lkhamsuren bayarjargal- recent developments of the laser-heating facility in frankfurt and at...
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Recent developments of the laser-heating facility in Frankfurt and at Petra-III
Lkhamsuren BayarjargalInstitut für Geowissenschaften, Abt. Kristallographie:Goethe-Universität Frankfurt a. M., Germany
ContentsContents
Laser heating facility in Frankfurt •CO2 laser heating set-up
•Pressure measurement•Temperature measurement •Problems of temperature measurement •Raman measurement
Sample preparation•Laser drilling•Gas loading
Laser-heating facility at Petra-III
Outlook
The COThe CO22-laser heating system in Frankfurt-laser heating system in Frankfurt
The COThe CO22-laser heating system in Frankfurt-laser heating system in Frankfurt
The COThe CO22-laser heating system in Frankfurt-laser heating system in Frankfurt
Pressure determination (ruby fluorescence)
The mobile spectrometer for pressure measurement. A green laser (532 nm, 100 mW, cw) and mini spectrometer (HR4000, Ocean optics) are used for the measurement of ruby fluorescence signals. (H. Ahsbahs)
λ
[MX78] Mao, H. K., Bell, P. M., Shaner, J. W., Steinberg, D. J. J. appl. Phys. 49, 3276−3283 (1978)
[MX86] H.K.Mao,J.Xu,andP.M.Bell,J.Geophys.Res.91,4673,1986.
112
/5
2
−= kThce
hcI λλπε
h: the Planck’s constantc: the speed of light
k: the Boltzmann’s constantλ: the wavelength of light
T: the temperatureε: the emissivity
Planck’s law
Temperature determination
The Wien radiation law:For low temperatures, where hc/λkT >> ln (1), the Wien approximation can be used.
Sliding two-color pyrometry
ελλ
π ln112ln 5
2
hck
TIhc
hckWien −=
=
)()())/(1()/1()(
δλλδλλλ
+−+−=
WienWienT
Benedetti, L.R., Loubeyre, P., High Press. Res. 24, 423–445 (2004)
Program for temperature determination from the
thermal radiant emission
The COThe CO22-laser heating system in Frankfurt-laser heating system in Frankfurt
Problems: the emissivity and the chromatic aberration
Normal spectral emissivities for liquid and solid iron at melting point. (1808 K)
H. Watanabe, et al. International Journal of Thermophysics, Vol. 24, No. 2, March 2003E. Schultz et al. High Pressure Research Vol. 25, No. 1, March 2005, 71–83
112
/5
2
−= kThce
hcI λλπε
ε: The wavelength dependence of the emissivity is unknown for most crystals
Schwarzfeld objective
Problems: Pressure and temperature distribution in laser heated DAC
Laser-heated diamond–anvil cell geometry.
A. Dewaele, et al.REVIEW OF SCIENTIFIC INSTRUMENTS VOLUME 69, NUMBER 6 JUNE 1998
Temperature distribution in the diamond–anvil cell (10GPa) with a) coesite sample and solid argon, with a total heating power W=19 W; b) corresponding thermal pressure distribution.
Width defined by the entrance slit of spectrograph
Height defined by pixel size and binning
Image of hot area
Problems: Temperature determination for pulsed laser heating
Shape of our laser pulse measured with a photodetector ~solid line with filled points! and the corresponding calculated temperature of the stainless steel.
S. Rekhi, et al. REVIEW OF SCIENTIFIC INSTRUMENTS VOLUME 74, NUMBER 8 AUGUST 2003
CO2 laser heating
Raman measurementRaman measurement
Micro-Raman spectrometer (Renishaw)50 mW, 633 nm HeNe-Laser(200 mW, 532 nm Nd:YAG Laser)
AG Prof A. Woodland
PbCO3 in NaCl at 6 GPa in DAC
ContentsContents
Laser heating facility in Frankfurt •CO2 laser heating set-up
•Pressure measurement•Temperature measurement •Problems of temperature measurement •Raman measurement
Sample preparation•Laser drilling•Gas loading
Laser-heating facility in Petra III
Outlook
Laser drilling - overview (after R. Boehler)Laser drilling - overview (after R. Boehler)
GasketGasket
Spark erosion machine (H. Ahsbahs)
Gasket materials: Steel, Tungsten and Rhenium
The laser drilled hole
Gas loadingGas loading (N2, Ar, He, Ne)
ContentsContents
Laser heating facility in Frankfurt •CO2 laser heating set-up
•Pressure measurement•Temperature measurement •Problems of temperature measurement •Raman measurement
Sample preparation•Laser drilling•Gas loading
Laser-heating facility at Petra-III
Outlook
The fiberThe fiber laser heating system laser heating systemfor ‚extreme conditions‘-station@PETRA-III.
The fiberThe fiber laser heating system laser heating systemfor ‚extreme conditions‘-station@PETRA-III.
The fiberThe fiber laser heating system laser heating systemfor ‚extreme conditions‘-station@PETRA-III.
.
• CO2 and Yb:fiber laser system works for one-sided annealing and heating of transparent and not transparent samples
• Sample preparation:Autumn 2008: First gas loading in DAC
• CO2: Improvement of T- and Raman measurement
• Petra III:June 2008: Alignment and first laser heating experimentDecember 2008: one-sided laser heating system with half automationSummer 2009: double-sided laser heating system with automation
OutlookOutlook.
Acknowledgement
Dr. Alexandra Friedrich (Frankfurt University)Dr. Reinhard Boehler (MPI für Chemie, Mainz)Prof. Björn Winkler (Frankfurt University)Dr. Leonid Dubrovinsky (BGI Bayreuth)The workshop
Financial support:BMBF projekt (05KS7RF1): Laserheizung für die 'extreme conditions'-Station an Petra-III . Deutsche Forschungsgemeinschaft SPP1236 (Wi1232/25-1)JWGU Frankfurt: Cooling system for the laserChristiane-Nüsslein-Volhard Stiftung
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