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High Brightness and High Polarization Electron Source for Electron Microscope

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Title: High Brightness and High Polarization Electron Source for Electron Microscope


1
High Brightness and High Polarization Electron
Source for Electron Microscope
PESP-2008 Workshop (3. October, 2008 _at_J-Lab)
  • Tsutomu NAKANISHI
  • (Department of Physics, Graduate School of
    Science,
  • Nagoya University)

2
Beam requirements for electron sources
fromthree kinds of electron accelerators
High peak current (10A)
F10mm
ILC
High average current (10mA)
ERL
F1mm
High current density ( 1A/mm2 )
F1µm
SPLEEM
3
Contents of this talkhave already explained
partially in1) Talk by Toru Ujihara, R/D of
transmission PC 2) Poster by Naoto Yamamoto
(small Y) Proto-type SPLEEM gunperformances

4
LEEM / PEEM type Electron Microscope (developed
by E. Bauer)
Energy analyzer ( 90or 180bend)
LaB6 emitter
Focus lens
Image lens
LEEM
Objective lens
Beam separator
Contrast aperture
Screen
Objective lens
hn
PEEM
Specimen
5
SPELEEM (??????OECU)
Koshikawa Yasue Group
CCD???
????????
LaB6 Gun
???
?????
?????? ??????
????????????
???? ??????
????????? (???????? ??????)
???
?????
????????
Made by ELMITEC co. (Germany)
6
LEEM images
Dynamic observation of Cu thin film growth on
W(110) at 100 ?
FOV10mmf 0-3.2MLbcc
layer-by-layer growth
(Room temp. - 150?)
The third layer does not start just after
2.13MLbcc and it start at around 2.47 MLbcc.
7
Imaging of magnetic domains
I I ?
LEEM Image
I? I ? ?
?
?
Mag. Domain Image
A Magnetic contrast (Asymmetry)
?


P
Polarization of incident beam

  • Pure Spin effects can be obtained in Magnetic
    domain images

8
Proposal of this work (April 2008)
Real-time observation of magnetic domain
formation process
Approved at September 2005 by Japan Science and
Technology Agency (JST), as Technology
Development Program for Advanced Measurement and
Analysis (Program-T)
9
talk contents
  • 1. Procedure for Higher Brightness
  • Transmission Type Photocathode

2. A 20keV Test-Gun Apparatus Performances Beam
Performances
3. A 20keV gun for SPLEEM Assembling
finished Beam test in Progress
10
Our first trial toward higher brightness (2003?)
HV-20kV?gap-width5.34mm
Needle-tip (?20nm? radius) NEA-GaAs emitter
M.Kuwahara et al. JJAP 45 (2006) 6245 ? Field
emitter polarized electron source
? Serious Problem Current limit ( Tip
melt-down by self-heating) (current / tip ? 30
nA)
11
This work toward much higher brightness (2005?)
? Conventional Type Laser spot size ? 50?m
? New transmission type Laser spot size
diffraction limit ? a few ?m
Advantage Electron Laser beam lines do not
interfere
Laser spot size (exp.) 1.3µm(FWHM) _at_?777nm)?
12
Lens stage to make the minimum laser spot
Optical Fiber
Ti-Sapphire Laser
Fiber Collimater
Polarizing Beam splitter
Quarter Waveplate
Imaging Lens
Positioner
XHV
Focusing Lens
Focusing Lens
Photocathode
Photo- cathode
Electron Beam
13
talk contents
  • 1. Procedure for Higher Brightness
  • Transmission Type Photocathode

2. A 20keV Test-Gun Apparatus Performances Beam
Performances
3. A 20keV gun for SPLEEM Assembling
finished Beam test in Progress
14
A 20keV test-guns Compositions
NEA activation chamber
Laser optics equipment
Gun chamber
100keV-Mott Analyzer
Beam size monitor
Spherical condenser
15
Beam simulation
20keV
adopted
? Laser spotf3µm ? Electrode gap4mm ?
Voltage20kV Field gradient5MV/m ?
Electrode Mo (cathode) material Ti
(anode) ? Photocathode exchanged by a
load-lock system
Beam simulation
4keV
Dark current could be suppressed below 10nA under
25kV
16
20keV proto-type-gun designed for SPLEEM (JPES-1)
17
Mott detector system
18
Apparatus performance of JPES-1
Gun assembly
Activation chamber
Load-lock transfer-rod
19
Beam size (Brightness) measurement?
Conditions Beam energy (U) 20keV,Beam current
(I)5.3µA
Current (I)
Current density (dI/dx)
L531mm
Source size (S) estimation Laser spot size
Electron diffusion length 0.65µm(HWHM) ?1µm
1.50.3µm
Beam size R1.000.02mm (HWHM)?
1.00.4107 A m-2 sr-1 V-1
20
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21
Performance of GaAs-GaAsP superlattice
(Reflection PC by Nagoya group)
_at_778nm
? GaAs-GaAsP superlattice shows the
best performance !
Polarization 92 Q.E. 0.5
22
Transmission PC
90 Polarization achieved (2007/10/26)
Position dependence of Polarization
Uniformity of Polarization assured
23
Polarization improvement by change of strain
property of GaAsP buffer-layer
Pol.? 65
Pol.? 90
24
Summary of JPES-1Performances
Performances of 20keV polarized electron gun with
transmission type photocathode (PC)
  • Beam size at PC ? 1.3?m? (780nm laser)
  • Polarization 90
  • Quantum efficiency 0.1
  • Average Current 15?A
  • Brightness 2?107A/cm2/str (_at_20keV)
  • Brightness (reduced) 1?107A/m2/str/V
  • NEA lifetime 200h (without beam)
  • NEA lifetime 30h (with 5 ?A)
  • Vacuum at PC ? 9.0 ?10-10 Pa

