WH. Mini-symposium: Non-covalent Interactions
Wednesday, 2019-06-19, 01:45 PM
Noyes Laboratory 100
SESSION CHAIR: María Mar Quesada-Moreno (Deutsches Elektronen-Synchrotron (DESY), Hamburg, Germany)
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WH01 |
Contributed Talk |
15 min |
01:45 PM - 02:00 PM |
P3824: JET-COOLED HIGH RESOLUTION INFRARED LASER SPECTROSCOPY OF Kr-H2O IN THE REGION OF THE BENDING MODE OF H2O |
S BELKHODJA, PIERRE ASSELIN, YANN BERGER, CNRS, De la Molécule aux Nano-Objets: Réactivité, Interactions, Spectroscopies, MONARIS, Sorbonne Université , PARIS, France; |
IDEALS Archive (Abstract PDF / Presentation File) |
DOI: https://dx.doi.org/10.15278/isms.2019.WH01 |
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The high sensitivity of our experimental setup (SPIRALES) [1] which couples an external cavity quantum cascade laser tunable from 1620 to 1690 cm−1to a pulsed jet enabled the recording of a series of rovibrational transitions of Kr-H 2O van der Waals (vdW) complex. As for the Ar-H 2O complex [2], the barriers to internal rotation in the Kr-H 2O complex states are comparable to the H 2O rotational constants and so the H 2O subunit behaves like a nearly free internal rotor [3]. The quantum number K is used for describing the projection of J onto the vdW axis, with K = 0 for Σ, K = 1 for Π, etc. A previous jet-cooled microwave study [4] evidenced that the ground vibrational state involves 2 internal rotor states corresponding to different spin modifications, namely a para state Σ(0 00) and an ortho state Σ(1 01). The present work reports the observation of two new bands around 1634.5 cm−1and 1659.7 cm−1which can be interpreted according to a pseudo-atomic model. By analogy with Ar-H 2O bands observed in the same regions [2], the Kr-H 2O ones are tentatively assigned to para Π(1 11) ← Σ(0 00) and ortho Π(2 12) ← Σ(1 01) transitions, respectively, confirmed by the presence of Q branches. The ortho band displays strongly unequal spacings characteristic of a Coriolis coupling between Σ and Π states in vibrational excited states. c0pt
Figure
Moreover the high resolution achieved with the SPIRALES set-up allowed the observation of several isotopes of Kr. The analysis of these two bands and further investigations in the 1580-1620 cm−1region are undergoing.
References :
[1] P. Asselin , A. Potapov, A. C. Turner, V. Boudon, L. Bruel, M.-A. Gaveau, M. Mons. PCCP 19, 17224-17232 (2017).
[2] X. Liu , Y. Xu. J. Mol. Spectr. 301, 1-8 (2014).
[3] R.C. Cohen , K . L . Busarow , Y. T. Lee, R. J. Saykally. JCP, 92, 169-177 (1990).
[4] J. Van Wijngaarden, W. Jäger. Mol. Phys. 98, 19,1575-1588 (2000).
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WH02 |
Contributed Talk |
15 min |
02:03 PM - 02:18 PM |
P3838: THE WATER–CARBON MONOXIDE DIMER: NEW INFRARED SPECTRA, AB INITIO ENERGY LEVEL CALCULATIONS, AND A CURIOUS INTERMOLECULAR MODE |
A. J. BARCLAY, KOOROSH ESTEKI, Department of Physics and Astronomy, University of Calgary, Calgary, AB, Canada; BOB McKELLAR, Steacie Laboratory, National Research Council of Canada, Ottawa, ON, Canada; NASSER MOAZZEN-AHMADI, Physics and Astronomy/Institute for Quantum Science and Technology, University of Calgary, Calgary, AB, Canada; |
IDEALS Archive (Abstract PDF / Presentation File) |
DOI: https://dx.doi.org/10.15278/isms.2019.WH02 |
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Weakly-bound H 2O-CO has a planar structure with approximately co-linear heavy atoms (O, C, O) and a hydrogen bond between the water and the carbon of the CO. Proton tunneling (H atom interchange) gives rise to two states corresponding to distinct nuclear spin modifications. The magnitude of the splitting in the ground rotational state is about 0.8 cm−1for H 2O-CO and 0.04 cm−1for D 2O-CO. Due to the almost linear heavy atom configuration, H 2O-CO has a large A rotational constant, equal to about 19 cm−1(12 cm−1for D 2O-CO), so the K quantum number is highly significant. Water-CO was first studied in the microwave and millimeter regions. Infrared spectra have been observed in the regions of the C-O stretch, the O-H stretch, the D 2O bend, and the H 2O bend.
