Daniel M. Neumark

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Name: Neumark, Daniel M.
Organization: University of California , USA
Department: Department of Chemistry
Title: (PhD)

TOPICS

Co-reporter:Bethan Nichols;Erin. N. Sullivan;Mikhail Ryazanov
The Journal of Physical Chemistry A January 26, 2017 Volume 121(Issue 3) pp:579-586
Publication Date(Web):December 19, 2016
DOI:10.1021/acs.jpca.6b10570
The photodissociation dynamics of the i-methylvinoxy (CH3COCH2) radical have been studied by means of fast beam coincidence translational spectroscopy. The radical was produced by photodetachment of the i-methylvinoxide anion at 700 nm, followed by dissociation at 225 nm (5.51 eV), 248 nm (5.00 eV), and 308 nm (4.03 eV). At all three dissociation energies, the major products were found to be CH3 + CH2CO, with a small amount of CO + C2H5 produced at the higher dissociation energies. Photofragment mass distributions and translational energy distributions were recorded for each wavelength. Comparison of the mass distributions with dissociation of fully deuterated i-methylvinoxy aided the assignment of the observed channels. Electronic structure calculations were performed to determine the relative energies of minima and transition states involved in the dissociation and to aid interpretation of the experimental results. The proposed dissociation mechanism involves internal conversion from the initially excited electronic state, followed by dissociation over a barrier on the ground state.
Co-reporter:Isaac A. Ramphal;Mark Shapero;Courtney Haibach-Morris
Physical Chemistry Chemical Physics 2017 vol. 19(Issue 43) pp:29305-29314
Publication Date(Web):2017/11/08
DOI:10.1039/C7CP05490D
Photofragment translational spectroscopy was used to study the photodissociation of fulvenallene, C7H6, and the fulvenallenyl radical, C7H5, at 248 nm and 193 nm. Starting from fulvenallene, only the H-atom loss channel producing the fulvenallenyl radical, C7H5, was observed. Fulvenallene dissociation occurs on the ground state surface with no exit barrier, and there is good agreement between our experimentally determined photofragment translational energy distribution and a prior distribution for a statistical process. Subsequent absorption at both wavelengths by fulvenallenyl enabled investigation of the photodissociation of this radical. Two channels were observed: C5H3 + C2H2 and C4H2 + C3H3. The photofragment translational energy distributions for these channels are peaked away from 0 kcal mol−1, which is consistent with ground state dissociation over an exit barrier. At 248 nm, the C3H3-loss channel accounted for 85 ± 10% of fulvenallenyl dissociation, while at 193 nm it accounted for 80 ± 15%. The experimental branching between these channels is in reasonable agreement with Rice–Ramsperger–Kassel–Marcus theory calculations, which predict C3H3-loss to account for 70% and 63% of dissociation for 248 nm and 193 nm respectively.
Co-reporter:Isaac A. Ramphal;Mark Shapero;Courtney Haibach-Morris
Physical Chemistry Chemical Physics 2017 vol. 19(Issue 44) pp:30277-30277
Publication Date(Web):2017/11/15
DOI:10.1039/C7CP90250F
Correction for ‘Photodissociation dynamics of fulvenallene and the fulvenallenyl radical at 248 and 193 nm’ by Isaac A. Ramphal et al., Phys. Chem. Chem. Phys., 2017, DOI: 10.1039/c7cp05490d.
Co-reporter:Erika R. Warrick, Jens E. Bækhøj, Wei Cao, Ashley P. Fidler, Frank Jensen, Lars Bojer Madsen, Stephen R. Leone, Daniel M. Neumark
Chemical Physics Letters 2017 Volume 683(Volume 683) pp:
Publication Date(Web):1 September 2017
DOI:10.1016/j.cplett.2017.02.013
•Attosecond excitation of multiple state wavepacket in molecular nitrogen in the 12–15 eV region.•Femtosecond probe reveals vibrational quantum beats in valence state.•Multi-state calculations assess internuclear-distance dependent probe.•Anharmonicity value measured from observed quantum beats.Nuclear and electronic dynamics in a wavepacket comprising bound Rydberg and valence electronic states of nitrogen from 12 to 15 eV are investigated using attosecond transient absorption. Vibrational quantum beats with a fundamental period of 50 femtoseconds persist for a picosecond in the b′ 1Σ+u valence state. Multi-state calculations show that these coherences result primarily from near infrared-induced coupling between the inner and outer regions of the b′ 1Σ+u state potential and the dark a″ 1Σ+g state. The excellent spectral and temporal resolution of this technique allows measurement of the anharmonicity of the b′ 1Σ+u potential directly from the observed quantum beats.Download high-res image (185KB)Download full-size image
Co-reporter:Jessalyn A. DeVineMarissa L. Weichman, Xueyao ZhouJianyi Ma, Bin JiangHua Guo, Daniel M. Neumark
Journal of the American Chemical Society 2016 Volume 138(Issue 50) pp:16417-16425
Publication Date(Web):November 27, 2016
DOI:10.1021/jacs.6b10233
High-resolution slow photoelectron velocity-map imaging spectra of cryogenically cooled X̃2B2 H2CC– and D2CC– in the region of the vinylidene triplet excited states are reported. Three electronic bands are observed and, with the assistance of electronic structure calculations and quantum dynamics on ab initio-based near-equilibrium potential energy surfaces, are assigned as detachment to the 3B2 (T1), b̃ 3A2 (T2), and à 1A2 (S1) excited states of neutral vinylidene. This work provides the first experimental observation of the à singlet excited state of H2CC. While regular vibrational structure is observed for the ã and à electronic bands, a number of irregular features are resolved in the vicinity of the b̃ band vibrational origin. High-level ab initio calculations suggest that this anomalous structure arises from a conical intersection between the ã and b̃ triplet states near the b̃ state minimum, which strongly perturbs the vibrational levels in the two electronic states through nonadiabatic coupling. Using the adiabatic electron affinity of H2CC previously measured to be 0.490(6) eV by Ervin and co-workers [J. Chem. Phys. 1989, 91, 5974], term energies for the excited neutral states of H2CC are found to be T0(ã 3B2) = 2.064(6), T0(b̃ 3A2) = 2.738(6), and T0(à 1A2) = 2.991(6) eV.
Co-reporter:Torsten Wende, Nadja Heine, Tara I. Yacovitch, Knut R. Asmis, Daniel M. Neumark and Ling Jiang  
Physical Chemistry Chemical Physics 2016 vol. 18(Issue 1) pp:267-277
Publication Date(Web):18 Nov 2015
DOI:10.1039/C5CP05762K
We report infrared multiple photon dissociation spectra of cryogenically-cooled (NaSO4−)2(H2O)n dianions (n = 0–6, 8) in the spectral range of the sulfate stretching and bending modes (580–1750 cm−1). Characteristic absorption bands and structural trends are identified based on a comparison to harmonic spectra of minimum-energy structures. The bare quarternary complex (NaSO4−)2 exhibits a C2h structure containing two fourfold-coordinated sodium cations in-between the two chelating sulfate dianions. Its stepwise solvation is driven by an interplay of SO42−–H2O and Na+–H2O interactions. The first water binds in a tridentate intersulfate-bridging fashion. The second and third water molecules bind to the sulfate groups at either end of the complex, which is followed by the onset of water hydrogen-bond network formation. In contrast to the binary ion pair, NaSO4−, no clear evidence for the disruption of the quaternary ion complex upon microhydration is found up to n = 8, underlining its remarkable stability and suggesting that the formation of quaternary ion complexes plays a central role in the initial stages of prenucleation in aqueous Na2SO4 solutions.
Co-reporter:Neil C. Cole-Filipiak, Mark Shapero, Courtney Haibach-Morris, and Daniel M. Neumark
The Journal of Physical Chemistry A 2016 Volume 120(Issue 27) pp:4818-4826
Publication Date(Web):February 9, 2016
DOI:10.1021/acs.jpca.5b12284
The photodissociation dynamics of the methyl perthiyl (CH3SS) radical are investigated via molecular beam photofragment translational spectroscopy, using “soft” electron ionization to detect the radicals and their photofragments. With this new capability, we have shown that CH3SS can be generated from flash pyrolysis of dimethyl trisulfide. Utilizing this source of radicals and the advantages afforded by soft electron ionization, we have reinvestigated the photodissociation dynamics of CH3SS at 248 nm, finding CH3S + S to be the dominant dissociation channel with CH3 + SS as a minor process. These results differ from previous work reported in our laboratory in which we found CH3 + SS and CH2S + SH as the main dissociation channels. The difference in results is discussed in light of our new capabilities for characterization of radical production.
Co-reporter:Erika R. Warrick, Wei Cao, Daniel M. Neumark, and Stephen R. Leone
The Journal of Physical Chemistry A 2016 Volume 120(Issue 19) pp:3165-3174
Publication Date(Web):February 10, 2016
DOI:10.1021/acs.jpca.5b11570
An attosecond pulse is used to create a wavepacket in molecular nitrogen composed of multiple bound and autoionizing electronic states of Rydberg and valence character between 12 and 16.7 eV. A time-delayed, few-femtosecond, near-infrared (NIR) laser pulse is used to couple individual states in the wavepacket to multiple neighboring states, resulting in time-dependent modification of the absorption spectrum and revealing both individual quantum beats of the wavepacket and the energy shifts of the excited states in the presence of the strong NIR field. The broad bandwidth of the attosecond pulse and high energy resolution of the extreme ultraviolet spectrometer allow the simultaneous observation of time-dependent dynamics for many individual vibrational levels in each electronic state. Quantum beating with periods from 1.3 to 12 fs and transient line shape changes are observed among vibrational levels of a progression of electronically autoionizing Rydberg states leading to the excited A 2Πu N2+ ion core. Vibrational levels in the valence b 1Πu state exhibit 50 fs oscillation periods, revealing superpositions between individual vibrational levels within this state. Comparisons are made to previous studies of electronic wavepackets in atoms that highlight similarities to atomic behavior yet illustrate unique contributions of the diatomic molecular structure to the wavepacket, including the influence of different electronic potentials and vibrational-level-specific electronic dynamics.
Co-reporter:Jessalyn A. DeVine;Marissa L. Weichman;Daniel S. Levine;Jongjin B. Kim
PNAS 2016 Volume 113 (Issue 7 ) pp:1698-1705
Publication Date(Web):2016-02-16
DOI:10.1073/pnas.1520862113
Polycyclic aromatic hydrocarbons, in various charge and protonation states, are key compounds relevant to combustion chemistry and astrochemistry. Here, we probe the vibrational and electronic spectroscopy of gas-phase 9-, 1-, and 2-anthracenyl radicals (C14H9) by photodetachment of the corresponding cryogenically cooled anions via slow photoelectron velocity-map imaging (cryo-SEVI). The use of a newly designed velocity-map imaging lens in combination with ion cooling yields photoelectron spectra with <2 cm−1 resolution. Isomer selection of the anions is achieved using gas-phase synthesis techniques, resulting in observation and interpretation of detailed vibronic structure of the ground and lowest excited states for the three anthracenyl radical isomers. The ground-state bands yield electron affinities and vibrational frequencies for several Franck–Condon active modes of the 9-, 1-, and 2-anthracenyl radicals; term energies of the first excited states of these species are also measured. Spectra are interpreted through comparison with ab initio quantum chemistry calculations, Franck–Condon simulations, and calculations of threshold photodetachment cross sections and anisotropies. Experimental measures of the subtle differences in energetics and relative stabilities of these radical isomers are of interest from the perspective of fundamental physical organic chemistry and aid in understanding their behavior and reactivity in interstellar and combustion environments. Additionally, spectroscopic characterization of these species in the laboratory is essential for their potential identification in astrochemical data.
Co-reporter:Marissa L. Weichman; Jongjin B. Kim; Jessalyn A. DeVine; Daniel S. Levine
Journal of the American Chemical Society 2015 Volume 137(Issue 4) pp:1420-1423
Publication Date(Web):January 20, 2015
DOI:10.1021/ja5124896
Slow photoelectron velocity-map imaging (SEVI) spectroscopy has been used to study the vibronic structure of gas-phase α- and β-naphthyl radicals (C10H7). SEVI of cryogenically cooled anions yields spectra with <4 cm–1 resolution, allowing for the observation and interpretation of congested vibrational structure. Isomer-specific photoelectron spectra of detachment to the radical ground electronic states show detailed structure, allowing assignment of vibrational fundamental frequencies. Transitions to the first excited states of both radical isomers are also observed; vibronic coupling and photodetachment threshold effects are considered to explain the structure of the excited bands.
Co-reporter:Shou-Tian Sun, Ling Jiang, J.W. Liu, Nadja Heine, Tara I. Yacovitch, Torsten Wende, Knut R. Asmis, Daniel M. Neumark and Zhi-Feng Liu  
Physical Chemistry Chemical Physics 2015 vol. 17(Issue 39) pp:25714-25724
Publication Date(Web):05 Jun 2015
DOI:10.1039/C5CP02253C
We report infrared multiple photon dissociation (IRMPD) spectra of cryogenically-cooled H2PO4−(H2O)n anions (n = 2–12) in the spectral range of the stretching and bending modes of the solute anion (600–1800 cm−1). The spectra cannot be fully understood using the standard technique of comparison to harmonic spectra of minimum-energy structures; a satisfactory assignment requires considering anharmonic effects as well as entropy-driven hydrogen bond network fluctuations. Aided by finite temperature ab initio molecular dynamics simulations, the observed changes in the position, width and intensity of the IRMPD bands with cluster size are related to the sequence of microsolvation. Due to stronger hydrogen bonding to the two terminal PO groups, these are hydrated before the two P–OH groups. By n = 6, all four end groups are involved in the hydrogen bond network and by n = 12, the cluster spectra show similarities to the condensed phase spectrum of H2PO4−(aq). Our results reveal some of the microscopic details concerning the formation of the aqueous solvation environment around H2PO4−, provide ample testing grounds for the design of model solvation potentials for this biologically relevant anion, and support a new paradigm for the interpretation of IRMPD spectra of microhydrated ions.
Co-reporter:Mark Shapero, Neil C. Cole-Filipiak, Courtney Haibach-Morris, and Daniel M. Neumark
The Journal of Physical Chemistry A 2015 Volume 119(Issue 50) pp:12349-12356
Publication Date(Web):September 8, 2015
DOI:10.1021/acs.jpca.5b07125
The photodissociation of jet cooled benzyl radicals, C7H7, at 248 nm has been studied using photofragment translational spectroscopy. Two dissociation channels were observed, H + C7H6 and CH3 + C6H4. The translational energy distribution determined for each channel suggests that both dissociation mechanisms occur via internal conversion to the ground state followed by intramolecular vibrational redistribution and dissociation. The branching ratio between these two channels has been measured to be (CH3 + C6H4)/(H + C7H6) = 0.011 ± 0.004. The dominance of the H + C7H6 channel is corroborated by the branching ratio calculated using Rice–Ramsperger–Kassel–Marcus theory.
Co-reporter:Marissa L. Weichman, Jongjin B. Kim, and Daniel M. Neumark
The Journal of Physical Chemistry A 2015 Volume 119(Issue 23) pp:6140-6147
Publication Date(Web):March 6, 2015
DOI:10.1021/acs.jpca.5b00768
We report high-resolution photodetachment spectra of cryogenically cooled ortho-hydroxyphenoxide anions (o-HOC6H4O–) using slow photoelectron velocity-map imaging spectroscopy (cryo-SEVI). We observe transitions to the three lowest-lying electronic states of the ortho-hydroxyphenoxy radical, and resolve detailed vibrational features. Comparison to Franck–Condon simulations allows for clear assignment of vibronic structure. We find an electron affinity of 2.3292(4) eV for the neutral X̃2A″ ground state, improving upon the accuracy of previous experiments. We measure term energies of 1.4574(7) eV and 1.5922(48) eV for the Ã2A′ and B̃2A″ excited states respectively, representing their first resolution and clear assignment. Photodetachment threshold effects are considered to explain the structure of these bands.
Co-reporter:Marissa L. Weichman;Tobias F. Sjolander;David E. Manolopoulos;Millard H. Alexander;Jongjin B. Kim;Jacek Kłos
Science 2015 Volume 349(Issue 6247) pp:
Publication Date(Web):
DOI:10.1126/science.aac6939

