Bibliografías temáticas / Quantum condensed matter

Literatura académica sobre el tema "Quantum condensed matter"

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Publicado: 6 de septiembre de 2023

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Artículos de revistas sobre el tema "Quantum condensed matter"

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Bramwell, Steven T. y Bernhard Keimer. "Neutron scattering from quantum condensed matter". Nature Materials 13, n.º 8 (23 de julio de 2014): 763–67. http://dx.doi.org/10.1038/nmat4045.

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Laflorencie, Nicolas. "Quantum entanglement in condensed matter systems". Physics Reports 646 (agosto de 2016): 1–59. http://dx.doi.org/10.1016/j.physrep.2016.06.008.

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D'Errico, C., S. Scaffidi Abbate y G. Modugno. "Quantum phase slips: from condensed matter to ultracold quantum gases". Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 375, n.º 2108 (30 de octubre de 2017): 20160425. http://dx.doi.org/10.1098/rsta.2016.0425.

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Quantum phase slips (QPS) are the primary excitations in one-dimensional superfluids and superconductors at low temperatures. They have been well characterized in most condensed-matter systems, and signatures of their existence have been recently observed in superfluids based on quantum gases too. In this review, we briefly summarize the main results obtained on the investigation of phase slips from superconductors to quantum gases. In particular, we focus our attention on recent experimental results of the dissipation in one-dimensional Bose superfluids flowing along a shallow periodic potential, which show signatures of QPS. This article is part of the themed issue ‘Breakdown of ergodicity in quantum systems: from solids to synthetic matter’.
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Baranov, M. A., M. Dalmonte, G. Pupillo y P. Zoller. "Condensed Matter Theory of Dipolar Quantum Gases". Chemical Reviews 112, n.º 9 (9 de agosto de 2012): 5012–61. http://dx.doi.org/10.1021/cr2003568.

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Miyashita, Seiji. "Quantum mechanical effects on condensed matter phenomena". Physica A: Statistical Mechanics and its Applications 281, n.º 1-4 (junio de 2000): 420–31. http://dx.doi.org/10.1016/s0378-4371(00)00029-7.

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Schrieffer, J. R. "Novel quantum numbers in condensed matter physics". Current Applied Physics 4, n.º 5 (agosto de 2004): 465–72. http://dx.doi.org/10.1016/j.cap.2004.01.001.

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Tsvelik, Alexi M. y Allan Macdonald. "Quantum Field Theory in Condensed Matter Physics". Physics Today 50, n.º 2 (febrero de 1997): 66. http://dx.doi.org/10.1063/1.881712.

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Inoshita, T. "CONDENSED MATTER PHYSICS:Kondo Effect in Quantum Dots". Science 281, n.º 5376 (24 de julio de 1998): 526–27. http://dx.doi.org/10.1126/science.281.5376.526.

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Dovesi, Roberto, Alessandro Erba, Roberto Orlando, Claudio M. Zicovich-Wilson, Bartolomeo Civalleri, Lorenzo Maschio, Michel Rérat et al. "Quantum-mechanical condensed matter simulations with CRYSTAL". Wiley Interdisciplinary Reviews: Computational Molecular Science 8, n.º 4 (4 de marzo de 2018): e1360. http://dx.doi.org/10.1002/wcms.1360.

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CHAPLINE, GEORGE. "QUANTUM PHASE TRANSITIONS AND EVENT HORIZONS: CONDENSED MATTER ANALOGIES". International Journal of Modern Physics B 20, n.º 19 (30 de julio de 2006): 2647–50. http://dx.doi.org/10.1142/s0217979206035126.