Here we study the O-D stretch region (3.6 μm) for the first time, observing D 2O-CO, HOD-CO, and DOH-CO. We also extend the C-O stretch region results to include the K = 1 ← 0 subbands, thus determining A rotational constants for the v(CO) = 1 excited state. But more significantly, we also observe additional K = 1 ← 0 combination bands in both regions which involve the lowest intermolecular vibration of water-CO. This mode, which lies at 43 – 49 cm−1depending on isotopologue, can be identified as the in-plane CO bend. It is observed for H 2O-CO, D 2O-CO, and HOD-CO, and exhibits anomalous isotope shifts: even though their A-values are quite different, the D 2O-CO mode is only slightly lower in energy than that of H 2O-CO. Detailed rotational energy level calculations, based on a recent high-level ab initio potential energy surface Y. N. Kalugina, A. Faure, A. van der Avoird, K. Walker, and F. Lique, Phys. Chem. Chem. Phys. 20, 5469 (2018). are in good agreement with experiment, including the newly observed intermolecular mode. As well, the calculations show that the unobserved K = 0 level of this mode lies above the observed K = 1 level, thus explaining the anomalous isotope shifts.
Footnotes:
Y. N. Kalugina, A. Faure, A. van der Avoird, K. Walker, and F. Lique, Phys. Chem. Chem. Phys. 20, 5469 (2018).,
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WH03 |
Contributed Talk |
15 min |
02:21 PM - 02:36 PM |
P3695: INTERNAL ROTATION OF INTRAMOLECULAR HYDROGEN BONDING OF OH OR NH2 GROUPS ATTACHED TO THREE-MEMBERED RING MOLECULES |
ESTHER JULIANA OCOLA, JAAN LAANE, Department of Chemistry, Texas A \& M University, College Station, TX, USA; |
IDEALS Archive (Abstract PDF / Presentation File) |
DOI: https://dx.doi.org/10.15278/isms.2019.WH03 |
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The internal rotations about the single bonds connecting OH or NH2 groups to cyclopropyl or cyclopropene rings were investigated. The experimental fits to the infrared data of the one-dimensional torsional potential energy functions were compared to theoretical calculations. MP2/cc-pVTZ and CCSD/cc-pVTZ computations were found to be in good agreement with the experimental results for cyclopropanol and cyclopropylamine. Calculations were also carried out on the internal rotations of 1-cyclopropen-1-ol and 2-cyclopropen-1-amine. Each of these molecules has a calculated energy minimum corresponding to a conformation with an intramolecular π-type hydrogen bond. The π-bonding stabilization is 2.3 kcal/mol for the alcohol and 2.5 kcal/mol for the amine. The calculated O-H, N-H, and C=C stretching frequencies are lower for the hydrogen bonded conformers than for the conformations without the π-type hydrogen bonds. The C=C bond stretching frequencies show the largest decreases resulting from the hydrogen bonding.
