Effect of a cylindrical thin-shell of matter on the electrostatic self-force on a charge
The electrostatic self-force on a point charge in cylindrical thin-shell space-times is interpreted as the sum of a bulk field and a shell field. The bulk part corresponds to a field sourced by the test charge placed in a space-time without the shell. The shell field accounts for the discontinuity o...
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Published in | The European physical journal. C, Particles and fields Vol. 76; no. 2; p. 1 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
Berlin/Heidelberg
Springer Berlin Heidelberg
22.02.2016
Springer Springer Nature B.V |
Subjects | |
Online Access | Get full text |
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Summary: | The electrostatic self-force on a point charge in cylindrical thin-shell space-times is interpreted as the sum of a
bulk
field and a
shell
field. The
bulk
part corresponds to a field sourced by the test charge placed in a space-time without the shell. The
shell
field accounts for the discontinuity of the extrinsic curvature
κ
p
q
. An equivalent electric problem is stated, in which the effect of the shell of matter on the field is reconstructed with the electric potential produced by a non-gravitating charge distribution of total image charge
Q
, to interpret the shell field in both the interior and exterior regions of the space-time. The self-force on a point charge
q
in a locally flat geometry with a cylindrical thin-shell of matter is calculated. The charge is repelled from the shell if
κ
p
p
=
κ
<
0
(ordinary matter) and attracted toward the shell if
κ
>
0
(exotic matter). The total image charge is zero for exterior problems, while for interior problems
Q
/
q
=
-
κ
r
e
, with
r
e
the external radius of the shell. The procedure is general and can be applied to interpret self-forces in other space-times with shells, e.g., for locally flat wormholes we found
Q
∓
w
h
/
q
=
-
1
/
(
κ
w
h
r
±
)
. |
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ISSN: | 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-016-3939-6 |