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Although it has been generally believed that classical general relativity is always correct for macroscopic length scales, certain predictions such as event horizons and closed time-like curves are inconsistent with ordinary quantum mechanics. It has recently been pointed out that the event horizon problem can be resolved if space-time undergoes a quantum phase transition as one approaches the surface where general relativity predicts that the redshift becomes infinite. Indeed a thought experiment involving a superfluid with a critical point makes such a suggestion appear plausible. Furthermore the behavior of space-time near an event horizon may resemble quantum phase transitions that have been observed in the laboratory. For example, the phenomenology of metamagnetic quantum critical points in heavy fermion materials resembles the behavior expected, both in terms of time standing still and the behavior of quantum correlation functions. Martensitic transformations accompanied by non-adiabatic changes in the electronic wave function are also interesting in this connection.
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Tesis sobre el tema "Quantum condensed matter"

1

Zonzo, Giuseppe. "Quantum Information Theory in Condensed Matter Physics". Doctoral thesis, Universita degli studi di Salerno, 2017. http://hdl.handle.net/10556/2625.

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2015 - 2016
Inthe“standard”Gizburg-Landauapproach,aphasetransitionisintimately connected to a local order parameter, that spontaneously breaks some symmetries. In addition to the “traditional” symmetry-breaking ordered phases, a complex quantum system exhibits exotic phases, without classical counterpart, that can be described, for example, by introducing non-local order parameters that preserve symmetries. In this scenario, this thesis aims to shed light on open problems, such as the localdistinguishabilitybetweengroundstatesofasymmetry-breakingordered phase and the classification of one dimensional quantum orders, in terms of entanglement measures, in systems for which the Gizburg-Landau approach fails. In particular, I briefly introduce the basic tools that allow to understand the nature of entangled states and to quantify non-classical correlations. Therefore, I analyze the conjecture for which the maximally symmetry-breaking ground states (MSBGSs) are the most classical ones, and thus the only ones selected in real-world situations, among all the ground states of a symmetry-breaking ordered phase. I make the conjecture quantitatively precise, by proving that the MSBGSs are the only ones that: i) minimize pairwise quantum correlations, as measured by the quantum discord; ii) are always local convertible, by only applying LOCC transformations; iii) minimize the residual tangle, satisfying at its minimum the monogamy of entanglement. Moreover,Ianalyzehowevolvesthedistinguishability,afterasuddenchange of the Hamiltonian parameters. I introduce a quantitative measure of distinguishability, in terms of the trace distance between two reduced density matrices. Therefore, in the framework of two integrable models that falls in two different classes of symmetries, i.e. XY models in a transverse magnetic field and the N-cluster Ising models, I prove that the maximum of the distinguishability shows a time-exponential decay. Hence, in the limit of diverging time, all the informations about the particular initial ground state disappear, even if a system is integrable. Far away from the Gizburg-Landau scenario, I analyze a family of fullyanalyticalsolvableonedimensionalspin-1/2models,namedtheN-clustermodels in a transverse magnetic field. Regardless of the cluster size N + 2, these modelsexhibitaquantumphasetransition,thatseparatesaparamagneticphase from a cluster one. The cluster phase coresponds to a nematic ordered phase or a symmetry-protected topological ordered one, for even or odd N respectively. Using the Jordan-Wigner transformations, it is possible to diagonalize these models and derive all their spin correlation functions, with which reconstruct their entanglement properties. In particular, I prove that these models have only a non-vanishing bipartite entanglement, as measured by the concurrence, between spins at the endpoints of the cluster, for a magnetic field strong enough. Moreover, I introduce the minimal set of nonlinear ground-states functionals to detect all 1-D quantum orders for systems of spin-1/2 and fermions. I show that the von Neumann entanglement entropy distinguishes a critical systemfromanoncriticalone,becauseofthelogarithmicdivergenceataquantum critical point. The Schmidt gap detect the disorder of a system , because it saturates to a constant value in a paramagnetic phase and goes to zero otherwise. The mutual information, between two subsystems macroscopically separated, identifiesthesymmetry-breakingorderedphases,becauseofitsdependenceon the order parameters. The topological order phases, instead, via their deeply non-locality, can be characterized by analyzing all three functionals. [edited by author]
