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Dive into the research topics where Ian A. Finneran is active.

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Featured researches published by Ian A. Finneran.


Science | 2016

Discovery of the interstellar chiral molecule propylene oxide (CH3CHCH2O)

Brett A. McGuire; P. Brandon Carroll; Ryan A. Loomis; Ian A. Finneran; Philip R. Jewell; Anthony J. Remijan; Geoffrey A. Blake

Chiral molecule discovered in space A chiral molecule is one that has two forms that are mirror images of each other: enantiomers. Biological systems overwhelmingly use one enantiomer over another, and some meteorites show an excess of one type. The two forms are almost identical chemically, so how this excess first arose is unknown. McGuire et al. used radio astronomy to detect the first known chiral molecule in space: propylene oxide. The work raises the prospect of measuring the enantiomer excess in various astronomical objects, including regions where planets are being formed, to discover how and why the excess first appeared. Science, this issue p. 1449 The first chiral molecule detected in space may offer clues to the origin of enantiomer excess. Life on Earth relies on chiral molecules—that is, species not superimposable on their mirror images. This manifests itself in the selection of a single molecular handedness, or homochirality, across the biosphere. We present the astronomical detection of a chiral molecule, propylene oxide (CH3CHCH2O), in absorption toward the Galactic center. Propylene oxide is detected in the gas phase in a cold, extended molecular shell around the embedded, massive protostellar clusters in the Sagittarius B2 star-forming region. This material is representative of the earliest stage of solar system evolution in which a chiral molecule has been found.


Journal of The Optical Society of America B-optical Physics | 2017

Gas-phase broadband spectroscopy using active sources: progress, status, and applications [Invited]

Kevin C. Cossel; Eleanor M. Waxman; Ian A. Finneran; Geoffrey A. Blake; J. Ye; Nathan R. Newbury

Broadband spectroscopy is an invaluable tool for measuring multiple gas-phase species simultaneously. In this work we review basic techniques, implementations, and current applications for broadband spectroscopy. We discuss components of broad-band spectroscopy including light sources, absorption cells, and detection methods and then discuss specific combinations of these components in commonly-used techniques. We finish this review by discussing potential future advances in techniques and applications of broad-band spectroscopy.


Proceedings of the National Academy of Sciences of the United States of America | 2016

Coherent two-dimensional terahertz-terahertz-Raman spectroscopy

Ian A. Finneran; Ralph Welsch; Marco A. Allodi; Thomas F. Miller; Geoffrey A. Blake

Significance The thermally populated motions of liquids, including hydrogen bonds, low-energy bending vibrations, conformational torsions, and hindered rotations, are resonant in the terahertz region of the spectrum. These motions regulate solvation, macromolecular structure, and vibrational energy flow in liquid-phase chemistry. By exciting terahertz motions nonlinearly with multiple pulses of terahertz light, we can measure their anharmonic coupling and distribution of chemical environments. We can also begin to control their quantum coherence and population, a critical step forward in the control of liquid-phase chemistry with light. We present 2D terahertz-terahertz-Raman (2D TTR) spectroscopy, the first technique, to our knowledge, to interrogate a liquid with multiple pulses of terahertz (THz) light. This hybrid approach isolates nonlinear signatures in isotropic media, and is sensitive to the coupling and anharmonicity of thermally activated THz modes that play a central role in liquid-phase chemistry. Specifically, by varying the timing between two intense THz pulses, we control the orientational alignment of molecules in a liquid, and nonlinearly excite vibrational coherences. A comparison of experimental and simulated 2D TTR spectra of bromoform (CHBr3), carbon tetrachloride (CCl4), and dibromodichloromethane (CBr2Cl2) shows previously unobserved off-diagonal anharmonic coupling between thermally populated vibrational modes.


