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Introduction to Nanophotonics [Kõva köide]

(Full Professor, Institut d'Optique, Université Paris-Saclay), (CNRS Research Director, Laboratoire Photonique, Numérique et Nanosciences), (Full Professor, Institut d'Optique, Université Paris-Saclay)
  • Formaat: Hardback, 670 pages, kõrgus x laius x paksus: 253x174x33 mm, kaal: 1352 g, 211 line diagrams and colour halftones
  • Sari: Oxford Graduate Texts
  • Ilmumisaeg: 12-Apr-2022
  • Kirjastus: Oxford University Press
  • ISBN-10: 0198786131
  • ISBN-13: 9780198786139
Teised raamatud teemal:
Introduction to NanophotonicsSuurem pilt
  • Formaat: Hardback, 670 pages, kõrgus x laius x paksus: 253x174x33 mm, kaal: 1352 g, 211 line diagrams and colour halftones
  • Sari: Oxford Graduate Texts
  • Ilmumisaeg: 12-Apr-2022
  • Kirjastus: Oxford University Press
  • ISBN-10: 0198786131
  • ISBN-13: 9780198786139
Teised raamatud teemal:
Püsilink: https://www.kriso.ee/db/9780198786139.html
Märksõnad:
The aim of this textbook is to provide an overview of nanophotonics, a discipline which was developed around the turn of the millennium. This unique and rapidly evolving subject area is the result of a collaboration between various scientific communities working on different aspects of
light-matter interaction at the nanoscale. These include near-field optics and super-resolution microscopy, photonic crystals, diffractive optics, plasmonics, optoelectronics, synthesis of metallic and semiconductor nanoparticles, two-dimensional materials, and metamaterials.

The book is aimed at graduate students with a background in physics, electrical engineering, material science, or chemistry, as well as lecturers and researchers working within these fields.

Arvustused

The last decade has seen a true revolution in the field of nanophotonics. This textbook provides a comprehensive overview at an introductory level, written by three eminent figures in the field. It will be invaluable to students and researchers alike. * Andrea Alù, City University of New York * Introduction to Nanophotonics is more than a treatise on photons and electrons being lost on tiny metallic islands or in a jungle of nano-structured materials; the authors discuss numerous useful configurations while ensuring the reader does not lose sight of the underlying principles, including an unprecedentedly clear description of the role of plasmons. * Dieter Pohl, University of Basel * This is a comprehensive, unified account of the subject of nanophotonics written by highly respected members of the optics and solid-state physics communities. * Mark Fox, University of Sheffield * Written by leading authorities working at the cutting edge of the field, this textbook is a uniquely comprehensive, coherent, and rigorous introduction to nanophotonics. * Lucio Andreani, University of Pavia *

