r. doerner, 8 th eu pwi task force meeting, warsaw, poland, nov. 4-6, 2009 directions of the us-eu...
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U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Directions of the US-EU Collaboration on Mixed Materials for ITER
R. P. Doerner, M. J. Baldwin, E. Hollmann,
D. Nishijima, G. R. Tynan, K. Umstadter and J. Yu
Center for Energy Research, University of California – San Diego, USA
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Future Directions of PISCES Program*
• Retention in, and release from, mixed-material codeposits• Mixed-species plasma-surface interactions• Transient heating of elemental and mixed-material
surfaces during plasma exposure using laser pulses• Ablation plume physics
– Material transport along B (vapor shielding)– Material transport across B (laser blow off, macroscopic particles)
• Angular and energy distributions of sputtered W particles
• Addition of transient particle source to the PISCES facility (longer term direction, still conceptual)
PISCES
* Taken from 2008 US-EU PWI Task Force talk
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
US-EU collaboration is contributing to several ITPA DIV/SOL High Priority ITER R&D tasks
• Changes in retention due to mixed plasma species
• Tritium release increase during 240°C - 350°C bake
• Impact of material mixing on retention
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Different materials, heating profiles and implantation doses are being studied
10-10
10-9
10-8
10-7
0
100
200
300
400
500
600
700
800
0 1000 2000 3000 4000
Be2C_2 [3.0E17 D implanted - 3.35E16 D retained]
Time (s)
Six types of material – Be on W Be on CFC Be12W Be2C C on Be W on Be
Four implantation doses - 3 E 16 D atoms (at room temp.) 3 E 17 D atoms
3 E 18 D atoms 3 E 19 D atoms
10-10
10-9
10-8
10-7
0
200
400
600
800
1000
0 500 1000 1500 2000 2500 3000 3500
Be2C_3 [2.8E18 D implanted - 7.37E16 D retained]
Time[s]
350C
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Retention and release from mixed material samples with Be-containing overlayers
• 200 nm Be layers deposited on substrates at MEdC, Romania
• Alloys formed and verified at IPP, Garching
• Samples implanted at room temperature with 200 eV D ions at IPP, Garching to a fluence of 4-5 E22 D/m2 (~3 E18 D atoms)
• TDS performed on samples at PISCES, UCSD
• Assumes all D is released from samples by TDS at 800C (to be confirmed by post-TDS NRA at IPP, Garching)
0
20
40
60
80
100
Annealed to 240CAnnealed to 350CAnnealed to 800C
Be on W Be on CFC Be2C Be12W
Total Dreleased
1.3E17 1.3E17 7.4E16 5.2E16
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Annealing to 350C is ineffective for release from C layers
W layers retain very little implanted D
10-10
10-9
10-8
10-7
0
200
400
600
800
1000
0 500 1000 1500 2000 2500 3000 3500
W on Be_3 [3E18 D implanted, 9.5E15 retained]
Time[s]
10-10
10-9
10-8
10-7
0
200
400
600
800
1000
0 500 1000 1500 2000 2500 3000 3500
C on Be_3 [3E18 D implanted - 8.3E16 retained]
Time[s]
350 C
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
W Temperature & PMI are coupled
NAGDIS-II: He plasmaD. Nishijima et al. JNM (2004) 329-333 1029• Surface morphology • Shallow depth• Micro-scale
PISCES-A: D2-He plasmaM. Miyamoto et al. NF (2009) 065035600 K, 1000 s, 2.0x1024 He+/m2, 55 eV He+
• Little morphology• Occasional blisters
(b) Under focused (c) Over focused
10nm
10nm
(a) Bright field image (under focused image)
PISCES-B: pure He plasma M.J. Baldwin et al, NF 48 (2008) 0350011200 K, 4290 s, 2x1026 He+/m2, 25 eV He+
NAGDIS-II: pure He plasmaN. Ohno et al., in IAEA-TM, Vienna, 20061250 K, 36000 s, 3.5x1027 He+/m2, 11 eV He+
100 nm (VPS W on C) (TEM)
~ 600 - 700 K > 2000 K~ 900 – 1900 K
• Surface morphology • Evolving surface• Nano-scale ‘fuzz’
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
A small amount of He (5-20%) in deuterium plasma results in suppression of blisters on W
[from M. Miyamoto et al., NF 49(2009)065035]
Plasma exposure conditions : fluence 5e25 m-2, 300ºC, Eion ~ 55 eV, 20% He.
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Mixed D/He plasma exposure creates nano-bubbles in the near surface of W and reduces D retention
TEM image of nano voids TDS of mass 4, He and D2
[from M. Miyamoto et al., NF 49(2009)065035]
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Mixed D/He reduces D migration in W at low temperature
date D Fluence
1026 D/m2
D retained
1020 D/m2
12/08 0.75 (+He) 0.109
12/08 1 3.77
12/08 0.5 3.84
03/08 1 3.27
03/08 0.1 2.37
0
0.001
0.002
0.003
0.004
-0.5 0 0.5 1 1.5 2 2.5 3
Depth (microns)
D/W
D+He 12/08 0.75E26 D/m2no He 12/08 1E26 D/m2no He 12/08 5E25 D/m2no He 03/08 1E26 D/m2no He 03/08 1E25 D/m2
W.R.WamplerSandia National Laboratories
200°C
With He
● Addition of He to the D plasma reduced D retention by about a factor of 35.
