impact of the cathode roughness on the emittance of an electron beam m.krasilnikov, desy zeuthen...
DESCRIPTION
3 Motivation. XFEL Photo Injector L-Band (1.3GHz) 1.5-cell RF gun with Cs2Te photo cathode Ecath=60MV/m Ek = thermal kinetic energy of electrons at photo cathode Normalized transverse emittance after XFEL injector as function of the initial kinetic energy of the photo emitted electrons Slice RMS normalized emittance in XFEL injectorTRANSCRIPT
![Page 1: Impact of the Cathode Roughness on the Emittance of an Electron Beam M.Krasilnikov, DESY Zeuthen WSHQE, Milano 4-6.10.2006](https://reader035.vdocuments.us/reader035/viewer/2022081515/5a4d1b477f8b9ab0599a4173/html5/thumbnails/1.jpg)
Impact of the Cathode Roughness on the Emittance of an Electron Beam
M.Krasilnikov, DESY Zeuthen
WSHQE, Milano4-6.10.2006
![Page 2: Impact of the Cathode Roughness on the Emittance of an Electron Beam M.Krasilnikov, DESY Zeuthen WSHQE, Milano 4-6.10.2006](https://reader035.vdocuments.us/reader035/viewer/2022081515/5a4d1b477f8b9ab0599a4173/html5/thumbnails/2.jpg)
2
Outline
• Motivation• Cathode roughness models• Cathode roughness effects:
– Geometric• Normal emission, 2D vs. 3D• 2D model with emission distribution
– Electric field• Schottky effect, electron affinity• Single bump model
• Conclusion
![Page 3: Impact of the Cathode Roughness on the Emittance of an Electron Beam M.Krasilnikov, DESY Zeuthen WSHQE, Milano 4-6.10.2006](https://reader035.vdocuments.us/reader035/viewer/2022081515/5a4d1b477f8b9ab0599a4173/html5/thumbnails/3.jpg)
3
Motivation. XFEL Photo Injector
0
1
2
3
4
5
6
7
8
0 2 4 6 8 10 12 14 16 18z, m
mm
mra
d
Xemit (Ek=0.55eV), mm mrad
Xemit (Ek=0.65eV), mm mrad
Xemit (Ek=0.75eV), mm mrad
Xemit (Ek=1eV), mm mrad
Xrms, mm
L-Band (1.3GHz) 1.5-cell RF gun with
Cs2Te photo cathodeEcath=60MV/m
Ek = thermal kinetic energy of electrons at photo cathode
Normalized transverse emittance after XFEL injector
as function of the initial kinetic energy of the photo
emitted electrons
0.8
0.85
0.9
0.95
1
1.05
1.1
0.4 0.6 0.8 1 1.2Ek, eV
emitt
ance
, mm
mra
dSlice emittance @z=18m
0
0.5
1
1.5
2
2.5
3
-5 -4 -3 -2 -1 0 1 2 3 4 5z-<z>, mm
sl.e
mit.
, mm
mra
d
0
0.2
0.4
0.6
0.8
1
1.2
1.4
sl.emittance (Ek=0.55eV), mm mradsl.emittance (Ek=0.75eV), mm mrad
sl.emittance (Ek=1eV), mm mradcharge density, a.u.
