1,274 research outputs found
Universal quantum measurements
We introduce a family of operations in quantum mechanics that one can regard as "universal quantum measurements" (UQMs). These measurements are applicable to all finite dimensional quantum systems and entail the specification of only a minimal amount of structure. The first class of UQM that we consider involves the specification of the initial state of the system—no further structure is brought into play. We call operations of this type "tomographic measurements", since given the statistics of the outcomes one can deduce the original state of the system. Next, we construct a disentangling operation, the outcome of which, when the procedure is applied to a general mixed state of an entangled composite system, is a disentangled product of pure constituent states. This operation exists whenever the dimension of the Hilbert space is not a prime, and can be used to model the decay of a composite system. As another example, we show how one can make a measurement of the direction along which the spin of a particle of spin s is oriented (s = 1/2, 1,...). The required additional structure in this case involves the embedding of CP^1 as a rational curve of degree 2s in CP^2s
Pricing Fixed-Income Securities in an Information-Based Framework
In this paper we introduce a class of information-based models for the
pricing of fixed-income securities. We consider a set of continuous- time
information processes that describe the flow of information about market
factors in a monetary economy. The nominal pricing kernel is at any given time
assumed to be given by a function of the values of information processes at
that time. By use of a change-of-measure technique we derive explicit
expressions for the price processes of nominal discount bonds, and deduce the
associated dynamics of the short rate of interest and the market price of risk.
The interest rate positivity condition is expressed as a differential
inequality. We proceed to the modelling of the price-level, which at any given
time is also taken to be a function of the values of the information processes
at that time. A simple model for a stochastic monetary economy is introduced in
which the prices of nominal discount bonds and inflation-linked notes can be
expressed in terms of aggregate consumption and the liquidity benefit generated
by the money supply
On the Representation of General Interest Rate Models as Square Integrable Wiener Functionals
In the setting proposed by Hughston & Rafailidis (2005) we consider general
interest rate models in the case of a Brownian market information filtration
. Let be a square-integrable
-measurable random variable, and assume the non-degeneracy
condition that for all the random variable is not
-measurable. Let denote the integrand appearing in
the representation of as a stochastic integral, write for the
conditional variance of at time , and set .
Then is a potential, and as such can act as a model for a pricing
kernel (or state price density), where is the associated interest rate.
Under the stated assumptions, we prove the following: (a) that the money market
account process defined by is finite almost
surely at all finite times; and (b) that the product of the money-market
account and the pricing kernel is a local martingale, and is a martingale
provided a certain integrability condition is satisfied. The fact that a
martingale is thus obtained shows that from any non-degenerate element of
Wiener space satisfying the integrability condition we can construct an
associated interest-rate model. The model thereby constructed is valid over an
infinite time horizon, with strictly positive interest, and satisfies the
relevant intertemporal relations associated with the absence of arbitrage. The
results thus stated pave the way for the use of Wiener chaos methods in
interest rate modelling, since any such square-integrable Wiener functional
admits a chaos expansion, the individual terms of which can be regarded as
parametric degrees of freedom in the associated interest rate model to be fixed
by calibration to appropriately liquid sectors of the interest rate derivatives
markets.Comment: 17 page
Discrete-Time Interest Rate Modelling
This paper presents an axiomatic scheme for interest rate models in discrete
time. We take a pricing kernel approach, which builds in the arbitrage-free
property and provides a link to equilibrium economics. We require that the
pricing kernel be consistent with a pair of axioms, one giving the
inter-temporal relations for dividend-paying assets, and the other ensuring the
existence of a money-market asset. We show that the existence of a
positive-return asset implies the existence of a previsible money-market
account. A general expression for the price process of a limited-liability
asset is derived. This expression includes two terms, one being the discounted
risk-adjusted value of the dividend stream, the other characterising retained
earnings. The vanishing of the latter is given by a transversality condition.
We show (under the assumed axioms) that, in the case of a limited-liability
asset with no permanently-retained earnings, the price process is given by the
ratio of a pair of potentials. Explicit examples of discrete-time models are
provided
Information, Inflation, and Interest
We propose a class of discrete-time stochastic models for the pricing of
inflation-linked assets. The paper begins with an axiomatic scheme for asset
pricing and interest rate theory in a discrete-time setting. The first axiom
introduces a "risk-free" asset, and the second axiom determines the
intertemporal pricing relations that hold for dividend-paying assets. The
nominal and real pricing kernels, in terms of which the price index can be
expressed, are then modelled by introducing a Sidrauski-type utility function
depending on (a) the aggregate rate of consumption, and (b) the aggregate rate
of real liquidity benefit conferred by the money supply. Consumption and money
supply policies are chosen such that the expected joint utility obtained over a
specified time horizon is maximised subject to a budget constraint that takes
into account the "value" of the liquidity benefit associated with the money
supply. For any choice of the bivariate utility function, the resulting model
determines a relation between the rate of consumption, the price level, and the
money supply. The model also produces explicit expressions for the real and
nominal pricing kernels, and hence establishes a basis for the valuation of
inflation-linked securities
Coherent States and Duality
We formulate a relation between quantum-mechanical coherent states and
complex-differentiable structures on the classical phase space of a
finite number of degrees of freedom. Locally-defined coherent states
parametrised by the points of exist when there is an almost complex
structure on . When admits a complex structure, such
coherent states are globally defined on . The picture of quantum
mechanics that emerges allows to implement duality transformations.Comment: 7 pages, LaTe
Quantum states and space-time causality
Space-time symmetries and internal quantum symmetries can be placed on equal
footing in a hyperspin geometry. Four-dimensional classical space-time emerges
as a result of a decoherence that disentangles the quantum and the space-time
degrees of freedom. A map from the quantum space-time to classical space-time
that preserves the causality relations of space-time events is necessarily a
density matrix.Comment: 9 pages, to appear in the Proceedings of the 2nd International
Symposium on Information Geometry and its Application
Information Content for Quantum States
A method of representing probabilistic aspects of quantum systems is
introduced by means of a density function on the space of pure quantum states.
In particular, a maximum entropy argument allows us to obtain a natural density
function that only reflects the information provided by the density matrix.
This result is applied to derive the Shannon entropy of a quantum state. The
information theoretic quantum entropy thereby obtained is shown to have the
desired concavity property, and to differ from the the conventional von Neumann
entropy. This is illustrated explicitly for a two-state system.Comment: RevTex file, 4 pages, 1 fi
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