Advanced Accelerator Concepts -...
55
Rasmus Ischebeck – Advanced Accelerator Concepts. 2009-04-29 Advanced Accelerator Concepts Rasmus Ischebeck, Paul Scherrer Institut Accelerators for Basic Research and Applications Present Technologies Dielectric Structures Plasma Wakefield Accelerators
Transcript of Advanced Accelerator Concepts -...
Rasm
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ajim
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PR
L,
43
, 2
67
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79
)
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eled
driv
ebe
am
Gui
ding
ove
r >
10
ZR
~ 2
mm
rela
tivis
tic in
tens
ity
11/1
9/0
3gv
1
Inpu
t
Vac
uum
Out
put
Ung
uide
dO
utpu
t
11/1
9/0
3
Gi
2
Gui
ded
Out
put
Hig
hqu
ality
guid
ing
upto
4TW
No
chan
nel l
eaka
geC
hann
el p
rofil
e
C.G
.R.G
edde
set
al,P
RL,
2005
Cam
ero
n G
eddes
22
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us
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nce
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once
pts
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00
9-0
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9�
Pla
sma W
ave
guid
es
~3
5µ
m
Rad
ially
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ps
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ser
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ula
ted
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sm
aw
ave
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ide
70
fsT
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ap
ph
ire
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er
pu
lse
Axic
on
(e)
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(a)
70
fstr
an
sve
rse
inte
rfer.
pro
be
13
µm 10
00
µm2
00µ
m
(e)
13
µm
(c)
(d)
65
0µ
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50
0µ
m
50
µm
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oron
lin
e)E
xper
imen
talg
eom
etry
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iall
ym
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late
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AG
lase
rpu
lse
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–50
0m
J,10
0ps
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4n
m)
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ndre
w Y
ork
Arg
on
Air
Nitro
ge
n
Ph
ase
Im
ag
es f
rom
tra
nsve
rse
pro
be
23
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
Pla
sma A
ccele
rati
on in C
apilla
ries
Jens
Ost
erh
o�
,Ste
fan K
ars
ch
Ga
s i
n
Ch
an
nel cen
ter
15
mm
Off
-ax
is p
ara
bo
la(2
0°,
1.5
4 m
, f/
22
)
La
se
r
Ga
s i
n
Sa
pp
hir
e b
loc
k
Dip
ole
ma
gn
et
Screen S2
Screen S1(movable)
Ele
ctr
on
be
am
25
0 µ
m
Gas velocity (km/s)
2.4
2.0
1.6
1.2
0.8
0.4
Ch
an
nel en
tran
ce a
nd
exit
0.6
mm
1.8
mm
a)
b)
Mk
140
250
)
24
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
“Monoenerg
eti
c” P
art
icle
Bunch
es
Hig
hq
ual
ity,
inte
nse
bea
ms*
2e9
elec
tron
sD
iver
genc
e3m
rad
Ene
rgy
Spr
