david hammer- the x-pinch, a remarkable x-ray source and high energy density plasma
TRANSCRIPT
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The X-pinch, a Remarkable X-ray Sourceand High Energy Density Plasma
David HammerLaboratory of Plasma Studies
Electrical and Computer EngineeringCornell University
Cornell University
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Presenting the Work ofSergei Pikuz, Tania Shelkovenko, Dan Sinars,
Byungmoo Song, Kathy Chandler, Marc Mitchell, Jon
Douglass, John Greenly and Ryan McBride
With Thanks to The P.N. Lebedev Institute group (Zakharov, Pikuz et al. plus Jiri Ullshmeid)
that conceived of the X pinch (1981)
Maxwell Laboratories, Inc., for introducing the X pinch to the U.S. (1984)
Nian-Sheng Qi, who helped start X pinch (“x-ray laser”) at Cornell (1987)
Dan Kalantar, who investigated X pinches for x-ray lithography (1989)
- and demonstrated x-ray backlighting is useful (Ph.D. 1993)
And Andrey Lebedev, who convinced me to invite Sergei Pikuz (1992)
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Outline
1. Introduction to X pinches(what and how, why, where)
2. X-pinch x-ray sourceDurationSize
3. Conclusions
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What and how …
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Experimental Schematic DiagramX pinch
Two-wire Multi-wire Double
XP pulser diode
Anode
Cathode
Rog.1
Rog.2
Vacuum chamber
Insulator PFL
X-pinch
Water gaps
Start with crossed fine metalwires as the load of the 450kA, 100 ns (fwhm) XPpulsed-power generator.Two X pinches in parallelalso works.
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Experimental Arrangement
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Start by exploding 2 or more 10-50 µm metal wires in the form of an Xusing 250-450 kA, 100 ns pulse, generating X-shaped plasma. A 300-400 µm long Z-pinch forms in the middle, implodes toward theaxis, goes unstable, develops hot, dense plasma spots that emit an x-rayburst, and then opens up.The time from the start of the current can be reproducible to ± 1-2 ns.
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Schleiren Images (<0.2 ns)
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Why ….
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Not to pump an x-ray laser
Not for x-ray lithography
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Atomic physics/x-ray spectroscopy of dense high-Z plasmasDynamics of current-driven dense plasmasIntense, short pulse x-ray sourceMany materials have been studied (Mo, W, Nb, Al, Ti, NiCr,Conichrome, Alloy 188, etc.).Intense x-ray bursts last 10-1000 ps (x-ray streak camera),and have energies of up to ~ 1 J in > 1.5 keV x-rays at 400 kA.
These numbers imply a source volume power density up to 1022
W/cm3 and a surface flux up to 1016 W/cm2.Time resolved x-ray spectroscopy -->, for example, Te as high as 2.5keV and ne > 3x1023 cm-3 in Ti X-pinches (Sinars et al, JSQRT, 2003).
It is a really interesting HighEnergy Density Plasma
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And they are good for imaging (forbusiness and for fun)
Point-projection radiographs have µm-scale resolution, implying source sizes of~1 µm or less. The resolution was “toogood to be true.” Also, the pulse is short.
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Where?
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Those Represented at DZP2005• Lebedev Institute• Cornell• Imperial College• University of Nevada, Reno• Pontificia Universidad Catolica de Chile• Ecole Polytechnique• Florida A&M University• University of California, San Diego
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Pulse DurationOriginally, we used 400 MHz oscilloscopesThen an X-ray streak camera with Al (D. Kalantar)
- SubnanosecondThen a 1-2 GHz digitizer with Mo
- Sub-half nanoscecondRecently, streak camera with ~ 10 ps resolution
- Pulses as short as 10 ps (above 4 keV)
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An x-ray streak camera was used to recordenlarged radiographic images of fineopaque and semitransparent objects (wires,fibers, fibers with a metal core) through anentrance slit placed in front of thephotocathode. Variation in the intensitydistribution of the images through thevarious objects provides time dependentinformation on the source size and spectralcharacteristics.
