Abstract
AbstractLet H be a (past directed) horizon in a time-oriented Lorentz manifold and $$\gamma :[\left( \alpha ,\beta \right) \rightarrow H$$
γ
:
[
α
,
β
→
H
a past directed generator of the horizon, where $$[\left( \alpha ,\beta \right) $$
[
α
,
β
is $$[\alpha ,\beta )$$
[
α
,
β
)
or $$\left( \alpha ,\beta \right) $$
α
,
β
. It is proved that either at every point of $$\gamma \left( t\right) ,~t\in \left( \alpha ,\beta \right) $$
γ
t
,
t
∈
α
,
β
the differentiability order of H is the same, or there is a so-called differentiability jumping point $$\gamma \left( t_{0}\right) ,~t_{0}\in \left( \alpha ,\beta \right) $$
γ
t
0
,
t
0
∈
α
,
β
such that H is only differentiable at every point $$\gamma \left( t\right) ,~t\in \left( \alpha ,t_{0}\right) $$
γ
t
,
t
∈
α
,
t
0
but not of class $$C^{1}$$
C
1
and H is exactly of class $$C^{1}$$
C
1
at every point $$\gamma \left( t\right) ,~t\in \left( t_{0},\beta \right) $$
γ
t
,
t
∈
t
0
,
β
. We will use in the proof a result which shows that every mathematical horizon in the sense of P. T. Chruściel locally coincides with a Cauchy horizon.
Publisher
Springer Science and Business Media LLC
Subject
Mathematical Physics,Nuclear and High Energy Physics,Statistical and Nonlinear Physics
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