Glimpsing resonances as F and H2 react

The reaction of fluorine atoms with hydrogen molecules has long provided a window into the subtle effects of quantum mechanics on chemical dynamics. Kim et al. now show that the system still has some secrets left to reveal. The authors applied photodetachment to FH2 anions and their deuterated analogs. This allowed them to intercept the reaction trajectory in the middle and thereby uncover unanticipated weakly bound resonances. Theoretical calculations explain these observations and predict additional similar features that have yet to be seen.

Science, this issue p. 510

Co-reporter:Jongjin B. Kim ; Marissa L. Weichman
Journal of the American Chemical Society 2014 Volume 136(Issue 19) pp:7159-7168
Publication Date(Web):May 5, 2014
DOI:10.1021/ja502713v
High-resolution anion photoelectron spectra are reported for the group 4 metal dioxide clusters Ti2O4– and Zr2O4–. Slow photoelectron velocity-map imaging (SEVI) spectroscopy of cryogenically cooled, mass-selected anions yields photoelectron spectra with submillielectronvolt resolution, revealing extensive and well-resolved vibrational progressions. By comparison of the spectra with Franck–Condon simulations, we have identified the C2v and C3v isomers as the ground states of Ti2O4– and Zr2O4– anions, respectively. Minor contributions from the C2h isomer of Ti2O4– and the C2v isomer of Zr2O4– are also seen. The SEVI spectra yield upper bounds for the adiabatic detachment energies, as well as vibrational frequencies for various modes of the neutral Ti2O4 and Zr2O4 species.
Co-reporter:Jongjin B. Kim, Marissa L. Weichman, and Daniel M. Neumark
Journal of Chemical Theory and Computation 2014 Volume 10(Issue 12) pp:5235-5237
Publication Date(Web):November 7, 2014
DOI:10.1021/ct5007949
Assignments of electronic bands in the high resolution photoelectron spectrum of the VO2¯ anion obtained via slow electron velocity-map imaging are discussed in light of a recent theoretical paper that questioned them and proposed an alternate assignment.
Co-reporter:Ling Jiang, Shou-Tian Sun, Nadja Heine, Jian-Wen Liu, Tara I. Yacovitch, Torsten Wende, Zhi-Feng Liu, Daniel M. Neumark and Knut R. Asmis  
Physical Chemistry Chemical Physics 2014 vol. 16(Issue 4) pp:1314-1318
Publication Date(Web):15 Nov 2013
DOI:10.1039/C3CP54250E
The vibrational spectroscopy of monohydrated dihydrogen phosphate anions, H2PO4−(H2O), is studied in the O–H stretching (2700–3900 cm−1) and the fingerprint regions (600–1800 cm−1). Assignment of the experimental infrared multiple photon photodissociation spectra based on the predicted harmonic spectra of energetically low-lying 0 K structures is not conclusive. Ab initio molecular dynamics simulations reveal that the water molecule undergoes large amplitude motion, even at low internal temperatures, and that the dipole time correlation function qualitatively captures the anharmonic effects of the low-barrier isomerization reaction on the infrared intensities.
Co-reporter:Nadja Heine, Tara I. Yacovitch, Franziska Schubert, Claudia Brieger, Daniel M. Neumark, and Knut R. Asmis
The Journal of Physical Chemistry A 2014 Volume 118(Issue 35) pp:7613-7622
Publication Date(Web):March 25, 2014
DOI:10.1021/jp412222q
Infrared multiple photon dissociation (IRMPD) spectra of NO3–(HNO3)m(H2O)n(H2)z with m = 1–3, up to n = 8 and z ≥ 1, are measured in the fingerprint region (550–1880 cm–1), directly probing the NO-stretching modes, as well as bending and other lower frequency modes. The assignment of the spectra is aided by electronic structure calculations. The IRMPD spectrum of the m = 1, n = 0 cluster is distinctly different from all the other measured spectra as a result of strong hydrogen bonding, leading to an equally shared proton in between two nitrate moieties (O2NO–···H+···ONO2–). It exhibits a strong absorption at 877 cm–1 and lacks the characteristic NO2-antisymmetric stretching/NOH-bending mode absorption close to 1650 cm–1. Addition of at least one more nitric acid molecule or two more water molecules weakens the hydrogen bond network, breaking the symmetry of this arrangement and leading to localization of the proton near one of the nitrate cores, effectively forming HNO3 hydrogen-bonded to NO3–. Not all IR active modes are observed in the IRMPD spectra of the bare nitrate–nitric acid clusters. Addition of a water or a hydrogen molecule lowers the dissociation limit of the complexes and relaxes (H2O) or lifts (H2) this IRMPD transparency.
Co-reporter:Martin Schultze;Krupa Ramasesha;C.D. Pemmaraju;S.A. Sato;D. Whitmore;A. Gandman;James S. Prell;L. J. Borja;D. Prendergast;K. Yabana;Stephen R. Leone
Science 2014 Volume 346(Issue 6215) pp:1348-1352
Publication Date(Web):12 Dec 2014
DOI:10.1126/science.1260311

Abstract

Electron transfer from valence to conduction band states in semiconductors is the basis of modern electronics. Here, attosecond extreme ultraviolet (XUV) spectroscopy is used to resolve this process in silicon in real time. Electrons injected into the conduction band by few-cycle laser pulses alter the silicon XUV absorption spectrum in sharp steps synchronized with the laser electric field oscillations. The observed ~450-attosecond step rise time provides an upper limit for the carrier-induced band-gap reduction and the electron-electron scattering time in the conduction band. This electronic response is separated from the subsequent band-gap modifications due to lattice motion, which occurs on a time scale of 60 ± 10 femtoseconds, characteristic of the fastest optical phonon. Quantum dynamical simulations interpret the carrier injection step as light-field–induced electron tunneling.

Co-reporter:Margaret A. Yandell ; Sarah B. King
Journal of the American Chemical Society 2013 Volume 135(Issue 6) pp:2128-2131
Publication Date(Web):January 25, 2013
DOI:10.1021/ja312414y
Time-resolved photoelectron imaging has been utilized to probe the energetics and dynamics of the transient negative ion of the nucleobase uracil. This species was created through charge transfer from an iodide anion within a binary iodide-uracil complex using a UV pump pulse; the ensuing dynamics were followed by photodetachment with a near-IR probe pulse. The photoelectron spectra show two time-dependent features, one from probe-induced photodetachment of the transient anion state and another from very low energy electron signal attributed to autodetachment. The transient anion was observed to decay biexponentially with time constants of hundreds of femtoseconds and tens of picoseconds, depending on the excitation energy. These dynamics are interpreted in terms of autodetachment from the initially excited state and a second, longer-lived species relaxed by iodine loss. Hydrogen loss from the N1 position may also occur in parallel.
Co-reporter:Alexander T. Shreve, Madeline H. Elkins and Daniel M. Neumark  
Chemical Science 2013 vol. 4(Issue 4) pp:1633-1639
Publication Date(Web):31 Jan 2013
DOI:10.1039/C3SC22063J
Photoelectron spectra of solvated electrons in methanol, ethanol, and acetonitrile microjets are reported. Solvated electrons are generated in and detached from microjets using two photons from single nanosecond laser pulses at wavelengths ranging 266 to 213 nm. We find vertical binding energies of 3.38 ± 0.11 eV in methanol and 3.38 ± 0.10 eV in ethanol. Two features are observed in acetonitrile at 2.61 ± 0.11 eV and 3.67 ± 0.15 eV, attributed to the solvated and dimer-bound binding geometries respectively. These results are compared to previous work on solvated cluster anions and alkali-doped solvent clusters.
Co-reporter:Jongjin B. Kim, Marissa L. Weichman and Daniel M. Neumark  
Physical Chemistry Chemical Physics 2013 vol. 15(Issue 48) pp:20973-20981
Publication Date(Web):11 Nov 2013
DOI:10.1039/C3CP54084G
High-resolution anion photoelectron spectra of the Group 4 metal dioxides TiO2−, ZrO2−, and HfO2− are reported, using slow electron velocity-map imaging (SEVI) combined with ion trapping and cryogenic cooling. The resulting spectra exhibit sub-meV resolution with no congestion from hot bands. Electron affinities are obtained with greater precision than in previous photodetachment experiments, with values of 1.5892(5) eV, 1.6397(5) eV, and 2.1045(5) eV, for TiO2, ZrO2, and HfO2, respectively. We obtain precise values for all of the vibrational frequencies of the neutral 1A1 ground states, except for the ν3 mode of HfO2. Weak activity observed in the forbidden ν3 mode for TiO2 and ZrO2 is attributed to Herzberg–Teller coupling to the Ã2B2 excited state.
Co-reporter:Aaron W. Harrison, Jeong Sik Lim, Mikhail Ryazanov, Gregory Wang, Shumin Gao, and Daniel M. Neumark
The Journal of Physical Chemistry A 2013 Volume 117(Issue 46) pp:11970-11978
Publication Date(Web):July 3, 2013
DOI:10.1021/jp403229h
The photodissociation dynamics of the thiophenoxy radical (C6H5S) have been investigated using fast beam coincidence translational spectroscopy. Thiophenoxy radicals were produced by photodetachment of the thiophenoxide anion followed by photodissociation at 248 nm (5.0 eV), 193 nm (6.4 eV), and 157 nm (7.9 eV). Experimental results indicate two major competing dissociation channels leading to SH + C6H4 (o-benzyne) and CS + C5H5 (cyclopentadienyl) with a minor contribution of S + C6H5 (phenyl). Photofragment mass distributions and translational energy distributions were measured at each dissociation wavelength. Transition states and minima for each reaction pathway were calculated using density functional theory to facilitate experimental interpretation. The proposed dissociation mechanism involves internal conversion from the initially prepared electronic excited state to the ground electronic state followed by statistical dissociation. Calculations show that SH loss involves a single isomerization step followed by simple bond fission. For both SH and S loss, C–S bond cleavage proceeds without an exit barrier. By contrast, the CS loss pathway entails multiple transition states and minima as it undergoes five membered ring formation and presents a small barrier with respect to products. The calculated reaction pathway is consistent with the experimental translational energy distributions in which the CS loss channel has a broader distribution peaking farther away from zero than the corresponding distributions for SH loss.
Co-reporter:Jongjin B. Kim, Christian Hock, Tara I. Yacovitch, and Daniel M. Neumark
The Journal of Physical Chemistry A 2013 Volume 117(Issue 34) pp:8126-8131
Publication Date(Web):March 5, 2013
DOI:10.1021/jp401083u
We report high-resolution anion photoelectron spectra of thiozonide (S3–) acquired by slow electron velocity-map imaging (SEVI). The ions were cryogenically cooled within an ion trap before photodetachment. We measure an electron affinity of 2.3630(9) eV, resolving discrepancies in previously reported photoelectron spectra that resulted from the presence of vibrational hot bands. The SEVI spectrum shows well-resolved, extended vibrational progressions in the symmetric stretch and bending modes of S3, yielding accurate frequencies for both.
Co-reporter:Tara I. Yacovitch, Nadja Heine, Claudia Brieger, Torsten Wende, Christian Hock, Daniel M. Neumark, and Knut R. Asmis
The Journal of Physical Chemistry A 2013 Volume 117(Issue 32) pp:7081-7090
Publication Date(Web):May 29, 2013
DOI:10.1021/jp400154v
The structure and stability of mass-selected bisulfate, sulfuric acid, and water cluster anions, HSO4–(H2SO4)m(H2O)n, are studied by infrared photodissociation spectroscopy aided by electronic structure calculations. The triply hydrogen-bound HSO4–(H2SO4) configuration appears as a recurring motif in the bare clusters, while incorporation of water disrupts this stable motif for clusters with m > 1. Infrared-active vibrations predominantly involving distortions of the hydrogen-bound network are notably missing from the infrared multiple-photon dissociation (IRMPD) spectra of these ions but are fully recovered by messenger-tagging the clusters with H2. A simple model is used to explain the observed “IRMPD transparency”.
Co-reporter:Holly L. Williams;Madeline H. Elkins;Alexander T. Shreve
Science 2013 Volume 342(Issue 6165) pp:1496-1499
Publication Date(Web):20 Dec 2013
DOI:10.1126/science.1246291

Relaxing in a Water Jet

High-energy irradiation of liquid water and its solutes can transiently liberate electrons, which act as potent chemical reductants, but they are challenging to characterize precisely. Seeking to bridge the gap between liquid and gas, Elkins et al. (p. 1496) report results from photoelectron spectroscopy of hydrated electron dynamics in a liquid jet. The results reveal a very rapid transition from the electronic excited state to the ground state, prior to full relaxation of the solvent shell.