ead<
4MeV
Nor
mal
ized
Geo
met
ricE
mitt
ance
2�m
m-m
rad
e-
Mag
netic
Spe
ctro
met
er
Mag
net
CC
D
LA
NE
X
Sli
t
7%
>1
15
2%
>1
34
Em
ax=
15
34927500-1
0.1
Am
p
Divergence
(mrad)
>1
15
MeV
>1
53
MeV
>1
34
MeV
Hig
h qu
ality
bea
ms:
300
pC @
86
MeV
Pea
k en
ergi
es 1
50-1
70M
eV
Las
er=
9TW
,50
fs,Z
R=
200μ
mP
lasm
a=
1.8e
19cm
-3,1
.7m
m
Cam
ero
n G
eddes
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
Part
icle
Energ
ies
up t
o 1
GeV
��a
0 ~
1.4
6 (
40 T
W, 37 fs)
��n
e ~
4x10
18
cm
-3,P
crit ~
7 T
W
1 G
eV B
EA
M�
��
Div
erge
nce(
rms)
: 1.6
mra
d���
Ene
rgy
spre
ad (
rms)
: 2.5
%�
��
Res
olut
ion:
2.4
%�
��
Cha
rge:
35
pC�
Cam
ero
n G
eddes
25
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
Pla
sma W
akefi
eld
Acc
ele
rati
on
wit
h E
lect
ron B
unch
es
U C
L
A
~ 0
.5
m~
10
m
26
Energ
y so
urc
e:
ele
ctro
n b
eam
•4
2 G
eV
part
icle
energ
y
•3
.2 n
C b
unch
charg
e
•Beam
pow
er:
�1
015
W =
1 T
W
•Pow
er
densi
ty: �1
024
W/m
2=
1 Y
W/m
2
Pla
sma s
ourc
e:
Lith
ium
ove
n
•Part
icle
densi
ty: �1
023
/ m
3
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
6 m
m
0.0
8 %
1.2
mm
1.6
%
5
0 μ
m
1.6
%
1
2 μ
m
1.5
%
Pla
sma W
akefi
eld
Acc
ele
rati
on a
t SLA
C
Acc
ele
rati
on,
com
pre
ssio
n a
nd f
ocu
ssin
g o
f bunch
es
to r
each
a p
eak p
ow
er
densi
ty o
f 5
YW
/m2
Paul Em
ma
P.
Em
ma e
t al.,
PA
C
(20
05
)
U C
L
A
27
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
Experi
menta
l Setu
pU
C
L
A
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
Firs
t Resu
lts
More
than 3
GeV
energ
y g
ain
in 1
0 c
m p
lasm
a length
U C
L
A
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
Incr
easi
ng t
he P
lasm
a L
ength
to 3
0.5
cm
Patr
ic M
uggli
no p
lasm
a
13
cm
FW
HM
2
2.5
cm
FW
HM
3
0.5
cm
FW
HM
U C
L
A
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
1 m
Long P
lasm
a
Longer
pla
sm
a o
ven
New
spectr
om
ete
r
Dia
gnosti
cs f
or
low
-energ
y p
art
icle
s
Incre
ased t
he e
nerg
y in t
he d
rive b
eam
U C
L
A
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
Images
from
both
Spect
rom
ete
r Pla
nes
800 C
onse
cuti
ve E
vents
Cha
rge
dens
ity[-
e/μ
m2 ]
60120
180
240
U C
L
A
31
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
Energ
y D
oubling
•Pla
sma length
: 85 c
m
•D
ensi
ty: 2,7
•10
17
cm
3
•Entr
ance
energ
y: 4
2 G
eV
•Peak e
nerg
y: 8
5 G
eV
I. B
lum
enfe
ld e
t al.,
Natu
re 4
45
, p.
74
1 (
20
07
)
U C
L
A
32
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
Tra
ppin
g o
f Pla
sma E
lect
rons
•V
ery
sm
all a
ngle
of
em
issi
on a
t th
epla
sma e
xit
:
•Li
mit
ed b
yca
mera
reso
luti
on
Rasm
us Ischebeck,
Energ
y D
oubling o
f 4
2 G
eV
Ele
ctr
ons.
AA
C 2
00
6
U C
L
A
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
Tra
ppin
g o
f Pla
sma E
lect
rons
(Short
Pla
sma)
•Im
agin
g t
he a
ngle
of
ere
nkov
radia
tion
•Li
ght
inte
nsi
ty is
incr
ease
d b
y m
ore
than t
hre
e o
rders
of
magnit
ude
•Part
icle
energ
y E is
pro
port
ional to
pla
sma length
L:
wit
hout
pla
sm
aw
ith p
lasm
a
Neil
Kir
by
N.
