wtaru*mizutani* mitsutoshi*aramaki* daiyu**hayashi
TRANSCRIPT
Preliminary Experiment on Plasma Wave Guide for PWFA
Tatsuo Shoji Nagoya University, Japan
Wtaru Mizutani Mitsutoshi Aramaki Daiyu Hayashi Eindhoven University, Nederland
Supported by KEK, K. Nakajima and M. Yoshida
Tokyo Workshop IZEST 2013.11.20
Demands for plasma channel for 100Gev laser
plasma wake-field accelerator experiment
Discharge plasma with neutral structure + Laser discharge method is developed
・Stable long (~meter scale) plasma channel with narrow diameter (less than mm)
• ne=1015~17cm-3 electron density with hollow radial profile (Δne/ne~0.2)
• Fully ionized
Impossible for conventional discharge plasmas
New method to make plasma wave guide
ne
ne
n0
r
■ 1st step Efficient low density plasma production by helicon discharge to make hollow neutral density profile
ne=1013-14cm-3
■ 2nd step Laser ionization of neutrals to make fully ionized hollow plasma density profile
Partially ionized plasma
Short pulse laser ne=1015-16cm-3
Subjects need to be developed for helicon discharge with small diameter (~ ρion)
• Develop antennas for helicon waves (m= 1) coupled to small diameter (<1mm) and long (~1m module) plasma tube. ( ion Larmor radiuns ~plasma radius ) Helical antenna could efficiently produced only for >20mm Φ [1]
• Simple magnetic coils system -> pulse small magnetic coils, permanent magnets array.
• Measure hollow neutral density profile made by helicon discharge.
hollow neutral density was observed in ~50mmΦ helicon discharge
[1] T.Shoji, et. al., PIasma Sources Sci. Technol. 2 (1993)5-10
Helicon plasma as an efficient high density rf discharge with external magne<c field
■ne(r), R(wall radius) , ω, B0, m -> (1)->kz -> antenna design
m=1 mode
l
wave length λ(cm) [1] T.Shoji, et. al., PIasma Sources Sci. Technol. 2 (1993)5-10
ne0
z B0 R
[1]
R=0.2mm
m=1 helicon antenna for small diameter plasma
z θ
x
y
y
xz
m=1 mode
■m=1 helicon antenna
h Brf
Irf
B0 Ez l
Irf
Helicon wave B field
Experimental set-‐up
Spectrometer PC
Maching Box
Φ4mm, 50cm glass tube
magneRc coil
13.56MHz, 5kW duty 0.03 pluse width 5ms
antenna
B0 ~1.3kG
RF
CCD camera
probe
Optical filter
HeI(492nm)
(ne)
Electron density measurement
x
yy
xz
probe
plasma
Iis(x)
mi: ion mass
Te: electron temperature
nc: electron density
Integrated ion saturation current
Abel Transformation
0.2Φ, 32mm long(W)
Δ (>>λd ) : probe diameter
Δ
ne(r) €
Iis(x) = Δ−y0
y0∫ 0.61e nc (x)CS dy
€
CS = Te /Mi
y0
-y0
Laser Thomson scaFering for Ne(r), Te(r) measurement
Scattered signal
He0 (neutral) density measurement by Laser absorp<on
Isolator
FPI
Fabry-Perot
ECDL 707nm PD or CCD
Absorption Spectrum
PD
Wavemeter
PD:<He0*>ex -‐>(CR model)-‐> <He0> grand state CCD:He0* (r) -‐> (CR model)-‐>He0 (r)
Emission spectrum of He plasma
HeI(492nm)
492nm HI
388
395 402
446
471 486
501
492
587
667
656 706
727
775
Wave length
Light emission measurement
Emission intensity
ne : electron density n0 : neutral density
HeI(492nm)
Emission profile by using band pass filter
σex: excitation cross section
X(mm)
Emission intensity profile in x dirextion
x B0
1kW
2kW
2.5kW
n e [a
.u.]
~5x1013cm-3
Prf
B=1.0kG、p[He]=19mTorr
3cm
13
Plasma and neutral profile
14
1.0kW 2.5kW
Increasing ne
Δn/n0=0.4 Δn/n0=0.65
Rf power dependence on n0(r)
Δne
2.5
2.5kW 2kW
1kW
Glass tube radius=2mm
Neutral density profile Dependence of antenna pitch on Δn/n0
l=2cm 5cm
3cm
fast electrons by E acceleration of
l
Dependence of antenna pitch on the depth of neutral profile on axsis
ne
16
l
Summary
• Precise neutral density profile measurement by He line ratio and laser absorption method
• Obtain scaling low for the plasma diameter, length for the antenna, density dip ratio, rf power, B0 etc.
• Antenna design for 1m compact plasma wave guide with Permanent magnet.
• New method of making plasma wave guide has been developed and first experiment to produce small diameter (4mmΦ)plasma by helicon discharge (?) for PWFA has been performed .
• ・Develop m=1 helicon antenna for small plasma
• Hollow neutral density profile was observed (needs more careful measurement by LIF)
Need to be developed further
Thank you for Attention. Please wait till
we get good plasma.
T.Shoji