Spectrum

Glassy silicate grains (1-x)MgO-xSiO2, x=0.40, T = 100 K

Title
Glassy silicate grains (1-x)MgO-xSiO2, x=0.40, T = 100 K
DOI
10.26302/SSHADE/EXPERIMENT_KD_20170711
Data reference
Demyk, Karine; Meny, Claude; Lu, Xing-Heng (2015): Mass Absorption Coefficient of 4 Mg-rich glassy silicates (1-x)MgO-xSiO2, 10 - 300 K. SSHADE/STOPCODA (OSUG Data Center). Dataset/Spectral Data. https://doi.org/10.26302/SSHADE/EXPERIMENT_KD_20170711
Publications
Experiment type
laboratory measurement
Type
absorption coefficient
Intensity unit
$cm^{2}.g^{-1}$
Instrument
vertex70v-transmission-MIR
Standard medium
vacuum
Observation mode
spectrum
Spectral range type(s)
MIR
Valid spectral range(s)
Min - Max ($cm^{-1}$) Sampling ($cm^{-1}$) Resolution ($cm^{-1}$) Position accuracy ($cm^{-1}$) Absorption edge
#1 250.0 - 2000.0 2.0
Observation geometry
direct
Observation mode
fixed angles
Observation mode
single spot
Instrument
vertex70v-transmission-FIR
Standard medium
vacuum
Observation mode
spectrum
Spectral range type(s)
FIR
Valid spectral range(s)
Min - Max ($cm^{-1}$) Sampling ($cm^{-1}$) Resolution ($cm^{-1}$) Position accuracy ($cm^{-1}$) Absorption edge
#1 10.0 - 300.0 1.0
Observation geometry
direct
Observation mode
fixed angles
Observation mode
single spot
Instrument
Brucker125V-transmission-FIR
Standard medium
vacuum
Observation mode
spectrum
Spectral range type(s)
FIR, sub-mm
Valid spectral range(s)
Min - Max ($cm^{-1}$) Sampling ($cm^{-1}$) Resolution ($cm^{-1}$) Position accuracy ($cm^{-1}$) Absorption edge
#1 10.0 - 40.0 1.0
Observation geometry
direct
Observation mode
fixed angles
Observation mode
single spot
Experiment
Mass Absorption Coefficient of 4 Mg-rich glassy silicates (1-x)MgO-xSiO2, 10 - 300 K
Date begin
2015-12-12
Release date
2018-01-31 23:51:01 UTC+0000
Version (Date)
#1 (2018-01-31 23:51:01 UTC+0000, Updated: 2022-03-31 15:13:37 UTC+0000)
History
Date Mode Version Status Comments
2017-07-13 12:50:18 UTC+0000 first import #1 valid version first import
Analysis
The spectrum is the mass absorption coeffcient (MAC, cm2/g). It is constructed from the MAC curves of KBr and PE pellets containing different masses of sample. The effect of the KBr and PE matrix is taken into account following the procedure described in Mennella et al. (1998). The error on the measured MAC is the quadratic sum of the uncertainty on the thermal stability of the spectrometer and on the uncertainty on the mass of sample in the pellet. The analysis of the spectral data to reconstruct the MAC of the samples and the details on the error determination are explained in Demyk et al. (2017).
Quality flag
5