Modules  Area  Type  Hours  Teacher(s)  
QUANTUM LIQUIDS  FIS/03  LEZIONI  54 

Quantum Liquids è un corso per il Dottorato in Fisica, mutuato per la LM in Fisica (versione da 9 CFU e da 6 CFU), e per la LT in Materials and Nanotechnologies (6 CFU). Si tiene a cavallo tra il primo e il secondo semestre, a partire da Novembre del primo semestre.
Obiettivi di apprendimento. Al termine dell’insegnamento, la/lo studente avrà sviluppato le conoscenze concettuali, procedurali e fattuali nella fisica dei liquidi quantistici all’equilibrio (modulo da 6 CFU) e dei sistemi quantistici aperti drivendissipative (modulo da 3 CFU), e loro ingegnerizzazione come simulatori quantistici in piattaforme attuali di tecnologie quantistiche. In particolare:
(a) Metodi teorici avanzati per predire e caratterizzare la fisica di liquidi quantistici all’equilibrio, loro relazione con metodi di simulazione quantistica, e classificazione per funzionalità e tipologie di problemi. Tra i metodi: risposta lineare, idrodinamica quantistica, funzionale di densità e di corrente, funzioni di Green e metodi non perturbativi, bosonizzazione.
(b) Metodi teorici e numerici per sistemi quantistici fuori dall’equilibrio e drivendissipative: sistemi Markoviani e non Markoviani, dissipation engineering, simulazione quantistica con metodi stocastici e tensor networks, misura e feedback, e applicazioni a tecnologie quantistiche, chimica e biologia quantistiche.
(c) Principi di funzionamento delle principali piattaforme di tecnologie quantistiche: atomi, atomi dipolari e di Rydberg, ioni ultrafreddi, atomi in cavità QED; circuiti a superconduttore; fluidi di luce in cavità ottiche; sistemi a bassa dimensionalità. Loro uso come simulatori quantistici per materia condensata, fisica fondamentale, metrologia quantistica, gravità analoga, e cosmologia.
Quantum Liquids is a PhD course in Physics, borrowed for the LM in Physics (9 CFU), and for the LT in Materials and Nanotechnologies (6 CFU). It is held between the first and second semesters, starting from November of the first semester.
At the end of the course, the student/student will have developed conceptual, procedural and factual knowledge in the physics of quantum liquids at equilibrium (6 CFU module) and of open drivendissipative quantum systems (3 CFU module) and their engineering as quantum simulators in current quantum technology platforms. In particular:
(a) Advanced theoretical methods to predict and characterize the physics of quantum liquids at equilibrium, their relationship to quantum simulation methods, and their classification by functionality and problem types. Among the methods: linear response, quantum hydrodynamics, functional density and current, Green functions and nonperturbative methods, bosonization.
(b) Theoretical and simulational methods for outofequilibrium and drivendissipative quantum systems: Markovian and nonMarkovian systems, dissipative engineering, simulation through stochastic methods and tensor networks, measurement and feedback, and applications to quantum technologies, quantum chemistry and biology.
(c) Principles of operation of the main platforms of quantum technologies: atoms, dipolar and Rydberg atoms, ultracold ions, atoms in QED cavities; superconducting circuits; light fluids in optical cavities; low dimensional systems. Their use as quantum simulators for condensed matter, fundamental physics, quantum metrology, analogous gravity, and cosmology.
La verifica è realizzata discutendo in una prova orale una dissertazione su un problema di fisica dei liquidi quantistici tra quelli non specificamente discussi nel corso e che faccia uso delle conoscenze e dei metodi teorici sviluppati durante il corso.
The assessment is performed by oral discussion of an essay on problem in the physics of quantum liquids, selected among those that have not specifically treated within the course and that uses understanding and methods developed in the course.
Al termine dell’insegnamento lo/a studente avrà appreso a
Riconoscere l'emergere delle proprietà macroscopiche nella complessità dei modelli microscopici che descrivono i liquidi quantistici all’equilibrio e drivendissipative.
Formalizzare i concetti e imparare ad affrontarli con i metodi sviluppati.
Collegare la conoscenza concettuale e la formalizzazione con la fenomenologia e le applicazioni.
Organizzare la conoscenza disciplinare in una mappa concettuale che include campi come termodinamica, meccanica statistica e transizioni di fase, teorie di campo.
Valutare criticamente articoli di ricerca specializzati.
Progettare descrizioni teoriche per il comportamento dei liquidi quantici in diverse piattaforme sperimentali.
Comunicare in modo efficace ed efficiente.
Lavorare con autonomia, consapevolezza e capacità di autovalutazione.
Sviluppare capacità di lavoro di squadra.
At the end of the course, the student will have learned to
La verifica è realizzata discutendo in una prova orale una dissertazione individuale e  in modo facoltativo  un lavoro di gruppo.
