6 research outputs found
High-Resolution Electron Spectroscopy of Gas-Phase Metal−Aromatic Complexes
High-resolution electron spectroscopy combines pulsed field
ionization zero-electron kinetic energy (ZEKE) detection with in situ
laser-assisted synthesis and supersonic expansion. The technique offers
sub-meV spectral resolution for the electron spectra of metal complexes
and is a powerful tool to study their bonding and structures. This
Perspective presents recent progress in single-photon ZEKE spectroscopy
of metal−aromatic complexes and focuses on the determination
of the electron spin multiplicities, metal binding sites and modes,
rotational conformers, and conformational changes of these critical
species in organometallic chemistry
High-Resolution Electron Spectroscopy and Rotational Conformers of Group 6 Metal (Cr, Mo, and W) Bis(mesitylene) Sandwich Complexes
Group 6 metal–bisÂ(mesitylene)
sandwich complexes are produced by interactions between the laser-vaporized
metal atoms and mesitylene vapor in a pulsed molecular beam source,
identified by photoionization time-of-flight mass spectrometry, and
studied by pulsed-field ionization zero-electron kinetic energy spectroscopy
and density functional theory calculations. Although transition metal–bisÂ(arene)
sandwich complexes may adopt eclipsed and staggered conformations,
the group 6 metal–bisÂ(mesitylene) complexes are determined
to be in the eclipsed form. In this form, rotational conformers with
methyl group dihedral angles of 0 and 60° are identified for
the Cr complex, whereas the 0° rotamer is observed for the Mo
and W species. The 0° rotamer is in a <i>C</i><sub>2<i>v</i></sub> symmetry with the neutral ground state
of <sup>1</sup>A<sub>1</sub> and the singly positive charged ion state
of <sup>2</sup>A<sub>1</sub>. The 60° rotamer is in a <i>C</i><sub><i>i</i></sub> symmetry with the neutral
ground state of <sup>1</sup>A<sub>g</sub> and the ion state of <sup>2</sup>A<sub>g</sub>. Partial conversion of the 60 to 0° rotamer
is observed from He to He/Ar supersonic expansion for Cr–bisÂ(mesitylene).
The unsuccessful observation of the 60° rotamer for the Mo and
W complexes is the result of its complete conversion to the 0°
rotamer in both He and He/Ar expansions. The adiabatic ionization
energies of the 0° rotamers of the three complexes are in the
order of Cr–bisÂ(mesitylene) < W–bisÂ(mesitylene) <
Mo–bisÂ(mesitylene), which is different from that of the metal
atoms. These metal–bisÂ(mesitylene) complexes have lower ionization
energies than the corresponding metal–bisÂ(benzene) and −bisÂ(toluene)
species
Spectroscopic Characterization of Lanthanum-Mediated Dehydrogenation and C–C Bond Coupling of Ethylene
LaÂ(C<sub>2</sub>H<sub>2</sub>) and LaÂ(C<sub>4</sub>H<sub>6</sub>) are observed
from the reaction of laser-vaporized La atoms with
ethylene molecules by photoionization time-of-flight mass spectrometry
and characterized by mass-analyzed threshold ionization spectroscopy.
LaÂ(C<sub>2</sub>H<sub>2</sub>) is identified as a metallacyclopropene
and LaÂ(C<sub>4</sub>H<sub>6</sub>) as a metallacyclopentene. The three-membered
ring is formed by concerted H<sub>2</sub> elimination and the five-membered
cycle by dehydrogenation and C–C bond coupling. Both metallacycles
prefer a doublet ground state with a La 6s-based unpaired electron.
