Frequencies of cw FIR laser lines from optically pumped CH2F2

The frequencies of 48 optically pumped cw FIR CH₂F₂ laser lines have been measured relative to stabilized CO₂ lasers. Uncertainties are estimated to be about 5 parts in 10⁷.     

New cw FIR laser lines from optically pumped ammonia analogues

Two new cw submillimetre lines optically pumped by the 9 μR(30) CO₂ laser have been observed for¹⁴NH₃ and assigned to thea(6,0)→s(5,0) transition and to its cascade transitions(5,0)→a(4,0) in thev ₂=1 state. In addition, six new emission lines have been observed for NH₂D, and one tentatively assigned to the (11,1)→(10,1) transition of ND₃. Methylamine has also been investigated and twenty-eight new emission lines have been discovered.     

Dispersion in a cw optically pumped FIR laser

Direct frequency measurements of a¹³CO₂/¹⁵NH₃ OPFIRL output show that laser pulling effects give shifts of a few MHz, which agree well with a density matrix calculation.     

New FIR laser lines from CHD2OH optically pumped by a cw CO2 laser

This work reports 83 new optically pumped far infrared laser lines, using deuterated methyl alcohol, CHD₂OH, as active medium. For each line we list the measured wavelength, its polarization relative to the pump line, the optimum gas pressure and the CO₂ laser pump power at the maximum absorption.     

Anisotropic gain in an optically pumped cw FIR laser

The observed asymmetry of tuning curves of a 70.6 μm CH₃OH laser is interpreted as a consequence of unidirectional amplification in the optically pumped gas, a quantum mechanical double resonance effect. The occurrence of this effect. was verified by FIR gain measurements.     

New cw FIR laser lines from optically pumped silyl fluoride (SiH3F)

FIR laser action has been observed for the first time in a molecule containing silicon: silyl fluoride, SiH₃F. Eleven new cw optically pumped lines between 187 and 1014m were detected from both open resonator and waveguide structures. Although the chlorine analogue, SiH₃Cl, showed strong absorption at every CO₂ laser frequency no FIR laser emission was detected at the pump powers available.     

Nonlinear refraction spectroscopy in resonance with laser lines in solids

We report a simple extension of the Z-scan technique that permits a spectral line-shape measurement of the real and the imaginary parts of n(2) . In this technique the sample is placed at the peak position of the usual Z-scan curve while the laser frequency is scanned. We employed this method to investigate the nonlinear susceptibility of the R lines of ruby and alexandrite, using a cw dye laser. This susceptibility can be explained by the resonant interaction and by a nonresonant contribution that is due to the difference in polarizability between Cr(3+) excited and ground states. For ruby, the nonresonant contribution to the technique is 1 order of magnitude larger than the resonant contribution. However, for alexandrite both contributions are comparable, and their interference leads to a shift between n(2)(?) and n(2)(??) spectra that is not observed in ruby.     

FIR gain measurements in cw laser pumped CH3OD

Direct measurements of small signal and saturated gain in cw laser pumped CH₃OD are reported for three lasing transitions of 57 m, 82 m and 103 m. The 57 m transition has a measured gain of 0.6/m, the strongest gain in methanol reported so far. Moreover small gain saturation of this line makes it to be one of the strongest known cw FIR laser lines.     

A frequency stabilized,cw dye laser for high resolution spectroscopy

A single frequency, jet stream cw dye laser spectrometer locked to a stable high finesse optical reference cavity is described. This system is capable of maintaining a frequency stability of ± 1 MHz/min and a continuous scan of up to 6 GHz.     

Frequencies of some optically pumped submillimetre laser lines

Precise frequencies of far infrared (FIR-) laser lines of HCOOH, CH₃OH, CH₃I, CH₃F have been measured by comparison with harmonics of frequency-locked mm-wave klystrons.     

Nondestructive probing of free jets using cw laser Raman spectroscopy

Experimental fluid dynamic studies have been performed using cw laser Raman spectroscopy. The system capabilities for concentration measurements are shown in initially laminar and turbulent free jets.     