La dissertazione individuale è su un problema di fisica dei liquidi quantistici tra quelli non specificamente discussi nel corso e che faccia uso delle conoscenze e dei metodi teorici sviluppati durante il corso. Si richiede alla/o studente di individuare il problema oggetto della dissertazione:
La verifica individuale è concepita in modo da valutare lo stato delle conoscenze dello/a studente, e di sviluppo di competenze nelle seguenti aree:
(a) aver compreso idee e concetti e saperli comunicare utilizzando conoscenze di fisica di base;
(b) saper formalizzare i concetti e saperli trattare attraverso l'uso di uno o più tra i metodi sviluppati nel corso e relative procedure;
(c) saper connettere la comprensione concettuale e la formalizzazione del problema con la fenomenologia e i fatti sperimentali disponibili, e avere un'idea delle applicazioni;
(d) autonomia, consapevolezza della mappa concettuale e di quanto appreso, efficacia ed efficienza nella comunicazione scientifica.
Il lavoro di gruppo è su un problema pratico relativo all’applicazione di idee e metodi appresi nel corso in una particolare piattaforma sperimentale per le tecnologie quantistiche – concordata con gli e le studenti. Il problema viene discusso in gruppo in una apposita sessione di esame utilizzando tecniche del teambased learning (questa sessione avrà luogo alla fine del corso). Si richiede di discutere la metodologia più funzionale di trattamento, sviluppare la comprensione del problema, e comunicare i risultati, conducendo le diverse attività attraverso una suddivisione di compiti, condivisione dei risultati, e gestione autonoma del gruppo.
The assessment is performed by oral discussion of an essay on problem in the physics of quantum liquids, selected among those that have not specifically treated within the course and that uses understanding and methods developed in the course. The student is required to identify the essay subject:
The individual testing is conceived to assess the development of student’s knowledge and competences in the following areas:
(a) understand ideas and concepts and be able to communicate them also after using basic physics tools (besides advanced);
(b) be able to express concepts in formal manner and manage them via the methods developed during the course, along with the corresponding procedures;
(c) be able to connect the conceptual understanding of the problem and its formal expression with the phenomenology and experimental fact that are available, and envision possible applications;
(d) autonomy, awareness of the course conceptual map and of the learning outcomes, effectiveness and efficiency in scientific communication.
The group work is conceived to be on practical problem related to the application of ideas and methods learned during the course to either one among the different experimental platforms for quantum technologies. The problem will be selected by the students with the supervision of the lecturer. The problem will be discussed within the participating group in an onpurpose examination session operated by means of teambased learning techniques (this session will take place at the end of the course). It is required to discuss the methodology that is best suited to the problem, develop the comprehension of the problem, communicate the results, conduct the different activities by distributing the different assignments among the group members, sharing the results, and managing the group in autonomy.
Ci si attende che la/lo studente sviluppi:
(a) Interesse per le idee a fondamento della scienza e tecnologie quantistiche
(b) Curiosità e spirito critico
(c) Spirito di iniziativa e partecipazione attiva
(d) Correttezza al momento della valutazione
It is expected that the student will develop:
La verifica del comportamenti viene operata in aula nel corso e in sede di prova d’esame mediante osservazione, e mediante possibili attività di valutazione formativa in itinere sul portale elearning.
The behaviors’ evaluation is performed during classroom activities and at the assessment time via observation, and by means of possible activities of formative evaluation on the elearning portal.
Prerequisito è la conoscenza di base di dinamica, termodinamica ed elementi di meccanica statistica, elettromagnetismo, struttura della materia e meccanica quantistica acquisiti nel corso di studi triennale. Utili sebbene non indispensabili sono conoscenze di fisica dei solidi.
Prerequisite is the basic knowledge of classical dynamics, thermodynamics and elements of statistical mechanics, electromagnetism, structure of matter, quantum physics.
Very useful and preferable, though not compulsory, is the knowledge of solidstate physics
Le attività d’aula e online sono disegnate attorno agli obiettivi di apprendimento. In particolare:
(a) discutere qualitativamente mediante la fisica di base le idee emergenti da fatti sperimentali ed esempi di vita quotidiana, approfondendo all'occorrenza metodi sperimentali e possibili applicazioni, anche utilizzando slides e spezzoni di seminari di esperti/e qualificati disponibii online ;
(b) formalizzare i concetti (conoscenza concettuale);
(c) ovunque possibile discutere il problema complesso attraverso semplici modelli che usano la fisica di base;
(d) sviluppare e classificare la conoscenza di metodi teorici e di simulazione per le predizioni quantitative (conoscenza procedurale e fattuale), avendo cura di sviluppare alla lavagna tutti i passaggi per ogni tipologia di calcolo;
(e) al termine di ogni macroargomento, costruire in modo interattivo una mappa concettuale che lo rappresenta, evidenziando concetti e relazioni tra questi;
(f) l’ultima parte del corso è dedicata a studi di casi in differenti piattaforme per le tecnologie quantistiche, allo scopo di acquisire pratica d'applicazione della conoscenza procedurale e fattuale
Classroom and online activities are tailored on the expected learning outcomes. In particular:
The course is composed of two modules: 6 CFU on equilibrium systems (Marilù Chiofalo) and 3 CFU on open quantum systems (Jorge Yago Malo), amounting to 54 hours. PhD students can make their own selection of topics, amounting to the planned 40 hours.
