- DOI
- 10.26302/SSHADE/EXPERIMENT_ZED_20241125_01
- Data reference
- Dionnet, Zélia; Djouadi, Zahia (2022): MIR transmission spectra of two Ryugu fragments from chamber C. SSHADE/DAYSY (OSUG Data Center). Dataset/Spectral Data. https://doi.org/10.26302/SSHADE/EXPERIMENT_ZED_20241125_01
- Publications
- Database(s)
- Experimentalists
- Type(s)
- laboratory measurement
- Description
- Hyper-spectrale MIR spectroscopy of Ryugu framents from chamber C in tranmission (samples crushed in a diamand compression cell)
- Number of spectra
- 6
- Variable type(s)
-
- sample composition
- Laboratory
- Institut d'Astrophysique Spatiale (IAS)
- Instrument
- SMIS Cary 670 - trans Mid-IR
- Sample holder
- The sample was crushed in a diamond compression cell, which is transparent in the IR range.
- 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 #1 850.0 - 3900.0 4.0 4.0 1.0
Definition: incidence and emergence angles are positive with origin at nadir. Emergence angle in transmission is larger than 90° (=180°-i).
- Observation geometry
- direct
- Observation mode
- fixed angles
- Observation mode
- averaged
- Spots number
- 16384
- Objective type
- x25
- Pixels separation
- 0.66 x 0.66 ${\mu}m$
- Pixels number
- 128 x 128
- Image size
- 84.48 x 84.48 ${\mu}m$
- Comments
- The resolution changes with the wavelenght according to the Abbe's equation.Average spectra was calculted over various area in sample C0002-FC027 and C0002-FC028. We removed pixels with no sample and noisy pixels from the IR hyperspectral images, by filtering the images based on the signal-to-noise ratio in the range of aliphatic CH stretching modes; we selected the spectra with a signal-to-noise ratio greater than 10
- Date begin - end
- 2022-01-01 - 2023-09-01
Versions
- Release date
- 2024-11-25 15:46:04 UTC+0000
- Version (Date)
- #1 (2024-11-25 15:46:04 UTC+0000, Updated: 2024-11-25 16:11:00 UTC+0000)