Robert W. Field

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Name: Field, Robert
Organization: Massachusetts Institute of Technology , USA
Department: Department of Chemistry
Title: Professor(PhD)

TOPICS

Co-reporter:Joshua H. Baraban;P. Bryan Changala;Georg Ch. Mellau;John F. Stanton;Anthony J. Merer
Science 2015 Vol 350(6266) pp:1338-1342
Publication Date(Web):11 Dec 2015
DOI:10.1126/science.aac9668

Shaking out details of transition states

Chemists liken reaction energetics to a landscape with hills and valleys. In this context, the transition state represents the highest barrier that reagents must pass over en route to forming products. Baraban et al. introduce a framework for extracting details about the transition state of rearrangement reactions directly from vibrational spectral data. They identified a characteristic pattern in the spacing between vibrational energy levels near the transition state, which revealed its energy as well as the specific motions involved in surmounting the barrier.

Science, this issue p. 1338

Co-reporter:Kirill Prozument, G. Barratt Park, Rachel G. Shaver, AnGayle K. Vasiliou, James M. Oldham, Donald E. David, John S. Muenter, John F. Stanton, Arthur G. Suits, G. Barney Ellison and Robert W. Field  
Physical Chemistry Chemical Physics 2014 vol. 16(Issue 30) pp:15739-15751
Publication Date(Web):31 Mar 2014
DOI:10.1039/C3CP55352C
A Chirped-Pulse millimeter-Wave (CPmmW) spectrometer is applied to the study of chemical reaction products that result from pyrolysis in a Chen nozzle heated to 1000–1800 K. Millimeter-wave rotational spectroscopy unambiguously determines, for each polar reaction product, the species, the conformers, relative concentrations, conversion percentage from precursor to each product, and, in some cases, vibrational state population distributions. A chirped-pulse spectrometer can, within the frequency range of a single chirp, sample spectral regions of up to ∼10 GHz and simultaneously detect many reaction products. Here we introduce a modification to the CPmmW technique in which multiple chirps of different spectral content are applied to a molecular beam pulse that contains the pyrolysis reaction products. This technique allows for controlled allocation of its sensitivity to specific molecular transitions and effectively doubles the bandwidth of the spectrometer. As an example, the pyrolysis reaction of ethyl nitrite, CH3CH2ONO, is studied, and CH3CHO, H2CO, and HNO products are simultaneously observed and quantified, exploiting the multi-chirp CPmmW technique. Rotational and vibrational temperatures of some product molecules are determined. Subsequent to supersonic expansion from the heated nozzle, acetaldehyde molecules display a rotational temperature of 4 ± 1 K. Vibrational temperatures are found to be controlled by the collisional cooling in the expansion, and to be both species- and vibrational mode-dependent. Rotational transitions of vibrationally excited formaldehyde in levels ν4, 2ν4, 3ν4, ν2, ν3, and ν6 are observed and effective vibrational temperatures for modes 2, 3, 4, and 6 are determined and discussed.
Co-reporter:Hyunwoo Lee, Joshua H. Baraban, Robert W. Field, and John F. Stanton
The Journal of Physical Chemistry A 2013 Volume 117(Issue 46) pp:11679-11683
Publication Date(Web):April 26, 2013
DOI:10.1021/jp400035a
Highly accurate calculations are reported for properties of vinylidene (H2C═C:), specifically the position of its zero-point vibrational level relative to that of acetylene and its equilibrium structure and ground state rotational constants. The isomerization energy of vinylidene calculated at the HEAT-456QP level of theory is 43.53 ± 0.15 kcal mol–1, in agreement with the previous best estimate, but associated with a much smaller uncertainty. In addition, the thermochemical calculations presented here also allow a determination of the H2CC–H bond energy of the vinyl radical at the HEAT-345(Q) level of theory, which is 77.7 ± 0.3 kcal mol–1. The equilibrium structure of vinylidene, estimated with an additivity scheme that includes treatment of correlation effects beyond CCSD(T) as well as relativistic and adiabatic (diagonal Born–Oppenheimer correction) contributions, is rCC = 1.2982 ± 0.0003 Å, rCH = 1.0844 ± 0.0003 Å, and θCCH = 120.05 ± 0.05°, with zero-point rotational constants (including vibrational contributions and electronic contributions to the moment of inertia) estimated to be A0 = 9.4925 ± 0.0150 cm–1, B0 = 1.3217 ± 0.0017 cm–1, and C0 = 1.1602 ± 0.0016 cm–1.
Co-reporter:Kyle L. Bittinger, Wilton L. Virgo, and Robert W. Field
The Journal of Physical Chemistry A 2011 Volume 115(Issue 43) pp:11921-11943
Publication Date(Web):September 13, 2011
DOI:10.1021/jp2037894
We review recent research on the acetylene S1 state that illustrates how mechanistic rather than phenomenological information about intersystem crossing (ISC) may be obtained directly from frequency-domain spectra. The focus is on the dynamically rich “doorway-mediated” ISC domain that lies between isolated spectroscopic spin–orbit perturbations and statistical-limit interactions between one singlet “bright state” and a quasi-continuum of triplet “dark states”. New and improved experimental and data processing techniques permit the statistical-model curtain to be drawn back to reveal mechanistically explicit pathways via one or more identifiable, hence, manipulatable, doorway states, between a user-selected bright state and the undifferentiated bath of dark states.
Co-reporter:Adam H. Steeves, Hans A. Bechtel, Anthony J. Merer, Nami Yamakita, Soji Tsuchiya, Robert W. Field
Journal of Molecular Spectroscopy 2009 Volume 256(Issue 2) pp:256-278
Publication Date(Web):August 2009
DOI:10.1016/j.jms.2009.05.005
Rotational analyses are reported for a number of newly-discovered vibrational levels of the S1-trans (Ã1Au) state of C2H2. These levels are combinations where the Franck–Condon active ν2′ and ν3′ vibrational modes are excited together with the low-lying bending vibrations, ν4′ and ν6′. The structures of the bands are complicated by strong a- and b  -axis Coriolis coupling, as well as Darling–Dennison resonance for those bands that involve overtones of the bending vibrations. The most interesting result is the strong anharmonicity in the combinations of ν3′ (trans bend, ag  ) and ν6′ (in-plane cis bend, bu). This anharmonicity presumably represents the approach of the molecule to the trans–cis isomerization barrier, where ab initio   results have predicted the transition state to be half-linear, corresponding to simultaneous excitation of ν3′ and ν6′. The anharmonicity also causes difficulty in the least squares fitting of some of the polyads, because the simple model of Coriolis coupling and Darling–Dennison resonance starts to break down. The effective Darling–Dennison parameter, K4466, is found to increase rapidly with excitation of ν3′, while many small centrifugal distortion terms have had to be included in the least squares fits in order to reproduce the rotational structure correctly. Fermi resonances become important where the K-structures of different polyads overlap, as happens with the 2131B1 and 31B3 polyads (B = 4 or 6). The aim of this work is to establish the detailed vibrational level structure of the S1-trans state in order to search for possible S1-cis (1A2) levels. This work, along with results from other workers, identifies at least one K sub-level of every single vibrational level expected up to a vibrational energy of 3500 cm−1.
Co-reporter:HansA. Bechtel Dr.;AdamH. Steeves;BryanM. Wong Dr.;RobertW. Field
Angewandte Chemie 2008 Volume 120( Issue 16) pp:3011-3014
Publication Date(Web):
DOI:10.1002/ange.200705399
Co-reporter:HansA. Bechtel Dr.;AdamH. Steeves;BryanM. Wong Dr.;RobertW. Field
Angewandte Chemie International Edition 2008 Volume 47( Issue 16) pp:2969-2972
Publication Date(Web):
DOI:10.1002/anie.200705399
Co-reporter:Zicheng Duan, Robert W. Field, Nami Yamakita, Soji Tsuchiya
Chemical Physics 2006 Volume 324(2–3) pp:709-720
Publication Date(Web):31 May 2006
DOI:10.1016/j.chemphys.2005.12.017