In aggiunta alle tradizionali fasi ordinate con rottura spontanea di simmetria, ben descritte con un approccio alla Gizburg-Landau, dove una transizione di fase `e intimamente connessa alla rottura spontanea di qualche simmetria e ad un parametro d’ordine locale, un sistema quantistico presenta anche fasi esotiche,senzaanalogoclassico,chesonoperesempiocaratterizzatedaparametri d’ordine non locali, senza una necessaria rottura di simmetria. Partendo da questi presupposti, questa tesi si pone come obiettivo quello di fare luce su alcuni problemi ancora aperti, come la distinguibilit`a tra stati fondamentaliinsistemiquantisticiconrotturaspontaneadisimmetriaelaclassificazionedituttelefasipresentiinsistemiunidimensionalidispin-1/2efermioni, per i quali l’approccio alla Gizburg-Landau non fornisce una descrizione adeguata. Inparticolare,sid`aunaspiegazioneall’ipotesisecondolaqualeglistatifondamentali che rompono massimamente la simmetria sono quelli pi`u classici, e quindi selezionati dalla decoerenza dell’ambiente, tra tutti gli stati fondamentali,edenergeticamenteequivalenti,diunafaseordinataconrotturaspontanea di simmetria. Si dimostra, infatti, che gli stati che rompono massimamente la simmetria sono gli unici stati che soddisfano tre criteri di classicalit`a: i) minimizzano l’entanglement bipartito, come quantificato dalla discord; ii) sono gli uniciversocuituttiglialtristatifondamentalisonolocalmenteconvertibili,mediante LOCC; iii) minimizzano il tangle residuo, soddisfacendo al minimo la monogamia dell’entanglement. Viene analizzato, inoltre, come evolve la distinguibilit`a tra stati fondamentali, dopo un quench dei parametri Hamiltoniani. Dopo aver introdotto una misura quantitativa della distinguibilit`a, in termini della distanza tra due matrici densit`a ridotte, si dimostra, per due sistemi integrabili con diverse classi di simmetria, nel dettaglio il modello XY in campo magnetico e i modelli NclusterIsing,cheladistinguibilit`adecadeesponenzialmenteneltempoequindi, nel limite di tempi lunghi, tutte le informazioni sullo stato fondamentale di partenza si perdono, anche per sistemi integrabili, nei quali la termalizzazione non si verifica. LontanodalloscenarioGizburg-Landau,sianalizzaunafamigliadimodelli di spin-1/2 esattamente risolvibili, nel dettaglio i modelli N-cluster in campo magnetico, che mostrano una transizione tra una fase disordinata e una di tipo cluster, che pu`o essere nematica o topologica, rispettivamente per N pari o dispari. Usando le trasformazioni di Jordan-Wigner `e possibile diagonalizzare questi modelli, ricavare lo stato fondamentale, le funzioni di correlazione fermioniche e tutte le loro propriet`a di entanglement di. Si dimostra che questi modellinonhannoentanglementmultipartito,masoloentanglementbipartito, come misurato dalla concurrence, tra due spin alle estremit`a del cluster, per un campo magnetico sufficientemente intenso. Inoltre, sidimostrachel’entropiadivonNeumann,loSchmidtgapelamutualinformationrappresentanoilsetminimodifunzionalinonlinearidellamatrice densit`a ridotta, mediante le quali caratterizzare tutte le fasi presenti in sistemi unidimensionali di spin -1/2 e fermioni. In particolare, l’entropia di von Neumann caratterizza la criticalit`a del sistema, per la sua divergenza logaritmica al punto critico; lo Schmidt gap caratterizza il disordine di un sistema, perch´e satura ad un valore costante nelle fasi disordinate e va rapidamente a zero altrove; la mutual information cattura le fasi ordinate con rottura spontanea di simmetria, per le quali cio` e `e possibile definire un parametro d’ordine diverso da zero su un supporto finito. Le fasi topologiche, per via della loro natura fortemente non locale, necessitano di tutte e tre i funzionali per essere individuate. [a cura dell'autore]
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Gauger, E. M. "Applications of quantum coherence in condensed matter nanostructures". Thesis, University of Oxford, 2010. http://ora.ox.ac.uk/objects/uuid:fb792980-bfc4-4771-b5d5-b9ecc7d40cd8.