PART I BASICS OF ELECTROMAGNETIC OPTICS
1 Basics of electrodynamics of continuous media
3(24)
1.1 Microscopic Maxwell equations
3(2)
1.2 Potentials
5(3)
1.3 Macroscopic Maxwell equations
8(6)
1.4 Energy conservation
14(2)
1.5 Reciprocity theorem
16(4)
1.6 Radiation, propagation, scattering, and diffraction
20(1)
1.A Complement: Temporal coherence and spectral analysis of light (stationary random electromagnetic fields)
21(6)
Exercises
24(3)
2 Radiation
27(22)
2.1 Green function: Electrostatic potential produced by a point-like charge
28(2)
2.2 Retarded potentials
30(2)
2.3 Far-field radiation
32(8)
2.4 Antennas: Basic concepts
40(4)
2.A Complement: Derivation of the Green function of the propagation equation
44(5)
Exercises
45(4)
3 Electrodynamics in material media: Constitutive relations
49(30)
3.1 Introduction
49(1)
3.2 General properties of constitutive relations
50(2)
3.3 Current density and polarization: Is it the same?
52(2)
3.4 Energy in material media
54(1)
3.5 Absorption in material media
55(1)
3.6 Permittivity of a gas: Lorentz-Lorenz model
56(2)
3.7 Local-field correction
58(1)
3.8 Permittivity of an electron gas: The Drude model
59(2)
3.9 Permittivity of a polar liquid: Orientation polarization
61(1)
3.10 Permittivity of an ionic crystal: The Lyddane-Sachs-Teller relation
61(1)
3.11 Kramers-Kronig relations
62(3)
3.A Complement: Microscopic interpretation of absorption
65(1)
3.B Complement: Light-matter interaction in metals: Physical mechanisms
66(4)
3.C Complement: Hydrodynamic model of the permittivity of an electron gas: Non-local effects
70(1)
3.D Complement: Non-local effects: Beyond the hydrodynamic model
71(8)
Exercises
75(4)
4 Propagation
79(28)
4.1 Propagation in vacuum: Angular spectrum
79(5)
4.2 The Huygens-Fresnel principle revisited
84(2)
4.3 Propagation equation in homogeneous non-dispersive media
86(1)
4.4 Propagation in homogeneous dispersive media and the Helmholtz equation
87(2)
4.5 Mode of the Helmholtz equation in a homogeneous medium
89(2)
4.6 3D propagation in a lossy medium
91(1)
4.7 Quasinormal modes of uniform media
92(1)
4.8 Group, phase, and energy velocity
92(5)
4.A Complement: Weyl expansion
97(1)
4.B Complement: Choice of the square-root solution
97(1)
4.C Complement: Modes of the propagation equation in a lossy homogeneous medium
98(9)
Exercises
102(5)
5 Reflection and refraction at an interface
107(24)
5.1 Introduction
107(1)
5.2 Continuity conditions
108(2)
5.3 Snell's laws
110(1)
5.4 Reflection factor and TE polarization
111(4)
5.5 Intensity reflection factor
115(2)
5.6 Normal incidence
117(3)
5.7 Angle dependence of the Fresnel factors
120(1)
5.A Complement: Energy conservation at an interface
121(2)
5.B Complement: Scattering by a slightly rough surface and perturbative treatment
123(8)
Exercises
125(6)
6 Guided modes
131(28)
6.1 Introduction to guided modes
131(4)
6.2 The slab waveguide
135(7)
6.3 Mode orthogonality
142(3)
6.A Complement: Pairs of counter-propagating modes for reciprocal materials
145(1)
6.B Complement: Equivalence between the group and energy velocities in lossless waveguides
146(2)
6.C Complement: Mode orthogonality in lossy/amplifying waveguides and radiation mode treatment
148(1)
6.D Complement: Metal-insulator-metal waveguides with perfect metals: TE modes
149(2)
6.E Complement: Application example: The multimode interferometer
151(8)
Exercises
153(6)
7 Basics of resonators and cavities
159(40)
7.1 Introduction
159(1)
7.2 Overview of micro- and nanoresonators
160(2)
7.3 Modes in conservative and non-conservative contexts
162(3)
7.4 Quasinormal modes of Fabry-Perot resonators
165(5)
7.5 Cavity Q's and V's
170(4)
7.6 Resonant external excitation
174(3)
7.7 Critical coupling of a single resonator
177(1)
7.8 Coupled-mode theory
178(6)
7.A Complement: LDOS and quasinormal modes
184(3)
7.B Complement: The Fabry-Perot cavity and the finesse
187(4)
7.C Complement: Coupled-mode theories: Spatial vs temporal
191(8)
Exercises
192(7)
PART II OPTICAL PROPERTIES OF CONFINED ELECTRONS
8 Semiconductors and quantum wells
199(46)
8.1 From wavefunctions to band formation
200(3)
8.2 Bands and carriers