0. Introduction to the course: conceptual map of the essential ideas qualitatively discussed via examples anticipated from the course itself
A. Theoretical Methods for strongly correlated quantum fluids at equilibrium
[LMPhysics course: 38 h. PhD course: 20 h]
In this part A, the theoretical concepts and methods are developed for equilibrium systems, starting from the measurement of correlation functions which are first phenomenologically introduced in A1. The relationships among the different methods are discussed, highlighting goods and bads. The methods will be first developed in A2 for systems with maximal symmetry and then, after bridging in A3 with a crash dictionary on broken symmetries and quantum phase transitions, completed in A4 by introducing their peculiarities in correspondence of phase transitions driven by tuning interactions strength, disorder, temperature, and dimensionality. During the development of the formal tools, care will be taken to establish and discuss links between the learned theoretical methods and simulational/numerical methods on one side and experimental methods on the other, with examples from different spectroscopies (matter, spin, and optical probes) and from transport measurements.
A1. Measurements and correlation functions [4 h]
Generalities and essential concepts. Measurements and Correlation functions, response functions, quantum hydrodynamics via a simple model.
A2. Systems with maximal symmetry [LM course: 24h. PhD course: 16 h]
Only for PhD course: choose either A2.1 or A2.2
A2.1 Formal development of the Theory of Linear Response: Definitions and properties Fluctuation Dissipation Theorem  Sum rules  Applications: calculation of response functions within the RandomPhase Approximation (fermions and bosons)  Concept of local field factor and self.consistent theories beyond meanfield. Dictionary between response functions and Green’s functions methods [8 h]
A2.2 Correlation functions and Green's functions (zero and finite temperature): Definitions and properties  Boundary conditions  Equations of motion as a technique to derive consistent approximations  Nonequilibrium Green's functions  A dictionary with response functions  Generating functionals  Wick's theorem  Finite temperature and the contourintegral method  Perturbative techniques and Feynman diagrams  Examples including phonon and fermion systems to loworder – Methods based on selfconsistent integral equations. Dictionary between response functions and Green’s functions methods [8 h]
A2.3 Landau Fermi and Bose liquids [2 h]
A2.4 Quantum Hydrodynamics: Microscopic derivation of the equations starting from conservation laws  Transport coefficients as special limits of response functions and Kubo relations Static susceptibilities as thermodynamic derivatives of conserved quantities. Relationship with Linear Response. Relationship with experiments: LandauPlaczek ratio and examples. [6 h]
A2.5 A crash dictionary of (TimeDependent) Density Functional Theory (only upon request from students): Definitions  Theorem of Hohenberg and Kohn  Kohn and Sham scheme  Local Density Approximation  Exchange and correlation potentials and relationship with linear response theory – Hints on current functionals and TDDFT, relationship with Linear Response and microscopic formulation of NavierStokes equations. [2 h]
A3. Systems with broken symmetries [10 h]
A3.0 A crash dictionary on broken symmetries and (quantum) phase transitions
Concept of order parameter Landau and LandauGinzburg theory for uniform (Ising model) and nonuniform order parameter – Complex order parameter and neutral/charged superfluid – Introduction to the concepts of scaling, critical exponents and universality Dynamical effects: AndersonHiggs mechanism and Goldstone modes  Analogy between superconductivity and electroweak theory Conditions of validity for meanfield theories and thermal and quantum (as e.g. due to correlations and reduced dimensionality) fluctuations. [2h]
A3.1 Superfluidity/superconductivity and BoseEinstein Condensation of neutral and charged Fermi and Bose systems
Application of the theory of linear response to the microscopic calculation of the superfluid density/moment of inertia and the relationship between superfluid and condensate fraction – Peculiarities in hydrodynamic treatment and microscopic twofluid equations – Peculiarities in the Green's functions treatment: Ward identities and conserving vs. gapless approximations. [6h]
Of the following A4.2 and A4.3, only one will be treated – choosing in accord with the class.
