A FABRY-PERÓT CAVITY PULSED FOURIER TRANSFORM W-BAND SPECTROMETER WITH A PULSED NOZZLE SOURCE. GARRY S. GRUBBS II, CHRISTOPHER T. DEWBERRY AND STEPHEN.

Slides:



Advertisements
Similar presentations
Investigation of the Use of He-Diatomic Van der Waals Complexes as a Probe of Time Reversal Violation Jacob Stinnett, Dr. Neil Shafer-Ray, and Dr. Eric.
Advertisements

Direct Frequency Comb Spectroscopy for the Study of Molecular Dynamics in the Infrared Fingerprint Region Adam J. Fleisher, Bryce Bjork, Kevin C. Cossel,
CAVITY RING DOWN SPECTROSCOPY
FOURIER TRANSFORM MICROWAVE SPECTROSCOPY OF ALKALI METAL ACETYLIDES P. M. SHERIDAN, M. K. L. BINNS Department of Chemistry and Biochemistry, Canisius College.
Alternating Current Electromagnetic Waves. Sinusoidal Function of Distance A sinusoidal function of distance is characterized by its: amplitude, wavelength,
AUSTIN L. MCJUNKINS, K. MICHELLE THOMAS, APRIL RUTHVEN, AND GORDON G. BROWN Department of Science and Mathematics, Coker College, 300 E College Ave., Hartsville,
Broadband Cavity Enhanced Absorption Spectroscopy With a Supercontinuum Source Paul S. Johnston Kevin K. Lehmann Departments of Chemistry & Physics University.
The Search is Over: Design and Applications of a Chirped Pulse Fourier Transform Microwave (CP- FTMW) Spectrometer for Ground State Rotational Spectroscopy.
1 숙명여자대학교 지구환경연구소 Ground-Based Microwave Observation of Stratospheric Ozone April 3, 2003 Jung Jin Oh Sookmyung Women’s University Seoul, South Korea.
Measurement of the Vibrational Population Distribution of Barium Sulfide, Seeded in an Argon Supersonic Expansion, Following Production Through the Reaction.
Microwave Spectroscopy I
Design of Standing-Wave Accelerator Structure
Radar: Acronym for Radio Detection and Ranging
Electron Paramagnetic Resonance spectrometer
Laser System for Atom Interferometry Andrew Chew.
Construction of a 480 MHz Chirped-Pulse Fourier-Transform Microwave Spectrometer: The Rotational Spectra of Divinyl Silane and 3,3-Difluoropentane Daniel.
Physical and Chemical Tests 10-1 Purification: Chromatography Distillation Recrystallization Comparison to known compounds: Melting point Boiling point.
Rotational Spectra of Methylene Cyclobutane and Argon-Methylene Cyclobutane Wei Lin, Jovan Gayle Wallace Pringle, Stewart E. Novick Department of Chemistry.
An Acoustic Demonstration Model for CW and Pulsed Spectroscopy Experiments Torben Starck, Heinrich Mäder Institut für Physikalische Chemie Christian-Albrechts-Universität.
Chirped Pulse Fourier Transform Microwave Spectroscopy of SnCl Garry S. Grubbs II and Stephen A. Cooke Department of Chemistry, University of North Texas,
Galen Sedo, Jane Curtis, Kenneth R. Leopold Department of Chemistry, University of Minnesota The Dipole Moment of the Sulfuric Acid Monomer.
Chirped-Pulse Fourier Transform mm-Wave Spectroscopy from GHz Brent J. Harris, Amanda L. Steber, Justin L. Neill *, Brooks H. Pate University of.
High Resolution Measurements and Electronic Structure Calculations of a Diazanaphthalene: [1,6]-naphthyridine. Sébastien Gruet, Manuel Goubet, Olivier.
