• Aucun résultat trouvé

Errata : “Cylindrically symmetric Einstein-Maxwell and scalar fields and stiff fluid distributions”

N/A
N/A
Protected

Academic year: 2022

Partager "Errata : “Cylindrically symmetric Einstein-Maxwell and scalar fields and stiff fluid distributions”"

Copied!
3
0
0

Texte intégral

(1)

A NNALES DE L ’I. H. P., SECTION A

G. M OHANTY

R. N. T IWARI J. R. R AO

Errata : “Cylindrically symmetric Einstein-Maxwell and scalar fields and stiff fluid distributions”

Annales de l’I. H. P., section A, tome 39, n

o

1 (1983), p. 99-100

<http://www.numdam.org/item?id=AIHPA_1983__39_1_99_0>

© Gauthier-Villars, 1983, tous droits réservés.

L’accès aux archives de la revue « Annales de l’I. H. P., section A » implique l’accord avec les conditions générales d’utilisation (http://www.numdam.

org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright.

Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques

http://www.numdam.org/

(2)

99

ERRATA

Cylindrically Symmetric

Einstein - Maxwell and scalar fields and stiff fluid distributions

by

G. MOHANTY

(*),

R. N. TIWARI and J. R. RAO Department of Mathematics, Indian Institute of Technology,

Kharagpur, 721302 (W. B) India

Ann. Henri Poincaré, # Vol. XXXIX, 1, 1983,

Section A :

Physique theorique.

Page

240 : The first line should read 1~

where ð == 2 + - - is the

Laplace

operator...

~ 3r r~r

Equation (3.2)

should read

Page

241 : The relation

(3.9)

should read

244 : V,

03B2 and p

in case should read

V = k log r + at + e

(*) Present address, P. G. Department of Mathematics, Khallikote college, Berhampur,

76000, Orissa, India. j

Vol. XXXIX, 1-1983.

(3)

Page 245 : The relation

(3 . 32)

should read

and the second line from bottom should read

Références

Documents relatifs

In summary, we have employed entangled states of classical Maxwell fields coupling the polarization and spatial parity degrees of freedom in order to implement the analog of

We then show that the form of the unbiased estimator of the quadratic prediction loss under a Gaussian assumption still holds under a more general distributional assumption, the

This problem asks for, given a smooth compact Riemannian manifold with boundary, the existence of a conformally related metric with zero scalar curvature and constant mean

We therefore study in section 4.3 solutions the boundary conditions of which, while being again nonpolynomial, can be resummed into bounded functions of the field variable and thus

In Section IV, the use of Lagrange’s formula [8, 10] for Taylor’s remainder in connection with partition of unity test functions is shown to simplify also the analysis of

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des

For example, the canonical parametrization of the stress equations is just described by the formal adjoint of the n 2 (n 2 − 1)/12 components of the linearized Riemann tensor