Co-reporter:Ryan M. Young and Daniel M. Neumark
Chemical Reviews 2012 Volume 112(Issue 11) pp:5553
Publication Date(Web):June 28, 2012
DOI:10.1021/cr300042h
Co-reporter:Knut R. Asmis and Daniel M. Neumark
Accounts of Chemical Research 2012 Volume 45(Issue 1) pp:43
Publication Date(Web):June 15, 2011
DOI:10.1021/ar2000748
Conjugate-base anions are ubiquitous in aqueous solution. Understanding the hydration of these anions at the molecular level represents a long-standing goal in chemistry. A molecular-level perspective on ion hydration is also important for understanding the surface speciation and reactivity of aerosols, which are a central component of atmospheric and oceanic chemical cycles. In this Account, as a means of studying conjugate-base anions in water, we describe infrared multiple-photon dissociation spectroscopy on clusters in which the sulfate, nitrate, bicarbonate, and suberate anions are hydrated by a known number of water molecules.This spectral technique, used over the range of 550–1800 cm–1, serves as a structural probe of these clusters. The experiments follow how the solvent network around the conjugate-base anion evolves, one water molecule at a time. We make structural assignments by comparing the experimental infrared spectra to those obtained from electronic structure calculations. Our results show how changes in anion structure, symmetry, and charge state have a profound effect on the structure of the solvent network. Conversely, they indicate how hydration can markedly affect the structure of the anion core in a microhydrated cluster.Some key results include the following. The first few water molecules bind to the anion terminal oxo groups in a bridging fashion, forming two anion–water hydrogen bonds. Each oxo group can form up to three hydrogen bonds; one structural result, for example, is the highly symmetric, fully coordinated SO42–(H2O)6 cluster, which only contains bridging water molecules. Adding more water molecules results in the formation of a solvent network comprising water–water hydrogen bonding in addition to hydrogen bonding to the anion. For the nitrate, bicarbonate, and suberate anions, fewer bridging sites are available, namely, three, two, and one (per carboxylate group), respectively. As a result, an earlier onset of water–water hydrogen bonding is observed.When there are more than three hydrating water molecules (n > 3), the formation of a particularly stable four-membered water ring is observed for hydrated nitrate and bicarbonate clusters. This ring binds in either a side-on (bicarbonate) or top-on (nitrate) fashion. In the case of bicarbonate, additional water molecules then add to this water ring rather than directly to the anion, indicating a preference for surface hydration. In contrast, doubly charged sulfate dianions are internally hydrated and characterized by the closing of the first hydration shell at n = 12. The situation is different for the –O2C(CH2)6CO2– (suberate) dianion, which adapts to the hydration network by changing from a linear to a folded structure at n > 15. This change is driven by the formation of additional solute–solvent hydrogen bonds.
Co-reporter:Gabriel M. P. Just, Bogdan Negru, Dayoung Park and Daniel M. Neumark  
Physical Chemistry Chemical Physics 2012 vol. 14(Issue 2) pp:675-680
Publication Date(Web):28 Nov 2011
DOI:10.1039/C1CP22651G
The collisionless photodissociation dynamics of isobutene (i-C4H8) at 193 nm via photofragment translational spectroscopy are reported. Two major photodissociation channels were identified: H + C4H7 and CH3 + CH3CCH2. Translational energy distributions indicate that both channels result from statistical decay on the ground state surface. Although the CH3 loss channel lies 13 kcal mol−1 higher in energy, the CH3:H branching ratio was found to be 1.7 (5), in reasonable agreement with RRKM calculations.
Co-reporter:Margaret A. Yandell, Ryan M. Young, Sarah B. King, and Daniel M. Neumark
The Journal of Physical Chemistry A 2012 Volume 116(Issue 11) pp:2750-2757
Publication Date(Web):November 1, 2011
DOI:10.1021/jp208016w
The effect of excitation energy on the lifetimes of the charge-transfer-to-solvent (CTTS) states of small (4 ≤ n ≤ 10) iodide-doped water and alcohol clusters was explored using femtosecond time-resolved photoelectron imaging. Excitation of the CTTS state at wavelengths ranging from 272 to 238 nm leads to the formation of the I···(ROH)n– (R═H–, CH3–, and CH3CH2−) species, which can be thought of as a vibrationally excited bare solvent cluster anion perturbed by an iodine atom. Autodetachment lifetimes for alcohol-containing clusters range from 1 to 71 ps, while water clusters survive for hundreds of ps in this size range. Autodetachment lifetimes were observed to decrease significantly with increasing excitation energy for a particular number and type of solvent molecules. The application of Klots’ model for thermionic emission from clusters to I–(H2O)5 and I–(CH3OH)7 qualitatively reproduces experimental trends and reveals a high sensitivity to energy parametrization while remaining relatively insensitive to the number of vibrational modes. Experimental and computational results therefore suggest that the rate of electron emission is primarily determined by the energetics of the cluster system rather than by details of molecular structure.
Co-reporter:Bogdan Negru, Gabriel M. P. Just, Dayoung Park and Daniel M. Neumark  
Physical Chemistry Chemical Physics 2011 vol. 13(Issue 18) pp:8180-8185
Publication Date(Web):03 Feb 2011
DOI:10.1039/C0CP02461A
The photodissociation dynamics of the tert-butyl radical (t-C4H9) were investigated using photofragment translational spectroscopy. The tert-butyl radical was produced from flash pyrolysis of azo-tert-butane and dissociated at 248 nm. Two distinct channels of approximately equal importance were identified: dissociation to H + 2-methylpropene, and CH3 + dimethylcarbene. Neither the translational energy distributions that describe these two channels nor the product branching ratio are consistent with statistical dissociation on the ground state, and instead favor a mechanism taking place on excited state surfaces.
Co-reporter:Jongjin B. Kim, Tara I. Yacovitch, Christian Hock and Daniel M. Neumark  
Physical Chemistry Chemical Physics 2011 vol. 13(Issue 38) pp:17378-17383
Publication Date(Web):31 Aug 2011
DOI:10.1039/C1CP22211B
High resolution anion photodetachment spectra of the phenoxide and thiophenoxide anions were obtained with slow electron velocity-map imaging. The spectra show transitions to the 2B1 neutral states of both species and to the Ã2B2 state of the thiophenoxy radical. Comparison of the spectra with Franck-Condon simulations allows several gas-phase vibrations to be assigned. The adiabatic electron affinities are determined to be 2.2538(8) eV and 2.3542(6) eV for phenoxy and thiophenoxy, respectively. The term energy of the Ã2B2 state of thiophenoxy is found to be 0.3719(9) eV, higher than the values reported in photodissociation experiments of thiophenol.
Co-reporter:Aaron W. Harrison, Jeong Sik Lim, Paul E. Crider, Daniel M. Neumark
Chemical Physics Letters 2011 Volume 512(1–3) pp:30-34
Publication Date(Web):16 August 2011
DOI:10.1016/j.cplett.2011.07.001

Abstract

The three-body dissociation of (CO2) following excitation of the chromophore to the repulsive A2Πg,1/2 and electronic states at 1.72 and 3.21 eV has been investigated using fast beam photofragment translational spectroscopy. The translational energy distributions for three-body dissociation provide a direct measurement of the CO2 binding energy, yielding a value of 218 ± 10 meV. These distributions are vibrationally resolved and show that some CO2 is produced with bend excitation. Dalitz plots show that the dominant three-body decay mechanism is asynchronous–concerted decay, in which the two bond cleavages are distinct but nearly simultaneous events.