The inversion motion in the Ne – NH 3 van der Waals dimer studied via microwave spectroscopy Laura E. Downie, Julie M. Michaud and Wolfgang Jäger Department.
PURE ROTATIONAL SPECTRA OF THE REACTION PRODUCTS OF LASER ABLATED THORIUM METAL AND OXYGEN MOLECULES ENTRAINED WITHIN SUPERSONIC EXPANSIONS OF NOBLE GASES.
HYPERFINE SPLITTING AND ROTATIONAL ANALYSIS OF THE DIATOMIC MOLECULE ZINC MONOSULFIDE, ZnS DANIEL J. FROHMAN, G. S. GRUBBS II AND STEWART E. NOVICK O.S.U.
High-Resolution Spectroscopy of the ν 8 Band of Methylene Bromide Using a Quantum Cascade Laser-Based Cavity Ringdown Spectrometer Jacob T. Stewart and.
1 Fourier transform microwave and infrared study of silacyclobutane Cody van Dijk, Samantha van Nest, Ziqiu Chen and Jennifer van Wijngaarden Department.
Spectral Simplification Methods Development Using Waveguide Chirped-Pulse Fourier Transform Microwave Spectroscopy Erin Kent, Steven Shipman New College.
FOURIER TRANSFORM MICROWAVE SPECTROSCOPY OF ALKALI METAL HYDROSULFIDES: DETECTION OF KSH P. M. SHERIDAN, M. K. L. BINNS, J. P. YOUNG Department of Chemistry.
The Low Frequency Broadband Fourier Transform Microwave Spectroscopy of Hexafluoropropylene Oxide, CF 3 CFOCF 2 Lu Kang 1, Steven T. Shipman 2, Justin.
Microwave Spectra and Structures of H 2 S-CuCl and H 2 O-CuCl Nicholas R. Walker, Felicity J. Roberts, Susanna L. Stephens, David Wheatley, Anthony C.
THE PURE ROTATIONAL SPECTRA OF THE TWO LOWEST ENERGY CONFORMERS OF n-BUTYL ETHYL ETHER. B. E. Long, G. S. Grubbs II, and S. A. Cooke RH13.
A New E-Band (60 – 90 GHz) Fourier Transform Millimeter-wave Spectrometer DeWayne T. Halfen and Lucy M. Ziurys Department of Chemistry Department of Astronomy.
1 Ab initio and Infrared Studies of Carbon Dioxide Containing Complex Zheng Su and Yunjie Xu Department of Chemistry, University of Alberta, Edmonton,
The pure Inversion-Tunneling Transition of Ammonia in Helium Droplets Rudi Lehnig and Wolfgang Jäger Department of Chemistry, University of Alberta, Edmonton,
The Pure Rotational Spectrum of Pivaloyl Chloride, (CH 3 ) 3 CCOCl, between 800 and MHz. Garry S. Grubbs II, Christopher T. Dewberry, Kerry C. Etchison,
Beam Action Spectroscopy via Inelastic Scattering BASIS Technique Bobby H. Layne and Liam M. Duffy Department of Chemistry & Biochemistry, the University.
Tue. Nov. 11, 2008Physics 208, Lecture 211 From last time… EM waves Inductors in circuits I? + -
65 th International Symposium on Molecular Spectroscopy June 21, 2010 Lindsay N. Zack Brent J. Harris Matthew P. Bucchino Ming Sun Lucy M Ziurys Department.
RF scheme of electron linear accelerator with energy MeV Levichev A.E. Budker Institute of Nuclear Physics SB RAS.
June 18, rd International Symposium On Molecular Spectroscopy Gas-Phase Rotational Spectrum Of HZnCN (Χ 1 Σ + ) by Fourier Transform Microwave Techniques.
June 20, rd International Symposium On Molecular Spectroscopy Microwave Spectrum And Structure Determination Of the CCP ( X 2 П Ω ) Radical Ming.
Numerical and experimental study of the mode tuning technique effects. Application to the cavity ring-down spectroscopy. J. Remy, G.M.W. Kroesen, W.W.