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WH04 |
Contributed Talk |
15 min |
02:39 PM - 02:54 PM |
P3840: INFRARED BANDS OF CS2 DIMER AND TRIMER AT 4.5 μm |
A. J. BARCLAY, KOOROSH ESTEKI, Department of Physics and Astronomy, University of Calgary, Calgary, AB, Canada; K. H. MICHAELIAN, CanmetENERGY, Natural Resources Canada, Edmonton, Alberta, Canada; BOB McKELLAR, Steacie Laboratory, National Research Council of Canada, Ottawa, ON, Canada; NASSER MOAZZEN-AHMADI, Physics and Astronomy/Institute for Quantum Science and Technology, University of Calgary, Calgary, AB, Canada; |
IDEALS Archive (Abstract PDF / Presentation File) |
DOI: https://dx.doi.org/10.15278/isms.2019.WH04 |
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We report observation of new infrared bands of (CS2)2 and (CS2)3 in the region of the CS2 ν1 + ν3 combination band (at 4.5 μm) using a quantum cascade laser. The complexes are formed in a pulsed supersonic slit-jet expansion of a gas mixture of carbon disulfide in helium. We have previously shown that the most stable isomer of (CS2)2 is a cross-shaped structure with D2d symmetry and that for (CS2)3 is a barrel-shaped structure with D3 symmetry. The dimer has one doubly degenerate infrared-active band in the ν1 + ν3 region of the CS2 monomer. This band is observed to have a rather small vibrational shift of -0.846 cm−1. We expect one parallel and one perpendicular infrared-active band for the trimer but observe two parallel and one perpendicular bands. Much larger vibrational shifts of -8.953 cm−1for the perpendicular band and -8.845 cm−1and +16.681 cm−1for the parallel bands are observed. Vibrational shifts and possible vibrational assignments, in the case of the parallel bands of the trimer, are discussed using group theoretical arguments.
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WH05 |
Contributed Talk |
15 min |
02:57 PM - 03:12 PM |
P3912: IN SITU STUDIES OF ELECTROCHEMICAL REACTIONS USING VIBRATIONAL SUM FREQUENCY GENERATION |
SPENCER WALLENTINE, SAVINI SANDUNIKA BANDARANAYAKE, ROBERT BAKER, Department of Chemistry and Biochemistry, The Ohio State University, Columbus, OH, USA; |
IDEALS Archive (Abstract PDF / Presentation File) |
DOI: https://dx.doi.org/10.15278/isms.2019.WH05 |
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Electrochemical reactions play important roles in chemical energy conversion. However, the surface reactions that govern these processes are not well understood because of the difficulties associated with accessing the electrode/electrolyte interface and making chemically specific measurements with interface sensitivity. Vibrational spectroscopy offers the required chemical specificity and can be used to elucidate reaction pathways based on the formation of key functional groups along a reaction coordinate. However, the challenge is to implement infrared spectroscopy as a surface sensitive probe at the electrode/electrolyte interface. Vibrational sum frequency generation spectroscopy is an inherently interface specific technique, but most people who study electrode/electrolyte interfaces employ a thin film of electrolyte which leads to wavelength-dependent attenuation of the infrared field and also presents mass transport limitations when seeking to probe electrocatalytic reaction kinetics. We present a method to overcome these limitations with high signal quality and under conditions that are compatible with electrocatalysis at high current densities. Under these conditions we study CO2 reduction on polycrystalline gold thin films and gold nanoparticles which show faradaic efficiencies for carbon monoxide of 20% and 60% respectively. We identify possible reasons for the observed difference in selectivity.