Co-reporter:Tara I. Yacovitch, Torsten Wende, Ling Jiang, Nadja Heine, Gerard Meijer, Daniel M. Neumark, and Knut R. Asmis
The Journal of Physical Chemistry Letters 2011 Volume 2(Issue 17) pp:2135-2140
Publication Date(Web):August 11, 2011
DOI:10.1021/jz200917f
Gas-phase infrared photodissociation spectra of the microhydrated bisulfate anions HSO4¯(H2O)n, with n = 1–16, are reported in the spectral range of 550–1800 cm–1. The spectra show extensive vibrational structure assigned to stretching and bending modes of the bisulfate core, as well as to water bending and librational modes. Comparison with electronic structure calculations suggests that the acidic proton of HSO4– is involved in the formation of a hydrogen bond from n ≥ 1 and that water–water hydrogen bonds form for n ≥ 2. The water network for the larger clusters forms hydrogen-bonded “bands” about the bisulfate core. The blue shifting of the SOH bending mode from 1193 (n = 1) to 1381 cm–1 (n = 12) accompanied by a dramatic decrease in its IR intensity suggests increased incorporation of the bisulfate hydrogen atom into the hydrogen-bonding network, the first step toward acid dissociation.Keywords: free electron laser; microsolvation; multiple photon dissociation; weak acid;
Co-reporter:Etienne Garand, Tara I. Yacovitch, Jia Zhou, Sean M. Sheehan and Daniel M. Neumark  
Chemical Science 2010 vol. 1(Issue 2) pp:192-201
Publication Date(Web):25 May 2010
DOI:10.1039/C0SC00164C
High-resolution photoelectron spectra of the CnH− anions with n = 5–9 are acquired with slow electron velocity-map imaging (SEVI). Spectral features are assigned with the help of electronic structure calculations and Franck–Condon simulations. Well-resolved transitions to the linear 2Π and ã4Σ− neutral states are observed for species with an odd number of carbon atoms. For C6H− and C8H−, transitions to the 2Π neutral ground state and the low lying Ã2Σ+ excited state are observed. Precise electron affinities, term energies, fine structure splittings, and gas-phase vibrational frequencies are determined. The C5H−, C7H− and C9H− SEVI spectra are consistent with the anions having 3Σ− linear triplet ground states.
Co-reporter:Luca Castiglioni, Sinisa Vukovic, Paul E. Crider, William A. Lester and Daniel M. Neumark  
Physical Chemistry Chemical Physics 2010 vol. 12(Issue 36) pp:10714-10722
Publication Date(Web):16 Aug 2010
DOI:10.1039/C0CP00380H
Motivated by recent experimental work, a theoretical study of the photodissociation of perdeuterated propargyl (D2CCD) and propynyl (D3CCC) radicals has been carried out, focusing on the C–C bond cleavage and D2 loss channels. High-level ab initio calculations were carried out, and RRKM rate constants were calculated for isomerization and dissociation pathways. The resulting reaction barriers, microcanonical rate constants and product branching ratios are consistent with the experimental findings, supporting the overall mechanism of internal conversion followed by statistical dissociation on the ground state surface. We found loose transition states and very low exit barriers for two of the C–C bond cleavage channels and an additional CD2 + CCD channel, which had not been reported previously. Our results probe the extent of propargyl and propynyl isomerization prior to dissociation at 248 and 193 nm and deliver a comprehensive picture of all ongoing molecular dynamics.
Co-reporter:Ryan M. Young, Graham B. Griffin, Aster Kammrath, Oli T. Ehrler, Daniel M. Neumark
Chemical Physics Letters 2010 Volume 485(1–3) pp:59-63
Publication Date(Web):18 January 2010
DOI:10.1016/j.cplett.2009.12.058

Abstract

Excited state dynamics of acetonitrile cluster anions, , were investigated using time-resolved photoelectron imaging (TRPEI) for 20 ⩽ n ⩽ 50. The clusters were excited and then photodetached with femtosecond pump and probe pulses at 790 and 395 nm, respectively. Excited state lifetimes varied between 200 and 270 fs over this size range, showing no obvious size trend. Experimental evidence indicates that we are exciting ‘isomer II’ clusters in which the excess electron is valence-bound to a solvated anionic dimer core. The absence of an obvious size-dependence in the excited state lifetimes is consistent with such a structure.

Co-reporter:Alexander T. Shreve, Terry A. Yen, Daniel M. Neumark
Chemical Physics Letters 2010 Volume 493(4–6) pp:216-219
Publication Date(Web):25 June 2010
DOI:10.1016/j.cplett.2010.05.059

Abstract

We report a systematic study of the photoelectron spectroscopy of hydrated electrons in liquid water jets using multiple precursors and photodetachment wavelengths. Hydrated electrons were generated in and detached from liquid microjets using two photons from a single nanosecond laser pulse at 266 or 213 nm. Solutions of 50 to 250 mM potassium hexacyanoferrate(II) or potassium iodide were used to provide precursor anions. All of our experimental conditions yield similar results, giving a mean vertical binding energy of 3.6 ± 0.1 eV at a temperature of ∼280 K, a slightly higher value than in recent reports.