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
5 7 9 11 13 15 17
RMS normalized emittance in XFEL injector
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4
Motivation. Cathode roughnessRoughness measurements by INFN/LASA
Profile
Paolo Michelato, INFN Milano – LASA“High QE Photocathodes lifetime and dark current investigation”,PITZ collaboration meeting 4-5.02.006
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5
Motivation. Cathode roughnessRoughness measurements (imaging) by INFN/LASA
Paolo Michelato, INFN Milano – LASA“High QE Photocathodes lifetime and dark current investigation”,PITZ collaboration meeting 4-5.02.006
![Page 6: Impact of the Cathode Roughness on the Emittance of an Electron Beam M.Krasilnikov, DESY Zeuthen WSHQE, Milano 4-6.10.2006](https://reader035.vdocuments.us/reader035/viewer/2022081515/5a4d1b477f8b9ab0599a4173/html5/thumbnails/6.jpg)
6
Motivation. Thermal emittance
Measurements at PITZ
cathode #61, QE ~ 1.5%
0.30
0.35
0.40
0.45
0.50
0.55
0.60
0.65
5.0 10.0 15.0 20.0 25.0Efield , MV/m
emitt
ance
, mm
mra
d
emitt Xemitt Y
Ecath=42MV/mEemis=24MV/m
Ecath=60MV/mEemis=42MV/m
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Cathode Roughness Models
-1
0
1
-4 -2 0 2 4 k*x
z/h
n
v
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Periodic Roughness. 2D vs. 3D
n
v
-1
0
1
-4 -2 0 2 4 k*x
z/h n
v k/2
period roughness
hkh 2
parameter roughness
)(sin1
)sin(220
kx
kxvvx
)cos(kxhz )cos()cos( kykxhz
22022
1
112
hmceEp xxx
Dx
)(sin)(cos)(cos)(sin1
)cos()sin(222220
kykxkykx
kykxvvx
,)(2 2023 Ih
mceE
p xxxD
x
.
sincoscossin1cossin
4)(
where
22222
22
2
2
dYYXYX
YXdXI
emission normal ,0 Case
Transverse component of the velocity at the cathode surface
Transverse emittance induced by the cathode roughness0.7
0.71
0.72
0.73
0.74
0.75
0.76
0 1 2 3 4 5 6 7 8 9 10=2*h/
3D/ 2D
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2D Periodic Model with Emission Distribution
-1
0
1
-4 -2 0 2 4 k*x
z/h
n
v
dxpdd
mcEp
x
kx
m2
2
00
2
sin
sincoscoscossin2
surface cathoderough at the momentum Transverse
Without roughness
)cos1(6cos3cos22 3
2,
m
mmkx
flatthx mc
E
eVEeVETeCs kA 75.0;2.0:cathode photo For 2
affinityelectron where,arccos AkAm EEE
];0[ Case m
2D (x,z) cathode roughness
![Page 10: Impact of the Cathode Roughness on the Emittance of an Electron Beam M.Krasilnikov, DESY Zeuthen WSHQE, Milano 4-6.10.2006](https://reader035.vdocuments.us/reader035/viewer/2022081515/5a4d1b477f8b9ab0599a4173/html5/thumbnails/10.jpg)
10
2D Periodic Model with Emission Distribution
-1
0
1
-4 -2 0 2 4 k*x
z/h n
v
m
m
mmmmmkx
roughthx mc
E
tan where
,)cos1(6
)cos1)(cos1(2cos)cos3cos2(2
cathoderough thefrom emittance Thermal33
2,
)cos1(cos3cos2
cos12cos 3
3
,
,
mmm
mmflatth
x
roughthx
Thermal emittance growth due to the cathode roughness Vs. roughness parameter Vs. roughness period (h=10nm)
0
20
40
60
80
0 2 4 6 8 10 12 14 16 18 20=2*h/
ther
mal
em
ittan
ce
grow
th, %
0
10
20
30
40
50
60
0 100 200 300 400 500 600 700 800 900 1000, roughness period, nm
ther
mal
em
ittan
cegr
owth
, %
h=10nmh=70nmh=100nm
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11
Dependence on Electric FieldThermal emittance growth due to the cathode roughness as
function of electron affinity and roughness period (h=10nm)
1 1 1 12 2 2
2
4 4
4
4
6
6
6
6
8
8
8
8
10
10
10
10
15
15
15
15
20
20
20
20
25
25
25
30
30
30
35
35
35
40
40
45
45
50
50
55
55
60
60
65
65
7075
80859095
, nm
EA, e
V
20 40 60 80 100 120 1400
0.05
0.1
0.15
0.2
0.25
emission theofmoment at the cathode at the field electric
factor t enhancemen fieldstatus surface
cathode theof change the todue increased
affinity initial
,4
:affinityelectron effect,Schottky Including
0
0,
00
3
0,
E
E
EeEE
ph
A
phAA
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12
Dependence on Electric Field
00.20.40.60.8
11.2
-10 -8 -6 -4 -2 0 2 4 6 8 10x/b
z/z(0)a/b=0.01a/b=10a/b=100
11 22
2
xb
abz
Single Bump Model
Electric field of the bumped surface
ow EE
-8 -6 -4 -2 0 2 4 6 80
5
10
15
x. a.u.
z, a
.u.
