sub-doppler spectroscopy of molecular ions in the mid-ir james n. hodges, kyle n. crabtree, &...
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Sub-Doppler Spectroscopy of Molecular Ions in the Mid-IR
James N. Hodges, Kyle N. Crabtree, & Benjamin J. McCall WI06 – June 20, 2012 University of Illinois at Urbana-Champaign
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Outline Motivation Spectroscopic Techniques for Ions: N2
+
Mid-IR Instrument H3
+ Spectroscopy Conclusions
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AstrochemistryIons reactive
intermediates in ISM
~20 ions have been observed
Many carbo-cations have transitions in mid-IR
Lab spectra help observations
H2
+
H3+
CH+
CH2+
CH3+
CH5+
CH4
C2H3+
C2H2
C3H+
C3H3+
C4H2+
C4H3+
C6H5+
C6H7+ C6H6
H2
H2
H2
H2
H2
C
e
C+
e
C+
C
H
C2H2
H2
e
OH+H2O+
H3O+H2O
OHe
O
H2
H2
HCO+
CO
HCNCH3NH2
CH3CN
C2H5CN
N, e
NH3, e
HCN, eCH3
CN, e
eCO, e
H2O, e
CH3OH, e
CHCH2CO
CH3OH
CH3OCH3
CH3+
C2H5+e
C2H4
e
C3H2
eC3H
eC2H
B.J. McCall. Ph.D. Thesis, U. Chicago, 2001.
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Indirect THz Spectroscopy
Combination differences extract energy spacings for rotational levels.
Useful for ions with transitions in the THz region - Herschel, SOFIA
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Fundamental ScienceFluxional species
Spectrum remains unassigned
WI07 up next!
White et al. Science, 284, 135 (1999).
CH5+
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MotivationGeneral, Sensitive, High Precision, Mid-IR Spectrometer for Molecular Ions
General – Multiple Ions of InterestSensitive – Weak Transitions & Trace DetectionHigh Precision – Reduced Uncertainty in Combination
Differences
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Velocity Modulation SpectroscopyCations go to cathode
Plasma Discharge Cell
+HV -HV
S.K. Stephenson and R. J. Saykally. Chem. Rev., 105, 3220-3234, (2005).
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Velocity Modulation SpectroscopyCations go to cathodeDoppler Shifted
Plasma Discharge Cell
+HV -HV
Plasma Discharge Cell
+HV -HV
Laser
Detector
S.K. Stephenson and R. J. Saykally. Chem. Rev., 105, 3220-3234, (2005).
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Velocity Modulation SpectroscopyCations go to cathodeDoppler Shifted
Plasma Discharge Cell
-HV +HV
Plasma Discharge Cell
Laser
DetectorPlasma Discharge Cell
Laser
Detector
S.K. Stephenson and R. J. Saykally. Chem. Rev., 105, 3220-3234, (2005).
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Velocity Modulation SpectroscopyCations go to cathodeDoppler Shifted AC Driven – Absorption Profile ModulatedVelocity Modulation Provides Ion-Neutral Discrimination
Plasma Discharge CellPlasma Discharge Cell
Laser
DetectorPlasma Discharge Cell
Laser
Detector
S.K. Stephenson and R. J. Saykally. Chem. Rev., 105, 3220-3234, (2005).
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Velocity Modulation of N2+
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Heterodyne Spectroscopy
Creates fm-triplet with spacing typically in the rfMixers demodulate rf signal Sensitive to relative sizes/phases of sidebandsAbsorption/Dispersion - 90o Phase Separation“Zero background”Operation at rf frequencies reduces 1/f noise
LaserDetector
EOM
Signal
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Velocity Modulation of N2+
Velocity Modulation & Heterodyne at 1 GHz
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Cavity EnhancementLaser
CavityDetector
Enhances Pathlength
Increases Intracavity Power
Allows saturation of rovibrational transitions – sub-Doppler features
Requires active locking to maintain resonance – PDH locking
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Velocity Modulation in a CavityVelocity Modulation Provides Ion-Neutral Discrimination
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Velocity Modulation
Ion Signal Encoded at 2x the Plasma Frequency
Velocity Modulation Provides Ion-Neutral Discrimination
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Cavity Enhanced Velocity Modulation Spectroscopy of N2+
PZT Detector
Detector
EOMLaser Lock-In Amplifier2f
B. M. Siller et al., Opt. Lett., 35, 1266-1268. (2010)
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NICE-OHVMS
Large Signal Small Noise
Cavity Enhancement
Heterodyne Spectroscopy
NICE-OHVMS
N oiseI mmuneC avityE nhanced-O pticalH eterodyneV elocityM odulationS pectroscopy
Velocity Modulation
Sensitivity to Ions
B. M. Siller et al., Opt. Exp., 19, 24822-24827. (2011)
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NICE-OHVMSHeterodyne sidebands at the cavity FSR allows the combination of heterodyne spectroscopy with a cavity. Cavity Modes
Laser
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NICE-OHVMS
Lock-In Amplifier
AbsorptionSignal
PlasmaFrequency
Detector
Lock-In Amplifier
DispersionSignal
90° PhaseShift
1 × Cavity FSR
Laser EOM
2f
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Comparison of Techniques on N2+
NICE-OHVMS
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Mid-IR Instrument
Optical Parametric Oscillator (OPO)
High optical powerSaturation of rovibrational transitions
Spans 3.2 – 3.9 μm range
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OPO Light Generation
Yb Doped Fiber Laser OPOEOM Am
p
1064 nm
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OPO Light Generation
Signal 1.5-1.6 m
Pump1064 nm
Idler 3.2-3.9 m
Periodically Poled Li:NbO3
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Ion Production/Velocity Modulation
~AC HV40 kHz
L-N2 InL-N2 Out Gas In
Liquid Nitrogen Cooled Positive Column Discharge Cell- ”Black Widow”
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Ion Production
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Mid-IR Instrument
OPO
YDFL
EOMLock-In
Amplifier
AbsorptionSignal
Lock-In Amplifier
DispersionSignal
Wave-meter
40 kHzPlasma
Frequency
80 MHz1 × Cavity FSR
90o Phase Shift
IPS
2f
ni = np - ns
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H3+ Spectra
Sensitivity = 2 x 10-9 cm-1 Hz-1/2
Shot Noise Limit = 8 x 10-11 cm-1 Hz-1/2
Sig
nal
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H3+ Spectra
S/N ~ 500Precision of Line Center ~ 300 kHz
Sig
nal
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Summary & Conclusions
• Constructed a general high precision mid-IR spectrometer• Demonstrated the first NICE-OHVMS spectra of H3
+
• 1.5 orders of magnitude from the shot noise limit
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Acknowledgements
McCall Group with Special thanks to:Brian Siller &Joseph Kelly
NSF GRF# DGE 11-44245 FLLWSpringborn Endowment