Co-reporter:Terry A. Yen, Etienne Garand, Alexander T. Shreve and Daniel M. Neumark
The Journal of Physical Chemistry A 2010 Volume 114(Issue 9) pp:3215-3220
Publication Date(Web):December 10, 2009
DOI:10.1021/jp9093996
Anion photoelectron spectroscopy of C3N− and C5N− is performed using slow electron velocity-map imaging (SEVI) and field-free time-of-flight (TOF), respectively. The SEVI spectrum exhibits well-resolved vibrational transitions from the linear C3N− ground state to the corresponding C3N ground state. The TOF spectrum comprises transitions arising from the linear C5N− ground state to the corresponding neutral ground and excited states. This study yields the adiabatic electron affinities of C3N and C5N to be 4.305 ± 0.001 and 4.45 ± 0.03 eV, respectively, and a term value of 560 ± 120 cm−1 for the Ã2Π state of C5N. Vibrational frequencies for the degenerate cis and trans bending modes of C3N− are also extracted.
Co-reporter:Tara I. Yacovitch, Etienne Garand, and Daniel M. Neumark
The Journal of Physical Chemistry A 2010 Volume 114(Issue 42) pp:11091-11099
Publication Date(Web):May 5, 2010
DOI:10.1021/jp101930b
High-resolution photoelectron spectra of the i-methylvinoxide anion are obtained by slow electron velocity-map imaging. The transitions between the anion ground electronic state, X̃ 1A′, and the radical X̃ 2A′′, and à 2A′ states are measured. Franck−Condon simulations of the X̃ 2A′′ ← X̃ 1A′ transition are performed to aid in assigning peaks, yielding several vibrational frequencies for the first time. Additional structure in the spectrum of the X̃ 2A′′ ← X̃ 1A′ transition is attributed to hindered rotor motion of the methyl group. Simulation of methyl torsional states allows identification of the true origin peak, yielding the experimental adiabatic electron affinity, EA = 1.747 ± 0.002 eV, and the à state term energy, T0 = 1.037 ± 0.002 eV. Comparison with the fully deuterated isotopologue further supports the assignment of hindered rotor progressions. The favored methyl rotor position is eclipsed in the radical X̃ state and staggered in the anion X̃ and radical à states.
Co-reporter:Etienne Garand, Kerstin Klein, John F. Stanton, Jia Zhou, Tara I. Yacovitch and Daniel M. Neumark
The Journal of Physical Chemistry A 2010 Volume 114(Issue 3) pp:1374-1383
Publication Date(Web):September 8, 2009
DOI:10.1021/jp9067894
We report high-resolution photoelectron spectra of HCO2− and DCO2− obtained with slow photoelectron velocity-map imaging. Well-resolved photodetachment transitions to the 2A1 and 2B2 states of the neutral radicals were observed. In addition, vibronic levels of the HCO2 and DCO2 radicals with up to 2000 cm−1 of internal energy were calculated using a quasidiabatic Hamiltonian approach and high-level ab initio calculations. Spectral simulations using the calculated levels were found to be in excellent agreement with the experimental spectra and used to assign many of its features. This study unambiguously determined that the 2A1 state is the ground state of both HCO2 and DCO2, in contrast to earlier work that indicated the 2B2 state was the ground state for DCO2. For both isotopologs, the 2B2 state is a very low-lying excited state with term energies of T0 = 318 ± 8 cm−1 for HCO2 and T0 = 87 ± 8 cm−1 for DCO2. The adiabatic electron affinities are determined to be EA(HCO2) = 3.4961 ± 0.0010 eV and EA(DCO2) = 3.5164 ± 0.0010 eV.
Co-reporter:Etienne Garand ; Torsten Wende ; Daniel J. Goebbert ; Risshu Bergmann ; Gerard Meijer ; Daniel M. Neumark ;Knut R. Asmis
Journal of the American Chemical Society 2009 Volume 132(Issue 2) pp:849-856
Publication Date(Web):December 23, 2009
DOI:10.1021/ja9093132
Infrared multiple photon dissociation spectra are reported for HCO3−(H2O)1−10 clusters in the spectral range of 600−1800 cm−1. In addition, electronic structure calculations at the MP2/6-311+G(d,p) level have been performed on the n = 1−8 clusters to identify the structure of the low-lying isomers and to assign the observed spectral features. General trends in the stepwise solvation motifs of the bicarbonate anion can be deduced from the overall agreement between the calculated and experimental spectra. The most important of these is the strong preference of the water molecules to bind to the negatively charged CO2 moiety of the HCO3− anion. However, a maximum of four water molecules interact directly with this site. The binding motif in the most stable isomer of the n = 4 cluster, a four-membered ring with each water forming a single H-bond with the CO2 moiety, is retained in all of the lowest-energy isomers of the larger clusters. Starting at n = 6, additional solvent molecules are found to form a second hydration layer, resulting in a water−water network bound to the CO2 moiety of the bicarbonate anion. Binding of a water to the hydroxyl group of HCO3− is particularly disfavored and apparently does not occur in any of the clusters investigated here. Similarities and differences with the infrared spectrum of aqueous bicarbonate are discussed in light of these trends.
Co-reporter:Daniel J. Goebbert, Etienne Garand, Torsten Wende, Risshu Bergmann, Gerard Meijer, Knut R. Asmis and Daniel M. Neumark
The Journal of Physical Chemistry A 2009 Volume 113(Issue 26) pp:7584-7592
Publication Date(Web):May 15, 2009
DOI:10.1021/jp9017103
We present infrared photodissociation spectra of the microhydrated nitrate ions NO3−(H2O)1−6, measured from 600 to 1800 cm−1. The assignment of the spectra is aided by comparison with calculated B3LYP/aug-cc-pVDZ harmonic frequencies, as well as with higher-level calculations. The IR spectra are dominated by the antisymmetric stretching mode of NO3−, which is doubly degenerate in the bare ion but splits into its two components for most microhydrated ions studied here due to asymmetric solvation of the nitrate core. However, for NO3−(H2O)3, the spectrum reveals no lifting of this degeneracy, indicating an ion with a highly symmetric solvation shell. The first three water molecules bind in a bidentate fashion to the terminal oxygen atoms of the nitrate ion, keeping the planar symmetry. The onset of extensive water−water hydrogen bonding is observed starting with four water molecules and persists in the larger clusters.
Co-reporter:Etienne Garand, Alexei A. Buchachenko, Tara I. Yacovitch, Małgorzata M. Szczȩśniak, Grzegorz Chałasiński and Daniel M. Neumark
The Journal of Physical Chemistry A 2009 Volume 113(Issue 52) pp:14439-14446
Publication Date(Web):July 1, 2009
DOI:10.1021/jp903819m
The high-resolution photoelectron spectrum of KrO− was obtained using slow electron velocity-map imaging (SEVI). The SEVI spectrum reveals numerous vibronic transitions between multiple electronic states of KrO− and KrO, both of which are open-shell species. Detailed assignments are made by comparison with theoretical simulations based on high level ab initio calculations and an atoms-in-molecule model that accounts for spin−orbit coupling in the anion and neutral. Several KrO− and KrO vibrational frequencies and excited-state term energies are accurately determined from the analysis of the experimental spectra and are found to be in good agreement with the calculated values.
Co-reporter:Oli T. Ehrler, Graham B. Griffin, Ryan M. Young and Daniel M. Neumark
The Journal of Physical Chemistry B 2009 Volume 113(Issue 13) pp:4031-4037
Publication Date(Web):November 8, 2008
DOI:10.1021/jp806856m
We have used ultrafast time-resolved photoelectron imaging to measure charge transfer dynamics in iodide-doped acetonitrile clusters I−(CH3CN)n with n = 5−10. Strong modulations of vertical detachment energies were observed following charge transfer from the halide, allowing interpretation of the ongoing dynamics. We observe a sharp drop in the vertical detachment energy (VDE) within 300−400 fs, followed by a biexponential increase that is complete by ∼10 ps. Comparison to theory suggests that the iodide is internally solvated and that photodetachment results in formation of a diffuse electron cloud in a confined cavity. We interpret the initial drop in VDE as a combination of expansion of the cavity and localization of the excess electron on one or two solvent molecules. The subsequent increase in VDE is attributed to a combination of the I atom leaving the cavity and rearrangement of the acetonitrile molecules to solvate the electron. The n = 5−8 clusters then show a drop in VDE of around 50 meV on a much longer time scale. The long-time VDEs are consistent with those of (CH3CN)n− clusters with internally solvated electrons. Although the excited-state created by the pump pulse decays by emission of a slow electron, no such decay is seen by 200 ps.
