Method Article

Characterizing Far-infrared Laser Emissions and the Measurement of Their Frequencies

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DOI:

10.3791/53399

December 18th, 2015

In This Article

Summary

We describe the generation of far-infrared radiation using an optically pumped molecular laser along with the measurement of their frequencies with heterodyne techniques. The experimental system and techniques are demonstrated using difluoromethane (CH2F2) as the laser medium whose results include three new laser emissions and eight measured laser frequencies.

Abstract

The generation and subsequent measurement of far-infrared radiation has found numerous applications in high-resolution spectroscopy, radio astronomy, and Terahertz imaging. For about 45 years, the generation of coherent, far-infrared radiation has been accomplished using the optically pumped molecular laser. Once far-infrared laser radiation is detected, the frequencies of these laser emissions are measured using a three-laser heterodyne technique. With this technique, the unknown frequency from the optically pumped molecular laser is mixed with the difference frequency between two stabilized, infrared reference frequencies. These reference frequencies are generated by independent carbon dioxide lasers, each stabilized using the fluorescence signal from an external, low pressure reference cell. The resulting beat between the known and unknown laser frequencies is monitored by a metal-insulator-metal point contact diode detector whose output is observed on a spectrum analyzer. The beat frequency between these laser emissions is subsequently measured and combined with the known reference frequencies to extrapolate the unknown far-infrared laser frequency. The resulting one-sigma fractional uncertainty for laser frequencies measured with this technique is ± 5 parts in 107. Accurately determining the frequency of far-infrared laser emissions is critical as they are often used as a reference for other measurements, as in the high-resolution spectroscopic investigations of free radicals using laser magnetic resonance. As part of this investigation, difluoromethane, CH2F2, was used as the far-infrared laser medium. In all, eight far-infrared laser frequencies were measured for the first time with frequencies ranging from 0.359 to 1.273 THz. Three of these laser emissions were discovered during this investigation and are reported with their optimal operating pressure, polarization with respect to the CO2 pump laser, and strength.

Introduction

The measurement of far-infrared laser frequencies was first performed by Hocker and co-workers in 1967. They measured the frequencies for the 311 and 337 μm emissions from the direct-discharge hydrogen cyanide laser by mixing them with high order harmonics of a microwave signal in a silicon diode1. To measure higher frequencies, a chain of lasers and harmonic mixing devices were used to generate the laser harmonics2. Eventually two stabilized carbon dioxide (CO2) lasers were chosen to synthesize the necessary difference frequencies3,4. Today, far-infrared laser frequencies up to 4 THz can be measured with this technique....

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Protocol

1. Planning of Experiments

  1. Conduct a survey of the literature to assess prior work performed using the laser medium of interest, which for this experiment is CH2F2. Identify all known laser emissions along with all information about the lines such as their wavelength and frequency. Several surveys of known laser emissions are available13,3137.
  2. Compile all spectroscopic investigations of the molecule used as the laser medium with a focus on prior Fourier transform34 and optoacoustic studies38,39.

2. Generating Far-Infrared Laser Emi....

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Results

As mentioned, the frequency reported for a far-infrared laser emission is an average of at least twelve measurements performed with at least two different sets of CO2 reference laser lines. Table 2 outlines the data recorded for the 235.5 μm laser emission when using the 9P04 CO2 pump laser. For this far-infrared laser emission, fourteen individual measurements of the beat frequency were recorded. The first set of measurements were recorded while using the 9R10 and.......

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Discussion

There are several critical steps within the protocol that require some additional discussion. When measuring the far-infrared laser wavelength, as outlined in step 2.5.3, it is important to ensure the same mode of the far-infrared laser emission is being used. Multiple modes of a far-infrared laser wavelength (i.e., TEM00, TEM01, etc.) can be generated within the laser cavity and thus it is important to identify the appropriate adjacent cavity modes being used to measure the wavelength.......

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Disclosures

Certain commercial equipment is identified in this paper to foster understanding. Such identification does not imply recommendation or endorsement by the authors, nor does it imply that the equipment identified is necessarily the best available for the purpose.

Acknowledgements

This work was supported in part by the Washington Space Grant Consortium under Award NNX10AK64H.

