144 research outputs found
A Quartic Conformally Covariant Differential Operator for Arbitrary Pseudo-Riemannian Manifolds (Summary)
This is the original manuscript dated March 9th 1983, typeset by the Editors
for the Proceedings of the Midwest Geometry Conference 2007 held in memory of
Thomas Branson. Stephen Paneitz passed away on September 1st 1983 while
attending a conference in Clausthal and the manuscript was never published. For
more than 20 years these few pages were circulated informally. In November
2004, as a service to the mathematical community, Tom Branson added a scan of
the manuscript to his website. Here we make it available more formally. It is
surely one of the most cited unpublished articles. The differential operator
defined in this article plays a key role in conformal differential geometry in
dimension 4 and is now known as the Paneitz operator.Comment: This is a contribution to the Proceedings of the 2007 Midwest
Geometry Conference in honor of Thomas P. Branson, published in SIGMA
(Symmetry, Integrability and Geometry: Methods and Applications) at
http://www.emis.de/journals/SIGMA
Indecomposable finite-dimensional representations of a class of Lie algebras and Lie superalgebras
In the article at hand, we sketch how, by utilizing nilpotency to its fullest
extent (Engel, Super Engel) while using methods from the theory of universal
enveloping algebras, a complete description of the indecomposable
representations may be reached. In practice, the combinatorics is still
formidable, though.
It turns out that the method applies to both a class of ordinary Lie algebras
and to a similar class of Lie superalgebras.
Besides some examples, due to the level of complexity we will only describe a
few precise results. One of these is a complete classification of which ideals
can occur in the enveloping algebra of the translation subgroup of the
Poincar\'e group. Equivalently, this determines all indecomposable
representations with a single, 1-dimensional source. Another result is the
construction of an infinite-dimensional family of inequivalent representations
already in dimension 12. This is much lower than the 24-dimensional
representations which were thought to be the lowest possible. The complexity
increases considerably, though yet in a manageable fashion, in the
supersymmetric setting. Besides a few examples, only a subclass of ideals of
the enveloping algebra of the super Poincar\'e algebra will be determined in
the present article.Comment: LaTeX 14 page
Positive mass theorem for the Paneitz-Branson operator
We prove that under suitable assumptions, the constant term in the Green
function of the Paneitz-Branson operator on a compact Riemannian manifold
is positive unless is conformally diffeomophic to the standard
sphere. The proof is inspired by the positive mass theorem on spin manifolds by
Ammann-Humbert.Comment: 7 page
A New Family of Gauges in Linearized General Relativity
For vacuum Maxwell theory in four dimensions, a supplementary condition
exists (due to Eastwood and Singer) which is invariant under conformal
rescalings of the metric, in agreement with the conformal symmetry of the
Maxwell equations. Thus, starting from the de Donder gauge, which is not
conformally invariant but is the gravitational counterpart of the Lorenz gauge,
one can consider, led by formal analogy, a new family of gauges in general
relativity, which involve fifth-order covariant derivatives of metric
perturbations. The admissibility of such gauges in the classical theory is
first proven in the cases of linearized theory about flat Euclidean space or
flat Minkowski space-time. In the former, the general solution of the equation
for the fulfillment of the gauge condition after infinitesimal diffeomorphisms
involves a 3-harmonic 1-form and an inverse Fourier transform. In the latter,
one needs instead the kernel of powers of the wave operator, and a contour
integral. The analysis is also used to put restrictions on the dimensionless
parameter occurring in the DeWitt supermetric, while the proof of admissibility
is generalized to a suitable class of curved Riemannian backgrounds.
Eventually, a non-local construction is obtained of the tensor field which
makes it possible to achieve conformal invariance of the above gauges.Comment: 28 pages, plain Tex. In the revised version, sections 4 and 5 are
completely ne
Singular limits for the bi-laplacian operator with exponential nonlinearity in
Let be a bounded smooth domain in such that for
some integer its -th singular cohomology group with coefficients in
some field is not zero, then problem
{\Delta^{2}u-\rho^{4}k(x)e^{u}=0 & \hbox{in}\Omega,
u=\Delta u=0 & \hbox{on}\partial\Omega,
has a solution blowing-up, as , at points of , for any
given number .Comment: 30 pages, to appear in Ann. IHP Non Linear Analysi
Vacuum polarization in Schwarzschild space-time by anomaly induced effective actions
The characteristic features of in the Boulware, Unruh and
Hartle-Hawking states for a conformal massless scalar field propagating in the
Schwarzschild space-time are obtained by means of effective actions deduced by
the trace anomaly. The actions are made local by the introduction of auxiliary
fields and boundary conditions are carefully imposed on them in order to select
the different quantum states.Comment: 20 pages, latex; misprints corrected and references adde
Back reaction of vacuum and the renormalization group flow from the conformal fixed point
We consider the GUT-like model with two scalar fields which has infinitesimal
deviation from the conformal invariant fixed point at high energy region. In
this case the dominating quantum effect is the conformal trace anomaly and the
interaction between the anomaly-generated propagating conformal factor of the
metric and the usual dimensional scalar field. This interaction leads to the
renormalization group flow from the conformal point. In the supersymmetric
conformal invariant model such an effect produces a very weak violation of
sypersymmetry at lower energies.Comment: 15 pages, LaTex, ten figures, uuencoded fil
Quantum mechanics on spaces of nonconstant curvature: the oscillator problem and superintegrability
The full spectrum and eigenfunctions of the quantum version of a nonlinear
oscillator defined on an N-dimensional space with nonconstant curvature are
rigorously found. Since the underlying curved space generates a
position-dependent kinetic energy, three different quantization prescriptions
are worked out by imposing that the maximal superintegrability of the system
has to be preserved after quantization. The relationships among these three
Schroedinger problems are described in detail through appropriate similarity
transformations. These three approaches are used to illustrate different
features of the quantization problem on N-dimensional curved spaces or,
alternatively, of position-dependent mass quantum Hamiltonians. This quantum
oscillator is, to the best of our knowledge, the first example of a maximally
superintegrable quantum system on an N-dimensional space with nonconstant
curvature.Comment: 26 pages, 5 figure
Conformally invariant bending energy for hypersurfaces
The most general conformally invariant bending energy of a closed
four-dimensional surface, polynomial in the extrinsic curvature and its
derivatives, is constructed. This invariance manifests itself as a set of
constraints on the corresponding stress tensor. If the topology is fixed, there
are three independent polynomial invariants: two of these are the
straighforward quartic analogues of the quadratic Willmore energy for a
two-dimensional surface; one is intrinsic (the Weyl invariant), the other
extrinsic; the third invariant involves a sum of a quadratic in gradients of
the extrinsic curvature -- which is not itself invariant -- and a quartic in
the curvature. The four-dimensional energy quadratic in extrinsic curvature
plays a central role in this construction.Comment: 16 page
Logarithmic correction to BH entropy as Noether charge
We consider the role of the type-A trace anomaly in static black hole
solutions to semiclassical Einstein equation in four dimensions. Via Wald's
Noether charge formalism, we compute the contribution to the entropy coming
from the anomaly induced effective action and unveil a logarithmic correction
to the Bekenstein-Hawking area law.
The corrected entropy is given by a seemingly universal formula involving the
coefficient of the type-A trace anomaly, the Euler characteristic of the
horizon and the value at the horizon of the solution to the uniformization
problem for Q-curvature. Two instances are examined in detail: Schwarzschild
and a four-dimensional massless topological black hole. We also find agreement
with the logarithmic correction due to one-loop contribution of conformal
fields in the Schwarzschild background.Comment: 14 pages, JHEP styl
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