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03:15 PM |
INTERMISSION |
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WH06 |
Contributed Talk |
15 min |
03:51 PM - 04:06 PM |
P3950: THE MOST STABLE ISOMER OF C4H2-(OCS)2 VAN DER WAALS COMPLEX: THEORY AND EXPERIMENT CONFIRM A STRUCTURE WITH C2 SYMMETRY |
A. J. BARCLAY, Department of Physics and Astronomy, University of Calgary, Calgary, AB, Canada; ANDREA PIETROPOLLI CHARMET, Dipartimento di Scienze Molecolari e Nanosistemi, Università Ca' Foscari, Venezia, Italy; BOB McKELLAR, Steacie Laboratory, National Research Council of Canada, Ottawa, ON, Canada; NASSER MOAZZEN-AHMADI, Physics and Astronomy/Institute for Quantum Science and Technology, University of Calgary, Calgary, AB, Canada; |
IDEALS Archive (Abstract PDF / Presentation File) |
DOI: https://dx.doi.org/10.15278/isms.2019.WH06 |
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We report the infrared spectrum of C4H2-(OCS)2 trimer in the region of the ν1 fundamental vibration of the OCS monomer. The van der Waals complexes are generated in a supersonic slit-jet apparatus and probed using a rapid-scan tunable diode laser. Both C4H2-(OCS)2 and C4D2-(OCS)2 are studied. Analysis of their spectra establishes that the trimer has C2 symmetry. Theoretical calculations performed to find stationary points on the potential energy surface confirm that the experimental structure is the most stable form of the trimer. The rotational parameters computed using double hybrid functionals are in very good agreement with those obtained from the observed spectra.
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WH07 |
Contributed Talk |
15 min |
04:09 PM - 04:24 PM |
P3631: LASER SPECTROSCOPY OF OCS-WATER COMPLEXES IN SUPERFLUID HELIUM NANODROPLETS |
ISAAC JAMES MILLER, TYLER WELLS, TY FAULKNER, PAUL RASTON, Chemistry and Biochemistry , James Madison University, Harrisonburg, VA, USA; |
IDEALS Archive (Abstract PDF / Presentation File) |
DOI: https://dx.doi.org/10.15278/isms.2019.WH07 |
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Superfluid helium nanodroplets are particularly useful for synthesizing molecular complexes, and several investigations have focused on investigating the hydration of atmospherically important molecules, such as the hydroxyl radical [1]. While carbonyl sulphide is the most abundant sulphur containing molecule in the atmosphere, little is known experimentally about how it interacts with water. In this study we focus on isolating OCS-(H 2O) N complexes in helium nanodroplets, and on uncovering their infrared signatures with quantum cascade laser spectroscopy. For the dimer, we identified two isomers, which is consistent with what was observed in solid neon [2]. One of the isomers has C s symmetry with the water near the oxygen end of OCS, and the other has C 2v symmetry, with the water at the sulphur end. The latter isomer displays well resolved rotational substructure in its C-O stretching band, and Stark spectroscopy has been performed, which should allow for determination of its dipole moment. Larger clusters seem to build off of the dimers, as evidenced by two sets of infrared bands that grow in with increasing water concentrations, near the corresponding OCS-H 2O bands.
[1] F. J. Hernandez et al. The Journal of Chemical Physics 143, 164304 (2015).
[2] P. Soulard et al. The Journal of Chemical Physics 146, 234303 (2017).
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WH08 |
Contributed Talk |
15 min |
04:27 PM - 04:42 PM |
P3681: CHARACTERIZATION OF A HYDROGEN PEROXIDE-BENZENE COMPLEX USING MATRIX ISOLATION INFRARED SPECTROSCOPY |
JAY C. AMICANGELO, DYLAN JOHNSON, CATHERINE KAISER, YUDHISHTARA PAYAGALA, JACOB OSLOSKY, LIA TOTLEBEN, School of Science (Chemistry), Penn State Erie, Erie, PA, USA; |
IDEALS Archive (Abstract PDF / Presentation File) |
DOI: https://dx.doi.org/10.15278/isms.2019.WH08 |
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Matrix isolation infrared spectroscopy was used to characterize a 1:1 complex of hydrogen peroxide (H2O2) with benzene (C6H6). Co-deposition experiments with H2O2 and C6H6 were performed at 20 K using argon as the matrix gas. New infrared peaks attributable to the H2O2-C6H6 complex were observed near the O-H stretching vibrations and the OH bending vibrations of the H2O2 monomer and near the hydrogen out-of-plane bending vibration of the C6H6 monomer. The initial identification of the newly observed infrared peaks to those of a H2O2-C6H6 complex was established by performing several concentration studies in which the sample-to-matrix ratios of the monomers were varied between 1:100 to 1:1600, by comparing the resulting co-deposition spectra with the spectra of the individual monomers, and by matrix annealing experiments (30 – 35 K). Co-deposition experiments using isotopically labeled hydrogen peroxide (D2O2 and HDO2) and benzene (C6D6) in argon were also performed and the analogous peaks for the isotopically labelled complexes were observed. A series of co-deposition experiments with H2O2 and C6H6 was also performed using nitrogen as the matrix gas. Quantum chemical calculations were performed for the H2O2-C6H6 complex at the MP2/aug-cc-pVDZ and M06-2X/aug-cc-pVDZ levels of theory in order to obtain optimized complex geometries and predicted vibrational frequencies of the complex, which were compared to the experimental infrared spectra.