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This thesis is concerned with studying the fascinating quantum properties of real-world nanostructures embedded in a noisy condensed matter environment. The interaction with light is used for controlling and manipulating the quantum state of the systems considered here. In some instances, laser pulses also provide a way of actively probing and controlling environmental interactions. The first two research chapters assess two different ways of performing all-optical spin qubit gates in self-assembled quantum dots. The principal conclusion is that an `adiabatic' control technique holds the promise of achieving a high fidelity when all primary sources of decoherence are taken into account. In the next chapter, it is shown that an optically driven quantum dot exciton interacting with the phonons of the surrounding lattice acts as a heat pump. Further, a model is developed which predicts the temperature-dependent damping of Rabi oscillations caused by bulk phonons, finding an excellent agreement with experimental data. A different system is studied in the following chapter: two electron spin qubits with no direct interaction, yet both exchange-coupled to an optically active mediator spin. The results of this study show that these general assumptions are sufficient for generating controlled electron spin entanglement over a wide range of parameters, even in the presence of noise. Finally, the Radical Pair model of the avian compass is investigated in the light of recent experimental results, leading to the surprising prediction that the electron spin coherence time in this molecular system seems to approach the millisecond timescale.
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Baggioli, Matteo. "Gravity, holography and applications to condensed matter". Doctoral thesis, Universitat Autònoma de Barcelona, 2016. http://hdl.handle.net/10803/395205.

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Los sistemas fisicos fuertemente acoplados, junto a sus correspondientes y por lo general exoticas caracteristicas, son imposibles de tratar mediante los enfoques perturbativos convencionales que en estos casos no son capaces de proporcionar una herramienta controlable y robusta. Sin embargo, los efectos no perturbativos y fenomenos fuertemente correlacionados abundan en la fisica, especialmente en la Fisica de la Materia Condensada. La correspondencia AdS / CFT, que nace de el estimulo de las ideas y esfuerzos empleados en descubrir una posible descripcion de la gravedad cuantica, proporciona una perspectiva inesperada e innovadora para hacer frente a las teorías de campo fuertemente acopladas. En su formulacion mas general este planteamiento ofrece un arma efectiva para hacer frente a ese tipo de problemas utilizando una descripcion dual de teorias gauge mediante teorias de gravedad que resulta ser mas simple que la original. En los ultimos anos ha habido un gran numero de avances aplicando esta dualidad a temas modernos e innovadores en materia condensada, tales como la naturaleza de los metales raros o el mecanismo que subyace la superconductividad de alta Tc. La relajacion del momento es un ingrediente omnipresente e inevitable de cualquier sistema realista en Materia Condensada. En los materiales del mundo real la presencia de un reticulo, de impurezas, o de desorden hacen que el momento se disipe, y se da lugar a efectos fisicos relevantes, tales como las propiedades de transporte de corriente continua sean finitas,es decir, la conductividad. Hay varias preguntas abiertas relacionadas a dichas cantidades, especialmente en el limite de maxima relajacion donde surgen nuevos estados aislantes y transiciones de fase cuantica inesperadas entre los