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International School of Physics "Enrico Fermi". Nanoscale quantum optics: proceedings of the International School of Physics "Enrico Fermi" course 204, Varenna on Lake Como, Villa Monastero, 23-28 July 2018 = Ottica quantistica a livello nanoscopico : rendiconti della Scuola internazionale di fisica "Enrico Fermi" CCIV corso, Varenna sul Lago di Como, Villa Monatero, 23-28 Luglio 2018 / edited by M. Agio, I D'Amico, and R. Zia, directors of the course and C. Toninelli. — Amsterdam: IOS Press, 2020. — 1 online resource : illustrations. — (Proceedings of the International School of Physics Enrico Fermi). — In English, includes parallel title page in Italian. — <URL:http://elib.fa.ru/ebsco/2664477.pdf>.Дата создания записи: 04.11.2020 Тематика: Quantum optics — Congresses.; Nanoscience — Congresses.; Quantum optics. Коллекции: EBSCO Разрешенные действия: –
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Оглавление
- Title Page
- Contents
- M. Agio, I. D'Amico, R. Zia and C. Toninelli - Preface
- Course group shot
- Irene D'Amico - Basic concepts for quantum optics and quantum technologies
- 1. Introduction
- 2. Quantization of the electromagnetic field and Fock states
- 2.1. Classical field, plane wave
- 2.2. Generic classical field
- 2.3. Quantization of the electromagnetic field
- 2.4. Fock states and their properties
- 3. Coherent states
- 3.1. Coherence in classical light
- 3.2. Quadrature operators and Fock states in the quadrature space
- 3.3. Coherent states and their properties
- 3.4. Coherent states and the displacement operator
- 4. Quadrature operators in quantum optics
- 4.1. Examples of visualization of quantum states of light
- 4.2. Squeezed states
- 5. Elementary building blocks for quantum technologies: quantum bits and quantum gates
- 6. Quantum entanglement
- 6.1. Entangled and unentangled states
- 6.2. Entanglement in systems with multiple degrees of freedom
- 6.3. Entanglement and Bell's inequality
- 7. "Spin chains" as eclectic quantum buses
- 8. The density operator
- 8.1. Why do we need a density operator?
- 8.2. Ensembles of quantum states: mixed and pure states
- 8.3. Characterization of a density operator
- 8.4. Separable mixed states
- Nathalie P. de Leon - Materials for quantum nanophotonics
- 1. Desiderata for applications in quantum nano-optics
- 1.1. Single-photon sources
- 1.2. Using quantum systems to control light
- 1.3. Quantum networks
- 1.4. Enhanced collection effciency from a quantum system
- 2. Examples of physical systems
- 2.1. Quantum dots
- 2.2. Shallow donors
- 2.3. Defects and impurities
- 3. Optical coherence and interactions with the environment
- 4. Spin coherence and interactions with the environment
- 4.1. Dephasing
- 4.2. Decoherence
- 4.3. Spin-lattice relaxation
- 5. Prospects for quantum technologies
- 1. Desiderata for applications in quantum nano-optics
- Rahul Trivedi, Daniil Lukin and Jelena Vuckovic - Quantum optics and nonclassical light generation
- 1. Quantum description of electromagnetic fields
- 1.1. Lossless cavities: Systems with discrete modes
- 1.2. Single-mode waveguide: System with a continuum of modes
- 1.3. Model for lossy cavities
- 2. Light-matter interaction
- 2.1. Interaction Hamiltonian
- 2.2. Two-level systems interacting with an optical continuum
- 2.3. Cavity quantum electrodynamics
- 3. Single-photon sources
- 3.1. Characterizing the quality of single-photon sources
- 3.2. Two-time correlation measurements
- 3.3. Solid-state implementation of single-photon sources
- 3.3.1. Quantum dots
- 3.3.2. Color centers
- AppendixA. Lindblad master equation
- AppendixB. Mollow transformation
- AppendixC. Decay of a two-level system into a lossy cavity mode
- AppendixD. Analysis of interferometers
- AppendixD.1. Linear optical elements in loss channels
- AppendixD.2. Analysis of Hanbury-Brown Twiss and Hong-Ou Mandel interferometers
- 1. Quantum description of electromagnetic fields
- M. Atature - Creating quantum correlations between quantum-dot spins
- 1. Proximity and quantum correlations
- 2. Optically active semiconductor quantum dots
- 2.1. Essential properties
- 2.2. QD spin devices
- 3. Measurement-based creation of quantum correlations
- 3.1. Entanglement concept
- 3.2. Experimental realisation
- 4. Outlook
- E. Polino, N. Spagnolo, F. Sciarrino, G. Corrielli, A. Crespi and R. Osellame - Platforms for telecom entangled photon sources
- 1. Introduction
- 2. Platforms for telecom entangled photons sources
- 2.1. SPDC sources
- 2.2. SFWM sources
- 2.3. Other sources
- 3. Femtosecond Laser Writing Technique for integrated source of telecom entangled states
- 3.1. FLW technique
- 3.2. FLW for fully integrated source of telecom entangled states
