234 research outputs found
Towards a Novel no-hair Theorem for Black Holes
We provide strong numerical evidence for a new no-scalar-hair theorem for
black holes in general relativity, which rules out spherical scalar hair of
static four dimensional black holes if the scalar field theory, when coupled to
gravity, satisfies the Positive Energy Theorem. This sheds light on the
no-scalar-hair conjecture for Calabi-Yau compactifications of string theory,
where the effective potential typically has negative regions but where
supersymmetry ensures the total energy is always positive. In theories where
the scalar tends to a negative local maximum of the potential at infinity, we
find the no-scalar-hair theorem holds provided the asymptotic conditions are
invariant under the full anti-de Sitter symmetry group.Comment: 25 pages, 11 figure
New Charged Black Holes with Conformal Scalar Hair
A new class of four-dimensional, hairy, stationary solutions of the
Einstein-Maxwell-Lambda system with a conformally coupled scalar field is
constructed in this paper. The metric belongs to the Plebanski-Demianski family
and hence its static limit has the form of the charged C-metric. It is shown
that, in the static case, a new family of hairy black holes arises. They turn
out to be cohomogeneity-two, with horizons that are neither Einstein nor
homogenous manifolds. The conical singularities in the C-metric can be removed
due to the back reaction of the scalar field providing a new kind of regular,
radiative spacetime. The scalar field carries a continuous parameter
proportional to the usual acceleration present in the C-metric. In the
zero-acceleration limit, the static solution reduces to the dyonic
Bocharova-Bronnikov-Melnikov-Bekenstein solution or the dyonic extension of the
Martinez-Troncoso-Zanelli black holes, depending on the value of the
cosmological constant.Comment: Published versio
Coexistence of black holes and a long-range scalar field in cosmology
The exactly solvable scalar hairy black hole model (originated from the
modern high-energy theory) is proposed. It turns out that the existence of
black holes (BH) is strongly correlated to global scalar field, in a sense that
they mutually impose bounds upon their physical parameters like the BH mass
(lower bound) or the cosmological constant (upper bound). We consider the same
model also as a cosmological one and show that it agrees with recent
experimental data; additionally, it provides a unified quintessence-like
description of dark energy and dark matter.Comment: 4 pages, 4 figure
Higher-dimensional solitons and black holes with a non-minimally coupled scalar field
We study higher-dimensional soliton and hairy black hole solutions of the
Einstein equations non-minimally coupled to a scalar field. The scalar field
has no self-interaction potential but a cosmological constant is included.