estados ultimos y metalicos (MIT) . El objetivo principal de esta tesis es la introduccion de disipacion de momento y sus efectos en el contexto Ads/CMT, es decir, las aplicaciones de la dualidad Gauge-Gravedad en materia condensada. Una manera conveniente y efectiva de romper la simetria traslacional de la teoria cuantica de campos dual es proporcionada por las teorias de gravedad masiva (GM), que constituye una herramienta facil y manejable para atacar varias e interesantes preguntas sobre sistemas fuertemente acoplados con disipacion de impulso. Originalmente concebido para resolver problemas en cosmologia, la GM puede ahora ser empleada bajo una perspectiva completamente nueva y podria convertirse en una herramienta útil para aplicaciones del ''mundo real'' y ''de bajas energias''. Consideramos modelos genericos de gravedad masiva en espacio-tiempos asintóticamente anti de Sitter y los analizamos usando tecnicas holograficas.
Strongly coupled physical systems along with their corresponding, and usually exotic, features are elusive and not suitable to be described by conventional and perturbative approaches, which in those cases are not able to provide a controllable and robust tool for computations. Nevertheless non perturbative effects and strongly correlated frameworks are ubiquitous in nature, expecially in Condensed Matter physics. The AdS/CFT correspondence, born from the excitement of ideas and efforts employed in finding out a possible description of Quantum Gravity, lead to a flurry of fresh air into the subject, introducing an unexpected and brandnew perspective for dealing with strongly coupled field theories. In its more general formulation, known as Gauge-Gravity duality, this setup accounts for an effective and efficient weapon to tackle those kind of problems using a dual gravitational description which turns out to be way easier than the original one. In the last years, a huge number of developments have been achieved in applying the duality towards modern and hot condensed matter misteries, such as the Strange Metals nature or the mechanism underlying the High-Tc Superconductivity.\\ Momentum relaxation is an ever-present and unavoidable ingredient of any realistic Condensed Matter system. In real-world materials the presence of a lattice, impurities or disorder forces momentum to dissipate and leads to relevant physical effects such as the finiteness of the DC transport properties, i.e. conductivities. Several open questions are connected to those quantities expecially in the limit of strong momentum relaxation where novel insulating states appear and unexpected quantum phase transitions between the latter and metallic states (MIT) arise.\\[0.2cm] The main purpose of this thesis is the introduction of momentum dissipation and its consequent effects into the framework of AdS/CMT, namely the applications of the Gauge-Gravity duality to Condensed Matter. \\ A convenient and effective way of breaking translational symmetry of the the dual quantum field theory is provided by Massive Gravity (MG) theories, which constitues a tractable and easy tool to adress several interesting questions in strongly coupled systems with momentum dissipation. Born to solve cosmological puzzles, MG can now be reconsidered under a completely new perspective and could become a useful framework for ''Real-world" phenomena and "low energy" applications. We consider generic massive gravity models embedded into asymptotically Anti de Sitter spacetime and we analyze them using holographic techniques.
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Babadi, Mehrtash. "Non-equilibrium dynamics of artificial quantum matter". Thesis, Harvard University, 2013. http://dissertations.umi.com/gsas.harvard:11114.

