scholarly journals Focal surfaces of hyperbolic cylinders

Author(s):  
Georgi Hristov Georgiev ◽  
Milen Dimov Pavlov
Keyword(s):  
2021 ◽  
Vol 2021 (1) ◽  
Author(s):  
Justin R. David ◽  
Jyotirmoy Mukherjee

Abstract We show that the entanglement entropy of D = 4 linearized gravitons across a sphere recently computed by Benedetti and Casini coincides with that obtained using the Kaluza-Klein tower of traceless transverse massive spin-2 fields on S1× AdS3. The mass of the constant mode on S1 saturates the Brietenholer-Freedman bound in AdS3. This condition also ensures that the entanglement entropy of higher spins determined from partition functions on the hyperbolic cylinder coincides with their recent conjecture. Starting from the action of the 2-form on S1× AdS5 and fixing gauge, we evaluate the entanglement entropy across a sphere as well as the dimensions of the corresponding twist operator. We demonstrate that the conformal dimensions of the corresponding twist operator agrees with that obtained using the expectation value of the stress tensor on the replica cone. For conformal p-forms in even dimensions it obeys the expected relations with the coefficients determining the 3-point function of the stress tensor of these fields.


2012 ◽  
Vol 393 (1) ◽  
pp. 166-176 ◽  
Author(s):  
R.M.B. Chaves ◽  
L.A.M. Sousa ◽  
B.C. Valério

1915 ◽  
Vol 34 ◽  
pp. 176-196 ◽  
Author(s):  
John Dougall

The determination of the harmonic functions of elliptic and hyperbolic cylinders depends on the solution of Mathieu's differential equation. This equation, it has been remarked by Professor Whittaker, is the one which naturally comes up for study after the hypergeometric equation has been disposed of. Its solution presents difficulties which do not arise in connection with the hypergeometric equation or its degenerate cases, and it cannot, I think, be said that any discussion of the equation has yet been given with which the student of analysis can rest content. The treatment given below, though certainly incomplete at some points, seetns to follow the lines along which a thoroughly successful theory may be hoped for.


2020 ◽  
Vol 126 (1) ◽  
pp. 61-72
Author(s):  
Cícero P. Aquino ◽  
Halyson I. Baltazar ◽  
Henrique F. De Lima

In this article, we deal with complete spacelike hypersurfaces immersed in an open region of the de Sitter space $\mathbb {S}^{n+1}_{1}$ which is known as the steady state space $\mathcal {H}^{n+1}$. Under suitable constraints on the behavior of the higher order mean curvatures of these hypersurfaces, we are able to prove that they must be spacelike hyperplanes of $\mathcal {H}^{n+1}$. Furthermore, through the analysis of the hyperbolic cylinders of $\mathcal {H}^{n+1}$, we discuss the importance of the main hypothesis in our results. Our approach is based on a generalized maximum principle at infinity for complete Riemannian manifolds.


2021 ◽  
Vol 2021 (10) ◽  
Author(s):  
Jyotirmoy Mukherjee

Abstract The character integral representation of one loop partition functions is useful to establish the relation between partition functions of conformal fields on Weyl equivalent spaces. The Euclidean space Sa × AdSb can be mapped to Sa+b provided Sa and AdSb are of the same radius. As an example, to begin with, we show that the partition function in the character integral representation of conformally coupled free scalars and fermions are identical on Sa × AdSb and Sa+b. We then demonstrate that the partition function of higher derivative conformal scalars and fermions are also the same on hyperbolic cylinders and branched spheres. The partition function of the four-derivative conformal vector gauge field on the branched sphere in d = 6 dimension can be expressed as an integral over ‘naive’ bulk and ‘naive’ edge characters. However, the partition function of the conformal vector gauge field on $$ {S}_q^1 $$ S q 1 × AdS5 contains only the ‘naive’ bulk part of the partition function. This follows the same pattern which was observed for the partition of conformal p-form fields on hyperbolic cylinders. We use the partition function of higher derivative conformal fields on hyperbolic cylinders to obtain a linear relationship between the Hofman-Maldacena variables which enables us to show that these theories are non-unitary.


1966 ◽  
Vol 40 (6) ◽  
pp. 1534-1539 ◽  
Author(s):  
Ebenezer N. Krishnappa ◽  
W. R. Callahan
Keyword(s):  

1927 ◽  
Vol 46 ◽  
pp. 206-209 ◽  
Author(s):  
Pierre Humbert

It is well known that two problems of harmonic analysis in ordinary three-dimensional space can be solved by Mathieu's functions, namely, (a) harmonic analysis for an orthogonal system of elliptic (or hyperbolic) cylinders,(b) harmonic analysis for a system of confocal paraboloïds,


The analysis of wave motion connected with the circular disc and circular aperture is of such great analytical and physical interest, that no excuse is required for a somewhat extended treatment. The theory of wave motion has been very fully developed when the surfaces bounding the medium in which the motion takes place are spheres and circular cones, or cylinders and planes. The functions involved in the analysis are of the hypergeometric type. Next in order of importance is the theory required for the treatment of problems in which the surfaces bounding the medium are :— A. Ellipsoids of revolution and hyperboloids of revolution of one and two sheets ; B. Elliptic and hyperbolic cylinders. The functions involved in case A are functions associated with the ellipsoid of revolution, or spheroid. The functions involved in case B are commonly called MATHIEU functions. The MATHIEU functions and the functions associated with the ellipsoid of revolution are of considerable importance but, unfortunately, of great complexity.


2016 ◽  
Vol 434 (1) ◽  
pp. 765-779
Author(s):  
Henrique F. de Lima ◽  
Fábio R. dos Santos ◽  
Marco Antonio L. Velásquez

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