A3.2 Effects of reduced dimensionality: the very special 1D case
Specialty of 1D systems: always strongly correlated and collectivization of excitations. Luttinger Liquids: structure and thermodynamic properties. Typical phase diagrams in 1D systems with Charge/density and SpinDensity Waves. Essentials on bosonization techniques. [2h]
A3.3 Effects of disorder and quantum transport in 1D
Transport properties of quantum fluids  Diagrammatic analysis and phenomenology  Quenched Green's functions  Scattering against disordered impurities – [Drude conductivity  Diffusion corrections]  Quantum corrections  Effect of dimensionality and quantum transport in 2D and 1D  AALK argument and Anderson localization Universal conductance – Concept of manybody localization. [2h]
B. Theoretical and numerical methods for outofequilibrium and drivendissipative quantum systems [6h]
After introducing the tools in B1, newly sprouting paradigmatic phenomena of manybody quantum matter physics are discussed in B2B4, that can be accessed within an open quantum system treatment, conceptually different than those occurring in equilibrium systems, and that are especially relevant for the engineering of quantum technologies.
B1. Tools for open quantum systems: Drivendissipative quantum systems. Reservoir engineering. Describing dissipation in quantum systems: GoriniKossakowskiSudarshanLindblad master equation. Stochastic unraveling description of open quantum systems. Quantum state diffusion. Beyond the BornMarkov approximation and nonMarkovian systems. Description via Tensor Networks. Matrix Product States and Operators: concepts and algorithms. Beyond 1D.
B2. Periodicallydriven systems: Floquet engineering
B3. Measurement, control, and feedback in Open Quantum Systems
B4. Dynamical phase transitions
C. Applications with quantum technologies [14 h]
The theoretical tools developed in A and B are now used to discuss in C0 their implementation to engineer quantum simulators in different quantumtechnology platforms: quantum gases (including dipolar and Rydberg atoms), trapped ions, superconducting circuits, matter in optical cavities, fluids of light. In C1C5 then, selected applications are discussed of phenomena that are simulated by coding their describing (microscopic or paradigmatic) theoretical Hamiltonian into these experimental quantum simulators, in what we can consider a new type of cooperation between theory and experiment in the scientific thinking process. The selection will be decided with the students within a participatory process.
C0. The basic toolboxes: 2or3 level systems, interactions, gauge fields, and dimensionality, qubits and addressing methods, in the following quantum technologies platforms: quantum gases and trapped ions, superconducting circuits, matter and optical cavities, fluids of light [6 h].
C1. Condensed matter physics: BCSBEC crossover, and its applications also beyond condensedmatter physics. Commensurateincommensurate phase transitions. Eigenstate thermalisation hypothesis (ETH) and Anderson/Many body localization. [2 h]
C2. Fundamental physics: Tests on the electric dipole moment. Lattice gauge field theories. Ultracompact stars and quark matter. Tests of the foundations of quantum mechanics: collapse models, DiosìPenrose theory, time in quantum mechanics [2 h]
C3. Cosmology and astrophysics. Gravity and general relativity tests by atom interferometry and atomic clocks: measurement of big G, variation of fundamental constants, equivalence principle tests. Detection of gravitational waves and quest for ultralight dark matter. Quantum simulators for gravity and cosmology problems by analogue gravity: analogue horizons and Hawking radiation, informationloss paradox, viscositytoentropy ration at black holes horizons [2h].
C4. Quantum simulators for biology and chemistry: Quantumlike paradigm and complex networks for biology applications  Transport and quantum effects in biology [2h]
The course is composed of two modules: 6 CFU on equilibrium systems (Marilù Chiofalo) and 3 CFU on open quantum systems (Jorge Yago Malo), amounting to 54 hours. PhD students can make their own selection of topics, amounting to the planned 40 hours.
0. Introduction to the course: conceptual map of the essential ideas qualitatively discussed via examples anticipated from the course itself
A. Theoretical Methods for strongly correlated quantum fluids at equilibrium
[LMPhysics course: 38 h. PhD course: 20 h]
In this part A, the theoretical concepts and methods are developed for equilibrium systems, starting from the measurement of correlation functions which are first phenomenologically introduced in A1. The relationships among the different methods are discussed, highlighting goods and bads. The methods will be first developed in A2 for systems with maximal symmetry and then, after bridging in A3 with a crash dictionary on broken symmetries and quantum phase transitions, completed in A4 by introducing their peculiarities in correspondence of phase transitions driven by tuning interactions strength, disorder, temperature, and dimensionality. During the development of the formal tools, care will be taken to establish and discuss links between the learned theoretical methods and simulational/numerical methods on one side and experimental methods on the other, with examples from different spectroscopies (matter, spin, and optical probes) and from transport measurements.
A1. Measurements and correlation functions [4 h]
Generalities and essential concepts. Measurements and Correlation functions, response functions, quantum hydrodynamics via a simple model.
