) approach described in Volume 2 of the Reliability of Multiphysical Systems Set, entitled Nanometer-scale Defect Detection Using Polarized Light. More generally, RBDO makes it possible to consider the uncertain parameters of manufacturing processes, measurement and operational conditions in order to optimize the manufacturing process, the design parameters and the overall quality of the product.
Nanometer-scale Defect Detection Using Polarized Light focused on three levels of design for manufacturing an industrial product:
- - Numerical methods developed in engineering from mathematical models and theories in order to optimize product quality from its design according to RBDO. This methodology is a source of applications in engineering science intended to address optimization problems in the industrial field.
- - Experimental methods developed in fundamental research relying on the light-matter interaction and on simulation-based analysis using theoretical models in order to make nanometer-scale measurements and conduct the analysis. These methods are used in nanosciences for the elaboration of knowledge leading to nanotechnologies.
- - Finally, the application of these two approaches in the example presented in Chapter 9 of Nanometer-scale Defect Detection Using Polarized Light to the measurement of the physical properties of a nanomaterial, carbon nanotube.
In sciences, there are various ways to measure a dimension. The measuring instruments or methods employed depend on the scale at which metrology is approached. In order to describe the issues at stake for measurement at a given scale, we present the methods employed for the measurement processes at two scales of interest for scientists, namely the infinitely small, which corresponds to the Planck length of 1.6 x 10-35 m, and the infinitely large, which corresponds to the diameter of the Universe evaluated at 8.8 x 1026 m. This is to help the reader understand that, even though becoming an expert in a scientific field or in a given subject is not the objective, it is necessary to understand some basic tenets in order to master the methods used for successful metrology at a given scale.
In 1899, Planck determined a unit of length , referred to as Planck length, based on fundamental constants: G, gravitational constant (6.6 x 10-11 Nm2 Kg-2), h, Planck's constant (6.64 x 10-34 Js) and c, the speed of light (2.99,729,458 x 108 ms-1). This length cannot be measured with the measurement technologies available on Earth. Indeed, the smallest length measurable at the LHC (Large Hadron Collider) of CERN, the particle accelerator in which two protons are made to frontally collide in a ring of 26,659 km, which led to the discovery in 2012 of the Higgs boson, is approximately 10-16 m, which is 19 orders of magnitude higher than the Planck length. CMS and ATLAS detectors were used in the observation of the Higgs boson, the latest prediction of the standard model not yet observed. The measurement at the scale of 10-16 m is made by compressing energy to reach an infinitely small spatial volume.
The principle of measurement at the scale of fundamental particles is mainly based on three relations: the de Broglie relation between the momentum p and the wavelength ?, p=h/?, which introduces the wave-particle duality for matter; the relation that links the energy E of a particle to its wave frequency or wavelength ?, such as proposed by Einstein to explain the photoelectric effect E = hc/?; and the relation that links the energy E of a particle of rest mass m to its rest mass energy and to its kinetic energy associated with its momentum p=mv, E2= m2c4 + p2c2, as mentioned in Einstein's special theory of relativity. In the above formulas, v is the speed of the particle of mass m and c is the speed of light. The energy E can also be expressed by the formula E= ?mc2, where ? is given by . The speed of a particle is therefore given by .
In the LHC, the energy of a proton is 7 TeV (1.2 10-6 J), far higher (by a factor of 7,500) than its rest energy, mc2, which is 938 MeV. The formula for speed can then be rewritten as v/c = (1-(m2c4/2E2)), which is equal to 1 to the nearest 10-8. Using the relation E= hc/?, the resulting value of the wavelength is of the order of 10-16 m, which gives the dimensions that can be reached in the LHC. The mass measured during two experiments at CERN in the LHC (8 TeV in 2012 and 13 TeV in 2015) is confirmed to the value of 125 GeV.