Non-trivial solutions exist only when the cosmological constant is negative and
the constant governing the coupling of the scalar field to the Ricci scalar
curvature is positive. At least some of these solutions are stable when this
coupling constant is not too large.Comment: 17 pages, revtex4, 21 figures, minor changes to match published
versio
Black holes in scalar-tensor gravity
Hawking has proven that black holes which are stationary as the endpoint of
gravitational collapse in Brans--Dicke theory (without a potential) are no
different than in general relativity. We extend this proof to the much more
general class of scalar-tensor and f(R) gravity theories, without assuming any
symmetries apart from stationarity.Comment: v1: 4 pages; v2: typos corrected, published versio
Conformal couplings of a scalar field to higher curvature terms
We present a simple way of constructing conformal couplings of a scalar field
to higher order Euler densities. This is done by constructing a four-rank
tensor involving the curvature and derivatives of the field, which transforms
covariantly under local Weyl rescalings. The equation of motion for the field,
as well as its energy momentum tensor are shown to be of second order. The
field equations for the spherically symmetric ansatz are integrated, and for
generic non-homogeneous couplings, the solution is given in terms of a
polynomial equation, in close analogy with Lovelock theories.Comment: 9 pages, no figures. Based on a talk given by one of the authors at
Centro de Estudios Cientificos, Valdivia, Chile, on June 22, 2011. V2: 11
pages, no figures. Typos fixed, appendices and references added. v3: to
appear in CQ
THE ROLE OF SIGNALING MOLECULES IN THE DEVELOPMENT OF CHEILITIS CAUSED BY UV IRRADIATION AND SEBORRHEIC ECZEMA
The subject of the study is the establishment of the role of signaling molecules in the development of cheilitis in patients after sensitizing effects on the skin of the red border of the lips of various factors. For this purpose, blood levels of substance P, histamine, tumor necrosis factor-alpha (TNFΞ±) in patients with actinic cheilitis and cheilitis developed against seborrheic eczema were studied. The reliability of the results of clinical and laboratory studies was established by methods of modern statistical processing. It was found that the development of clinical manifestations of lesions of the red border of the lips with sensitizing effects (UV rays and seborrheic process) is reliably associated with a synergistic increase in blood levels of signal molecules of different classes (not opioid neuropeptide, biogenic amine, pro-inflammatory cytokine). The obtained results substantiate new approaches to drawing up plans for examination, treatment and prevention of patients with development of cheilitis after sensitizing effects of UV rays and against seborrheic eczema.Key words: cheilitis (actinic and against the background of seborrheic eczema), signaling molecules (substance P, histamine, TNFΞ±).ΠΊΠ°Π½Π΄ΠΈΠ΄Π°Ρ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΡ