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The rapid progress of the field of ultracold atoms during the past two decades has set new milestones in our control over matter. By cooling dilute atomic gases and molecules to nano-Kelvin temperatures, novel quantum mechanical states of matter can be realized and studied on a table-top experimental setup while bulk matter can be tailored to faithfully simulate abstract theoretical models. Two of such models which have witnessed significant experimental and theoretical attention are (1) the two-component Fermi gas with resonant $s$-wave interactions, and (2) the single-component Fermi gas with dipole-dipole interactions. This thesis is devoted to studying the non-equilibrium collective dynamics of these systems using the general framework of quantum kinetic theory.
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Liu, Wensheng. "Applications of effective field theory to condensed matter /". Digital version accessible at:, 1999. http://wwwlib.umi.com/cr/utexas/main.

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Korkusinski, Marek. "Correlations in semiconductor quantum dots". Thesis, University of Ottawa (Canada), 2004. http://hdl.handle.net/10393/29128.

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In this Thesis, I present a theoretical study of correlation effects in strongly interacting electronic and electron-hole systems confined in semiconductor quantum dots. I focus on three systems: N electrons in a two-dimensional parabolic confinement in the absence and in the presence of a magnetic field, an electron-hole pair confined in a vertically coupled double-quantum-dot molecule, and a charged exciton in a quantum-ring confinement in a magnetic field. To analyse these systems I use the exact diagonalisation technique in the effective-mass approximation. This approach consists of three steps: construction of a basis set of particle configurations, writing the Hamiltonian in this basis in a matrix form, and numerical diagonalisation of this matrix. Each of these steps is described in detail in the text. Using the exact diagonalisation technique I identify the properties of the systems due to correlations and formulate predictions of how these properties could be observed experimentally. I confront these predictions with results of recent photoluminescence and transport measurements. First I treat the system of N electrons in a parabolic confinement in the absence of magnetic field and demonstrate how its properties, such as magnetic moments, can be engineered as a function of the system parameters and the size of the Hilbert space. Next I analyse the evolution of the ground state of this system as a function of the magnetic field. In the phase diagram of the system I identify the spin-singlet nu = 2 phase and discuss how correlations influence its phase boundaries both as a function of the magnetic field and the number of electrons. I also demonstrate that in higher magnetic fields electronic correlations lead to the appearance of spin-depolarised phases, whose stability regions separate the weakly correlated phases with higher spin. Further on, I consider electron-hole systems. I show that the Coulomb interaction leads to entanglement of the states of an electron and a hole confined in a pair of vertically coupled quantum dots. Finally I consider the system of two electrons and one hole (a negatively charged exciton) confined in a quantum ring and in the presence of the magnetic field. I show that the energy of a single electron in the ring geometry exhibits the Aharonov-Bohm oscillations as a function of the magnetic field. In the case of the negatively charged exciton these oscillations are nearly absent due to correlations among particles, and as a result the photoluminescence spectra of the charged complex are dominated by the energy of the final-state electron. The Aharonov-Bohm oscillations of the energy of a single electron are thus observed directly in the optical spectra.
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Gibb, Kevin. "The quantum confined Stark effect and Wannier Stark ladders in InxGa1-xAs quantum wells and superlattices". Thesis, University of Ottawa (Canada), 1992. http://hdl.handle.net/10393/7704.

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The effects of an applied bias in the longitudinal or growth direction on four In$\sb{\rm x}$Ga$\sb{\rm 1-x}$As-GaAs strained single quantum wells and three strained layer superlattices have been studied using photocurrent and electroreflectance spectroscopy at liquid helium temperature. Weak applied electric fields on the quantum well samples gives rise to a red quadratic shift to the lowest interband transition between the first confined electron (E1) and heavy-hole (H1) levels, the quantum confined Stark effect (QCSE). The magnitude of the QCSE increases with well width. This field dependence becomes subquadratic at high applied fields due to carrier accumulation on the low energy side of the wells. Superlattices with relatively small periods, i.e. 10 nm, exhibit interwell coupling giving rise to a miniband structure under flatband conditions. The application of an electric field removes the interwell coupling giving rise to a ladder like progression in energy for the interband transition energies, called Wannier Stark ladders. The measured exciton transition energies follow a linear field dependence given by the product of the Stark ladder index, the superlattice period, and the electric field. The low field behaviour is more complex due to the Coulomb interaction between the electrons and heavy-holes. The measured field dependent exciton transition energies for the quantum wells agree well with single particle model calculations, while for the superlattice samples the exciton Stark ladder calculations of Dignam and Sipe have yielded good agreement with the measured data.
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Morris, Richard. "Studies towards quantum magnonics". Thesis, University of Oxford, 2017. http://ora.ox.ac.uk/objects/uuid:89784b64-de31-457f-b9b2-54125c862632.

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This thesis reports on recent results which pave the way for future experiments in the emerging field of quantum magnonics. Chapter 1 presents a brief outline of the field of magnonics, which provides the context in which quantum magnonics has begun to develop. Chapter 2 provides an introduction to the theory of spin waves, which is necessary to understand the experiments reported in the thesis. In Chapter 3, the experimental methods and materials used to carry out the investigations in the thesis are described. Chapter 4 describes the coupling of resonant magnon modes in a sphere of yttrium-iron garnet to photon modes in a coplanar-waveguide resonator. Strong coupling is achieved to multiple magnon modes, and a theoretical model is used to identify the magnon modes which couple most strongly to the photon mode. In Chapter 5, the behaviour of propagating magnon modes is investigated in a waveguide formed from a thin film of yttrium-iron garnet. Two different configurations are investigated supporting different types of propagating mode, namely backward-volume and surface spin waves. Simulations are performed which reproduce the main features of the data. Chapter 6 characterises the effect of the gadolinium-gallium garnet substrate on propagating spin waves. The magnitude of this effect is dependent on both the orientation and temperature of the sample. Finally, Chapter 7 provides a short summary of the results of the thesis, and speculates on how they may inform future work in the field.
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Eastmond, John F. G. "Numerical studies of two problems in condensed matter physics : quantum transport and quantum antiferromagnets". Thesis, University of Oxford, 1992. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.315716.