Abstract

We describe a technique, differential temperature laser induced fluorescence (DT-LIF), and an analytical algorithm, structure-based cross correlation (SBCC), that are capable of separating overlapping cold and hot bands in a laser induced fluorescence (LIF) spectrum. DT-LIF/SBCC is illustrated by application to a pair of synthetic spectra, and is demonstrated by application to a segment of an experimental acetylene spectrum. The goal is to identify and separate hot and cold band spectral features numerically, prior to any attempt at assignment of the raw spectrum. The DT-LIF/SBCC combination is shown to be a useful tool for disentangling hot and cold band spectra.

Co-reporter:Kirill Prozument, G. Barratt Park, Rachel G. Shaver, AnGayle K. Vasiliou, James M. Oldham, Donald E. David, John S. Muenter, John F. Stanton, Arthur G. Suits, G. Barney Ellison and Robert W. Field
Physical Chemistry Chemical Physics 2014 - vol. 16(Issue 30) pp:NaN15751-15751
Publication Date(Web):2014/03/31
DOI:10.1039/C3CP55352C
A Chirped-Pulse millimeter-Wave (CPmmW) spectrometer is applied to the study of chemical reaction products that result from pyrolysis in a Chen nozzle heated to 1000–1800 K. Millimeter-wave rotational spectroscopy unambiguously determines, for each polar reaction product, the species, the conformers, relative concentrations, conversion percentage from precursor to each product, and, in some cases, vibrational state population distributions. A chirped-pulse spectrometer can, within the frequency range of a single chirp, sample spectral regions of up to ∼10 GHz and simultaneously detect many reaction products. Here we introduce a modification to the CPmmW technique in which multiple chirps of different spectral content are applied to a molecular beam pulse that contains the pyrolysis reaction products. This technique allows for controlled allocation of its sensitivity to specific molecular transitions and effectively doubles the bandwidth of the spectrometer. As an example, the pyrolysis reaction of ethyl nitrite, CH3CH2ONO, is studied, and CH3CHO, H2CO, and HNO products are simultaneously observed and quantified, exploiting the multi-chirp CPmmW technique. Rotational and vibrational temperatures of some product molecules are determined. Subsequent to supersonic expansion from the heated nozzle, acetaldehyde molecules display a rotational temperature of 4 ± 1 K. Vibrational temperatures are found to be controlled by the collisional cooling in the expansion, and to be both species- and vibrational mode-dependent. Rotational transitions of vibrationally excited formaldehyde in levels ν4, 2ν4, 3ν4, ν2, ν3, and ν6 are observed and effective vibrational temperatures for modes 2, 3, 4, and 6 are determined and discussed.
Phosphine,(tricyclo[3.3.1.13,7]dec-1-ylmethylidyne)-
4,7,13,16,21,24-Hexaoxa-1,10-diazabicyclo[8.8.8]hexacosane
Hydrogen isocyanide
Phosphorane,methylenetriphenyl-
9,10-dihydro-9,10-anthracenediylmagnesium*3THF
METHANEDIOL
ETHYNE
ethylenebis(triphenylphosphine)platinum(0)
Ethyne-d (9CI)
Ethenylidene