22 abzix
bzixiEiEE ozx
Conformal transformation
plane capacitorincluded!effect charge space no
1
1)(
;)()(
)(
EquationsMain
22
2
z
x
zx
z
x
z
x
pp
ppzx
ctdd
EE
mce
mcpmcp
ctdd
.0)0(;0)0(;)0(;)0(
:(emission) conditions Initial
00
tptpztzxtx
znxn
nnnn
Emission points for simulations
u
v
x
z
.
24
...1;;
22222222
0
0
aubauubabz
NnNunubz
bux
nnnn
Nnn
nn
bbazzN 2201.0)0(01.0
w
ibaibizxiwu 22
0 2 4 6 8 100
1
2
3
4
5
6
7
8
9
10
u,a.u.
v,a.
u.w
,a.u
.
u,a.u.0 1 2 3 4 5 6 7 8 9 10
0
1
2
3
4
5
6
7
8
9
10
x,a.u.
z,a.
u.z,
a.u.
x,a.u.
Conformal transformation
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13
Dependence on Electric FieldSimulated divergence (h=10nm)
00.20.40.60.8
11.21.41.61.8
2
0 0.2 0.4 0.6 0.8 1u/u0
px,m
rad
20MV/m 24MV/m36MV/m 42MV/m46MV/m
00.20.40.60.8
11.21.41.61.8
2
0 0.2 0.4 0.6 0.8 1u/uN
px,m
rad
20MV/m 24MV/m36MV/m 42MV/m46MV/m
00.10.20.30.40.50.60.70.80.9
1
0 0.2 0.4 0.6 0.8 1u/uN
px, m
rad
20MV/m 24MV/m36MV/m 42MV/m46MV/m
nm
10nm
100nm
nm
Ecath, MV/m E0=Ecath*sin(emission), MV/m
42 24
60 42
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
0 0.2 0.4 0.6 0.8 1u/uN
px,m
rad
20MV/m24MV/m36MV/m42MV/m46MV/mbump profile
p
![Page 14: Impact of the Cathode Roughness on the Emittance of an Electron Beam M.Krasilnikov, DESY Zeuthen WSHQE, Milano 4-6.10.2006](https://reader035.vdocuments.us/reader035/viewer/2022081515/5a4d1b477f8b9ab0599a4173/html5/thumbnails/14.jpg)
14
Dependence on Electric Field
Maximum divergence vs. Emission Field E0 for various roughness width (roughness depth h=10nm)
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
20 25 30 35 40 45 50E0, MV/m
max
(px)
, mra
d
=1nm
=10nm =100nm
Ecath, MV/m E0=Ecath*sin(emission), MV/m
42 24
60 42
px,max,px,max,px,max,
mMVEp
mMVEppmMVE
mMVE
emx
emxx
emthx
emthx
thx
/24/24
/24/24
-20%
-10%
0%
10%
20%
30%
40%
50%
20 25 30 35 40 45 50E0, MV/m
(E
0)/
(24M
V/m
)-1
Emit.growth, lym=1nm
Emit.growth, lym=10nm
Emit.growth, lym=100nm
![Page 15: Impact of the Cathode Roughness on the Emittance of an Electron Beam M.Krasilnikov, DESY Zeuthen WSHQE, Milano 4-6.10.2006](https://reader035.vdocuments.us/reader035/viewer/2022081515/5a4d1b477f8b9ab0599a4173/html5/thumbnails/15.jpg)
15
Conclusion
Thermal emittance growth due to the cathode roughness
)21(110 FFthth
“Geometric” roughness factor ~10-50% Induced by the electric field increase ~30%
-20%
-10%
0%
10%
20%
30%
40%
50%
20 25 30 35 40 45 50E0, MV/m
(E
0)/
(24M
V/m
)-1
Emit.growth, lym=1nm
Emit.growth, lym=10nm
Emit.growth, lym=100nm
Emittance growth ~10÷65%
0
10
20
30
40
50
60
0 100 200 300 400 500 600 700 800 900 1000, roughness period, nm
ther
mal
em
ittan
cegr
owth
, %
h=10nmh=70nmh=100nm