Review of Scientific Instruments | 2013

A direct digital synthesis chirped pulse Fourier transform microwave spectrometer

Ian A. Finneran; Daniel B. Holland; P. Brandon Carroll; Geoffrey A. Blake

Chirped pulse Fourier transform microwave (CP-FTMW) spectrometers have become the instrument of choice for acquiring rotational spectra, due to their high sensitivity, fast acquisition rate, and large bandwidth. Here we present the design and capabilities of a recently constructed CP-FTMW spectrometer using direct digital synthesis (DDS) as a new method for chirped pulse generation, through both a suite of extensive microwave characterizations and deep averaging of the 10-14 GHz spectrum of jet-cooled acetone. The use of DDS is more suited for in situ applications of CP-FTMW spectroscopy, as it reduces the size, weight, and power consumption of the chirp generation segment of the spectrometer all by more than an order of magnitude, while matching the performance of traditional designs. The performance of the instrument was further improved by the use of a high speed digitizer with dedicated signal averaging electronics, which facilitates a data acquisition rate of 2.1 kHz.


Journal of Chemical Physics | 2015

Nonlinear terahertz coherent excitation of vibrational modes of liquids

Marco A. Allodi; Ian A. Finneran; Geoffrey A. Blake

We report the first coherent excitation of intramolecular vibrational modes via the nonlinear interaction of a TeraHertz (THz) light field with molecular liquids. A terahertz-terahertz-Raman pulse sequence prepares the coherences with a broadband, high-energy, (sub)picosecond terahertz pulse, that are then measured in a terahertz Kerr effect spectrometer via phase-sensitive, heterodyne detection with an optical pulse. The spectrometer reported here has broader terahertz frequency coverage, and an increased sensitivity relative to previously reported terahertz Kerr effect experiments. Vibrational coherences are observed in liquid diiodomethane at 3.66 THz (122 cm(-1)), and in carbon tetrachloride at 6.50 THz (217 cm(-1)), in exact agreement with literature values of those intramolecular modes. This work opens the door to 2D spectroscopies, nonlinear in terahertz field, that can study the dynamics of condensed-phase molecular systems, as well as coherent control at terahertz frequencies.


Review of Scientific Instruments | 2015

A decade-spanning high-resolution asynchronous optical sampling terahertz time-domain and frequency comb spectrometer

Jacob T. Good; Daniel B. Holland; Ian A. Finneran; P. Brandon Carroll; Matthew J. Kelley; Geoffrey A. Blake

We present the design and capabilities of a high-resolution, decade-spanning ASynchronous OPtical Sampling (ASOPS)-based TeraHertz Time-Domain Spectroscopy (THz-TDS) instrument. Our system employs dual mode-locked femtosecond Ti:Sapphire oscillators with repetition rates offset locked at 100 Hz via a Phase-Locked Loop (PLL) operating at the 60th harmonic of the ∼80 MHz oscillator repetition rates. The respective time delays of the individual laser pulses are scanned across a 12.5 ns window in a laboratory scan time of 10 ms, supporting a time delay resolution as fine as 15.6 fs. The repetition rate of the pump oscillator is synchronized to a Rb frequency standard via a PLL operating at the 12th harmonic of the oscillator repetition rate, achieving milliHertz (mHz) stability. We characterize the timing jitter of the system using an air-spaced etalon, an optical cross correlator, and the phase noise spectrum of the PLL. Spectroscopic applications of ASOPS-THz-TDS are demonstrated by measuring water vapor absorption lines from 0.55 to 3.35 THz and acetonitrile absorption lines from 0.13 to 1.39 THz in a short pathlength gas cell. With 70 min of data acquisition, a 50 dB signal-to-noise ratio is achieved. The achieved root-mean-square deviation is 14.6 MHz, with a mean deviation of 11.6 MHz, for the measured water line center frequencies as compared to the JPL molecular spectroscopy database. Further, with the same instrument and data acquisition hardware, we use the ability to control the repetition rate of the pump oscillator to enable THz frequency comb spectroscopy (THz-FCS). Here, a frequency comb with a tooth width of 5 MHz is generated and used to fully resolve the pure rotational spectrum of acetonitrile with Doppler-limited precision. The oscillator repetition rate stability achieved by our PLL lock circuits enables sub-MHz tooth width generation, if desired. This instrument provides unprecedented decade-spanning, tunable resolution, from 80 MHz down to sub-MHz, and heralds a new generation of gas-phase spectroscopic tools in the THz region.