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WH09 |
Contributed Talk |
15 min |
04:45 PM - 05:00 PM |
P3773: WEAKLY-BOUND COMPLEXES OF THIOPHENE AND WATER AS INVESTIGATED BY MATRIX ISOLATION FTIR AND COMPUTATION |
JOSHUA G WASSERMAN, KESHIHITO J MURPHY, JOSH NEWBY, Department of Chemistry , Hobart and William Smith Colleges, Geneva, NY, USA; |
IDEALS Archive (Abstract PDF / Presentation File) |
DOI: https://dx.doi.org/10.15278/isms.2019.WH09 |
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Weakly-bound complexes containing aromatic species have been the subject of study for many years. Here, a study of the weakly-bound complexes of thiophene () with water will be presented. In this study, matrix isolation FTIR and computational methods were used to examine stable 1:1 complexes of thiophene : water (Tp:). Multiple density functional theories along with MP2 calculations were used to find four stable geometries. Two geometries can be described by interaction, one by interaction, and one by interaction. These geometries were found to be within 10 kJ/mol of each other by all computational methods. Matrix isolation FTIR experiments identified several peaks that were not associated with isolated water or thiophene, implying the bands are due to weakly-bound complexes of the two. In addition to normal water, and HDO complexes with thiophene were also observed. Possible interpretations of the experimental and computational results will be presented. Comparisons to the structure of furan () : water Lockwood, S. P.; Fuller, T. G.; and Newby, J. J. J. Phys. Chem. A 2018, 122, 36, 7160-7170ill also be discussed.
Footnotes:
Lockwood, S. P.; Fuller, T. G.; and Newby, J. J. J. Phys. Chem. A 2018, 122, 36, 7160-7170w
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WH10 |
Contributed Talk |
15 min |
05:03 PM - 05:18 PM |
P3942: INFRARED PHOTODISSOCIATION SPECTROSCOPY OF PROTONATED AMMONIA CLUSTERS IN THE GAS PHASE |
JASON E. COLLEY, J. PHILIPP WAGNER, MICHAEL A DUNCAN, Department of Chemistry, University of Georgia, Athens, GA, USA; |
IDEALS Archive (Abstract PDF / Presentation File) |
DOI: https://dx.doi.org/10.15278/isms.2019.WH10 |
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The clustering of protonated ammonia clusters, a known interstellar ion, are studied with infrared photodissociation spectroscopy in the region of 4700 to 7200 cm−1. H+(NH3)n clusters up to n=8 are produced using a pulsed electrical discharge in a supersonic expansion. Mass-selected ions are investigated using tunable infrared laser photodissociation in the turning region of a reflectron time of flight mass spectrometer. Clusters of protonated ammonia are probed through the dissociative elimination of an ammonia. The spectra gathered were assigned by comparing to B2PLYP/def2-TZVP computations. Two bands are consistently observed for the studied protonated ammonia clusters. A band at around 5000 cm−1 is attributed to a combination of the N-H stretching and bending modes. Another band at around 6500 cm−1 is assigned to either an overtone or a combination of the N-H stretching modes.
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