203(7)
8.3 Photoluminescence basics for direct bandgap configuration
210(8)
8.4 Photopumping and relaxation processes
218(3)
8.5 The double heterojunction (DH)
221(3)
8.6 Quantum well
224(6)
8.7 Laser threshold
230(7)
8.A Complement: Band structure of zinc-blende materials
237(1)
8.B Complement: Absorption beyond the basic sharp-band-edge picture
237(2)
8.C Complement: Silicon optical properties
239(6)
Exercises
240(5)
9 More confined electrons: Quantum dots and quantum wires
245(30)
9.1 Electronic description of quantum dots (QDs) and quantum wires
245(10)
9.2 Self-organized QDs
255(4)
9.3 Nanocrystals and colloidal QDs
259(5)
9.A Complement: Growth of epitaxial InAs QDs
264(3)
9.B Complement: Silicon-related nanostructures in photonics
267(8)
Exercises
268(7)
PART III ADVANCED CONCEPTS IN NANOPHOTONICS
10 Fundamental concepts of near-field optics
275(16)
10.1 Field confinement
275(3)
10.2 Radiation in the near field
278(4)
10.3 The quasi-electrostatic and quasi-magnetostatic fields
282(2)
10.4 Revisiting simple concepts in the near field
284(3)
10.5 Energy confinement in the near field
287(4)
Exercises
288(3)
11 Introduction to superresolution optical imaging
291(20)
11.1 Imaging and resolution
291(2)
11.2 Principles of near-field scanning optical microscopy (NSOM)
293(4)
11.3 Modelling the signal of a near-field optical microscope: What is imaged by a scanning tip?
297(2)
11.4 Superresolution in the far field: Inverse problem and structured illumination
299(4)
11.5 Superresolution in the far field: Localizing sparse markers with subwavelength accuracy
303(4)
11.6 Generating highly localized light spots with superoscillations
307(4)
Exercises
308(3)
12 Scattering, Green tensor, and local density of electromagnetic states
311(38)
12.1 The Green tensor and integral formulation of electromagnetism
311(6)
12.2 Far-field approximation: Scattering matrix
317(3)
12.3 Optical theorem
320(1)
12.4 Scattering by a particle
321(5)
12.5 Local density of states
326(6)
12.A Complement: Derivation of the integral equation
332(2)
12.B Complement: Green tensor in layered systems
334(3)
12.C Complement: Density of states, optical etendue, energy flux, second principle, and spatial coherence
337(2)
12.D Complement: Local electric and magnetic density of electromag-netic states
339(10)
Exercises
344(5)
PART IV PLASMONICS
13 Propagating surface plasmons
349(38)
13.1 Surface and particle electron oscillation modes: Introductory examples
350(3)
13.2 Bulk plasmon
353(2)
13.3 Surface electromagnetic wave
355(3)
13.4 SPPs
358(9)
13.5 Gap SPPs
367(8)
13.6 Graphene surface plasmons
375(1)
13.7 Surface phonon polaritons
376(1)
13.8 Surface plasmon contributions to the LDOS
377(3)
13.A Complement: Surface plasmon excited by an electric dipole
380(1)
13.B Complement: Surface plasmon launched by an isolated slit
381(6)
Exercises
383(4)
14 Localized surface plasmons
387(22)
14.1 Introduction
387(1)
14.2 A tutorial example: Metallic nanosphere
388(6)
14.3 Controlling particle modes
394(3)
14.4 Field enhancement
397(2)
14.5 Ultrafast dynamics of nanoparticles
399(1)
14.A Complement: Universal bounds of the absorption and scattering cross section of lossy and non-lossy dipolar scatterers
400(2)
14.B Complement: Radiative decay time, superradiance, and the Chu-Wheeler limit
402(7)
Exercises
403(6)
PART V ARTIFICIAL MEDIA: PHOTONIC CRYSTALS AND METAMATERIALS
15 Propagation in periodic media (I): Bloch modes and homogenization
409(28)
15.1 Thin-film stack: Effective index
410(4)
15.2 Periodic thin-film stacks with small periods
414(8)
15.3 Grating equation
422(2)
15.4 Homogenization of subwavelength gratings
424(5)
15.A Complement: Homogenization of disordered composites
429(8)
Exercises
431(6)
16 Propagation in periodic media (II): Photonic crystals
437(32)
16.1 Bandgap opening and bands: Qualitative discussion
438(4)
16.2 Coupled-wave method
442(3)
16.3 Semi-infinite and finite cases: Penetration depth and Bloch-mode resonances
445(5)
16.4 Structural slow light
450(1)
16.5 2D photonic crystals
451(12)
16.A Complement: 3D photonic crystals
463(1)
16.B Complement: Photonic-crystal fibres