Journal of Physical Chemistry Letters | 2017

2D THz-THz-Raman Photon-Echo Spectroscopy of Molecular Vibrations in Liquid Bromoform

Ian A. Finneran; Ralph Welsch; Marco A. Allodi; Thomas F. Miller; Geoffrey A. Blake

Fundamental properties of molecular liquids are governed by long-range interactions that most prominently manifest at terahertz (THz) frequencies. Here we report the detection of nonlinear THz photon-echo (rephasing) signals in liquid bromoform using THz-THz-Raman spectroscopy. Together, the many observed signatures span frequencies from 0.5 to 8.5 THz and result from couplings between thermally populated ladders of vibrational states. The strongest peaks in the spectrum are found to be multiquantum dipole and 1-quantum polarizability transitions and may arise from nonlinearities in the intramolecular dipole moment surface driven by intermolecular interactions.


71st International Symposium on Molecular Spectroscopy | 2016

Coherent nonlinear terahertz spectroscopy of halomethane liquids

Ian A. Finneran; Geoffrey A. Blake; Thomas F. Miller; Marco A. Allodi; Ralph Welsch

IAN A FINNERAN, RALPH WELSCH, Division of Chemistry and Chemical Engineering, California Institute of Technology, Pasadena, CA, USA; MARCO A. ALLODI, Department of Chemistry, The Institute for Biophysical Dynamics, and The James Franck Institute, The University of Chicago, Chicago, IL, USA; THOMAS F. MILLER III, GEOFFREY BLAKE, Division of Chemistry and Chemical Engineering, California Institute of Technology, Pasadena, CA, USA.


70th International Symposium on Molecular Spectroscopy | 2015

Ultrafast terahertz Kerr effect spectroscopy of aromatic liquids

Ian A. Finneran; Marco A. Allodi; Geoffrey A. Blake

Ultrafast Terahertz Kerr Effect (TKE) spectroscopy is a relatively new nonlinear THz technique that is sensitive to the orientational dynamics of anisotropic, condensed-phase samples. The sample is excited by a single high field strength ∼1 ps THz pulse, and the resulting transient birefringence is measured by a 40 fs 800 nm probe pulse. We have measured the TKE response of several arom. liqs. at room temp., including benzene, benzene-d6, hexafluorobenzene, pyridine, and toluene. The measured decay consts. range from 1-10 ps, and, along with previous optical Kerr effect results in the literature, give insights into intermol. interactions in these liqs.


69th International Symposium on Molecular Spectroscopy | 2014

THz Time-domain spectroscopy of complex interstellar ice analogs

S. Ioppolo; Geoffrey A. Blake; Brandon Carroll; Ian A. Finneran; Xander de Vries; Marco A. Allodi; Brett A. McGuire

SERGIO IOPPOLO, Geological and Planetary Sciences , California Institute of Techonolgy, Pasadena, CA, USA; BRETT A. McGUIRE, MARCO A. ALLODI, Division of Chemistry and Chemical Engineering, California Institute of Technology, Pasadena, CA, USA; XANDER DE VRIES, Theoretical Chemistry, University of Nijmegen, Nijmegen, Netherlands; IAN FINNERAN, BRANDON CARROLL, GEOFFREY BLAKE, Division of Chemistry and Chemical Engineering, California Institute of Technology, Pasadena, CA, USA.

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Geoffrey A. Blake

California Institute of Technology

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Marco A. Allodi

California Institute of Technology

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P. Brandon Carroll

California Institute of Technology

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Daniel B. Holland

California Institute of Technology

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Griffin J. Mead

California Institute of Technology

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Jacob T. Good

California Institute of Technology

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Ralph Welsch

California Institute of Technology

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Thomas F. Miller

California Institute of Technology

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