A2. Systems with maximal symmetry [LM course: 24h. PhD course: 16 h]
Only for PhD course: choose either A2.1 or A2.2
A2.1 Formal development of the Theory of Linear Response: Definitions and properties Fluctuation Dissipation Theorem  Sum rules  Applications: calculation of response functions within the RandomPhase Approximation (fermions and bosons)  Concept of local field factor and self.consistent theories beyond meanfield. Dictionary between response functions and Green’s functions methods [8 h]
A2.2 Correlation functions and Green's functions (zero and finite temperature): Definitions and properties  Boundary conditions  Equations of motion as a technique to derive consistent approximations  Nonequilibrium Green's functions  A dictionary with response functions  Generating functionals  Wick's theorem  Finite temperature and the contourintegral method  Perturbative techniques and Feynman diagrams  Examples including phonon and fermion systems to loworder – Methods based on selfconsistent integral equations. Dictionary between response functions and Green’s functions methods [8 h]
A2.3 Landau Fermi and Bose liquids [2 h]
A2.4 Quantum Hydrodynamics: Microscopic derivation of the equations starting from conservation laws  Transport coefficients as special limits of response functions and Kubo relations Static susceptibilities as thermodynamic derivatives of conserved quantities. Relationship with Linear Response. Relationship with experiments: LandauPlaczek ratio and examples. [6 h]
A2.5 A crash dictionary of (TimeDependent) Density Functional Theory (only upon request from students): Definitions  Theorem of Hohenberg and Kohn  Kohn and Sham scheme  Local Density Approximation  Exchange and correlation potentials and relationship with linear response theory – Hints on current functionals and TDDFT, relationship with Linear Response and microscopic formulation of NavierStokes equations. [2 h]
A3. Systems with broken symmetries [10 h]
A3.0 A crash dictionary on broken symmetries and (quantum) phase transitions
Concept of order parameter Landau and LandauGinzburg theory for uniform (Ising model) and nonuniform order parameter – Complex order parameter and neutral/charged superfluid – Introduction to the concepts of scaling, critical exponents and universality Dynamical effects: AndersonHiggs mechanism and Goldstone modes  Analogy between superconductivity and electroweak theory Conditions of validity for meanfield theories and thermal and quantum (as e.g. due to correlations and reduced dimensionality) fluctuations. [2h]
A3.1 Superfluidity/superconductivity and BoseEinstein Condensation of neutral and charged Fermi and Bose systems
Application of the theory of linear response to the microscopic calculation of the superfluid density/moment of inertia and the relationship between superfluid and condensate fraction – Peculiarities in hydrodynamic treatment and microscopic twofluid equations – Peculiarities in the Green's functions treatment: Ward identities and conserving vs. gapless approximations. [6h]
Of the following A4.2 and A4.3, only one will be treated – choosing in accord with the class.
A3.2 Effects of reduced dimensionality: the very special 1D case
Specialty of 1D systems: always strongly correlated and collectivization of excitations. Luttinger Liquids: structure and thermodynamic properties. Typical phase diagrams in 1D systems with Charge/density and SpinDensity Waves. Essentials on bosonization techniques. [2h]
A3.3 Effects of disorder and quantum transport in 1D
Transport properties of quantum fluids  Diagrammatic analysis and phenomenology  Quenched Green's functions  Scattering against disordered impurities – [Drude conductivity  Diffusion corrections]  Quantum corrections  Effect of dimensionality and quantum transport in 2D and 1D  AALK argument and Anderson localization Universal conductance – Concept of manybody localization. [2h]
B. Theoretical and numerical methods for outofequilibrium and drivendissipative quantum systems [6h]
After introducing the tools in B1, newly sprouting paradigmatic phenomena of manybody quantum matter physics are discussed in B2B4, that can be accessed within an open quantum system treatment, conceptually different than those occurring in equilibrium systems, and that are especially relevant for the engineering of quantum technologies.
B1. Tools for open quantum systems: Drivendissipative quantum systems. Reservoir engineering. Describing dissipation in quantum systems: GoriniKossakowskiSudarshanLindblad master equation. Stochastic unraveling description of open quantum systems. Quantum state diffusion. Beyond the BornMarkov approximation and nonMarkovian systems. Description via Tensor Networks. Matrix Product States and Operators: concepts and algorithms. Beyond 1D.
B2. Periodicallydriven systems: Floquet engineering
B3. Measurement, control, and feedback in Open Quantum Systems
B4. Dynamical phase transitions
C. Applications with quantum technologies [14 h]
The theoretical tools developed in A and B are now used to discuss in C0 their implementation to engineer quantum simulators in different quantumtechnology platforms: quantum gases (including dipolar and Rydberg atoms), trapped ions, superconducting circuits, matter in optical cavities, fluids of light. In C1C5 then, selected applications are discussed of phenomena that are simulated by coding their describing (microscopic or paradigmatic) theoretical Hamiltonian into these experimental quantum simulators, in what we can consider a new type of cooperation between theory and experiment in the scientific thinking process. The selection will be decided with the students within a participatory process.