464(5)
Exercises
466(3)
17 Periodic waveguide
469(32)
17.1 Waveguide and periodicity
469(10)
17.2 Periodic waveguiding geometries and effective index descriptions
479(5)
17.3 The resonant waveguide grating
484(4)
17.4 Longitudinal waveguide confinement: Cavities
488(4)
17.A Complement: Light extraction from guided modes in various LEDs
492(2)
17.B Complement: Fundamentals of the guided Bloch mode
494(7)
Exercises
497(4)
18 Metamaterials and metasurfaces
501(40)
18.1 Introduction: The ideas behind `meta'
501(1)
18.2 Metamaterials with a negative index
502(8)
18.3 Hyperbolic metamaterials and superresolution
510(3)
18.4 Dielectric metasurfaces
513(6)
18.5 Plasmonic metasurfaces
519(7)
18.6 Surface waves and surface modes on metal surfaces
526(15)
Exercises
532(9)
PART VI CONFINED PHOTONS: NANOANTENNAS, MICROCAVITIES, AND OPTOELECTRONIC DEVICES
19 Controlling light-matter interaction at the nanoscale with cavities and nanoantennas
541(32)
19.1 Introduction
541(1)
19.2 Spontaneous emission
542(6)
19.3 Controlling the spontaneous decay rate by modifying the environment
548(10)
19.4 Enhanced Raman scattering
558(1)
19.5 Fluorescence in the stationary regime
559(3)
19.6 Controlling the fluorescence spectrum of broad spectrum emitters
562(1)
19.7 Controlling angular pattern and polarization emission
563(1)
19.8 Plasmonic antenna design rules for light emission
563(1)
19.9 Nanoantenna impedance: Optimizing absorption
564(5)
19.A Complement: Fluorescence in the impulse regime
569(4)
Exercises
570(3)
20 From nanophotonics to devices
573(32)
20.1 Passive, active, and emitting devices
573(1)
20.2 Index sensing with confined waves
574(9)
20.3 Selected IO: passive and electro-optic devices
583(2)
20.4 Active devices and their multiple-efficiency definitions
585(2)
20.5 Stimulated emission: Laser diodes
587(6)
20.6 Other surface-emitting lasers
593(2)
20.7 Spontaneous emission devices
595(10)
Exercises
600(5)
PART VII FLUCTUATIONAL ELECTRODYNAMICS
21 Fluctuational electrodynamics
605(22)
21.1 Introduction
605(5)
21.2 Harnessing black-body radiation with metasurfaces
610(6)
21.3 Radiative heat transfer at the nanoscale
616(7)
21.A Complement: Spatial coherence
623(4)
Exercises
624(3)
References 627(18)
Index 645
Henri Benisty received his PhD in electrochemistry in 1989 in Paris, working on the photonics of semiconductor integrated optics devices and LEDs enhanced with microcavities and two-dimensional photonic crystals, with the aim to improve either light confinement or light extraction. He is the co-founder of the French startup Genewave (now merged with Finnish Mobidiag), which works on fluorescence biochips. He has contributed to studies of sensors featuring a resonant waveguide grating response in various contexts and was instrumental to introducing the the idea of plasmonic losses within the recently introduced topic of parity-time symmetry in optics.

Jean-Jacques Greffet is an alumnus of the Ecole Normale Supérieure de Paris-Saclay. He received his PhD in solid state physics in 1988 from Université Paris-Sud working in light scattering by rough surfaces. Between 1994 and 2005, he worked on the theory of image formation in near-field optics. Since 1998, he has made a number of seminal contributions to the field of thermal radiation at the nanoscale including the demonstration of coherent thermal sources and the prediction and measurement of giant radiative heat transfer at the nanoscale due to surface phonon polaritons. Since 2000, he has contributed to the field of quantum plasmonics and light emission with nanoantennas and metasurfaces.

Philippe Lalanne is an alumnus of the Ecole Normale Supérieure de St Cloud. Currently, he is a CNRS researcher working at Bordeaux University. He is an expert in nanoscale electrodynamics, with an emphasis on modelling and theory. His current research is devoted to understanding how light interacts with subwavelength structures to demonstrate novel optical functionalities. He has launched new modal theories and has pioneered the development of large-NA metalenses with high-index nanostructures in the 1990s.