EM27/SUN
Transcription
EM27/SUN
EM27/SUN Dr. Michael Gisi, Bruker Optik GmbH May 30, 2014 1 EM27/SUN • RockSolid™ pendulum FTIR-Spectrometer • Resolution: 0.5 cm-1, double-sided • RT-InGaAs Detector (NIR) • 470 x 630 x 350 cm • Mass: ~25 kg incl. tracker May 30, 2014 2 New-developed Solar-Tracker • Total weight: <5 kg • Beam diameter: 40 mm • High resolution • Optical feedback by Cam-Tracker principle: Gisi et al.: Camtracker: a new camera controlled high precision solar tracker system for FTIR-spectrometers, AMT 2011. May 30, 2014 3 Internal setup Adjustable aperture stop (default: 5mm) Camera for CamTracker Field stop and detector TCP/IP 24V USB Internal source May 30, 2014 Space for gas cell (5cm) + T-sensor Preliminary data - do not redistribute EM27/SUN: Solar NIR spectra 2 Detector options: CO2 CH4 • Narrow: 5000-11000cm-1 CO • Wide: 4000-11000cm-1 Note: Wide-band-detector has lower SNR (~x2) O2 For analysis results see: Gisi et al.: XCO2-measurements with a tabletop FTS using solar absorption spectroscopy AMT 2012 May 30, 2014 5 Sampling Ghost Artifacts EM27/SUN has the new linear laser diodes however: no possibility to adjust comparator level In addition: EM27/SUN not in conditioned environment: → influences on electronics by temperature Typical GPR-values ~ 2-4 May 30, 2014 6 Interpolation of zero crossings Current electronics (“M16”) enables linear interpolation of descending zero crossings from ascending crossings: Ghost May 30, 2014 No Ghost when interpolation enabled Parent signal 7 Interpolation of zero crossings Side-effects may be lower sampling position accuracy due to linear interpolation: • Statistical errors in interpolation position → Noise in spectra No significant increase of SNR observed even when exposed to vibrations. • Systematic sampling position errors due to systematic OPD-dependent change of scanner speed → kind of „OPD-dependent Ghost“ How strong are these distortions? May 30, 2014 8 Inspecting pendulum movement Scanner-velocity deviation (Hz) Using spectrometer‘s „Real-Time Diagnostics“ Java-applet: Scanner position (½λ) May 30, 2014 9 Real time-diagnostics Animation Scanner Speed: 10kHz May 30, 2014 Tapping on table with finger 10 Influence on interpolation Systematic increase of speed causes systematic missampling in this IFG-range However: Effect is small, here about 0.0002λHeNe @10kHz (for comparison: original ghosts of IFS125HR were ~ 0.01 λHeNe) In addition: further optimization possible (by user) by adapting mirror reversal parameters and increasing reversal-range. May 30, 2014 11 Knocking on spectrometer: May 30, 2014 12 Interpolation of zero crossings • Interpolation of descending zero crossings may be a good way to remove sampling ghost-artifacts. • Influences on spectra are estimated to be very small. • Further (spectrometer-dependent) optimizing possible Contact me… (e.g.: It is very hard to get Java-applet running on due to Java security settings) May 30, 2014 13 Thank you Comments, Questions, …. May 30, 2014 14 www.bruker.com For research use only. Not for use in diagnostic procedures. Copyright © 2010 Bruker Optics. All rights reserved. May 30, 2014 15 May 30, 2014 16