C0. The basic toolboxes: 2or3 level systems, interactions, gauge fields, and dimensionality, qubits and addressing methods, in the following quantum technologies platforms: quantum gases and trapped ions, superconducting circuits, matter and optical cavities, fluids of light [6 h].
C1. Condensed matter physics: BCSBEC crossover, and its applications also beyond condensedmatter physics. Commensurateincommensurate phase transitions. Eigenstate thermalisation hypothesis (ETH) and Anderson/Many body localization. [2 h]
C2. Fundamental physics: Tests on the electric dipole moment. Lattice gauge field theories. Ultracompact stars and quark matter. Tests of the foundations of quantum mechanics: collapse models, DiosìPenrose theory, time in quantum mechanics [2 h]
C3. Cosmology and astrophysics. Gravity and general relativity tests by atom interferometry and atomic clocks: measurement of big G, variation of fundamental constants, equivalence principle tests. Detection of gravitational waves and quest for ultralight dark matter. Quantum simulators for gravity and cosmology problems by analogue gravity: analogue horizons and Hawking radiation, informationloss paradox, viscositytoentropy ration at black holes horizons [2h].
C4. Quantum simulators for biology and chemistry: Quantumlike paradigm and complex networks for biology applications  Transport and quantum effects in biology [2h].
Note:
Generali:
– P.C. Martin, Measurements and Correlation Functions, Gordon and Breach (1968) [Con riferimento al Programma: Parte B]
 G. Giuliani and G. Vignale, Quantum Theory of the Electron Liquid, Cambridge University Press (2010) [Con riferimento al Programma: Parte C1]
 Piers Coleman, Introduction to ManyBody Physics, Cambridge University Press (2015) [Con riferimento al Programma: Parte C2 e C3]
 L.P. Kadanoff and G. Baym, Quantum Statistical Mechanics, Benjamin (1962) [Con riferimento al Programma: Parte C1 Nonequilibrium methods]
– Baym, Microscopic Description of Superfluidity, Math. Methods in SolidState&Superfluid Theory, Clark&Derrick Eds., Oliver&Boyd (1969) [Con riferimento al Programma: Parte C4]
– P.C. Hohenberg and P.C. Martin, Microscopic Theory of Superfluid Helium, Annals of Physics 34, 291359 (1965) [Con riferimento al Programma: Parte C4]
– Giamarchi, Quantum Physics in One Dimension, Oxford Science Pub. (2006) [Con riferimento al Programma: Parte C5]
 G. Iadonisi, G. Cantele, and M.L. Chiofalo, Introduction to Solid State Physics and Crystalline Nanostructures, Springer (2014) [Con riferimento al Programma: Background in solidstate physics]
 M. L. Chiofalo, L. Salvi, G. Tino, La Fisica della Materia, in Lezioni di Fisica, Corriere della Sera (2018) [Overview semidivulgativa sulle quantum technologies]
5.2 Parti specifiche del corso (materiale facoltativo, in aggiunta alle note di lezione disponibili sul portale)
– G. Vignale, C. A Ullrich, S. Conti, TimeDependent Density Functional Theory and beyond the Adiabatic Local Density Approximation, Phys. Rev. Lett. 79, 4878 (1997)
 A. Daley, Quantum trajectories and open manybody quantum systems, Adv. Phys. 63, 77 (2014)
Altre letture, per studenti particolarmente interessati/e:
– P. Nozières and D. Pines, Theory of Quantum Liquids I – II, Westview Press (1999); Pines, The ManyBody Problem, Wiley (1997)
– D. Forster, Hydrodynamic Fluctuations, Broken Symmetry, And Correlation Functions, Adv. Books Classics (1995)
– W.M. Foulkes, L. Mitas, R.J. Needs, and G. Rajagopal, Quantum Monte Carlo Simulations of Solids, Revue of Modern Physics 73, 33 (2001)
– U. Schollwok and S.R. White, Methods for Time Dependence in DMRG, in Effective Models for LowDimensional Strongly Correlated Systems, G.G. Batrouni and D. Poilblanc Eds., p. 155 AIP, Melville, New York (2006)
– L. A. Bloomfield, How Things Work, Wiley (2013)
Please check with the UNIPI library on the availability of the suggested textbooks and articles.
