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Near-Infrared High Resolution Diode Laser Spectrum of the CH2 &btilde;1B1 <-- ã1A1 Transition
Fockenberg1, Marr, Sears
1Department of Chemistry, Brookhaven National Laboratory, Upton, New York, 11973-5000
Journal of Molecular Spectroscopy
|February 25, 1998
Summary
Researchers developed a sensitive diode laser spectrometer for gas-phase transient absorption. This new instrument detected previously unobserved spectra of singlet methylene (CH2), providing insights into molecular bending potentials.
Area of Science:
- Physical Chemistry
- Molecular Spectroscopy
- Laser Instrumentation
Background:
- Transient absorption spectroscopy is crucial for studying short-lived molecular species.
- High sensitivity is required to detect weak spectral features of reactive intermediates like methylene.
- Understanding the electronic and bending potentials of small molecules like CH2 is fundamental in chemistry.
Purpose of the Study:
- To construct and characterize a novel diode laser-based spectrometer for gas-phase transient absorption measurements.
- To achieve high sensitivity for detecting previously unobserved molecular spectra.
- To investigate the rovibronic structure and bending potential of singlet methylene (CH2).
Main Methods:
- Development of a diode laser spectrometer operating near 1 µm.
- Implementation of a dual-beam detection system for noise cancellation.
- Measurement of transient absorption spectra of singlet methylene (CH2) in the 9780–10070 cm⁻¹ range.
Main Results:
- The spectrometer achieved a minimum detectable absorption of 1 x 10⁻⁴ in 0.5 µsec.
- Previously undetected rovibronic spectra of singlet methylene (CH2) were observed.
- Assignment of transitions involving low-lying Ka = 1 levels in the b̃ ¹B₁ state of CH2.
Conclusions:
- The new spectrometer is highly sensitive and effective for gas-phase transient absorption studies.
- The observed spectra provide new data on the lowest energy levels of singlet methylene in the b̃ ¹B₁ electronic state.
- These findings offer valuable insights into the bending potential energy surface of CH2, particularly near the conical intersection of its lowest singlet states.