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International School of Physics 'Enrico Fermi' ;.
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Table of Contents
- Title Page
- Contents
- Preface
- Course group shot
- Science in tumultuous times
- Introduction
- 1. The years of the First World War (1914-1918)
- 2. Post-War years (1919-1921)
- 3. Quantum mechanics (the 1920s)
- 4. Exile (1933)
- 5. The atom bomb (1945)
- 6. The Nobel Prize (1954)
- 7. Conclusion (1970)
- Appendix A
- Appendix B
- But God does play dice: The path to quantum mechanics
- Introduction
- 1. Breslau, Germany (now Wroclaw, Poland)
- 2. Gottingen
- 3. Frankfurt
- 4. Gottingen again
- 5. America
- 6. Gottingen
- From the Bohr model to Heisenberg's quantum mechanics
- 1. Introduction
- 2. From Balmer to Bohr
- 3. The Bohr model between success and failure
- 4. Heisenberg's path from classical physics to quantum mechanics
- 4.1. Action integral in Fourier space
- 4.2. Extension to an arbitrary frequency spectrum
- 4.3. The appearance of non-commuting quantities
- 5. Quantization of the linear harmonic oscillator
- 6. Light at the end of the tunnel
- The linearity of quantum mechanics and the birth of the Schrodinger equation
- 1. Introduction
- 1.1. Linearization of the non-linear wave equation
- 1.2. Key ideas of our previous approaches
- 1.3. Outline
- 2. Road towards the Schrodinger equation
- 3. Comparison with the literature
- 4. Why zero?
- 4.1. A curious mathematical identity
- 4.2. Definition of a quantum wave by its amplitude
- 4.3. Formulation of the problem
- 5. Classical mechanics guides the amplitude of the Schrodinger wave
- 5.1. Hamilton-Jacobi theory in a nutshell
- 5.2. Classical action as a phase field
- 6. Quantum condition implies linear Schrodinger equation
- 6.1. Emergence of a quantum phase
- 6.2. Continuity equation with quantum current
- 6.3. Quantum Hamilton-Jacobi equation
- 7. Classicality condition implies non-linear wave equation
- 7.1. General real amplitude
- 7.2. Amplitude given by Van Vleck determinant
- 7.2.1. Super-classical waves
- 7.2.2. Super-classical waves are WKB waves
- 8. From Van Vleck via Rosen to Schrodinger
- 8.1. The need for linearity
- 8.2. Linearization due to quantum current
- 9. Summary and outlook
- Appendix A. Van Vleck continuity equation
- Appendix A.1. One-dimensional case
- Appendix A.1.1. Derivation of continuity equation
- Appendix A.1.2. Explicit expressions for density and current from action
- Appendix A.1.3. Density and current from continuity equation
- Appendix A.2. Multi-dimensional case
- Appendix A.3. Differential of a determinant
- Appendix A.1. One-dimensional case
- Appendix B. Non-linear wave equation for WKB wave
- 1. Introduction
- Wave phenomena and wave equations
- 1. Preludium
- 2. Water waves
- 2.1. Wave equation for water waves
- 3. Matter wave
- 3.1. Wave equation for matter wave
- 4. Final remark
- 5. Further readings
- History leading to Bell's inequality and experiments
- 1. Introduction
- 2. Early history
- 3. The beginnings of quantum mechanics
- 4. Bell Inequalities
- 5. Initial experiments
- Sewing Greenberger-Horne-Zeilinger states with a quantum zipper
- 1. Introduction
- 2. Mechanism
- 3. Implementation
- Quantum state generation via frequency combs
- 1. Optical quantum state preparation
- 2. Quantum frequency combs from bulk-based systems
- 3. Integrated quantum frequency combs
- 4. Conclusion
- Time after time: From EPR to Wigner's friend and quantum eraser
- 1. Introduction
- 2. The Einstein-Podolsky-Rosen (EPR) problem
- 3. Of Wigner and Wigner's friends
- 4. Quantum eraser and the Mohrhoff conundrum
- 5. Summary
- QBism: Quantum theory as a hero's handbook
- 1. Introduction
- 2. Exactly how quantum states fail to exist
- 3. Teleportation
- 4. The meaning of no-cloning
- 5. The essence of Bell's theorem, QBism style
- 6. The quantum de Finetti theorem
- 7. Seeking SICs - The Born rule as fundamental
- 8. Mathematical intermezzo: The sporadic SICs
- 9. Hilbert-space dimension as a universal capacity
- 10. Quantum cosmology from the inside
- 11. The future
- Information-theoretic derivation of free quantum field theory
- 1. Introduction
- 2. Derivation from principles of the quantum-walk theory
- 2.1. The quantum system: qubit, fermion or boson?
- 2.2. Quantum walks on Cayley graphs
- 2.2.1. The homogeneity principle
- 2.2.2. The locality principle
- 2.2.3. The isotropy principle
- 2.2.4. The unitarity principle
- 2.3. Restriction to Euclidean emergent space
- 2.3.1. Geometric group theory
- 3. Quantum walks on Abelian groups and free QFT as their relativistic regime
- 3.1. Induced representation, and reduction from virtually-Abelian to Abelian quantum walks
- 3.2. Isotropy and orthogonal embedding in R3
- 3.3. Quantum walks with Abelian G
- 3.4. Dispersion relation
- 3.5. The relativistic regime
- 3.6. Schrodinger equation for the ultra-relativistic regime
- 3.7. Recovering the Weyl equation
- 3.8. Recovering the Dirac equation
- 3.8.1. Discriminability between quantum walk and quantum field dynamics
- 3.8.2. Mass and proper-time
- 3.8.3. Physical dimensions and scales for mass and discreteness
- 3.9. Recovering Maxwell fields
- 3.9.1. Photons made of pairs of fermions
- 3.9.2. Vacuum dispersion
- 4. Recovering special relativity in a discrete quantum universe
- 4.1. Quantum-digital Poincare group and the notion of particle
- 4.2. De Sitter group for non-vanishing mass
- 5. Conclusions and future perspectives: the interacting theory, ..., gravity?