Saturation spectroscopy of hydrogen 1-011-011-01lines with a multi-mode cw dye laser

With an intense, broadband multi-mode cw dye laser collisional studies of H_α fine-structure resonances with saturated absorption are extended to He buffer gas pressures larger than 30 mbar (0°C). The broadening and shift of the two prominent H_α(2P?3D) transitions are measured in a (He+4% H) gas discharge. The absolute magnitude and the differences in the width of the lines are explained theoretically by different inelastic fine-structure transfer cross sections which can also be deduced from the pressure effect data. Nuclear polarization of hydrogen atoms by H_α optical pumping and polarization transfer to the H(1S) ground state via Ly-α decay and further applications of the multimode laser are discussed.     

Discovery and characterization of optically pumped far-infrared laser emissions using laser magnetic resonance spectroscopy

A laser magnetic resonance spectrometer has been used to discover and subsequently measure a far-infrared laser emission: the 166.6-micron line of CH₂F₂, optically pumped by the 9P24 CO₂ laser. By recording spectra for the NH radical, the frequency of this laser emission has been determined to be 1799950±13 MHz. Spectra for the NH radical were also recorded with two other far-infrared laser emissions: the 160.4-micron line of N₂H₄ (9P46 CO₂ pump) and the 328.6-micron line of ¹³CH₃OH (9P12 CO₂ pump). From the NH spectra, a discrepancy of 2.1 GHz with the previously measured laser frequency was identified for the 160.4-micron line. A three-laser heterodyne system was then used to remeasure the frequency to be 1868475.5±0.5 MHz. The NH spectra were also used to determine the frequency for the 328.6-micron line to be 912366±7 MHz, in agreement with the value previously calculated from the Rydberg–Ritz combination principle. PACS 07.57.Hm; 32.60.+i; 42.62.Eh     

New FIR laser lines from hydrazine and assignments

Our new waveguide pulsed CO₂ laser, with peak powers above 1 kW, has allowed us to observe 24 new far-infrared laser lines emitted by hydrazine. Each of them is characterized in wavelength, relative polarization, intensity, optimum operating pressure and pump offset from the center of the exciting CO₂ line. These new laser emissions either form pairs sharing the same pump line, or complete such pairs with lines known from the literature. In the latter case, we have measured the relative polarization and offset of the partner lines whenever they were not reported in the literature. The availability of laser systems with two emission lines orthogonally polarized and sharing the same upper level is expected to facilitate the assignment work. We present complete assignments for four FIR laser emissions, and we propose J and K values for 12 further laser systems. PACS 42.55.Lt; 42.62.Fi     

High-resolution spectroscopy with and frequency stabilization of a cw dye laser

The hyperfine splittings of the Na D₁ and D₂ lines were investigated using a single mode cw dye laser. The light of the laser was scattered by the atoms of an atomic beam and the fluorescent light was observed as the frequency of the laser was tuned across the D lines. The Doppler width of the atomic beam was reduced to about 2.5 MHz so that the absorption width of the atoms of the beam was essentially determined by the natural width of the 3²P_1/2 and 3²P_3/2 levels, which is about 10 MHz. Since the linewidth observed for the hyperfine transitions was 30 MHz, most of the hyperfine components of the D₁ and D₂ lines could be resolved. In another experiment the frequency of the dye laser was locked to a hyperfine transition of the D₁ line. The observed variation of the output frequency of the dye laser was less than ±1.5 MHz. In addition, the intensity of the dye laser was controlled to about 10⁻³, using an electro-optically variable transmission filter.     

Double-resonance circuit for nuclear magnetic resonance spectroscopy

A new double-resonance probe circuit design is described. The circuit contains no quarter-wavelength elements or equivalents, yet nonetheless achieves adequate isolation between the two input channels. It contains relatively few components, and so is both compact and efficient. It has been incorporated in two solid-state nuclear magnetic resonance (NMR) probes, with excellent results.     

New FIR laser lines from optically pumped methanol analogues

Several new laser lines using optically pumped deuterated methanol molecules have been discovered. These not only increase the spectral coverage of pumped methanol isotopes but may assist in the assignment of a molecular structure.     

Relaxation studies in magnetic resonance spectroscopy

The electron spin and nuclear spin relaxation in liquid solution arising from the electron-nuclear interaction is determined for the general case when the g-tensor may be anisotropic and the nine hyperfine interaction tensor components may be all different. The theoretical expressions are used in an attempt to interpret the relaxation times T ₁ and T ₂ for the various nuclei in the complex ruthenium acetylacetonate.