Co-reporter:Etienne Garand, Alexei A. Buchachenko, Tara I. Yacovitch, Małgorzata M. Szcześniak, Grzegorz Chałasiński and Daniel M. Neumark
The Journal of Physical Chemistry A 2009 Volume 113(Issue 16) pp:4631-4638
Publication Date(Web):February 27, 2009
DOI:10.1021/jp8113682
The high-resolution photoelectron spectrum of ArO− was obtained using slow electron velocity-map imaging (SEVI). The SEVI spectrum reveals well-resolved vibrational transitions between multiple electronic states of ArO− and ArO, both of which are open-shell species. These transitions occur within the broad envelope of previous lower resolution photoelectron spectra. Detailed assignments are made by comparison with theoretical simulations based on high level ab initio calculations and an atoms-in-molecule model that accounts for spin−orbit coupling in the anion and neutral. The adiabatic electron affinity of ArO is found to be 12481 ± 2 cm−1. Several ArO− and ArO vibrational frequencies and excited-state term energies are accurately determined from the analysis of the experimental spectra and are found to be in excellent agreement with the calculated values.
Co-reporter:Etienne Garand, Daniel Goebbert, Gabriele Santambrogio, Ewald Janssens, Peter Lievens, Gerard Meijer, Daniel M. Neumark and Knut R. Asmis  
Physical Chemistry Chemical Physics 2008 vol. 10(Issue 11) pp:1502-1506
Publication Date(Web):30 Jan 2008
DOI:10.1039/B716627C
The first gas-phase infrared spectra of silicon monoxide cations (SiO)n+, n = 3–5, using multiple photon dissociation in the 550–1250 cm−1 frequency range, are reported. All clusters studied here fragment via loss of a neutral SiO unit. The experimental spectra are compared to simulated linear absorption spectra from calculated low energy isomers for each cluster. This analysis indicates that a “ring” isomer is the primary contributor to the (SiO)3+ spectrum, that the (SiO)4+ spectrum results from two close-lying bicyclic ring isomers, and that the (SiO)5+ spectrum is from a bicyclic ring with a central, fourfold-coordinated Si atom. Experiment and theory indicate that the energies and energetic orderings of (SiO)n+ isomers differ from those for neutral (SiO)n clusters.
Co-reporter:Chia C. Wang, Oleg Kornilov, Oliver Gessner, Jeong Hyun Kim, Darcy S. Peterka and Daniel M. Neumark
The Journal of Physical Chemistry A 2008 Volume 112(Issue 39) pp:9356-9365
Publication Date(Web):August 9, 2008
DOI:10.1021/jp802332f
Helium droplets doped with Xe and Kr atoms were photoionized by using VUV synchrotron radiation from the Advanced Light Source and the resulting photoelectron images were measured. A wide range of He droplet sizes, photon energies, and dopant pick-up conditions was investigated. Significant ionization of dopants was observed at 21.6 eV, the absorption maximum of 2p 1P1 electronic excited state of He droplets, indicating an indirect ionization mechanism via excitation transfer. The photoelectron images and spectra reveal multiple photoionization mechanisms and pathways for the photoelectrons to escape the droplet. Specifically, they show sets of sharp peaks assigned to two mechanisms for Penning ionization of the dopant by He* in which the photoelectrons leave the droplet with no detectable energy loss, a broad, intense feature representing electrons that undergo significant energy loss, and a small amount of ultraslow electrons that may result from electron trapping at the droplet surface. The droplet-size dependence of the broad, intense feature suggests the development of the conduction band edge in the largest droplets seen here (⟨N⟩ ≈ 250,000).
Co-reporter:Daniel M. Neumark
The Journal of Physical Chemistry A 2008 Volume 112(Issue 51) pp:13287-13301
Publication Date(Web):November 26, 2008
DOI:10.1021/jp807182q
Anion photoelectron spectroscopy (PES) has become one of the most versatile techniques in chemical physics. This article briefly reviews the history of anion PES and some of its applications. It describes efforts to improve the resolution of this technique, including anion zero electron kinetic energy (ZEKE) and the recently developed method of slow electron velocity-map imaging (SEVI). Applications of SEVI to studies of vibronic coupling in open-shell systems and the spectroscopy of prereactive van der Waals complexes are then discussed.
Co-reporter:Etienne Garand;David E. Manolopoulos;Millard H. Alexander;Jia Zhou
Science 2008 Volume 319(Issue 5859) pp:72-75
Publication Date(Web):04 Jan 2008
DOI:10.1126/science.1150602

Abstract

The degree of electronic and nuclear coupling in the Cl + H2 reaction has become a vexing problem in chemical dynamics. We report slow electron velocity-map imaging (SEVI) spectra of ClH2 and ClD2. These spectra probe the reactant valley of the neutral reaction potential energy surface, where nonadiabatic transitions responsible for reactivity of the Cl excited spin-orbit state with H2 would occur. The SEVI spectra reveal progressions in low-frequency Cl·H2 bending and stretching modes, and are compared to simulations with and without nonadiabatic couplings between the Cl spin-orbit states. Although nonadiabatic effects are small, their inclusion improves agreement with experiment. This comparison validates the theoretical treatment, especially of the nonadiabatic effects, in this critical region of the Cl + H2 reaction, and suggests strongly that these effects are minor.

Co-reporter:Bradley F. Parsons, Sean M. Sheehan, Terry A. Yen, Daniel M. Neumark, Nadine Wehres and Rainer Weinkauf  
Physical Chemistry Chemical Physics 2007 vol. 9(Issue 25) pp:3291-3297
Publication Date(Web):03 May 2007
DOI:10.1039/B703045B
We report the anion photoelectron spectra of deprotonated thymine and cytosine at 3.496 eV photodetachment energy using velocity-mapped imaging. The photoelectron spectra of both species exhibit bands resulting from detachment transitions between the anion ground state and the ground state of the neutral radical. Franck–Condon simulations identify the anion isomers that contribute to the observed photoelectron spectrum. For both thymine and cytosine, the photoelectron spectra are consistent with anions formed by removal of a proton from the N atom that normally attaches to the sugar in the nucleotide (N1). For deprotonated thymine, the photoelectron spectrum shows a band due to a ring breathing vibration excited during the photodetachment transition. The electron affinity for the dehydrogenated thymine radical is determined as 3.250 ± 0.015 eV. For deprotonated cytosine, the photoelectron spectrum lacks any resolved structure and the electron affinity of the dehydrogenated cytosine radical is determined to be 3.037 ± 0.015 eV. By combining the electron affinity with previously measured gas phase acidities of thymine and cytosine, we determine the bond dissociation energy for the N–H bond that is broken.
Co-reporter:Niels E. Sveum, Scott J. Goncher and Daniel M. Neumark  
Physical Chemistry Chemical Physics 2006 vol. 8(Issue 5) pp:592-598
Publication Date(Web):20 Dec 2005
DOI:10.1039/B513960K
Photoionization cross sections of the phenyl radical to form the phenyl cation were measured using tunable vacuum ultraviolet synchrotron radiation coupled with photofragment translational spectroscopy. The phenyl radical was produced via 193- or 248-nm dissociation of chlorobenzene. At 10.0 eV, the photoionization cross sections for the phenyl radical averaged over product channels were found to be 13.4 ± 2.0 and 13.2 ± 2.0 Mb, respectively, with very little effect seen from the range of internal excitation produced at the two photolysis wavelengths. Using the photoionization cross section values for each channel, photoionization efficiency curves for the phenyl radical were placed on an absolute scale from 7.8 to 10.8 eV.
Co-reporter:J. R. R. Verlet;A. E. Bragg;A. Kammrath;O. Cheshnovsky;D. M. Neumark
Science 2005 Vol 310(5755) pp:1769
Publication Date(Web):16 Dec 2005
DOI:10.1126/science.1119113

Abstract

The conclusion by Turi et al. (Reports, 5 August 2005, p. 914) that all experimental spectral and energetic data on water-cluster anions point toward surface-bound electrons is overstated. Comparison of experimental vertical detachment energies with their calculated values for (H2O) n clusters with surface-bound and internalized electrons supports previous arguments that both types of clusters exist.