Ionization of the neutral doublet state of either complex produces
a singlet ion state by removing the La-based electron. The ionization
allows accurate measurements of the adiabatic ionization energy of
the neutral doublet state and metal–ligand and ligand-based
vibrational frequencies of the neutral and ionic states. Although
the La atom is in a formal oxidation state of +2, the ionization energies
of these metal–hydrocarbon cycles are lower than that of the
neutral La atom. Deuteration has a small effect on the ionization
energies of the two cyclic radicals but distinctive effects on their
vibrational frequencies
Lanthanum-Mediated C–H Bond Activation of Propyne and Identification of La(C<sub>3</sub>H<sub>2</sub>) Isomers
η<sup>2</sup>-Propadienylidenelanthanum
[LaÂ(η<sup>2</sup>-CCCH<sub>2</sub>)] and deprotioÂlanthanaÂcyclobutadiene
[LaÂ(HCCCH)] of LaÂ(C<sub>3</sub>H<sub>2</sub>) are identified from
the reaction mixture of neutral La atom activation of propyne in the
gas phase. The two isomers are characterized with mass-analyzed threshold
ionization spectroscopy combined with electronic structure calculations
and spectral simulations. LaÂ(η<sup>2</sup>-CCCH<sub>2</sub>)
and LaÂ(HCCCH) are formed by concerted 1,3- and 3,3-dehydrogenation,
respectively. Both isomers prefer a doublet ground state with a La
6s-based unpaired electron, and LaÂ(η<sup>2</sup>-CCCH<sub>2</sub>) is slightly more stable than LaÂ(HCCCH). Ionization of the neutral
doublet state of either isomer produces a singlet ion state by removing
the La-based electron. The geometry change upon ionization results
in the excitation of a symmetric metal–hydrocarbon stretching
mode in the ionic state, whereas thermal excitation leads to the observation
of the same stretching mode in the neutral state. Although the La
atom is in a formal oxidation state of +2, the ionization energies
of these metal–hydrocarbon radicals are lower than that of
the neutral La atom. Deuteration has a very small effect on the ionization
energies of the two isomers and the metal–hydrocarbon stretching
mode of LaÂ(η<sup>2</sup>-CCCH<sub>2</sub>), but it reduces considerably
the metal–ligand stretching frequencies of LaÂ(HCCCH)
Threshold Ionization and Spin–Orbit Coupling of Ceracyclopropene Formed by Ethylene Dehydrogenation
A Ce
atom reaction with ethylene was carried out in a laser-vaporization
metal cluster beam source. CeÂ(C<sub>2</sub>H<sub>2</sub>) formed by
hydrogen elimination from ethylene was investigated by mass-analyzed
threshold ionization (MATI) spectroscopy, isotopic substitutions,
and relativistic quantum chemical computations. The theoretical calculations
include a scalar relativistic correction, dynamic electron correlation,
and spin–orbit coupling. The MATI spectrum exhibits two nearly
identical band systems separated by 128 cm<sup>–1</sup>. The
separation is not affected by deuteration. The two-band systems are
attributed to spin–orbit splitting and the vibrational bands
to the symmetric metal–ligand stretching and in-plane carbon–hydrogen
bending excitations. The spin–orbit splitting arises from interactions
of a pair of nearly degenerate triplets and a pair of nearly degenerate
singlets. The organolanthanide complex is a metallacyclopropene in <i>C</i><sub>2<i>v</i></sub> symmetry. The low-energy
valence electron configurations of the neutral and ion species are
Ce 4f<sup>1</sup>6s<sup>1</sup> and Ce 4f<sup>1</sup>, respectively.
The remaining two electrons that are associated with the isolated
Ce atom or ion are spin paired in a molecular orbital that is a bonding
combination between a 5d Ce orbital and a π* antibonding orbital
of acetylene
Spectroscopic Characterization of Nonconcerted [4 + 2] Cycloaddition of 1,3-Butadiene with Lanthanacyclopropene To Form Lanthanum–Benzene in the Gas Phase
The reaction between La atoms and
1,3-butadiene is carried out
in a laser-vaporization molecular beam source. Metal–hydrocarbon
species with formulas LaÂ(C<sub><i>n</i></sub>H<sub><i>n</i></sub>) (<i>n</i> = 2, 4, and 6) and LaÂ(C<sub><i>m</i></sub>H<sub><i>m</i>+2</sub>) (<i>m</i> = 4 and 6) are observed with time-of-flight mass spectrometry
and characterized with mass-analyzed threshold ionization spectroscopy.
A lanthanum–benzene complex [LaÂ(C<sub>6</sub>H<sub>6</sub>)]
is formed by 1,3-butadiene addition to lanthanaÂcyclopropene
[LaÂ(C<sub>2</sub>H<sub>2</sub>)] followed by molecular hydrogen elimination.
LanthanaÂcyclopropene is an intermediate generated by the primary
reaction between La and 1,3-butadiene. Two other intermediates produced
by the La + 1,3-butadiene reaction are LaÂ[η<sup>4</sup>-(1-buten-3-yne)]
[LaÂ(C<sub>4</sub>H<sub>4</sub>)] and 1-lanthanaÂcyclopent-3-ene
[LaÂ(C<sub>4</sub>H<sub>6</sub>)]. The LaÂ(benzene) complex exhibits
distinctive metal–ligand bonding from that of the three intermediates
as shown by the adiabatic ionization energies and ground electron
configurations