Transcript WH12_b.ppt

Amanda L. Steber, Brent J. Harris, Kevin K. Lehmann and
Brooks H. Pate
Department of Chemistry, University of Virginia,
Charlottesville, VA 22904
Fourier Transform Millimeter
Wave Spectroscopy
 Don’t detect against a light source
 High Power
 Double resonance capabilities
FT
Challenges?
 Low cost alternatives to current light source generation
and digitizers
 Needs to be coherent over long time acquisitions
 High Dynamic Range detections
Instrument Schematic
Nutation Experiments
p
p/2
Time
 25 ns resolution
 Fit to a bessel function
 Related to dipole moment
R = E/ 
Spectrometer Sensitivity
 Signal Averaging in the Time domain
 Coherent light source
 Fill up the memory depth (160ms)
 Stack
 FT
 Steps for
Frequency
Determination:
 Determine
experiment
length (time)
 Determine
frequency at
synth
 Determine
frequency at
which you
will have n*P
Spectrometer Performance
 18O13CS J=24-23
detected in natural
abundance in 10,000
averages (10:1)
 0.002% of the parent
(50,000:1)
 Pressure: 15 mT
Exact Resonance NOT Required
J = 22-21
OCS
FT
 Sync shape from FT
 Width of pulse dictates
width of power envelop
250 ns =4 MHz OR
1 s = 1 MHz
Verification/Analysis
n1 n2
 Double Resonance
P+Δ
P
“p” pulse
P+Δ
P
ΔP=2Δ
ΔP=Δ
P-Δ
Signal ∝ ΔP ∝ Δ
P-Δ
P1
 e  E / kT
P2
Double Resonance Modulation
60% modulation
J=22-21
Selection of Two Color Pulse
Duration
Uses and Application
 Spectroscopy
 Verify assignments
 Verify a gas detection
 Reduce false positives
 Important in overlaps
Application
Acrolein
10,000 averages
Pressure: 2 mTorr
Potential Limitations
 Speed issues
 USB 2.0 – slow transfer speeds
 Must change the frequency of the synthesizer (35.2 ms)
 The amount of memory dictates how many averages
can be collected
 For a measurement that is 5s, you can get 32,000 avgs
 Can’t do real time accumulation
Conclusions
 Advances in technology allow for the use of low cost
components
 Can be used to analyze/characterize a molecule
 Nutation experiment – helps determine correct pulse
lengths and helps determine the dipole moment
 Averaging in the time domain – increases sensitivity

Do NOT have to be on resonance
 Double Resonance – Spectrum Verification
Acknowledgements
 Pate Lab
 NSF CCI (Center for Chemistry of the Universe)
 CHE-0847919
Dual Color Detuning
 Monitoring the J = 22-
21 transition of OCS
while changing the
frequency of the pulse
to pump the J = 23-22
transition
 120 kHz resolution
 Near optimal
resolution occurs
within 360 kHz of
resonance