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Fidkowski, Lukasz. "Singularity resolution in string theory and new quantum condensed matter phases /". May be available electronically:, 2007. http://proquest.umi.com/login?COPT=REJTPTU1MTUmSU5UPTAmVkVSPTI=&clientId=12498.

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Libros sobre el tema "Quantum condensed matter"

1

Inc, ebrary, ed. Condensed matter theories. Singapore: World Scientific Pub., 2009.

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Accurate condensed-phase quantum chemistry. Boca Raton: Taylor & Francis, 2011.

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Manby, Frederick R. y Frederick R. Manby. Accurate condensed-phase quantum chemistry. Boca Raton: Taylor & Francis, 2011.

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I͡U︡, Kagan y Leggett A. J, eds. Quantum tunnelling in condensed media. Amsterdam: North-Holland, 1992.

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Agarwala, Adhip. Excursions in Ill-Condensed Quantum Matter. Cham: Springer International Publishing, 2019. http://dx.doi.org/10.1007/978-3-030-21511-8.

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Musser, George. Emergence in Condensed Matter and Quantum Gravity. Cham: Springer International Publishing, 2022. http://dx.doi.org/10.1007/978-3-031-09895-6.

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Nagaosa, Naoto. Quantum Field Theory in Condensed Matter Physics. Berlin, Heidelberg: Springer Berlin Heidelberg, 1999. http://dx.doi.org/10.1007/978-3-662-03774-4.

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Quantum field theory in condensed matter physics. Cambridge: Cambridge University Press, 1995.

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Quantum field theory in condensed matter physics. 2a ed. Cambridge: Cambridge University Press, 2003.

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1929-, Bassani G. F., Liedl G. L y Wyder Peter 1934-, eds. Encyclopedia of condensed matter physics. Amsterdam: Elsevier, 2005.

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Capítulos de libros sobre el tema "Quantum condensed matter"

1

Silver, R. N. "Quantum Statistical Inference". En Condensed Matter Theories, 315–29. Boston, MA: Springer US, 1993. http://dx.doi.org/10.1007/978-1-4615-2934-7_27.

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Aliaga, J., G. Crespo y A. N. Proto. "Dissipative Evolutions in Quantum Mechanics". En Condensed Matter Theories, 317–25. Boston, MA: Springer US, 1990. http://dx.doi.org/10.1007/978-1-4613-0605-4_33.

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Lyo, S. K. "Multiple Scattering in Semiconductor Quantum-Wells". En Condensed Matter Physics, 98–102. New York, NY: Springer New York, 1987. http://dx.doi.org/10.1007/978-1-4612-4772-2_8.

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Canosa, N., R. Rossignoli y A. Plastino. "Information Theory and Quantum Wave Functions". En Condensed Matter Theories, 69–77. Boston, MA: Springer US, 1992. http://dx.doi.org/10.1007/978-1-4615-3352-8_7.

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Brown, R. G. y M. Ciftan. "Quantum Statistical Microdynamics and Critical Phenomena". En Condensed Matter Theories, 25–35. Boston, MA: Springer US, 1991. http://dx.doi.org/10.1007/978-1-4615-3686-4_2.

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Aguilera-Navarro, V. C. "Quantum Many-Body Systems: Orthogonal Coordinates". En Condensed Matter Theories, 309–15. Boston, MA: Springer US, 1990. http://dx.doi.org/10.1007/978-1-4613-0605-4_32.

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Proto, Araceli N. "Maximum Entropy Principle and Quantum Mechanics". En Condensed Matter Theories, 355–64. Boston, MA: Springer US, 1990. http://dx.doi.org/10.1007/978-1-4613-0605-4_37.

