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Charles R. Markus, Adam J. Perry, James N. Hodges, Benjamin J. McCall

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1 Charles R. Markus, Adam J. Perry, James N. Hodges, Benjamin J. McCall
Improved Spectroscopy of Molecular Ions in the Mid-Infrared with Up-Conversion Detection Charles R. Markus, Adam J. Perry, James N. Hodges, Benjamin J. McCall 71st International Symposium on Molecular Spectroscopy University of Illinois at Urbana-Champaign 21 June, 2016 TC07

2 Overview NICE-OHVMS technique Removing parasitic etalons
Description Limitations Removing parasitic etalons Mechanism of detection Brewster-Spoiler plate Up-conversion detection Design Results Future directions

3 Molecular Ions H Over 190 molecules identified in the interstellar medium (ISM) Reactions must overcome cold and diffuse environment Ion-neutral reactions dominate chemistry of ISM Aleman, et al., A&A,2014, 566, A79. πœ‡m πœ‡m

4 Molecular Ions H Many of the simplest molecules are molecular ions Accurate ab initio calculations must go beyond Born-Oppenheimer approximation Laboratory spectra act as benchmarks for state-of-the-art methods H He H

5 Ion Spectroscopy Ion are orders of magnitude less abundant than neutral species

6 NICE-OHVMS Noise Immune Cavity Enhanced Optical Heterodyne Velocity Modulation Spectroscopy

7 Increased Signal and Precision
NICE-OHVMS Noise Immune Cavity Enhanced Optical Heterodyne Velocity Modulation Spectroscopy Increased Signal and Precision K. N. Crabtree, et al., Chem. Phys. Lett., 2012, 551, 1-6.

8 Increased Signal and Precision
NICE-OHVMS Noise Immune Cavity Enhanced Optical Heterodyne Velocity Modulation Spectroscopy Increased Signal and Precision Improved Sensitivity K. N. Crabtree, et al., Chem. Phys. Lett., 2012, 551, 1-6.

9 Increased Signal and Precision Ion-Neutral Discrimination
NICE-OHVMS Noise Immune Cavity Enhanced Optical Heterodyne Velocity Modulation Spectroscopy Increased Signal and Precision Ion-Neutral Discrimination Improved Sensitivity K. N. Crabtree, et al., Chem. Phys. Lett., 2012, 551, 1-6.

10 Velocity Modulation Velocity
C. S. Gudeman, et al., J. Chem. Phys., 1983, 78, 5873.

11 - - + + Velocity Modulation Velocity Lock-in Amplifier
C. S. Gudeman, et al., J. Chem. Phys., 1983, 78, 5873.

12 - - + + Velocity Modulation Velocity Lock-in Amplifier
B. M. Siller, et al., Opt. Lett., 2010, 35, 1266.

13 - - + + Velocity Modulation 𝜈 Lock-in Amplifier Lock-in Amplifier
Referenced at 2×𝑓 𝜈 B. M. Siller, et al., Opt. Lett., 2010, 35, 1266