Notes:
5.1 General:
– P.C. Martin, Measurements and Correlation Functions, Gordon and Breach (1968) [Referring to Programme: Part B]
 G. Giuliani and G. Vignale, Quantum Theory of the Electron Liquid, Cambridge University Press (2010) [Referring to Programme: Part C1]
 Piers Coleman, Introduction to ManyBody Physics, Cambridge University Press (2015) [Referring to Programme: Parts C2 and C3]
 L.P. Kadanoff and G. Baym, Quantum Statistical Mechanics, Benjamin (1962) [Referring to Programme: Part C1 Nonequilibrium methods]
– Baym, Microscopic Description of Superfluidity, Math. Methods in SolidState&Superfluid Theory, Clark&Derrick Eds., Oliver&Boyd (1969) [Referring to Programme: Part C4]
– P.C. Hohenberg and P.C. Martin, Microscopic Theory of Superfluid Helium, Annals of Physics 34, 291359 (1965) [Referring to Programme: Part C4]
– Giamarchi, Quantum Physics in One Dimension, Oxford Science Pub. (2006) [Referring to Programme: Part C5]
 G. Iadonisi, G. Cantele, and M.L. Chiofalo, Introduction to Solid State Physics and Crystalline Nanostructures, Springer (2014) [Referring to Programme: Background in solidstate physics]
 M. L. Chiofalo, L. Salvi, G. Tino, La Fisica della Materia, in Lezioni di Fisica, Corriere della Sera (2018) [Semipopularized overview on quantum technologies]
5.2 Specific course parts (optional material, in addition to the lecture notes on the portal)
– G. Vignale, C. A Ullrich, S. Conti, TimeDependent Density Functional Theory and beyond the Adiabatic Local Density Approximation, Phys. Rev. Lett. 79, 4878 (1997)
 A. Daley, Quantum trajectories and open manybody quantum systems, Adv. Phys. 63, 77 (2014)
More readings, for especially interested students:
– P. Nozières and D. Pines, Theory of Quantum Liquids I – II, Westview Press (1999); Pines, The ManyBody Problem, Wiley (1997)
– D. Forster, Hydrodynamic Fluctuations, Broken Symmetry, And Correlation Functions, Adv. Books Classics (1995)
– W.M. Foulkes, L. Mitas, R.J. Needs, and G. Rajagopal, Quantum Monte Carlo Simulations of Solids, Revue of Modern Physics 73, 33 (2001)
– U. Schollwok and S.R. White, Methods for Time Dependence in DMRG, in Effective Models for LowDimensional Strongly Correlated Systems, G.G. Batrouni and D. Poilblanc Eds., p. 155 AIP, Melville, New York (2006)
– L. A. Bloomfield, How Things Work, Wiley (2013)
Please check with the UNIPI library on the availability of the suggested textbooks and articles.
Si consiglia di utilizzare al massimo delle potenzialità il materiale e le opportunità di verifica sul portale elearning di Fisica
Follow the material organized on the elarning page of the course
La valutazione finale è il risultato della valutazione sull’essay e (in modo facoltativo) sul lavoro di gruppo. Per chi decide di partecipare al lavoro di gruppo, il 75% della valutazione è sull’essay, e il 25% sul lavoro di gruppo. Per chi non desidera partecipare al lavoro di gruppo, il 100% della valutazione è sull’essay.
Per entrambe le prove, la valutazione è formulata per competenze. Con riferimento alle aree (a)(d) illustrata nella sezione Modalità di verifica delle capacità:
– fino a 18 punti per l'Area (a)
– fino a 6 punti per l'Area (b)
– fino a 9 punti per l'Area (c)
The final assessment results from evaluating the essay and (optionally) the group work. For those who choose to participate to the group work, 75% of the evaluation is performed on the essay, and %25 on the group work. Who chooses to not participate to the group work, 100% of the evaluation is on the essay.
For both types of tests, the assessment is operated by evaluating competences. Referring to areas (a)(d) in section Assessment of competences:
– up to 18 points for Area (a)
– up to 6 punti for Area (b)
– up to 4 punti for Area (c)
– up to 5 punti for Area (d)
Course summary description and scientific agenda.
The course is designed to open a window on contemporary frontier science that is developing along with advances in physics and quantum technologies, that are in turn based on the knowledge and design of highly related quantum particle liquids. In a new form of cooperation between theory and experiment, through quantum technologies it is possible to engineer quantum simulators. These are a sort of onpurpose quantum computers, in fact highly controllable experimental systems, in which one can code problems relevant to the physics of condensed matter, interactions and fundamental physics, cosmology and astrophysics, the fundamentals of quantum mechanics, and biology and life sciences. These applications are the subject of the third and final part (C) of the course, after having introduced and discussed the main platforms of quantum technologies available today: quantum gases (including dipolar and Rydberg atoms), trapped ions, Superconducting circuits, matter in optical cavities, fluids of light.