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Clark, John W. y Manfred L. Ristig. "Generalized Momentum Distributions of Quantum Fluids". En Condensed Matter Theories, 47–60. Boston, MA: Springer US, 1990. http://dx.doi.org/10.1007/978-1-4613-0605-4_6.

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Solís, M. A., R. Guardiola y M. de Llano. "Quantum Thermodynamic Perturbation Theory for Fermions". En Condensed Matter Theories, 215–26. Boston, MA: Springer US, 1993. http://dx.doi.org/10.1007/978-1-4615-2934-7_20.

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Fortes, M., M. de Llano y J. del Río. "Hard Core Square Well Quantum Matter". En Condensed Matter Theories, 139–52. Boston, MA: Springer US, 1986. http://dx.doi.org/10.1007/978-1-4615-6707-3_14.

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Actas de conferencias sobre el tema "Quantum condensed matter"

1

Doll, J. D. y J. E. Gubernatis. "Quantum Simulations of Condensed Matter Phenomena". En International Workshop on Quantum Simulations of Condensed Matter Phenomena. WORLD SCIENTIFIC, 1989. http://dx.doi.org/10.1142/9789814541022.

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Shimano, Ryo. "Terahertz Frequency Magnetoelectric Phenomena in Condensed Matter". En Quantum Electronics and Laser Science Conference. Washington, D.C.: OSA, 2011. http://dx.doi.org/10.1364/qels.2011.qwd5.

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Randjbar-Daemi, S. y Yu Lu. "Quantum Field Theory and Condensed Matter Physics". En Fourth Trieste Conference. WORLD SCIENTIFIC, 1994. http://dx.doi.org/10.1142/9789814534826.

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Halperin, Betrand. "On the Quantum Theory of Condensed Matter". En Proceedings of the 24th Solvay Conference on Physics. WORLD SCIENTIFIC, 2010. http://dx.doi.org/10.1142/9789814304474_0001.

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Büttiker, M. "The quantum Hall effect in open conductors". En Frontiers in condensed matter theory. AIP, 1990. http://dx.doi.org/10.1063/1.39729.

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Angelakis, D. G. "Photonic Quantum Simulators: Mimicking Condensed Matter Physics Using Photons". En International Quantum Electronics Conference. Washington, D.C.: OSA, 2011. http://dx.doi.org/10.1364/iqec.2011.i1103.

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Imada, Masatoshi. "Tools for Studying Quantum Emergence near Phase Transitions". En HIGHLIGHTS IN CONDENSED MATTER PHYSICS. AIP, 2003. http://dx.doi.org/10.1063/1.1639578.

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Khalatnikov, I. M. "Hydrodynamics of classical and quantum liquids with free surfaces". En Frontiers in condensed matter theory. AIP, 1990. http://dx.doi.org/10.1063/1.39720.

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Stone, A. Douglas, A. Szafer, P. L. McEuen y J. K. Jain. "Understanding the quantum Hall effect using the s-matrix approach". En Frontiers in condensed matter theory. AIP, 1990. http://dx.doi.org/10.1063/1.39736.

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Anderson, P. W. y Y. Ren. "The normal state of high Tc superconductors: A new quantum liquid". En Frontiers in condensed matter theory. AIP, 1990. http://dx.doi.org/10.1063/1.39744.

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Informes sobre el tema "Quantum condensed matter"

1

Privman, Vladimr. Quantum Computing in Condensed Matter Systems. Fort Belvoir, VA: Defense Technical Information Center, abril de 1997. http://dx.doi.org/10.21236/ada327465.

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Privman, Vladimir y Lawrence S. Schulman. Quantum Mechanics of Computing in Condensed Matter Systems. Fort Belvoir, VA: Defense Technical Information Center, abril de 1998. http://dx.doi.org/10.21236/ada345671.

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Greiner, Markus. Quantum Simulations of Condensed Matter Systems Using Ultra-Cold Atomic Gases. Fort Belvoir, VA: Defense Technical Information Center, marzo de 2013. http://dx.doi.org/10.21236/ada583520.

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