Microwave Spectroscopy Wave length ~ 1 cm to 100  m Wave number ~ 1 to 100 cm -1. Frequency ~ 3 x to 3 x Hz Energy ~ 10 to 1000 Joules/mole.
Pure Rotational Spectra of the Rare Isotopologues of TiO (X 3 Δ r ) Andrew P. Lincowski, DeWayne T. Halfen, and Lucy M. Ziurys Department of Chemistry.
Infrared--Microwave Double Resonance Spectroscopy of Ar-DF (v = 0,1,2) Justin L. Neill, Gordon G. Brown, and Brooks H. Pate University of Virginia Department.
Superfluid effects in para-H 2 clusters probed by CO 2 rotation-vibration transitions Hui Li, Robert J. LeRoy, Pierre-Nicolas Roy Department of Chemistry.
Rotational Spectroscopy of OCS in Superfluid Helium Nanodroplets Paul Raston, Rudolf Lehnig, and Wolfgang Jäger Department of Chemistry, University of.
Extending the principles of the Flygare: Towards a FT-THz spectrometer Rogier Braakman Chemistry & Chemical Engineering California Institute of Technology.
The Rotational Spectroscopy of SrS Kerry C. Etchison, Chris T. Dewberry and Stephen A. Cooke Department of Chemistry, University of North Texas P.O. Box.
Fast Sweeping Double Resonance Microwave - (sub)Millimeter Spectrometer Based on Chirped Pulse Technology Brian Hays 1, Susanna Widicus Weaver 1, Steve.
Chirped-Pulse Microwave Spectroscopy in the Undergraduate Chemistry Curriculum Sydney Gaster, Taylor Hall, Sean Arnold, Deondre Parks, Gordon Brown Department.
Digital Control System for Microwave Spectroscopy Data Collection Amanda Olmut Dr. Stephen Kukolich, Principle Investigator Dr. Adam Daly, Project Lead.
SEEING IS BELIEVING: An 11 GHz molecular beam rotational spectrum (7.5 – 18.5 GHz) with 100 kHz resolution in 15  s measurement time Brian C. Dian, Kevin.
THE PURE ROTATIONAL SPECTRUM OF PERFLUOROOCTANONITRILE, C 7 F 15 CN, STUDIED USING CAVITY- AND CHIRPED-PULSED FOURIER TRANSFORM MICROWAVE SPECTROSCOPIES.
Spectroscopy of (He) N -Molecule Clusters: Tracing the Onset of Superfluidity Yunjie Xu and Wolfgang Jäger Department of Chemistry, University of Alberta,
Nathan Seifert, Wolfgang Jäger University of Alberta
CRISTOBAL PEREZ, MARINA SEKUTOR, ANDREY A
Christopher T. Dewberry, Garry S
CAVITY AND CHIRPED PULSE ROTATIONAL SPECTRUM OF THE LASER ABLATION SYNTHESIZED, OPEN-SHELL MOLECULE TIN MONOCHLORIDE, SnCl G. S. GRUBBS II, DANIEL J. FROHMAN,
A Chirped Pulse Fourier Transform Microwave (CP-FTMW) Spectrometer with Laser Ablation Source to Search for Actinide-Containing Molecules and Noble Metal.
Spectral methods for measurement of longitudinal beam profile
Characterisation and Control of Cold Chiral Compounds
Carlos Cabezas and Yasuki Endo
MICROWAVE FREQUENCY TRANSITIONS REQUIRING LASER ABLATED URANIUM METAL DISCOVERED USING CHIRP-PULSE FOURIER TRANSFORM MICROWAVE SPECTROSCOPY B. E. Long.
Application of the moderate peak power (6 MW) X-band klystron’s cluster for the CLIC accelerating structures testing program. I. Syratchev.
CHIRPED PULSE AND CAVITY FOURIER TRANSFORM MICROWAVE (CP-FTMW AND FTMW) INVESTIGATIONS INTO 3-BROMO-1,1,1,2,2-PENTAFLUOROPROPANE; A MOLECULE OF ATMOSPHERIC.
Microwave Spectrometer
Fourier transform microwave spectra of n-butanol and isobutanol
Presentation transcript:

