On the asymptotic behavior of a spectrum of the Hamiltonian in quantum theory for a large number of fields

Ovidiu I Pâţu, V. E. Korepin, D. V. Averin

This work presents the derivation of the large time and distance asymptotic behavior of the field-field correlation functions of impenetrable one-dimensional anyons at finite temperature. In the appropriate limits of the statistics parameter, we recover the well-known results for impenetrable bosons and free fermions. In the low-temperature (usually expected to be the "conformal") limit, and for all values of the statistics parameter away from the bosonic point, the leading term in the correlator does not agree with the prediction of the conformal field theory, and is determined by the singularity of the density of the single-particle states at the bottom of the single-particle energy spectrum.

Alexander Nikolaevich Pechen

Holger Gies A, Marta Picciau

We investigate a class of quantum field theories with relativistic Luttinger fermions and local self-interaction in scalar channels. For an understanding of possible low-energy phases, we first classify the set of mass terms arising from scalar fermion bilinears. For large flavor numbers, we show that each of our models features a coupling branch in which the theory is asymptotically free. In order to address the long-range behavior, we use mean-field theory which is exact in the limit of large flavor numbers. We identify two models which undergo dimensional transmutation, interconnecting the asymptotically free high-energy regime with an ordered low-energy phase sustaining a vacuum condensate. We also study the analytic structure of the Luttinger-fermionic propagator in the various possible gapped phases.

M. A. Antonets, G. M. Zhislin, Ilya A. Shereshevskii

Semjon A. Vugalter

Hiroshi Nagaoka

One of the principal themes of information theory is to establish a link between two different kinds of quantities: one is an operational quantity which is defined through the asymptotic optimality on some concrete concept such as code length, compression rate, error probability, etc., while the other is an abstract information quantity such as the entropy, divergence, mutual information, etc. The same theme is now being pursued extensively in quantum information theory, and lots of mathematical results have been reported so far. In the so-called information-spectrum methods in the classical information theory [1], the process of establishing a link between an operatinal quantity and an entropy-like information quantity is intentionally divided into two parts, making the third kind of quantities — information spectrum — intervene. In the methods, the asymptotic optimality of an operational quantity is characterized by a limiting expression on information spectra (asymptotic behavior of logarithmic likelihoods) in the most general setting, while the information-spectrum quantity is rewritten to an entropylike quantity in a specific situation mostly as a direct consequence of a limiting theorem in the probability theory such as the law of large numbers, the Shannon-McMillan-Breiman theorem, etc. Such a framework brings not only generality but also transparency of mathematical arguments. Extending the information-spectrum methods to the quantum case is an attractive subject, which is expected to provide both the asymptotic optimality of operational quantities and the limiting law governing quantum stochastic situations with transparent and comprehensive understanding. In this talk I would like to review recent attempts to develop the quantum informationspectrum methods made by Hayashi, Ogawa and myself, mainly based on [2, 3, 4], and discuss their significance in the quantum information theory.