14 Cavity Enhancement Signal increase of 2F/πœ‹ FSR =𝑐/2𝑛𝑙 𝐼 π‘‘π‘Ÿπ‘Žπ‘›π‘  𝜈

15 Heterodyne Detection

16 NICE-OHMS 𝐼 π‘‘π‘Ÿπ‘Žπ‘›π‘  𝜈 Fheterodyne = nΓ—FSR
J.Ye, et al., J. Opt. Soc. Am. B, 1998, 15, 6.

17 Saturation Spectroscopy
πœˆβˆ’ 𝜈 π‘Ÿπ‘’π‘ π‘‘ (MHz) Velocity (m/s)

18 Saturation Spectroscopy
πœˆβˆ’ 𝜈 π‘Ÿπ‘’π‘ π‘‘ (MHz) Velocity (m/s)

19 Saturation Spectroscopy
πœˆβˆ’ 𝜈 π‘Ÿπ‘’π‘ π‘‘ (MHz) Velocity (m/s)

20 Saturation Spectroscopy
πœˆβˆ’ 𝜈 π‘Ÿπ‘’π‘ π‘‘ (MHz) Velocity (m/s)

21 Saturation Spectroscopy
πœˆβˆ’ 𝜈 π‘Ÿπ‘’π‘ π‘‘ (MHz) Velocity (m/s)

22 Saturation Spectroscopy
πœˆβˆ’ 𝜈 π‘Ÿπ‘’π‘ π‘‘ (MHz) Velocity (m/s)

23 NICE-OHVMS Spectrometer
Frequency Calibration 40 kHz to PZT OPO PZT nidler = npump - nsignal ~3 MHz EOM Lock-In Amplifier Lock-In Amplifier Ξ½ 2xf = 80 kHz 80 MHz YDFL X & Y Channels X & Y Channels 90o Phase Shift Fast Lock Box Slow B. M. Siller, et al., Opt. Express,2011, 19,

24 NICE-OHVMS Results H3+ R(1,0), 2725.898 cm-1 80 MHz Mixer 1 Mixer 2
2Γ—40 kHz Lock-in 1 Lock-in 2 0o 90o Mixer 1 Output Mixer 2 Output H3+ R(1,0), cm-1

25 Parasitic Etalons 𝜈 𝐼 𝜈 𝐼 𝜈 𝐼 FSR = 𝑐 2𝒏𝑙 𝑛 𝑑 =𝛼×sin⁑(2 πœ” π‘£π‘šπ‘  𝑑)

26 Spoiling Parasitic Etalons
𝜈 𝐼

27 Spoiling Parasitic Etalons
𝜈 𝐼 C. Webster, et al., J. Opt. Soc. Am., 1985, 2, 1464.

28 Spoiling Parasitic Etalons
Mixer 1 Output H3+ R(1,0), cm-1 Mixer 2 Output Galvo S/N (best channel) Off 25 On 763 Galvo S/N (best channel) Off 25

29 Heterodyne Detection 𝑓 𝐻𝑒𝑑 = 20% FWHM Overlapping sub-Doppler features
Optimized signal Resolved Lamb dips Improved fits Improved Ξ”πœ†

30 Difference Frequency Generation
πœ‚ 𝐷𝐹𝐺 = 0.5% /W532 APD V10 Vigo PVM-10.6 Menlo APD 220 Ξ”πœˆ 150 (MHz) 1000 MHz NEP 4800 (pW/Hz1/2) 0.4 (pW/Hz1/2) Vigo PVM-10.6 Ξ”πœˆ 150 (MHz) NEP 4800 (pW/Hz1/2) Vigo PVM-10.6 Menlo APD 220 Ξ”πœˆ 150 (MHz) 1000 MHz NEP 4800 (pW/Hz1/2) 0.4 (pW/Hz1/2) NEP/( πœ‚ 𝐷𝐹𝐺 Γ— 𝑃 π‘π‘’π‘šπ‘ ) 10 (pW/Hz1/2)

31 Up-conversion Results
H3+ R(1,0), cm-1 Mixer 1 Output Mixer 2 Output Detection Method S/N (Best Channel) 78 MHz mid-IR 337 78 MHz up-conversion 2029 390 MHz up-conversion 1211 Detection Method S/N (Best Channel) 78 MHz mid-IR 337 Detection Method S/N (Best Channel) 78 MHz mid-IR 337 78 MHz up-conversion 2029

32 Up-conversion Results
4.2Γ— 10 βˆ’9 cm-1 3.5Γ— 10 βˆ’10 cm-1 Detection Method 78 MHz mid-IR 78 MHz up-conversion 390 MHz up-conversion 1.6Γ— 10 βˆ’10 cm-1

33 Future Directions H Apply up-conversion to survey of H3+
Measure fundamental band (3 – 4.5 πœ‡m) Hotband transitions Extend to measure overtone transitions (1.9 – 2.1 πœ‡m) Observe resolved Lamb dips Increase intracavity power Lock sidebands using DeVoe-Brewer locking H Ξ½ (c m βˆ’1 )

34 Conclusions Removed parasitic etalons in NICE-OHVMS experiment with Brewster-spoiler plate Improved sensitivity by an order of magnitude with DFG up-conversion of mid-IR beam

35 Acknowledgments Advisor: Ben McCall Special thanks to: James Hodges
Adam Perry G. Stephen Kocheril


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