Π½Π°ΡΠΊ, ΠΠΎΡΠ°ΡΠΎΠ²Π° Π.Π., Π΄ΠΎΠΊΡΠΎΡ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΡ
Π½Π°ΡΠΊ, ΠΏΡΠΎΡΠ΅ΡΡΠΎΡ, ΠΠ΅Π±Π΅Π΄ΡΠΊ Π.Π., *Π΄ΠΎΠΊΡΠΎΡ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΡ
Π½Π°ΡΠΊ, ΠΏΡΠΎΡΠ΅ΡΡΠΎΡ, ΠΠΎΡΠ°ΡΠΎΠ² Π.Π., **Π΄ΠΎΠΊΡΠΎΡ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΡ
Π½Π°ΡΠΊ, Π΄ΠΎΡΠ΅Π½Ρ, ΠΡΡ Π.Π. Π ΠΎΠ»Ρ ΡΠΈΠ³Π½Π°Π»ΡΠ½ΡΡ
ΠΌΠΎΠ»Π΅ΠΊΡΠ» Π² ΡΠ°Π·Π²ΠΈΡΠΈΠΈ Ρ
Π΅ΠΉΠ»ΠΈΡΠΎΠ², Π²ΡΠ·Π²Π°Π½Π½ΡΡ
ΡΡ-ΠΎΠ±Π»ΡΡΠ΅Π½ΠΈΠ΅ΠΌ ΠΈ ΡΠ΅Π±ΠΎΡΠ΅ΠΉΠ½ΠΎΠΉ ΡΠΊΠ·Π΅ΠΌΠΎΠΉ/ ΠΠ΄Π΅ΡΡΠΊΠΈΠΉ Π½Π°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΠΉ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΠΉ ΡΠ½ΠΈΠ²Π΅ΡΡΠΈΡΠ΅Ρ, Π£ΠΊΡΠ°ΠΈΠ½Π°, ΠΠ΄Π΅ΡΡΠ°; *ΠΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΠΉ ΠΈΠ½ΡΡΠΈΡΡΡ ΠΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΠΎΠ³ΠΎ Π³ΡΠΌΠ°Π½ΠΈΡΠ°ΡΠ½ΠΎΠ³ΠΎ ΡΠ½ΠΈΠ²Π΅ΡΡΠΈΡΠ΅ΡΠ°, Π£ΠΊΡΠ°ΠΈΠ½Π°, ΠΠ΄Π΅ΡΡΠ°; **ΠΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΈΠΉ ΠΈΠ½ΡΡΠΈΡΡΡ Π‘ΡΠΌΡΠΊΠΎΠ³ΠΎ Π³ΠΎΡΡΠ΄Π°ΡΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ ΡΠ½ΠΈΠ²Π΅ΡΡΠΈΡΠ΅ΡΠ°, Π£ΠΊΡΠ°ΠΈΠ½Π°, Π‘ΡΠΌΡΠΡΠ΅Π΄ΠΌΠ΅ΡΠΎΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠ²Π»ΡΠ΅ΡΡΡ ΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΈΠ΅ ΡΠΎΠ»ΠΈ ΡΠΈΠ³Π½Π°Π»ΡΠ½ΡΡ
ΠΌΠΎΠ»Π΅ΠΊΡΠ» Π² ΡΠ°Π·Π²ΠΈΡΠΈΠΈ Ρ
Π΅ΠΉΠ»ΠΈΡΠΎΠ² Ρ Π±ΠΎΠ»ΡΠ½ΡΡ
ΠΏΠΎΡΠ»Π΅ ΡΠ΅Π½ΡΠΈΠ±ΠΈΠ»ΠΈΠ·ΠΈΡΡΡΡΠΈΡ
Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠΉ Π½Π° ΠΊΠΎΠΆΡ ΠΊΡΠ°ΡΠ½ΠΎΠΉ ΠΊΠ°ΠΉΠΌΡ Π³ΡΠ± ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΡΠ°ΠΊΡΠΎΡΠΎΠ². Π‘ ΡΡΠΎΠΉ ΡΠ΅Π»ΡΡ Π±ΡΠ»ΠΈ ΠΈΠ·ΡΡΠ΅Π½Ρ ΡΡΠΎΠ²Π½ΠΈ ΡΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΈΡ Π² ΠΊΡΠΎΠ²ΠΈ ΡΡΠ±ΡΡΠ°Π½ΡΠΈΠΈ Π , Π³ΠΈΡΡΠ°ΠΌΠΈΠ½Π°, ΡΠ°ΠΊΡΠΎΡΠ° Π½Π΅ΠΊΡΠΎΠ·Π° ΠΎΠΏΡΡ
ΠΎΠ»ΠΈ-Π°Π»ΡΡΠ° (TNFΞ±) Ρ Π±ΠΎΠ»ΡΠ½ΡΡ
Ρ Π°ΠΊΡΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠΌ Ρ
Π΅ΠΉΠ»ΠΈΡΠΎΠΌ ΠΈ Ρ
Π΅ΠΉΠ»ΠΈΡΠΎΠΌ, ΡΠ°Π·Π²ΠΈΠ²ΡΠ΅ΠΌΡΡ Π½Π° ΡΠΎΠ½Π΅ ΡΠ΅Π±ΠΎΡΠ΅ΠΉΠ½ΠΎΠΉ ΡΠΊΠ·Π΅ΠΌΡ. ΠΠΎΡΡΠΎΠ²Π΅ΡΠ½ΠΎΡΡΡ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ Π»Π°Π±ΠΎΡΠ°ΡΠΎΡΠ½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΡΡΡΠ°Π½Π°Π²Π»ΠΈΠ²Π°Π»Π°ΡΡ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠΉ ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ. ΠΡΡΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΠ΅ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΡΠΎΡΠ²Π»Π΅Π½ΠΈΠΉ ΠΏΠΎΡΠ°ΠΆΠ΅Π½ΠΈΡ ΠΊΡΠ°ΡΠ½ΠΎΠΉ ΠΊΠ°ΠΉΠΌΡ Π³ΡΠ± ΠΏΡΠΈ ΡΠ΅Π½ΡΠΈΠ±ΠΈΠ»ΠΈΠ·ΠΈΡΡΡΡΠΈΡ
Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡΡ
(Π£Π€-Π»ΡΡΠ΅ΠΉ ΠΈ ΠΏΡΠΈ ΡΠ΅Π±ΠΎΡΠ΅ΠΉΠ½ΠΎΠΌ ΠΏΡΠΎΡΠ΅ΡΡΠ΅) Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΠΎ ΡΠ²ΡΠ·Π°Π½ΠΎ Ρ ΡΠΈΠ½Π΅ΡΠ³ΠΈΡΠ½ΡΠΌ ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΡΠΎΠ²Π½Π΅ΠΉ Π² ΠΊΡΠΎΠ²ΠΈ ΡΠΈΠ³Π½Π°Π»ΡΠ½ΡΡ
