Relativistic laser pulse compression and focusing in stratified plasma vacuum systems [Elektronische Ressource] / vorgelegt von Christoph Karle
135
pages
Documents
2007
Le téléchargement nécessite un accès à la bibliothèque YouScribe Tout savoir sur nos offres
135
pages
Documents
2007
Le téléchargement nécessite un accès à la bibliothèque YouScribe Tout savoir sur nos offres
Publié par
Publié le
01 janvier 2007
Nombre de lectures
23
Poids de l'ouvrage
7 Mo
Publié par
Publié le
01 janvier 2007
Nombre de lectures
23
Poids de l'ouvrage
7 Mo
on
Relativistic
der
laser
er
pulse
D?sseldorf
Dinslak
and
F
fo
h-Heine-Univ
orgelegt
in
Karle
stratied
Dezem
plasma-v
hen
acuum
akult?t
systems
Inaugural-Dissertation
ersit?t
zur
v
Erlangung
v
des
Christoph
Doktorgrades
aus
der
en
b
2007
t:
Aus
k
dem
tin:
Institut
25.01.2008
f?r
Spatsc
theoretisc
Ho
he
m
Ph
D?sseldorf
ysik
Dr.
I
K
der
Dr.
h
h-Heine-Univ
ag
ersit?t
hen
D?sseldorf
ersit?t
Gedruc
Referen
kt
Prof.
mit
K.-H.
der
hek
Genehmigung
orreferen
der
Prof.
M.
bruc
hen
T
F
der
akult?t
?ndlic
der
Pr?fung:
h-Heine-Univer
Relativistic
laser
Theo
pulse
rle
Institut
ression
Physik
and
rf
fo
2007
in
f?r
stratied
retische
plasma-vacuum
I
systems
D?sseldo
Christoph
Ka4.
Contents
.
1
the
Intro
Boundaries
.
7
.
2
o
Mo
vs.
del
.
equations
ransversal
10
.
2.1
.
.
Fluid-Maxw
.
ell
.
equations
Stratied
.
.
.
.
.
116
.
equation
.
.
.
lamen
.
.
.
.
.
.
.
with
.
ers
.
.
.
plasma
.
.
.
mo
.
tages
.
.
.
transv
.
.
.
tation
.
.
.
pulse
10
of
2.2
.
Equations
.
for
.
the
4.4
w
.
eakly
.
relativistic
.
regime
2D
.
.
.
.
.
.
.
T
.
ers
.
of
.
.
.
.
.
.
.
een
.
.
.
.
.
5.3
.
v
.
acuum
.
6.1
13
plasma
2.3
.
Slo
.
wly
96
v
.
arying
.
en
.
v
trolling
elop
.
e
.
appro
.
ximation
mo
.
2D
.
122
.
w
.
.
.
Gro
.
.
.
.
.
.
.
5
.
.
.
ransv
.
instabilit
.
.
.
.
.
.
.
.
.
.
.
4.5
.
3D
16
.
3
.
Pulse
.
.
ression
.
in
.
one
76
dimension
fo
18
la
3.1
5.1
Mo
prop
del
la
equations
.
in
.
1D
.
.
.
.
.
.
82
.
et
.
acuum
.
.
.
.
.
.
.
.
.
.
.
of
.
w
.
transv
.
in
.
90
.
systems
.
dv
.
m
.
y
.
.
.
.
.
.
.
.
.
.
.
Optimization
.
fo
.
.
.
.
18
.
3.2
.
.
metho
6.3
ds
ersal
.
.
.
.
.
.
.
.
.
.
.
7
.
V
.
fo
.
ression
.
B
.
instabilit
.
Stationary
.
.
v
.
.
.
.
.
122
.
rate
.
y
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
56
.
T
.
ersal
20
tation
3.3
y
A
.
.
and
.
.
of
.
the
.
n
.
umerical
.
sc
.
heme
.
.
64
.
Other
.
/
.
instabilities
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
24
.
3.4
.
Pulse
.
5
in
ransversal
1D
.
plasma
.
y
.
82
.
F
.
.
erties
.
plasma
.
y
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
5.2
.
b
.
w
.
v
.
and
.
.
.
.
.
.
.
.
.
.
32
.
4
.
Pulse
.
.
ression
87
in
Propagation
t
short
w
long
o
a
dimensions
elength
44
ersal
4.1
des
v
Metho
.
ds
6
.
plasma-vacuum
.
95
.
A
.
an
.
of
.
ultiple
.
la
.
ers
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
6.2
.
of
.
ersal
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
44
.
4.2
.
A
98
Con
and
transv
lamen
of
.
the
.
o
.
v
.
er-all
.
2D
.
sc
.
heme
.
.
.
.
.
.
105
.
Conclusion
.
A
.
AM
.
del
.
r
.
.
in
.
119
.
T
.
lamentation
52
y
4.3
B.1
Pulse
solution
the
in
nonlinear
2D
a
.
e
.
.
.
.
.
.
.
.
.
.
.
B.2
.
wth
.
of
.
instabilit
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
123
.
.125
Contents
129
C
Bibliography
3D
6
instabilitiesQ
Q
14 2I ∼ 10 W/cm
2 18 2 2Iλ ∼ 10 Wμm /cm0
μm
18 2I∼ 10 W/cm
6 12
10 30
b
to
group
surgery
en
and
the
ha
and
v
of
e
fron
b
ecome
whic
an
reac
indisp
ensable
b
to
ol
(or
in
the
scien
o
tic
gets
ossible
h
laser
due
use
to
to
the
hing
y
t
the
nature
e
of
same
laser
the
radiation.
During
the
original
rst
ed
t
stretc
w
o
disp
the
pulses
laser
univ
in
using
tensities
ab
w
laser
ere
th
in
rapidly
A
through
b
the
h
in
tro
ed
a
of
y
from
er
-switc
whic
hing
hing
and
pulse
mo
the
de
The
lo
amplied
the
king.
is
The
us
pulse
y
length
w
a
,
ha
from
exactly
fully
to
pulses
ecome
with
e
applications
Still,
-switc
e
hing
of
and
w
fem
to
lasers
with
mo
in
de
v
lo
1960,
of
k-
in
ing.
allo
This
relativistic
allo
The
w
of
ed
the
in
the
tensities
a
to
to
reac
thousand
h
a
This
umerous
ac
n
y
elding,
propagate
w
with
elo
pro
ersion
material
applications,
b
storage
a
data
has
and
After
already
frequencies,
lead
of
to
red-shifted,
relativistic
k
eects
is
for
v
electrons
hed
b
in
reac
the
limit
eld
medium.
of
infrared
ersed
lasers,
is
as
to
the
to
in
of
tensit
ac
y
this
for
.
relativistic
h
electrons
high,
is
and
digital
e
unication,
matc
otherwise
is
for
ensated.
used
are
higher
y
terms
da
ortan
to
ha
Lasers
b
tous.
to
ubiqui-
is
ecome
ac
b
ery
has
the
hnology
1
.
allo
If
ed
a
ersities
laser
build
pulse
of
at
(e.g.
this
Ti:sapphire
in
that
tensit
h
y
tensities
propagates
o
through
e
a
the
gas,
in
it
the
is
tion
v
ionized
and
and
us
a
w
plasma
study
is
eects
plasmas.
The
relativis-
hanism
CP
mass
is
stretc
then
of
lead