To detect the Higgs boson, a particle of mass 125 GeV associated with the Higgs field, while the mass of a proton is 938 MeV, the proton is accelerated and consequently its kinetic energy is increased so that its energy given by E= ?mc2 significantly exceeds 938 MeV (8 TeV in 2012 and 13 TeV in 2015). The disintegration of colliding protons, each contributing an energy load of 8 TeV or 13 TeV, releases sufficient energy so that the Higgs boson can be expected to emerge during the recombination of subatomic particles. As the Higgs boson decays quasi-instantaneously after its emergence, the products of its decay must be analyzed to identify the excess energy and therefore the excess mass about 125 GeV.
It is worth noting that at the Planck length, the required energies that cannot be expected in a particle accelerator would lead to the emergence of black holes.
The opposite dimensional extreme towards the infinitely large corresponds to the spatial extent of the Universe, whose estimated value according to cosmologists is 1026 m. In cosmology, the observable Universe is a term used to describe the visible part of our Universe, the point from which light reaches us. It is a sphere whose limit is located at the cosmological horizon, having the Earth at its center. It is therefore a relative notion, as for other observers located somewhere else in the Universe, the observable sphere would not be the same (while its radius would be identical).
In cosmology, distances are measured in light-years. A light-year is the distance that light travels in one year, which corresponds to approximately 9.5 x 1012 m. The megaparsec, which is 3.26 million (3.26 x 106) light-years, is another unit of distance that is also specific to extragalactic astrophysics. Finding the size of the Universe involves accurate measurements of fossil radiation, or of the cosmic microwave background (CMB) radiation that originated in the Big Bang and can be used to determine the volume filled by the Universe since its creation. Predicted for the first time by Ralph Alpher in 1948 in his thesis work, CMB was discovered by Arno Penzias and Robert Wilson at "Bell Telephone Laboratories" during the development of a new radio receiver following the interferences detected independently of the orientation of the antenna they were building. While in a first approximation CMB is isotropic, accurate measurements of this radiation lead to determining H0, the Hubble constant, which indicates the rate of expansion of the Universe.
In cosmology, detectors are above-ground telescopes. The WMAP (Wilkinson Microwave Anisotropy Probe) satellite launched in 2001 enabled the detection of CMB with good accuracy. Its intensity varies slightly in different directions of the sky and the fluctuations can be determined. Extremely accurate measurements of the WMAP in 2003 made it possible to calculate a value of H0 of 70 kilometers per second and per megaparsec, which is within 5% in the hypothesis of a constant rate of expansion. Since the Universe is accelerating, during its expansion, the correction brought to H0 made it possible to estimate the age of the Universe to 13.75 billion years, with a 0.1 billion margin of error. It is the scale fitting the domain to which corresponds the age of the Universe deduced from observations related to the Big Bang based on the inflationary model in an expanding Universe.
After the Big Bang, the elementary subatomic particles had no mass and could travel at the speed of light. After the expansion of the Universe and its cooling, the particles interacted with the Higgs field and consequently gained a mass.
In the history of the Universe, the elementary particles interacted with the Higgs field, 10-12 s after the Big Bang. The value of 125 GeV is considered as the critical value between a stable universe and a metastable universe. The "standard model...
System requirements
File format: ePUB
Copy protection: Adobe-DRM (Digital Rights Management)
System requirements:
- Computer (Windows; MacOS X; Linux): Install the free reader Adobe Digital Editions prior to download (see eBook Help).
- Tablet/smartphone (Android; iOS): Install the free app Adobe Digital Editions or the app PocketBook before downloading (see eBook Help).
- E-reader: Bookeen, Kobo, Pocketbook, Sony, Tolino and many more (not Kindle).
The file format ePub works well for novels and non-fiction books – i.e., „flowing” text without complex layout. On an e-reader or smartphone, line and page breaks automatically adjust to fit the small displays.
This eBook uses Adobe-DRM, a „hard” copy protection. If the necessary requirements are not met, unfortunately you will not be able to open the eBook. You will therefore need to prepare your reading hardware before downloading.
Please note: We strongly recommend that you authorise using your personal Adobe ID after installation of any reading software.
For more information, see our ebook Help page.