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Materials

List of materials used in this article
NameCompanyCatalog NumberComments
Vacuum pumpLeyboldTrivac D4AHE-175 oil; Quantity = 3
Vacuum pumpLeyboldTrivac D8B or D16BFomblin Fluid; Quantity = 1 of each
Vacuum pumpLeyboldTrivac D25BHE-175 oil; Quantity = 1
Optical chopper with controllerStanford Research SystemsSR540
Lock-in amplifierStanford Research SystemsSR830
Spectrum analyzerAgilentE4407BESA-E Series, 9 kHz to 26.5 GHz Spectrum Analyzer
Amplifier MiteqAFS-44Provides amplification of signals between 2 and 18 GHz. The amplifier is powered by a Hewlett Packard triple output DC power supply, model E3630A.
Amplifier AvantekAWL-1200BProvides amplification of signals less than 1.2 GHz.
Power supplyHewlett PackardE3630ALow voltage DC power supply for amplifier.
Power supplyGlassmanKL SeriesHigh voltage power supply for the CO2 lasers; Quantity = 2; negative polarity
Power supplyFluke412BHigh voltage power supply used with the NIST Asymmetric HV Amp
DetectorJudson Infrared IncJ10DFor fluorescence cell; Quantity = 2
CO2 laser spectrum analyzerOptical Engineering 16-ACurrently sold by Macken Instruments Inc.
Thermal imaging plates with UV lightOptical Engineering Primarily used for aligning the CO2 reference lasers. Currently sold by Macken Instruments Inc.
ResistorsOhmite L225J100K100 kW, 225 W. Between 4 to 6 resistors are used in each ballast system. Each CO2 laser has its own ballast system. Fans are used to cool the resistors.
HV relay, SPDTCII TechnologiesH-17Quantity = 3; one for each CO2 laser
Amplifier Princeton Applied ResearchPAR 113Used with fluorescence cell; Quantity = 2
OscilloscopeTektronix2235ASimilar models are also used; Quantity = 2
Oscilloscope/Differential amplifierTektronix7903 oscilloscope with 7A22 differential amplifier
Power meter with sensorCoherent200For use below 10 W.  This is the power meter shown in Figure 2.
Power meter with sensorScientech, IncVector S310For use below 30 W
MultimeterFluke73IIISimilar models are also used; Quantity = 3
Data acquisitionNational InstrumentsNI cDAQ 9174 chassis with NI 9223 input moduleUses LabVIEW software
Simichrome polishHappich GmbHPolish for the Nickel base used in the MIM diode detector. Although the Nickel base can be used immediately after polishing, a 12 hour lead time is typically recommended.
Pressure gaugeWallace and Tiernan61C-1D-0050Series 300; for CO2 laser; Quantity = 3
Pressure gauge with controllerGranville PhillipsSeries 375For far-infrared laser
Zirconium Oxide feltZircar ZirconiaZYF feltUsed as a beam stop
Zirconium Oxide boardZircar ZirconiaZYZ-3 boardUsed as a beam stop; Quantity = 4
Teflon sheetScientific Commodities, IncBB96312-12481/32 inch thick; used for the far-infrared laser output window
PolypropyleneC-Line sheet protectors61003used for the far-infrared laser output window
Vacuum greaseApiezon
Power supplyKepcoNTC 2000PZT power supply
PZT tubeMorgan Advanced Materials1 inch length, 1 inch outer diameter, 0.062 inch thickness, reverse polarity (positive voltage on outside); Quantity = 3
ZnSe (AR coated)II-VI IncCO2 laser window (Quantity = 3), lens, and beam splitter (Quantity 3)
NaCl windowEdmond OpticsQuantity = 1
CaF windowEdmond OpticsQuantity = 2
Laser mirrors and gratingsHyperfine, IncGold-coated; includes positioning mirrors
Glass laser tubes and reference cellsAllen Scientific Glass
MIM diode detectorCustom Microwave, Inc
OtherOther materials include magnetic bases, base plates, base clamps, XYZ translation stage, etc.

References

  1. Hocker, L. O., Javan, A., Ramachandra Rao, D., Frenkel, L., Sullivan, T. Absolute frequency measurement and spectroscopy of gas laser transitions in the far infrared. Appl. Phys. Lett. 10 (5), 147-149 (1967).
  2. Wells, J. S., Evenson, K. M., Day, G. W., Halford, D. Role of inf....

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Tags

Three Laser Heterodyne TechniqueOptically Pumped Molecular LaserCarbon Dioxide Reference LasersMetal Insulator Metal Diode DetectorSpectrum Analyzer Frequency MeasurementDifluoromethane Laser MediumBeat Frequency AnalysisLaser Frequency UncertaintyTerahertz Imaging Applications

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