A FABRY-PERÓT CAVITY PULSED FOURIER TRANSFORM W-BAND SPECTROMETER WITH A PULSED NOZZLE SOURCE. GARRY S. GRUBBS II, CHRISTOPHER T. DEWBERRY AND STEPHEN A. COOKE, Department of Chemistry, The University of North Texas, P. O. Box , Denton, Texas, 76203, U.S.A.

J. Phys. Chem. 71, (1979), 2723 Rev. Sci. Instrum. 52, (1981), 33 FT-3mm

Cavity based FTMW spectroscopy: Most spectrometers 6 – 26 GHz. Several operate from ~2 GHz to ~40 GHz

Below 1 GHz: This is our measurement of the 36 cm galactic methanol line, J KaKc = 1 10 – 1 11, detected in Sagitarius II. 500 averaging cycles. FT-3mm

W-band (75 – 110 GHz) Ultimately we hope to look at the pure rotational spectra of simple heavy element-containing species. For diatomic molecules containing one very heavy element and one light element rotational constants can be large (~ 50 GHz). Numerous lanthanide- and actinide-containing molecules have ground states with high orbital angular momentum. Often low J rotational levels are missing. 232 Th 17 O FT-3mm

Prior work. FT-3mm

J. Chem. Phys, 115, (2001), 6007 “With this spectrometer, we were able to observe the J: 6 – 5 line of O 13 C 34 S in natural abundance by integration of 600 shots with a repetition rate of 5 Hz”. FT-3mm

Int. J. Infrared and Millimeter Waves 4, (1983), 733 FT-3mm

Kolbe and Leskovar spectrometer 1 Klystron source from 67 to 73 GHz, passed through a high efficiency doubler Fabry-Perót cavity. Spherical mirrors, 50 mm in diameter, 148 mm radius of curvature, 74 mm apart. Loaded Q ~ Static gas at low pressure. Absorption spectroscopy. FT-3mm

Rev. Sci. Instrum. 56, (1985), 97 Time domain experiments. Static gas technique. 30 MHz Modulated frequency doubler. FT-3mm

Int. J. Infrared and Millimeter Waves 7, (1986), 1329 Numerous circuit improvements. Static gas. Dismantled more than 15 years ago. FT-3mm

Our Fourier transform W-band spectrometer: 75 – 110 GHz 1.MW synthesizer 2.Power divider 3.SPST switch 4.SSB modulator 5.Active multiplier chain 6.LNA (W-band) 7.LNA (RF) 8.O-scope FT-3mm

Small T vacuum chamber Pumped using Varian V-250 turbo pump backed by Varian SD40 rotary vane pump. Pulsed nozzle located perpendicular to the axis of microwave propagation. FT-3mm

Active Multiplier Chain (Millitech) FT-3mm

W-band pin diode switches (Millitech) FT-3mm

Model No: Bandwidth/GHz NF/dB (Max) Gain/dB (Min) SLW Low Noise Amplifier (Spacek Labs) FT-3mm

Coupling of microwaves into the cavity: Will likely be an iterative process: 1.Simply try butting the end of the waveguide up against the mirror. Waveguide will terminate on to waveguide dimensioned circular holes passing through the mirror?? 2.Try wire antenna. (Tough because of waveguide size) 3.Use horn antenna. Very efficient coupling but significantly reduce the Q.

On going… Need most of the circuit components to be inside the vacuum chamber. Waiting for machining of cooling blocks and vacuum chamber. Potential problems concerning the coupling of electromagnetic radiation into the cavity. Temporary/short term fall back is a “Q=1 experiment” using opposing horn antenna (on order). FT-3mm

Graduate Students: Kerry Etchison Smitty Grubbs II Chris Dewberry Physics Machine Shop. Chris Steve Smitty Kerry FT-3mm

We gratefully acknowledge financial support from: FT-3mm