Presented at Laser Heating Workshop at the APS, March 20, 2004 Choong-Shik Yoo Lawrence Livermore...
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Transcript of Presented at Laser Heating Workshop at the APS, March 20, 2004 Choong-Shik Yoo Lawrence Livermore...
![Page 1: Presented at Laser Heating Workshop at the APS, March 20, 2004 Choong-Shik Yoo Lawrence Livermore National Laboratory Livermore, California 94583 (yoo1@llnl.gov;](https://reader035.fdocuments.us/reader035/viewer/2022062802/56649e8f5503460f94b9394d/html5/thumbnails/1.jpg)
Presented at Laser Heating Workshop at the APS, March 20, 2004
Choong-Shik Yoo
Lawrence Livermore National LaboratoryLivermore, California 94583
([email protected]; (925) 422 - 5848)
CollaboratorsBruce Baer, Magnus Lipp, Alex Goncharov
Vibrational Spectroscopy on Laser-Heated Vibrational Spectroscopy on Laser-Heated High Density Fluids in Diamond Anvil CellHigh Density Fluids in Diamond Anvil Cell
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Laser-heated DAC creates the P,T conditions of energetic detonation and Giant planetary
interiors
Structures and stabilities of simple molecules are not known at high P,T
10-50 GPa1000-5000 K
N2
CO2
CH2O
10-700 GPa
8000 K
Giant planets
H2, HeH2O, CH4, NH3
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Extreme materials research with laser-heated DAC for synthesis
Laser-heated DAC is capable of exploring a delicate balance between mechanical (PV) and thermal (TS) energies
New opportunities for synthesis of exotic materials !!!
P- electron delocalization
Solid
MolecularAssociated
Molecularmetal
Ionization
Liquid
Extended
T-
ion
izat
ion
Kinetic line
Dissociation
P(GPa)
T (
K)
300
0
0
Atomicmetal
100
Strong disparity in bonding results in a huge kinetic barrier (metastability)
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Strong, coherently emitted CARS (Coherent Anti-stokes Raman
Spectroscopy) probes molecular vibration in-situ at high P,T
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Optical setup for CARS applied to laser-heated DAC
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LLNL- CARS setup ready for studies of high density fluids
ML,QS-Nd:Yag
Broad bandDye laser
Narrow bandDye laser
DAC
SPEC/CCD
Q/CW-YLF
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CARS of laser-heated N2 at high pressures
During heating
Before heating
N2
W-toroid
100 m
-N2
300 K at 13 GPa
Fluid-N2
2300 K at 13 GPa
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Spontaneous Raman spectroscopy on laser-heated materials at high pressures
DAC
Probe
Gasket
Sample
Hot plate
Laser Heating
Diamond Diamond cellcell
Fast spectrographFast spectrographradiometryradiometry
Tunable notch Tunable notch filtersfilters
Spatial filterSpatial filter
Dispersive Dispersive beamsplitterbeamsplitter
Fast spectrographFast spectrographRamanRaman
Laser heating Laser heating 1053 nm (YLF)1053 nm (YLF)
50 W50 W
Raman laser Raman laser 476 nm (Ar ion)476 nm (Ar ion)
CCD cameraCCD camera
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Lasers with different mode structures enable to heat selected areas in various configurations
TEM01* YLF (Quantronix)
HeNe
HeNe TEM00 -YLF (Antares)
4xBEWP
PBS
Ar-Ion laser (Spec-Phys)
Iris
PMHRLM
dual coated
Heating targets can be tailored into various shapes such as flat foils, toroids, micro-furnaces, steps, etc.
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Discrimination of thermal radiation using both spatial and spectral filters
• Spatial filtering to eliminate thermal radiation from hot donut
• Raman notch spectral filter to minimize straight laser light
• Use “blue” excitation to reduce thermal radiation
~ 100
m
Hot donut (W)
N2
Laser
Spatial filter
Intensity (a.u.)
800700600Wavelength (nm)
39 GPa1861 K
Planck-fit to thermal emission
80006000400020000
Wavenumber (cm-1
)
N2 at 20GPa &1700K
Ram
an in
ten
sity
N2 vibron
RubyDiamond Raman
Laser
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Spontaneous Raman spectroscopy on laser-heated N2 at high pressures
24002350
Raman Shift (cm-1
)
1
12
31 GPa
26 GPa
20 GPa
1500 - 2000 K 2
The presence of12 is evident for high temperature, yet that of 1 indicates a large temperature gradient near diamond surface
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Thermal insulation of hot plate by Al2O3
24002350
Raman Shift (cm-1
)
27 GPa
RT
~ 1820K
24002350
Raman Shift (cm-1
)
39 GPa
RT
~ 1700K
Probe
Laser Heating
Gasket
Sample
Hot donutAl2O3 matrix
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Challenges in vibrational spectroscopy on laser-heated materials
• Sample preparation: • Micro-fabrication of heat absorber • Thermal insulation of hot plate and sample from diamond• Highly reactive high density fluids
• Laser-heating:• Uniform heating of hot plate and sample • In-situ pressure measurements
• Spontaneous Raman:• Weak signal• Limited to low emissivity materials and relatively low T <2000K• Alternative routes: deep “blue”, pulse Raman, coherent Raman
• CARS: • Optical transparency of sample• Diamond damage
• Materials application: • Complex chemistry with multiple path ways
• Difficulties in characterization: structure, order, (meta-)stability, etc
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What are the most important experiments? • Melting and phase diagram studies above 100GPa:
- Melting vs. recrystallization, amorphorization vs. phase transitions vs. diffusive motions- Melt probes: speckle pattern, reflectivity, laser power, etc.
• Structural studies:- Ordered systems: polycrystals, single crystals, mixtures and alloys- Disordered systems: liquid, amorphous, glass
• Novel materials applications:
- Superhard, HEDM, optical, high-Tc, etc.
• Mechanical properties:- Materials strength, elastic properties, plastic deformation,- Microstructures, textures, preferred orientation
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What are the most important experiments?
• X-ray spectroscopy: elastic and inelastic- Interatomic potentials, molecular configuration, electronic structure
- X-ray induced chemistry: ionization, excite state fluorescence,
• Real-time structural studies:- Thermodynamic(stability) vs. kinetic(metastability)- Reology and dynamics- Transport properties: thermal diffusion, viscosity,
• Associated technology developments:- In-situ diagnostics for intrinsic material properties: X-ray, Raman, CARS, reflectivity
- In-situ P,T probes: pyrometer, calibrated thermocouple, X-ray induced fluorescence
- Internal P,T standard materials
- New DAC cells: Membrane-DAC, Large volume DAC, Dynamic DAC, etc.
- Laser-heating: CO2 heating, short pulse heating,
- Sample fabrication: Micro-furnace, insulation,
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What should the guiding philosophy be? • Time constraints:
- Simple and easy in operation: - Optimized alignment and calibration procedures
• Compatibility:- DAC in different types- Software: x-ray and laser-heating operation- Hardware: not too many computers, remote & manual controller, visual aids, fibers
• Balanced approach: x=10m at 50GPaP~2-5%, V~1~2%, T~2-5%- Unknown melt diagnostic, yet T < 10-20o (?)
• Practicality:- Experimental geometry: axial and radial x-ray experiments- Integrated experiments: laser-heating with ADXD, Raman, IXS, etc.
• Operational principles:- It is an x-ray experiment, not laser-heating- 24-hr operation: minimize downtime for laser alignment and sample preparation- Mentor/Buddy system: any first-time user should team up with an expert