535 research outputs found

    Single Cooper pair tunneling induced by non-classical microwaves

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    A mesoscopic Josephson junction interacting with a mode of non-classical microwaves with frequency ω\omega is considered. Squeezing of the electromagnetic field drastically affects the dynamics of Cooper tunneling. In particular, Bloch steps can be observed even when the microwaves are in the squeezed vacuum state with {\em zero} average amplitude of the field ⟨E(t)⟩=0\langle E(t) \rangle = 0. The interval between these steps is double in size in comparison to the conventional Bloch steps.Comment: 8 pages, 2 figures are available upon request to: [email protected]

    Symmetries of the finite Heisenberg group for composite systems

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    Symmetries of the finite Heisenberg group represent an important tool for the study of deeper structure of finite-dimensional quantum mechanics. As is well known, these symmetries are properly expressed in terms of certain normalizer. This paper extends previous investigations to composite quantum systems consisting of two subsystems - qudits - with arbitrary dimensions n and m. In this paper we present detailed descriptions - in the group of inner automorphisms of GL(nm,C) - of the normalizer of the Abelian subgroup generated by tensor products of generalized Pauli matrices of orders n and m. The symmetry group is then given by the quotient group of the normalizer.Comment: Submitted to J. Phys. A: Math. Theo

    Correlation properties of interfering electrons in a mesoscopic ring under nonclassical microwave radiation

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    Original paper can be found at: http://eproceedings.worldscinet.com/ Copyright World Scientific Publishing Co. DOI: 10.1142/9789812704474_0009Interfering electrons in a mesoscopic ring are irradiated with both classical and nonclassical microwaves. The average intensity of the charges is calculated as a function of time and it is found that it depends on the nature of the irradiating electromagnetic field. For various quantum states of the microwaves, the electron autocorrelation function is calculated and it shows that the quantum noise of the external field affects the interference of the charges. Two-mode entangled microwaves are also considered and the results for electron average intensity and autocorrelation are compared with those of the corresponding separable state. In both cases, the results depend on whether the ratio of the two frequencies is rational or irrational.Peer reviewe

    Production of a chaotic squeezed state from a ``pion liquid" and overbunching of identical pion correlations

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    It is shown that a one to one correspondence between quantum fields in two different "phases" as might be realized for pions produced from a "hadron liquid" leads to squeezed states. The single and double inclusive cross sections for at chaotic superposition of such states are calculated. The correlation of identical pions is overbunched in comparison with canonical Bose-Einstein correlations.Comment: Latex File, 6 page

    Essays on financial stability

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    Defence date: 31 May 2017Examining Board: Prof. Elena Carletti, EUI & Bocconi University (Supervisor); Prof. David K. Levine, EUI; Prof. Bruno Maria Parigi, University of Padua; Prof. Hans Degryse, University of LeuvenThis thesis consists of two essays concerning how banking regulations may promote financial stability. The first chapter investigates the competition-concentration-stability nexus from a novel perspective, by considering how concentration and, inter alia competition, affect the likelihood of an individual bank failing, and the likelihood of the bank failure spreading contagiously to the rest of the banking system. Competition is shown to reduce individual bank and systemic stability by reducing banks' profit buffers to absorb liquidity shocks. The impact of concentration on stability is more nuanced however, as increased concentration increases banks' profit buffers but also increases the concentration risk in the interbank market, widening the channel of contagion by which a liquidity shock can spread throughout the network. The second chapter concerns optimal ex-ante prudential regulation and ex-post resolution policy of globally systemically important banks. It characterises the conditions under which weakly capitalised, limitedly liable banks have incentives to 'gamble for resurrection' by investing in risky asset portfolios, in the knowledge that the downside risk is shifted onto the deposit insurance fund. In this context it is shown that a bank resolution by `bailing in' unsecured debt holders can restore the incentive for banks to act prudently, and that the bail-in should occur above the point of insolvency to ensure the bank has sufficient skin in the game. The interplay of three ex-ante prudential regulatory instruments is analysed: the minimum capital and total loss absorbing capacity requirements and the minimum capital buffer. The minimum capital and TLAC requirements are set to ensure that the bank has sufficient skin in the game to invest prudently and tradeoff the ex-post costs of bailing in unsecured debt holders, the cost of bailing out depositors and the cost of equity issuance, and minimum equity buffer is set to ensure an appropriate trigger for resolution.--1. Competition, concentration and contagion; --2. Debt, equity and moral hazard: the optimal structure of banks' loss absorbing capacit

    The Frobenius formalism in Galois quantum systems

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    Quantum systems in which the position and momentum take values in the ring Zd{\cal Z}_d and which are described with dd-dimensional Hilbert space, are considered. When dd is the power of a prime, the position and momentum take values in the Galois field GF(pâ„“)GF(p^ \ell), the position-momentum phase space is a finite geometry and the corresponding `Galois quantum systems' have stronger properties. The study of these systems uses ideas from the subject of field extension in the context of quantum mechanics. The Frobenius automorphism in Galois fields leads to Frobenius subspaces and Frobenius transformations in Galois quantum systems. Links between the Frobenius formalism and Riemann surfaces, are discussed

    Coherent spaces, Boolean rings and quantum gates

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    YesCoherent spaces spanned by a nite number of coherent states, are introduced. Their coherence properties are studied, using the Dirac contour representation. It is shown that the corresponding projectors resolve the identity, and that they transform into projectors of the same type, under displacement transformations, and also under time evolution. The set of these spaces, with the logical OR and AND operations is a distributive lattice, and with the logical XOR and AND operations is a Boolean ring (Stone's formalism). Applications of this Boolean ring into classical CNOT gates with n-ary variables, and also quantum CNOT gates with coherent states, are discussed

    Comonotonicity and Choquet integrals of Hermitian operators and their applications.

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    yesIn a quantum system with d-dimensional Hilbert space, the Q-function of a Hermitian positive semide nite operator , is de ned in terms of the d2 coherent states in this system. The Choquet integral CQ( ) of the Q-function of , is introduced using a ranking of the values of the Q-function, and M obius transforms which remove the overlaps between coherent states. It is a gure of merit of the quantum properties of Hermitian operators, and it provides upper and lower bounds to various physical quantities in terms of the Q-function. Comonotonicity is an important concept in the formalism, which is used to formalize the vague concept of physically similar operators. Comonotonic operators are shown to be bounded, with respect to an order based on Choquet integrals. Applications of the formalism to the study of the ground state of a physical system, are discussed. Bounds for partition functions, are also derived

    Weak mutually unbiased bases

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    Quantum systems with variables in Z(d){\mathbb Z}(d) are considered. The properties of lines in the Z(d)×Z(d){\mathbb Z}(d)\times {\mathbb Z}(d) phase space of these systems, are studied. Weak mutually unbiased bases in these systems are defined as bases for which the overlap of any two vectors in two different bases, is equal to d−1/2d^{-1/2} or alternatively to one of the di−1/2,0d_i^{-1/2},0 (where did_i is a divisor of dd apart from d,1d,1). They are designed for the geometry of the Z(d)×Z(d){\mathbb Z}(d)\times {\mathbb Z}(d) phase space, in the sense that there is a duality between the weak mutually unbiased bases and the maximal lines through the origin. In the special case of prime dd, there are no divisors of dd apart from 1,d1,d and the weak mutually unbiased bases are mutually unbiased bases
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