Kir
by e
t al.,
AIP
Conf
Pro
c 8
77
(20
06
)
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
There
is
More
to A
ccele
rati
ng S
truct
ure
s th
an t
he A
ccele
rati
ng F
ield
•Pow
er
sourc
es
•Beam
loadin
g•
Em
itta
nce
pre
serv
ati
on
There
is
Much
More
to a
n A
ccele
rato
r th
an A
ccele
rati
ng S
truct
ure
s•
Part
icle
sourc
es
(inje
ctors
)•
Bend m
agnets
for
stora
ge r
ings
•Fo
cusi
ng,
beam
dyn
am
ics
•D
ete
ctors
Dem
onst
rate
d O
nce
does
not
mean
Ava
ilable
for
Use
rs
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
But
•Fu
ture
part
icle
acc
ele
rato
rs c
annot
be b
uilt
wit
h t
oday’
s te
chnolo
gie
s
36
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
Livi
ngst
on P
lot
1
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
An U
nfa
ir C
om
pari
son
34
Rasm
us
Isch
ebeck
– A
dva
nce
d A
ccele
rato
r C
once
pts
. 2
00
9-0
4-2
9�
Thank Y
ou!
•The E
-167 C
ollabora
tion
•M
. Berr
y, I. Blu
menfe
ld, F.
-J. D
eck
er,
P. Em
ma, M
.J. H
ogan*,
R. Is
chebeck
, R.H
. Iv
ers
on, N
. K
irby,
P. K
rejc
ik,
R.H
. Sie
mann, and D
. W
alz
(SLA
C)
•C
.E. C
layt
on, C
. H
uang, D
. Jo
hnso
n, C
. Jo
shi*
, W
. Lu
, K
.A. M
ars
h, W
.B. M
ori
, and M
. Zhou (
UC
LA)
•S.�D
eng, T. K
ats
oule
as,
P.�M
uggli*
and E
.�O
z (
USC
)
•The E
-163 C
ollabora
tion
•R. Sie
mann, R. N
oble
, E. C
olb
y, J. Spence
r, R
. Is
chebeck
, M
. Li
nco
ln, B. C
ow
an, C
. Sears
, S. Tanta
wi, D
. W
alz
, D
.T. Palm
er,
N. N
a, C
.D. Barn
es,
M. Ja
vanm
ara
d, X.E
. Li
n, and Z
. Zhang (
SLA
C)
•R. Bye
r, T
.I. Sm
ith, Y.C
. H
uang, T. Ple
ttner,
P. Lu
, and J.A
. W
isdom
(Sta
nfo
rd)
•L.
Sch
äch
ter
(Tech
ion Isr
aeli Inst
itute
of
Tech
nolo
gy)
•J. R
ose
nzw
eig
(U
CLA
)
•The G
igaW
ake D
iele
ctri
c A
ccele
rato
r Experi
ment
•M
.C. Thom
pso
n, H
. Badakov,
J. Rose
nzw
eig
, and G
. Tra
vish
(U
CLA
)•
M.J. H
ogan, R. Is
chebeck
, N
. K
irby,
R. Sie
mann, and D
. W
alz
(SLA
C)
•P. M
uggli (
USC
)•
A. Sco
tt (
UC
SB)
•R. Yoder
(Manhatt
an C
ollege)
•Speci
al th
anks
for
resu
lts,
plo
ts a
nd illust
rati
ons
•H
. W
eis
e (
DESY),
F. Teck
er,
D. Sutt
er
(DO
E),
N. K
irby
(SLA
C),
E. O
z (
USC
), A
. York
, H
. M
ilch
berg
(U
MD
)•
S. Jo
hnso
n (
MTI), S. K
ars
ch (
MPQ
), inte
ract
ions.
org
, Paul Em
ma (
SLA
C),
JLN
Labs,
Vari
an, Sie
mens
AG
,•
Pete
r G
inte
r
•W
ork
support
ed b
y D
epart
ment
of
Energ
y co
ntr
act
s D
E-A
C02-76SF0
0515 (
SLA
C),
DE-FG
03-92ER40745, D
E-
FG03-98D
P00211, D
E-FG
03-92ER40727, D
E-A
C-0376SF0
098, D
E-A
C02-76SF0
0515 a
nd N
ati
onal Sci
ence
Fo
undati
on g
rants
No. EC
S-9632735, D
MS-9722121 a
nd P
HY-0078715.
http://people.web.psi.ch/ischebeck