ΠΌΠΎΠ»Π΅ΠΊΡΠ» ΡΠ°Π·Π½ΡΡ
ΠΊΠ»Π°ΡΡΠΎΠ² (Π½Π΅ΠΎΠΏΠΈΠΎΠΈΠ΄Π½ΠΎΠ³ΠΎ Π½Π΅ΠΉΡΠΎΠΏΠ΅ΠΏΡΠΈΠ΄Π°, Π±ΠΈΠΎΠ³Π΅Π½Π½ΠΎΠ³ΠΎ Π°ΠΌΠΈΠ½Π°, ΠΏΡΠΎΠ²ΠΎΡΠΏΠ°Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠΈΡΠΎΠΊΠΈΠ½Π°). ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΎΠ±ΠΎΡΠ½ΠΎΠ²ΡΠ²Π°ΡΡ Π½ΠΎΠ²ΡΠ΅ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄Ρ ΠΊ ΡΠΎΡΡΠ°Π²Π»Π΅Π½ΠΈΡ ΠΏΠ»Π°Π½ΠΎΠ² ΠΎΠ±ΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ, Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΈ ΠΏΡΠΎΡΠΈΠ»Π°ΠΊΡΠΈΠΊΠΈ Π±ΠΎΠ»ΡΠ½ΡΡ
Ρ ΡΠ°Π·Π²ΠΈΡΠΈΠ΅ΠΌ Ρ
Π΅ΠΉΠ»ΠΈΡΠΎΠ² ΠΏΠΎΡΠ»Π΅ ΡΠ΅Π½ΡΠΈΠ±ΠΈΠ»ΠΈΠ·ΠΈΡΡΡΡΠΈΡ
Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠΉ Π£Π€-Π»ΡΡΠ΅ΠΉ ΠΈ Π½Π° ΡΠΎΠ½Π΅ ΡΠ΅Π±ΠΎΡΠ΅ΠΉΠ½ΠΎΠΉ ΡΠΊΠ·Π΅ΠΌΡ.ΠΠ»ΡΡΠ΅Π²ΡΠ΅ ΡΠ»ΠΎΠ²Π°: Ρ
Π΅ΠΉΠ»ΠΈΡΡ (Π°ΠΊΡΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΠΈ Π½Π° ΡΠΎΠ½Π΅ ΡΠ΅Π±ΠΎΡΠ΅ΠΉΠ½ΠΎΠΉ ΡΠΊΠ·Π΅ΠΌΡ), ΡΠΈΠ³Π½Π°Π»ΡΠ½ΡΠ΅ ΠΌΠΎΠ»Π΅ΠΊΡΠ»Ρ (ΡΡΠ±ΡΡΠ°Π½ΡΠΈΡ Π , Π³ΠΈΡΡΠ°ΠΌΠΈΠ½, TNFΞ±).
Dressing a black hole with non-minimally coupled scalar field hair
We investigate the possibility of dressing a four-dimensional black hole with
classical scalar field hair which is non-minimally coupled to the space-time
curvature. Our model includes a cosmological constant but no self-interaction
potential for the scalar field. We are able to rule out black hole hair except
when the cosmological constant is negative and the constant governing the
coupling to the Ricci scalar curvature is positive. In this case, non-trivial
hairy black hole solutions exist, at least some of which are linearly stable.
However, when the coupling constant becomes too large, the black hole hair
becomes unstable.Comment: 17 pages, 7 figures, uses iopart.cls. Minor changes, accepted for
publication in Classical and Quantum Gravit
Cosmology and Static Spherically Symmetric solutions in D-dimensional Scalar Tensor Theories: Some Novel Features
We consider scalar tensor theories in D-dimensional spacetime, D \ge 4. They
consist of metric and a non minimally coupled scalar field, with its non
minimal coupling characterised by a function. The probes couple minimally to
the metric only. We obtain vacuum solutions - both cosmological and static
spherically symmetric ones - and study their properties. We find that, as seen
by the probes, there is no singularity in the cosmological solutions for a
class of functions which obey certain constraints. It turns out that for the
same class of functions, there are static spherically symmetric solutions which
exhibit novel properties: {\em e.g.} near the ``horizon'', the gravitational
force as seen by the probe becomes repulsive.Comment: Revtex. 21 pages. Version 2: More references added. Version 3: Issues
raised by the referee are addressed. Results unchanged. Title modified; a new
subsection and more references added. Verison to appear in Physical Review
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