25
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26
Documents on a transmission PC PES
  • Published Papers
  • (1)High brightness and high polarization
    electron source using
  • transmission photocathode with GaAs-GaAsP
    superlattice layers
  • N. Yamamoto et al. Journal of Applied Physics
    vol.103, (2008), 064905
  • (2) Super-high brightness and high
    spin-polarization photocathode
  • X. Jin et al. Applied Physics Express Vol. 1
    (2008), Article No. 045002

Doctor Thesis Naoto Yamamoto
NEA-GaAs?????????? ? ???????????????????????
??????? (Nagoya University?2007??)
  • Patents
  • T. Nakanishi ????????????? 2006-084303
  • T. Ujihara?T. Nakanishi ?5?????????????????????
    ?2008-079292 (2008/3/25??)

27
talk contents
  • 1. Procedure for Higher Brightness
  • Transmission Type Photocathode

2. A 20keV Test-Gun Apparatus Performances Beam
Performances
3. A 20keV gun for SPLEEM Assembling finished
and final beam test in progress
28
JPES-2 (gun, spin-manipulator beam SW line)
for SPLEEM
29
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30
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31
High Brightness High Polarization Electron
Source for LEEM
LEEM (Osaka)
PES (Nagoya)
Within one month, this PES system will be
transferred to Osaka and jointed with LEEM
32
Additional remarks (1)
? Advantages of transmission-PC PES
  • Freedom to design both of laser electron beam
  • Lines independently. ? Laser beam line can be
    optimized to satisfy various requirements.
  • Minimum laser spot size obtained (this work)
  • Symmetrical beam distribution to beam axis
  • Relax the laser heating problem for ERL-PC
  • Two photon excitation becomes easily.
  • Others, etc. etc. ..

33
Possible applications of the new-type PES
We start to contact with various fields
researchers (Looking for the academic users of
our PES)
Biology ? Chirality studies
SPLEEM Surface magnetic domain ? Magnetic
memories
TEM Bulk magnetic properties ? Electron
holography
HE Accelerators ? High current low emittance
electron source
Inverse Photo-emission Spectroscopy ? Spin IPES
34
SPLEEM collaboration
  • T. Nakanishi, S. Okumi, M. Yamamoto, M.
    Kuwahara,
  • N. Yamamoto, A. Mano, Y. Nakagawa
  • (Faculty of Science, Nagoya University)
  • Y. Takeda, T. Ujihara, X. J. Kim
  • (Faculty of Engineer, Nagoya University)?
  • T. Saka
  • (Daido Institute of Technology)
  • T. Kato
  • (Daido Steel Co. Ltd.)
  • T. Koshikawa, T. Yasue, M. Suzuki
  • (Osaka Electro-Communication University)?
  • T. Ohshima?T. Kohashi
  • (Central Research Laboratory, Hitachi Ltd.)?

High Energy Physics
Semiconductor Physics
LEEM Physics
Electron Microscope Physics
35
  • Thanks
  • for your attentions !

36
Examples of SPLEEM image
?
Electron injection energy Ei0.7 eV?50
sec/image
FOV30 ?m
FOV10 ?m
FOV6 ?m
f
37
Mechanisms of spin-flip depolariztion
Crystal defects of buffer-layer carried onto
SL-layer
GaAs-substrate
GaP-substrate
Spin-flip occurs
Spin-flip does not occur
SL-layers
GaAsP buffer-layer
GaP-substrate
Cracks do not meet with electrons
Dislocations meet with electrons
Crack-like defects are favorable than
dislocation-like defects
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