- 4. Conclusions
- Lee C. Bassett - Quantum optics with single spins
- 1. Introduction
- 2. Electronic structure of the diamond nitrogen-vacancy center
- 2.1. The electronic Hamiltonian
- 2.2. Low- and high-strain regimes
- 3. Coherent light-matter coupling
- 3.1. The Jaynes-Cummings Hamiltonian
- 3.2. The Faraday and optical Stark effects
- 3.3. Discussion and implications
- 4. All-optical coherent spin control
- 4.1. Dark states and coherent population trapping
- 4.2. Forming a Lambda system from the NV center
- 4.3. All-optical initialization, control, and readout
- 5. Ultrafast control
- 5.1. Quantum control with ultrafast optical pulses
- 5.2. Applications
- 6. Conclusions and future directions
- Friedemann Reinhard - Nanoscale sensing and quantum coherence
- 1. Introduction
- 2. Single molecules and spins as scanning probes
- 3. Sensing by quantum coherence -reaching the fundamental limit of sensitivity
- 3.1. Quantum coherence as a sensor
- 3.2. Creating and reading out quantum coherence -the Ramsey protocol
- 3.3. Decoherence and the fundamental limit to sensitivity
- 4. Sensing by dynamical decoupling -the hidden revolution
- 5. Outlook -prospects and hopes after one decade
- Jirawat Tangpanitanon and Dimitris G. Angelakis - Many-body physics and quantum simulations with strongly interacting photons
- 1. Introduction
- 1.1. Computer simulation
- 1.2. Quantum simulation
- 1.3. Platforms for quantum simulation
- 1.3.1. Cold neutral atoms in optical lattices
- 1.3.2. Trapped ions
- 1.3.3. Solid-state systems
- 1.3.4. Interacting photons
- 1.3.5. Conclusions
- 2. Quantum phase transitions
- 2.1. Example: the Mott-to-superfluid phase transition
- 2.2. The mean-field phase diagram
- 3. Quantum many-body phases of light
- 3.1. Light-matter interaction
- 3.1.1. Field quantization: mode of a simple optical resonator
- 3.1.2. The Jaynes-Cummings interaction
- 3.1.3. Eigenstates of the Jaynes-Cummings model
- 3.1.4. Early experimental realizations of strong light-matter coupling
- 3.1.5. Photon blockade effect
- 3.1.6. Quantum nonlinear optics with atomic ensembles
- 3.2. Mott-to-superfluid transition of light in coupled resonator arrays
- 3.2.1. The mean-field phase diagram
- 3.2.2. Existing works on equilibrium many-body phases of interacting photons
- 3.2.3. State-of-the-art experiments
- 3.3. Driven-dissipative many-body phases of interacting photons
- 3.1. Light-matter interaction
- 4. Strongly interacting photons from superconducting circuits
- 4.1. Microwave photons from an LC circuit
- 4.2. A Kerr resonator from a transmon qubit
- 4.3. Different types of superconducting qubits
- 4.4. Nonlinear lattices from arrays of coupled transmon qubits
- 4.4.1. The Bose-Hubbard model
- 4.4.2. The Jaynes-Cummings Hubbard model
- 5. Conclusions and future aspects
- 1. Introduction
- Ewold Verhagen - Nano-optomechanics
- 1. Introduction: coupling light and motion
- 1.1. The canonical cavity optomechanical resonator
- 2. Quantum measurements of motion with light
- 2.1. Measuring motion with a cavity
- 2.2. Mechanical frequency response
- 2.3. Mechanical fluctuation spectra and sidebands
- 2.4. Imprecision and backaction; the Standard Quantum Limit
- 3. A quantum optical description of cavity optomechanics
- 3.1. The optomechanical Hamiltonian
- 3.2. The linearized Hamiltonian
- 4. Optomechanical cooling and state transfer
- 4.1. The resolved sideband regime
- 4.2. Cooling rate and engineered reservoir
- 5. Controlling photons and phonons
- 5.1. Optomechanically-induced transparency and cooperativity
- 5.2. Beyond single-mode interactions
- 5.3. Beyond reciprocity
- 5.4. Beyond linearity
- 6. Conclusions
- 1. Introduction: coupling light and motion
- M. Colautti, G. Mazzamuto, F. S. Cataliotti, P. Lombardi, S. Pazzagli, A. P. Ovvyan, N. Gruhler, W. H. P. Pernice, G. Kewes, O. Neitzke, O. Benson and C. Toninelli - Photostable molecules on chip: a scalable approach to photonic quantum technologies
- 1. Introduction
- 2. Evanescent coupling of single molecules to a nearby dielectric waveguide
- 2.1. Single-molecule quantum emitters
- 2.2. Design and fabrication of the hybrid photonic chip
- 2.3. Experimental results
- 3. Conclusions
- S. Hernandez-Gomez, F. Poggiali, N. Fabbri and P. Cappellaro - Environment spectroscopy with an NV center in diamond
- 1. Introduction
- 2. Effect of the environment on the NV center
- 2.1. Spectroscopy method
- 2.2. Predictive power of the characterization
- 3. Conclusions
- S. Tarrago Velez and Christophe Galland - Ultrafast photonic quantum correlations mediated by individual phonons
- 1. Description
- 2. Experimental method
- 3. Results
- 4. Conclusion
- List of participants
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