While this landscape is so wide and diverse to be breathtaking, this course is aimed at developing suited navigation tools. This is the aim of the first two parts (A and B) of the course, that is dedicated to build the basic language, with the necessary tools and methods. The first part, A, concerns the conventional and evergreen physics of quantum liquids at equilibrium in conditions of maximum symmetry and in those, more interesting, in which one or more symmetries are broken. The second part, B, is dedicated to open quantum liquids under outof equilibrium, drivendissipative conditions, where contemporary, freshly sprouting paradigms are discussed such as the engineering of external driving, dissipation or noise to achieve specific characteristics of the system, and the socalled dynamical quantum phase transitions.
Course traits. Distinguished traits of this course are the high level of crossdisciplinary contents, the didacticmethodological approach, and the international context.
Crossdisciplinary approach. This course is specialized in interdisciplinary thinking, as apparent from the syllabus below.
Didactic methodology and approach. Connecting is the keyword here. For each topic, connections are established between theory and experiment, between experiment and applications. Within the theory, connections are established among different methods to address one same topic. For each topic, a progressively increasing level of formal difficulty is introduced, that starts with the discussion in terms of a simplest model (requiring at most bachelor competences), complications being added one at a time, to finally connect to the more general and formal framework. This approach favors the identification of the basic concepts before diving in the formal mathematical complications, the connections among the concepts to choose the suited general procedures for problem solving and, finally, the specific implementation of the procedures to the particular problem at hand.
International course context. This course is also part of the Europeanfunded DIGIQ (Digitally Enhanced Quantum Technology Master) project www.digiq.eu: innovative resources and didactic material are being designed that are specific to this course, which include digital learning paths enjoyable by students also in autonomy, shared didactic material with similar courses in the other 23 European partners, practice of quantumtechnology concepts in (remotely accessible) real labs. In addition, students have the opportunity of participating to the network of DIGIQ students and to the corresponding funded in person and/or remote activities, which include traineeships, collaborative master thesis projects, and events (please see the website for the list of the EU partner universities).
Course summary description and scientific agenda.
The course is designed to open a window on contemporary frontier science that is developing along with advances in physics and quantum technologies, that are in turn based on the knowledge and design of highly related quantum particle liquids. In a new form of cooperation between theory and experiment, through quantum technologies it is possible to engineer quantum simulators. These are a sort of onpurpose quantum computers, in fact highly controllable experimental systems, in which one can code problems relevant to the physics of condensed matter, interactions and fundamental physics, cosmology and astrophysics, the fundamentals of quantum mechanics, and biology and life sciences. These applications are the subject of the third and final part (C) of the course, after having introduced and discussed the main platforms of quantum technologies available today: quantum gases (including dipolar and Rydberg atoms), trapped ions, Superconducting circuits, matter in optical cavities, fluids of light.
While this landscape is so wide and diverse to be breathtaking, this course is aimed at developing suited navigation tools. This is the aim of the first two parts (A and B) of the course, that is dedicated to build the basic language, with the necessary tools and methods. The first part, A, concerns the conventional and evergreen physics of quantum liquids at equilibrium in conditions of maximum symmetry and in those, more interesting, in which one or more symmetries are broken. The second part, B, is dedicated to open quantum liquids under outof equilibrium, drivendissipative conditions, where contemporary, freshly sprouting paradigms are discussed such as the engineering of external driving, dissipation or noise to achieve specific characteristics of the system, and the socalled dynamical quantum phase transitions.
Course traits. Distinguished traits of this course are the high level of crossdisciplinary contents, the didacticmethodological approach, and the international context.
Crossdisciplinary approach. This course is specialized in interdisciplinary thinking, as apparent from the syllabus below.
Didactic methodology and approach. Connecting is the keyword here. For each topic, connections are established between theory and experiment, between experiment and applications. Within the theory, connections are established among different methods to address one same topic. For each topic, a progressively increasing level of formal difficulty is introduced, that starts with the discussion in terms of a simplest model (requiring at most bachelor competences), complications being added one at a time, to finally connect to the more general and formal framework. This approach favors the identification of the basic concepts before diving in the formal mathematical complications, the connections among the concepts to choose the suited general procedures for problem solving and, finally, the specific implementation of the procedures to the particular problem at hand.
International course context. This course is also part of the Europeanfunded DIGIQ (Digitally Enhanced Quantum Technology Master) project www.digiq.eu: innovative resources and didactic material are being designed that are specific to this course, which include digital learning paths enjoyable by students also in autonomy, shared didactic material with similar courses in the other 23 European partners, practice of quantumtechnology concepts in (remotely accessible) real labs. In addition, students have the opportunity of participating to the network of DIGIQ students and to the corresponding funded in person and/or remote activities, which include traineeships, collaborative master thesis projects, and events (please see the website for the list of the EU partner universities).