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Experimental setup for time resolvedX pinch x-ray source size measurements
Anode
Catode
X pinch
Wiregrid
FilterSlit
X-ray streakcamera
Glass fibersB+W fibers
Photocathode
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The image of a 1 ns x-ray streak4-wire NiCr X pinch (geometric distortion corrected)A portion of the image is shown enlarged to show thedecreasing pulse width with increasing photon energy.The x-rays reaching the photocathode through the 100µm glass core of the optical fiber (> 4 keV) have a pulsewidth of about 10 ps (resolution limit).The 20 µm W core of the B fiber does not becometransparent, which means there is not intense emissionat or above 15 keV from this X pinch.
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Streaked image of the wire grid in x-rayradiation of 4 x 20 µm NiCr X pinch
1 ns
1 m
m
0
1
2
0 50 100 150Time (ns)
X-ra
y In
tens
ity (A
rb.u
nits
)
50
100
150
0 1/3
Curre
nt (k
A)
PCD
Rogowski
T (ps)0
100 µm
W coreB shell
Plastic shellGlass core
Pulse 3626
100 200 300
(1)
(2)
(3)(4)
(5)
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Radial Size of the Source Vs Time
• The radial size of the first source is 10 µm orless for more than 100 ps even as the photonenergy of the radiation increases from thebeginning of the burst to the intensitymaximum. At the moment of maximumradiation intensity, this source seems to reachits minimum diameter, after which theradiation appears to drop very rapidly (withno visible expansion of the source size).
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Time integrated and streaked images of W wire inB shell in x-ray radiation of 4 x 20 µm NiCr X pinch
0
100
200
T (ps)
100 µm
17 µm
B shell
W core
Source 1 Source 2
1
234
Pulse 3626
10 µm
1
2
3
45
5
Planetime integrated
radiographimage
Streakedimage
Outline of plane
radiograph image
Outlines of streaked
image
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Source Size
Source sizes for variousmaterials are measured by
imaging known finefibers/wires or slits
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Wave-Optics-Enhanced Point-ProjectionRadiography Requires a Small Source
(Actual Wave-Optics Calculations for 8 µm B and 3 Å)
Wavelength Spread
Finite source size &Wavelength spread
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Experimental Arrangement
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Source size using a wire and fiber
8 µm Glass fiber image
Computed image for 1 ± 0.2 µm size Computed image for 1 ± 0.2 µm size
7.5 µm W wire image
Nb X pinch; 93:1 Experimentalmagnification Calculations include sourcebandwidth
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The Middle of an X pinch“Thermal x-rays” come from necks (bytriangulation using images of a mesh).
Electron-beams generate > 10 keV x-rays 100-500µm away on the anode side, adding “background.”
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The X pinch is a very interesting high energy density plasma
Pulse is a function of energy; can be < 100 ps
Refraction is responsible for a majority of the edge-enhancement in
radiographic images from X pinches
Direct Determination of Source Size
- 1. Agreement between fine objects in point projection and Fresnel-Kirchhoff
integral- 2. In 3-5 keV, Nb: 1 µm, Mo: 1.2 µm, W: 1.6 µm, NiCr: 2.8 µm, Ti: 14 µm
- 3. 1-2 µm source size up to 12 keV
High-Quality Coherence-Enhanced Imaging requires controlling X pinches to
produce one, intense micropinch with reduced E-beam radiation
Smaller drivers are more convenient … (UCSD, Ecole Polytechnique)
Conclusions
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Just when we thought we had moved beyond our past ….
Dr. Claudio Alonso, University Lecturer in Cell BiologyDepartment of Zoology, University of CambridgeDowning Street, Cambridge CB2 3EJUnited Kingdom
“I have an article just been accepted in Nature ReviewsGenetics (NRG) … about the … elements that controlanimal development and their potential for evolutionarychange - a subject area rather distant from your field ofresearch, I would imagine.”
He asked if they could use our image for the cover …
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