- Revealing quantum properties with simple measurements
- 1. Introduction
- 2. Wave-particle duality
- 2.1. Wave-particle duality: an inequality
- 2.1.1. Distinguishability
- 2.1.2. Visibility
- 2.1.3. The wave-particle inequality
- 2.2. Simultaneous measurements
- 2.3. Higher-order wave-particle duality
- 2.3.1. Higher-order distinguishability
- 2.3.2. Higher-order visibility
- 2.3.3. Higher-order wave-particle duality
- 2.4. Duality and entanglement
- 2.1. Wave-particle duality: an inequality
- 3. Entanglement
- 3.1. Bipartite entanglement
- 3.1.1. Schmidt decomposition
- 3.1.2. The positive partial transpose criterion
- 3.1.3. Detecting entanglement with the help of the Cauchy-Schwarz inequality
- 3.2. Tripartite entanglement
- 3.3. Multipartite entanglement
- 3.4. The spatial distribution of entanglement
- 3.1. Bipartite entanglement
- 4. Conclusion
- Appendix A. Proof of eq. (49)
- Complementarity and light modes
- 1. Introduction
- 2. Spontaneous parametric down-conversion (SPDC) as a tool
- 3. Induced coherence in the 3-crystal set up
- 4. Stimulated coherence
- 5. Complementarity in the spatial dimension
- 6. Complementarity for single photons in higher-order spatial modes
- 7. Conclusion
- Quantum imaging
- 1. What is quantum imaging?
- 2. Brief history of quantum methods in metrology
- 3. Parametric downconversion and the generation of entangled photons
- 4. What is ghost imaging and what are its properties?
- 5. Interaction-free imaging
- 6. Imaging by Mandel's induced coherence
- 7. Technology for quantum imaging
- 8. Summary and discussion
- Spekkens' toy model and contextuality as a resource in quantum computation
- 1. Spekkens' toy model
- 2. Contextuality
- 3. Restricting SM as a subtheory of QM
- Casimir forces in spherically symmetric dielectric media
- 1. Introduction
- The spherical problem
- 2. Renormalization and Lifshitz theory
- 3. Results
- The strange roles of proper time and mass in physics
- 1. Mass: The role it plays, and the role it ought to play
- 2. Proper time: The role it plays, and the role it ought to play
- 3. The equivalence principle and the extended equivalence principle
- 3.1. Stable particles: The equivalence principle
- 3.2. Unstable particles: The extended equivalence principle
- 4. Incorporating mass and proper time as dynamical variables
- 5. An extended Lorentz transformation and Schrodinger equation
- Some consequences of mass and proper time as dynamical variables
- 1. The Lorentz transformation and the Galilean transformation
- 1.1. The Bargmann theorem in non-relativistic physics
- 1.2. The problem with the Bargmann theorem
- 2. The mass-proper time uncertainty relation
- 3. The classical limit of the equivalence principle
- 3.1. The strange mass scaling in phase space
- 4. The different correspondence principles for gravity and non-gravity forces: matrix elements in the classical limit
- 1. The Lorentz transformation and the Galilean transformation
- Atom interferometry and its applications
- 1. Introduction
- 1.1. Applications of atom interferometry
- 1.2. Optical elements for atoms
- 1.3. Sources for atom optics
- 1.4. Overview
- 2. Tools of atom interferometry
- 2.1. Beam splitters and mirrors
- 2.1.1. Rabi oscillations and two-photon coupling
- 2.1.2. Bragg and Raman diffraction
- 2.1.3. Multi-photon coupling by Bragg diffraction
- 2.1.4. Influence of atom cloud and beam size
- 2.2. Optical lattices
- 2.2.1. Bloch theorem
- 2.2.2. Bloch oscillations
- 2.2.3. Landau-Zener transitions
- 2.3. Mach-Zehnder interferometer for gravity measurements
- 2.3.1. Set-up
- 2.3.2. Contributions to phase shift
- 2.3.3. Influence of non-zero pulse duration
- 2.3.4. Measurement of gravitational acceleration
- 2.1. Beam splitters and mirrors
- 3. Equivalence principle and atom interferometry
- 3.1. Frameworks for tests of the universality of free fall
- 3.2. Simultaneous 87Rb and 39K interferometer
- 3.3. Data analysis and result
- 4. Atom-chip-based BEC interferometry
- 4.1. Delta-kick collimation
- 4.2. Quantum tiltmeter based on double Bragg diffraction
- 4.2.1. Rabi oscillations
- 4.2.2. Tilt measurements
- 4.3. Sensitive atom-chip gravimeter on a compact baseline
- 4.3.1. Relaunch of atoms in a retro-reflected optical lattice
- 4.3.2. Experimental sequence of the atom-chip gravimeter
- 4.3.3. Analysis of the interferometer output
- 5. Outlook
- 5.1. Reduced systematic uncertainties in future devices
- 5.2. Very long baseline atom interferometry
- 5.3. Space-borne atom interferometers
- 1. Introduction
- Atom-chip-based quantum gravimetry with BECs
- 1. Introduction
- 2. Atom-chip-based gravimeter prototype in QUANTUS-1
- 3. Next generation quantum gravimeter QG-1 for mobile applications
- Gravitational properties of light
- List of participants
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