Co-reporter:J. R. R. Verlet;A. E. Bragg;A. Kammrath;O. Cheshnovsky;D. M. Neumark
Science 2005 Vol 307(5706) pp:93-96
Publication Date(Web):07 Jan 2005
DOI:10.1126/science.1106719

Abstract

Anionic water clusters have long been studied to infer properties of the bulk hydrated electron. We used photoelectron imaging to characterize a class of (H2O)n and (D2O)n cluster anions (n ≤ 200 molecules) with vertical binding energies that are significantly lower than those previously recorded. The data are consistent with a structure in which the excess electron is bound to the surface of the cluster. This result implies that the excess electron in previously observed water-cluster anions, with higher vertical binding energies, was internally solvated. Thus, the properties of those clusters could be extrapolated to those of the bulk hydrated electron.

Co-reporter:Jessalyn A. DeVine, Marissa L. Weichman, Steven J. Lyle, Daniel M. Neumark
Journal of Molecular Spectroscopy (February 2017) Volume 332() pp:
Publication Date(Web):February 2017
DOI:10.1016/j.jms.2016.09.002
•Cryo-SEVI yields high-resolution isomer-specific spectra of α- and β-furanyl.•Vibrational frequencies are extracted by comparison to Franck-Condon simulations.•Isomeric differences in orbital hybridization are inferred from the PADs.Isomer-specific, high-resolution photoelectron spectra of α- and β-furanyl obtained via slow electron velocity-map imaging of cryogenically cooled anions are reported. The spectra yield electron affinities of 1.8546(4) and 1.6566(4) eV for the α- and β-furanyl neutral radicals, respectively. New vibronic structure is resolved and assigned based on density functional theory and Franck-Condon simulations, providing several vibrational frequencies for the ground electronic state of both neutral isomers. Subtle differences in orbital hybridization resulting from varying proximity of the deprotonated carbon to the heteroatom are inferred from photoelectron angular distributions, and the CβH bond dissociation energy is estimated from a combination of experimental and theoretical results to be 119.9(2) kcal mol−1.
Co-reporter:Graham B. Griffin, Aster Kammrath, Oli T. Ehrler, Ryan M. Young, Ori Cheshnovsky, Daniel M. Neumark
Chemical Physics (23 June 2008) Volume 350(Issues 1–3) pp:
Publication Date(Web):23 June 2008
DOI:10.1016/j.chemphys.2007.12.005
Electronic relaxation dynamics following interband excitation from the 6s to the 6p band in mass selected Hg13- clusters are measured through femtosecond time-resolved photoelectron imaging (TRPEI). This interband transition is pumped at 4.65 eV and probed at 1.55 eV. Auger decay of occurs on a timescale of 490 ± 100 fs, and a similar time constant is seen for the transient excited state population created by the pump pulse. These time constants are an order of magnitude faster than those seen in previous experiments in which the lone p-electron in Hg13- was excited within the p-band. The results presented here imply that substantial relaxation of either electrons in the p-band or the hole in the s-band takes place prior to Auger emission, with electron–electron scattering playing a key role in the fast observed dynamics.
Co-reporter:Alice Kunin, Wei-Li Li and Daniel M. Neumark
Physical Chemistry Chemical Physics 2016 - vol. 18(Issue 48) pp:NaN33232-33232
Publication Date(Web):2016/11/22
DOI:10.1039/C6CP06646A
Femtosecond time-resolved photoelectron spectroscopy is used to probe the decay channels of iodide–nitromethane (I−·CH3NO2) binary clusters photoexcited at 3.56 eV, near the vertical detachment energy (VDE) of the cluster. The production of I− is observed, and its photoelectron signal exhibits a mono-exponential rise time of 21 ± 1 ps. Previous work has shown that excitation near the VDE of the I−·CH3NO2 complex transfers an electron from iodide to form a dipole-bound state of CH3NO2− that rapidly converts to a valence bound (VB) anion. The long appearance time for the I− fragment suggests that the VB anion decays by back transfer of the excess electron to iodide, reforming the I−·CH3NO2 anion and resulting in evaporation of iodide. Comparison of the measured lifetime to that predicted by RRKM theory suggests that the dissociation rate is limited by intramolecular vibrational energy redistribution in the re-formed anion between the high frequency CH3NO2 vibrational modes and the much lower frequency intermolecular I−·CH3NO2 stretch and bends, the predominant modes involved in cluster dissociation to form I−. Evidence for a weak channel identified as HI + CH2NO2− is also observed.
Co-reporter:Alexander T. Shreve, Madeline H. Elkins and Daniel M. Neumark
Chemical Science (2010-Present) 2013 - vol. 4(Issue 4) pp:NaN1639-1639
Publication Date(Web):2013/01/31
DOI:10.1039/C3SC22063J
Photoelectron spectra of solvated electrons in methanol, ethanol, and acetonitrile microjets are reported. Solvated electrons are generated in and detached from microjets using two photons from single nanosecond laser pulses at wavelengths ranging 266 to 213 nm. We find vertical binding energies of 3.38 ± 0.11 eV in methanol and 3.38 ± 0.10 eV in ethanol. Two features are observed in acetonitrile at 2.61 ± 0.11 eV and 3.67 ± 0.15 eV, attributed to the solvated and dimer-bound binding geometries respectively. These results are compared to previous work on solvated cluster anions and alkali-doped solvent clusters.
Co-reporter:Etienne Garand, Tara I. Yacovitch, Jia Zhou, Sean M. Sheehan and Daniel M. Neumark
Chemical Science (2010-Present) 2010 - vol. 1(Issue 2) pp:NaN201-201
Publication Date(Web):2010/05/25
DOI:10.1039/C0SC00164C
High-resolution photoelectron spectra of the CnH− anions with n = 5–9 are acquired with slow electron velocity-map imaging (SEVI). Spectral features are assigned with the help of electronic structure calculations and Franck–Condon simulations. Well-resolved transitions to the linear 2Π and ã4Σ− neutral states are observed for species with an odd number of carbon atoms. For C6H− and C8H−, transitions to the 2Π neutral ground state and the low lying Ã2Σ+ excited state are observed. Precise electron affinities, term energies, fine structure splittings, and gas-phase vibrational frequencies are determined. The C5H−, C7H− and C9H− SEVI spectra are consistent with the anions having 3Σ− linear triplet ground states.
Co-reporter:Torsten Wende, Nadja Heine, Tara I. Yacovitch, Knut R. Asmis, Daniel M. Neumark and Ling Jiang
Physical Chemistry Chemical Physics 2016 - vol. 18(Issue 1) pp:NaN277-277
Publication Date(Web):2015/11/18
DOI:10.1039/C5CP05762K
We report infrared multiple photon dissociation spectra of cryogenically-cooled (NaSO4−)2(H2O)n dianions (n = 0–6, 8) in the spectral range of the sulfate stretching and bending modes (580–1750 cm−1). Characteristic absorption bands and structural trends are identified based on a comparison to harmonic spectra of minimum-energy structures. The bare quarternary complex (NaSO4−)2 exhibits a C2h structure containing two fourfold-coordinated sodium cations in-between the two chelating sulfate dianions. Its stepwise solvation is driven by an interplay of SO42−–H2O and Na+–H2O interactions. The first water binds in a tridentate intersulfate-bridging fashion. The second and third water molecules bind to the sulfate groups at either end of the complex, which is followed by the onset of water hydrogen-bond network formation. In contrast to the binary ion pair, NaSO4−, no clear evidence for the disruption of the quaternary ion complex upon microhydration is found up to n = 8, underlining its remarkable stability and suggesting that the formation of quaternary ion complexes plays a central role in the initial stages of prenucleation in aqueous Na2SO4 solutions.
Co-reporter:Ling Jiang, Shou-Tian Sun, Nadja Heine, Jian-Wen Liu, Tara I. Yacovitch, Torsten Wende, Zhi-Feng Liu, Daniel M. Neumark and Knut R. Asmis
Physical Chemistry Chemical Physics 2014 - vol. 16(Issue 4) pp:NaN1318-1318
Publication Date(Web):2013/11/15
DOI:10.1039/C3CP54250E
The vibrational spectroscopy of monohydrated dihydrogen phosphate anions, H2PO4−(H2O), is studied in the O–H stretching (2700–3900 cm−1) and the fingerprint regions (600–1800 cm−1). Assignment of the experimental infrared multiple photon photodissociation spectra based on the predicted harmonic spectra of energetically low-lying 0 K structures is not conclusive. Ab initio molecular dynamics simulations reveal that the water molecule undergoes large amplitude motion, even at low internal temperatures, and that the dipole time correlation function qualitatively captures the anharmonic effects of the low-barrier isomerization reaction on the infrared intensities.
Co-reporter:Shou-Tian Sun, Ling Jiang, J.W. Liu, Nadja Heine, Tara I. Yacovitch, Torsten Wende, Knut R. Asmis, Daniel M. Neumark and Zhi-Feng Liu
