259,307 research outputs found
The role of Vitamin D and Parathyroid Hormone in Cardiovascular Health
Visser, M. [Promotor]Brouwer, I.A. [Copromotor
Quantum Interest in (3+1) dimensional Minkowski space
The so-called "Quantum Inequalities", and the "Quantum Interest Conjecture",
use quantum field theory to impose significant restrictions on the temporal
distribution of the energy density measured by a time-like observer,
potentially preventing the existence of exotic phenomena such as "Alcubierre
warp-drives" or "traversable wormholes". Both the quantum inequalities and the
quantum interest conjecture can be reduced to statements concerning the
existence or non-existence of bound states for a certain one-dimensional
quantum mechanical pseudo-Hamiltonian. Using this approach, we shall provide a
simple proof of one version of the Quantum Interest Conjecture in (3+1)
dimensional Minkowski space.Comment: V1: 8 pages, revtex4; V2: 10 pages, some technical changes in details
of the argument, no change in physics conclusions, this version essentially
identical to published versio
Lambda theories of effective lambda models
A longstanding open problem is whether there exists a non-syntactical model
of untyped lambda-calculus whose theory is exactly the least equational
lambda-theory (=Lb). In this paper we make use of the Visser topology for
investigating the more general question of whether the equational (resp. order)
theory of a non syntactical model M, say Eq(M) (resp. Ord(M)) can be
recursively enumerable (= r.e. below). We conjecture that no such model exists
and prove the conjecture for several large classes of models. In particular we
introduce a notion of effective lambda-model and show that for all effective
models M, Eq(M) is different from Lb, and Ord(M) is not r.e. If moreover M
belongs to the stable or strongly stable semantics, then Eq(M) is not r.e.
Concerning Scott's continuous semantics we explore the class of (all) graph
models, show that it satisfies Lowenheim Skolem theorem, that there exists a
minimum order/equational graph theory, and that both are the order/equ theories
of an effective graph model. We deduce that no graph model can have an r.e.
order theory, and also show that for some large subclasses, the same is true
for Eq(M).Comment: 15 pages, accepted CSL'0
An algorithm for the Baker-Campbell-Hausdorff formula
A simple algorithm, which exploits the associativity of the BCH formula, and
that can be generalized by iteration, extends the remarkable simplification of
the Baker-Campbell-Hausdorff (BCH) formula, recently derived by Van-Brunt and
Visser. We show that if
, , and, consistently with the Jacobi
identity, , then where , , and are
solutions of four equations. In particular, the Van-Brunt and Visser formula
extends to cases when
contains also elements different from and . Such a closed form of the
BCH formula may have interesting applications both in mathematics and physics.
As an application, we provide the closed form of the BCH formula in the case of
the exponentiation of the Virasoro algebra, with
following as a subcase. We also determine three-dimensional subalgebras of the
Virasoro algebra satisfying the Van-Brunt and Visser condition. It turns out
that the exponential form of has a nice representation in
terms of its eigenvalues and of the
fixed points of the corresponding M\"obius transformation. This may have
applications in Uniformization theory and Conformal Field Theories.Comment: 1+8 pages. Comments and refences added. Typos corrected. Version to
appear in JHE
Stable gravastars with generalised exteriors
New spherically symmetric gravastar solutions, stable to radial
perturbations, are found by utilising the construction of Visser and Wiltshire.
The solutions possess an anti--de Sitter or de Sitter interior and a
Schwarzschild--(anti)--de Sitter or Reissner--Nordstr\"{o}m exterior. We find a
wide range of parameters which allow stable gravastar solutions, and present
the different qualitative behaviours of the equation of state for these
parameters.Comment: 14 pages, 11 figures, to appear in Classical and Quantum Gravit
Horizon constraints and black hole entropy
To ask a question about a black hole in quantum gravity, one must restrict
initial or boundary data to ensure that a black hole is actually present. For
two-dimensional dilaton gravity, and probably a much wider class of theories as
well, the imposition of a "stretched horizon" constraint alters the algebra of
symmetries at the horizon, introducing a central term. Standard conformal field
theory techniques can then then be used to obtain the asymptotic density of
states, reproducing the Bekenstein-Hawking entropy. The microscopic states
responsible for black hole entropy can thus be viewed as "would-be pure gauge"
states that become physical because the symmetry is altered by the requirement
that a horizon exist.Comment: 20 pages, to appear in "The Kerr spacetime: rotating black holes in
general relativity," edited by S. Scott, M. Visser, and D. Wiltshire
(Cambridge University Press
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