● With He, D retention is mainly at the surface,whereas without He, D retention peaks ~ 1 micron beneath the surface.
NRA measurements byW. Wampler - SNLA
1e21 D/m2 ~ 3 mg/m2
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Above 900 K, W ‘fuzz’ occurs.Fuzz is approx. 95% space
• SEM used to profile ‘fuzz’ layer thickness over sample surface.
• Geometric vol. of ‘fuzz’ layer est. (7.8 x10-10 m3 ±10%).
Distance from center of target (mm)
-10 0 10
Cro
ss s
ectio
nal h
eigh
t (
m)
-150
00
24
6 t = 3600 sEion = 30 eV
Ts=1120 K
He
nano-structuredlayer
W bulk
• ‘Fuzz’ layer removed. Mass change (Dm=0.87 mg ±1%).
Comp. w/ pure W, ( = 19.25 x103 kgm-3), ‘fuzz’ layer is 94 % porous.
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
‘Fuzz’ growth consumes W bulk
22000 s, 1120 K60 eV He+ PISCES-Bpure He plasma
~50 ITER shots
9000 s, 1120 K60 eV He+ PISCES-Bpure He plasma
~20 ITER shots
2000 s, 1120 K60 eV He+ PISCES-Bpure He plasma
~4 ITER shots RN
061
5200
7
RN 0
9272
005
RN 0
6182
007
Confirmation of fuzz growth out of the surface, first suggested by Prof. Yoshida. This growth mechanism may present a concern for W divertor operation where surface fuzz may, or may not, withstand the harsh plasma bombardment environment.
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Effect of He plasma on various grades of W PISCES
Japanese ultra-fine-grain W
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Re-crystalized W responds very differently.
Re-crystalization may lead to greater ‘space’ in grain boundaries, due to defect migration to grain boundaries, (i.e. grain growth). Such space permits deep ‘fuzz’ growth at grain boundaries and may affect adhesion of W grains.
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Evidence of surface grain ejection ?
30 o ~20 m
Surface
X-section
beam
beam
X-section
Surface
SR WHeT ~1120 Kt = 2.2 x104 sHe
+ ~5 x1022 m-2s-1
EHe+ ~ 50 eV
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Small pits ~1m, are found on UFG-W nano-‘fuzz’. Grain ejection?
UFG-W (1.5 wt% TiC)He, T ~1120 K, t = 3.6 x103 s, He
+ ~2.5 x1022 m-2s-1, EHe+ ~40 eV
30 o
beam
Surface
Small impressions in the surface that have also developed nano-‘fuzz’
Typically, nano-‘fuzz’ is uniform in appearance
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Angular distribution measurements of sputtered W atoms (flat surface done, fuzz underway)
• RF plasma source is used to investigate sputtering details
• Hiden EQP analyzer can differentiate mass and energy of incoming ions and neutrals
• Variation in target angle allows measurement of angular distribution of sputtered species (always normal incident plasma ions)
• Sputtering of W atoms from flat and fuzzy surfaces (made in P-A) are being compared
E. Oyarzabal et al., J. App. Phys. 100(2006)063301
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
Erosion rate of W fuzz
• Measurements are underway to determine erosion yield and angular distribution of eroded W fuzz
0.01
0.1
1
0 100 200 300 400 500
W I/
Ar
II
Time [s]
Ei ~ 45 eV
Ei ~ 65 eV
Ei ~ 85 eV
Ei = 105 V
Integrated W atom surface loss rate from a nanostructured surface (in P-B)
Sputtered Ar on W angular distribution from a smooth surface in rf etcher
W fuzz
Smooth W
PISCES
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
PISCES collaborates in several areas within the EU fusion program
• MD simulations of Be chemical sputtering predicted ion energy dependence
• ERO modeling of mixed material effects
• JET ILW marker tiles being produced (with GA)
• W S/XB measurements
• Effects of nitrogen impurity seeding, performance test show PISCES can run N2 plasma (future direction)
MD simulations of D on Be predicted subsequent erosion measurements
PISCES
Exp. from D. Nishijima et al, PPCF 50(2008)125007.Sim. from C. Bjorkas, submit. to New J. Physics (2009).
U C S DU niversity o f C alifo rn ia S a n D iego
R. Doerner, 8th EU PWI Task Force Meeting, Warsaw, Poland, Nov. 4-6, 2009
UCSD, MIT and UC Berkeley recently received funding for a 5 yr. Plasma Science Center
• Center will focus on a multi-scale (experiment and modeling) approach to PMI
• Effort to focus on fundamental, rather than machine specific, PMI issues
• Collaborative possibilities abound
• Several postdoctoral positions available
PMI Center