Physical Chemistry Chemical Physics 2015 - vol. 17(Issue 39) pp:NaN25724-25724
Publication Date(Web):2015/06/05
DOI:10.1039/C5CP02253C
We report infrared multiple photon dissociation (IRMPD) spectra of cryogenically-cooled H2PO4−(H2O)n anions (n = 2–12) in the spectral range of the stretching and bending modes of the solute anion (600–1800 cm−1). The spectra cannot be fully understood using the standard technique of comparison to harmonic spectra of minimum-energy structures; a satisfactory assignment requires considering anharmonic effects as well as entropy-driven hydrogen bond network fluctuations. Aided by finite temperature ab initio molecular dynamics simulations, the observed changes in the position, width and intensity of the IRMPD bands with cluster size are related to the sequence of microsolvation. Due to stronger hydrogen bonding to the two terminal PO groups, these are hydrated before the two P–OH groups. By n = 6, all four end groups are involved in the hydrogen bond network and by n = 12, the cluster spectra show similarities to the condensed phase spectrum of H2PO4−(aq). Our results reveal some of the microscopic details concerning the formation of the aqueous solvation environment around H2PO4−, provide ample testing grounds for the design of model solvation potentials for this biologically relevant anion, and support a new paradigm for the interpretation of IRMPD spectra of microhydrated ions.
Co-reporter:Jongjin B. Kim, Marissa L. Weichman and Daniel M. Neumark
Physical Chemistry Chemical Physics 2013 - vol. 15(Issue 48) pp:NaN20981-20981
Publication Date(Web):2013/11/11
DOI:10.1039/C3CP54084G
High-resolution anion photoelectron spectra of the Group 4 metal dioxides TiO2−, ZrO2−, and HfO2− are reported, using slow electron velocity-map imaging (SEVI) combined with ion trapping and cryogenic cooling. The resulting spectra exhibit sub-meV resolution with no congestion from hot bands. Electron affinities are obtained with greater precision than in previous photodetachment experiments, with values of 1.5892(5) eV, 1.6397(5) eV, and 2.1045(5) eV, for TiO2, ZrO2, and HfO2, respectively. We obtain precise values for all of the vibrational frequencies of the neutral 1A1 ground states, except for the ν3 mode of HfO2. Weak activity observed in the forbidden ν3 mode for TiO2 and ZrO2 is attributed to Herzberg–Teller coupling to the Ã2B2 excited state.
Co-reporter:Gabriel M. P. Just, Bogdan Negru, Dayoung Park and Daniel M. Neumark
Physical Chemistry Chemical Physics 2012 - vol. 14(Issue 2) pp:NaN680-680
Publication Date(Web):2011/11/28
DOI:10.1039/C1CP22651G
The collisionless photodissociation dynamics of isobutene (i-C4H8) at 193 nm via photofragment translational spectroscopy are reported. Two major photodissociation channels were identified: H + C4H7 and CH3 + CH3CCH2. Translational energy distributions indicate that both channels result from statistical decay on the ground state surface. Although the CH3 loss channel lies 13 kcal mol−1 higher in energy, the CH3:H branching ratio was found to be 1.7 (5), in reasonable agreement with RRKM calculations.
Co-reporter:Bogdan Negru, Gabriel M. P. Just, Dayoung Park and Daniel M. Neumark
Physical Chemistry Chemical Physics 2011 - vol. 13(Issue 18) pp:NaN8185-8185
Publication Date(Web):2011/02/03
DOI:10.1039/C0CP02461A
The photodissociation dynamics of the tert-butyl radical (t-C4H9) were investigated using photofragment translational spectroscopy. The tert-butyl radical was produced from flash pyrolysis of azo-tert-butane and dissociated at 248 nm. Two distinct channels of approximately equal importance were identified: dissociation to H + 2-methylpropene, and CH3 + dimethylcarbene. Neither the translational energy distributions that describe these two channels nor the product branching ratio are consistent with statistical dissociation on the ground state, and instead favor a mechanism taking place on excited state surfaces.
Co-reporter:Jongjin B. Kim, Tara I. Yacovitch, Christian Hock and Daniel M. Neumark
Physical Chemistry Chemical Physics 2011 - vol. 13(Issue 38) pp:NaN17383-17383
Publication Date(Web):2011/08/31
DOI:10.1039/C1CP22211B
High resolution anion photodetachment spectra of the phenoxide and thiophenoxide anions were obtained with slow electron velocity-map imaging. The spectra show transitions to the 2B1 neutral states of both species and to the Ã2B2 state of the thiophenoxy radical. Comparison of the spectra with Franck-Condon simulations allows several gas-phase vibrations to be assigned. The adiabatic electron affinities are determined to be 2.2538(8) eV and 2.3542(6) eV for phenoxy and thiophenoxy, respectively. The term energy of the Ã2B2 state of thiophenoxy is found to be 0.3719(9) eV, higher than the values reported in photodissociation experiments of thiophenol.
Co-reporter:Luca Castiglioni, Sinisa Vukovic, Paul E. Crider, William A. Lester and Daniel M. Neumark
Physical Chemistry Chemical Physics 2010 - vol. 12(Issue 36) pp:NaN10722-10722
Publication Date(Web):2010/08/16
DOI:10.1039/C0CP00380H
Motivated by recent experimental work, a theoretical study of the photodissociation of perdeuterated propargyl (D2CCD) and propynyl (D3CCC) radicals has been carried out, focusing on the C–C bond cleavage and D2 loss channels. High-level ab initio calculations were carried out, and RRKM rate constants were calculated for isomerization and dissociation pathways. The resulting reaction barriers, microcanonical rate constants and product branching ratios are consistent with the experimental findings, supporting the overall mechanism of internal conversion followed by statistical dissociation on the ground state surface. We found loose transition states and very low exit barriers for two of the C–C bond cleavage channels and an additional CD2 + CCD channel, which had not been reported previously. Our results probe the extent of propargyl and propynyl isomerization prior to dissociation at 248 and 193 nm and deliver a comprehensive picture of all ongoing molecular dynamics.
Co-reporter:Etienne Garand, Daniel Goebbert, Gabriele Santambrogio, Ewald Janssens, Peter Lievens, Gerard Meijer, Daniel M. Neumark and Knut R. Asmis
Physical Chemistry Chemical Physics 2008 - vol. 10(Issue 11) pp:NaN1506-1506
Publication Date(Web):2008/01/30
DOI:10.1039/B716627C
The first gas-phase infrared spectra of silicon monoxide cations (SiO)n+, n = 3–5, using multiple photon dissociation in the 550–1250 cm−1 frequency range, are reported. All clusters studied here fragment via loss of a neutral SiO unit. The experimental spectra are compared to simulated linear absorption spectra from calculated low energy isomers for each cluster. This analysis indicates that a “ring” isomer is the primary contributor to the (SiO)3+ spectrum, that the (SiO)4+ spectrum results from two close-lying bicyclic ring isomers, and that the (SiO)5+ spectrum is from a bicyclic ring with a central, fourfold-coordinated Si atom. Experiment and theory indicate that the energies and energetic orderings of (SiO)n+ isomers differ from those for neutral (SiO)n clusters.
Co-reporter:Bradley F. Parsons, Sean M. Sheehan, Terry A. Yen, Daniel M. Neumark, Nadine Wehres and Rainer Weinkauf
Physical Chemistry Chemical Physics 2007 - vol. 9(Issue 25) pp:NaN3297-3297
Publication Date(Web):2007/05/03
DOI:10.1039/B703045B
We report the anion photoelectron spectra of deprotonated thymine and cytosine at 3.496 eV photodetachment energy using velocity-mapped imaging. The photoelectron spectra of both species exhibit bands resulting from detachment transitions between the anion ground state and the ground state of the neutral radical. Franck–Condon simulations identify the anion isomers that contribute to the observed photoelectron spectrum. For both thymine and cytosine, the photoelectron spectra are consistent with anions formed by removal of a proton from the N atom that normally attaches to the sugar in the nucleotide (N1). For deprotonated thymine, the photoelectron spectrum shows a band due to a ring breathing vibration excited during the photodetachment transition. The electron affinity for the dehydrogenated thymine radical is determined as 3.250 ± 0.015 eV. For deprotonated cytosine, the photoelectron spectrum lacks any resolved structure and the electron affinity of the dehydrogenated cytosine radical is determined to be 3.037 ± 0.015 eV. By combining the electron affinity with previously measured gas phase acidities of thymine and cytosine, we determine the bond dissociation energy for the N–H bond that is broken.
2-Anthracenyl
Silane, 9-anthracenyltrimethyl-
9-Anthracenyl
1-Anthracenyl
Benzenepropanaminium,3-hydroxy-N,N,N-trimethyl-
Ethenylidene
Sulfate, hydrogen, hexahydrate
Sulfate, hydrogen, dihydrate
Trithio
Sulfate, hydrogen, compd. with nitric acid and sulfuric acid (1:1:1)