8 research outputs found
Femtosecond Study of Dimolybdenum Paddlewheel Compounds with Amide/Thioamide Ligands: Symmetry, Electronic Structure, and Charge Distribution in the <sup>1</sup>MLCT S<sub>1</sub> State
Four
photophysically interesting dimolybdenum paddlewheel compounds are
synthesized and characterized: <b>I</b> and <b>II</b> contain
amide ligand (<i>N</i>,3-diphenyl-2-propynamide), and <b>III</b> and <b>IV</b> contain thioamide ligand (<i>N</i>,3-diphenyl-2-propynethioamide). <b>I</b> and <b>III</b> are <i>trans</i>-Mo<sub>2</sub>L<sub>2</sub>(O<sub>2</sub>C-T<sup><i>i</i></sup>PB)<sub>2</sub>-type
compounds, and <b>II</b> and <b>IV</b> are Mo<sub>2</sub>L<sub>4</sub>-type compounds, where O<sub>2</sub>C-T<sup><i>i</i></sup>PB is 2,4,6-triisopropylbenzoate. <b>I</b>–<b>IV</b> display strong light absorption due to metal to ligand
charge transfer (MLCT) transitions from molybdenum to the amide/thioamide
ligands. Charge transfer dynamics in the MLCT excited states of <b>I</b>–<b>IV</b> have been examined using femtosecond
transient absorption (fs-TA) spectroscopy and femtosecond time-resolved
infrared (fs-TRIR) spectroscopy. The asymmetric amide/thioamide ligands
show two forms of regioarrangements in the paddlewheel compounds.
Analyses of the νÂ(Cî—¼C) bands in the fs-TRIR spectra of <b>I</b> and <b>II</b> show similar electron density distribution
over ligands in their <sup>1</sup>MLCT S<sub>1</sub> states where
only two amide ligands are involved and the transferred electron is
mainly localized on one of them. The fs-TRIR spectra of <b>III</b> and <b>IV</b>, however, show different charge distribution
patterns where the transferred electron is fully delocalized over
two thioamide ligands in <b>III</b> and partially delocalized
in <b>IV</b>. Fast interligand electron transfer (ILET) was
recognized as the explanation for the various charge distribution
patterns, and ILET was shown to be influenced by both the ligands
and the ligand arrangements
Synthesis, Structure, and Photophysical Properties of Mo<sub>2</sub>(NN)<sub>4</sub> and Mo<sub>2</sub>(NN)<sub>2</sub>(T<sup><i>i</i></sup>PB)<sub>2</sub>, Where NN = <i>N</i>,<i>N</i>′‑Diphenylphenylpropiolamidinate and T<sup><i>i</i></sup>PB = 2,4,6-Triisopropylbenzoate
Two
dimolybdenum compounds featuring amidinate ligands with a Cî—¼C
bond, Mo<sub>2</sub>(NN)<sub>4</sub> (<b>I</b>), where NN = <i>N</i>,<i>N</i>′-diphenylphenylpropiolamidinate,
and <i>trans</i>-Mo<sub>2</sub>(NN)<sub>2</sub>(T<sup><i>i</i></sup>PB)<sub>2</sub> (<b>II</b>), where T<sup><i>i</i></sup>PB = 2,4,6-triisopropylbenzoate, have been prepared
and structurally characterized by single-crystal X-ray crystallography.
Together with Mo<sub>2</sub>(DAniF)<sub>4</sub> (<b>III</b>),
where DAniF = N,N′-bisÂ(<i>p</i>-anisyl)Âformamidinate,
all three compounds have been studied with steady-state UV–vis,
IR, and time-resolved spectroscopy methods. <b>I</b> and <b>II</b> display intense metal to ligand charge transfer (MLCT).
Singlet state (S<sub>1</sub>) lifetimes of <b>I</b>–<b>III</b> are determined to be 0.7, 19.1, and 2.0 ps, respectively.
All three compounds have long-lived triplet state (T<sub>1</sub>)
lifetimes around 100 μs. In femtosecond time-resolved infrared
(fs-TRIR) experiments, one νÂ(Cî—¼C) band is observed at
the S<sub>1</sub> state for <b>I</b> but two for <b>II</b>, which indicate different patterns of charge distribution. The electron
would have to be localized on one NN ligand in <b>I</b> and
partially delocalized over two NN ligands in <b>II</b> to account
for the observations. The result is a standard showcase of excited-state
mixed valence in coordination compounds
Femtosecond Study of Dimolybdenum Paddlewheel Compounds with Amide/Thioamide Ligands: Symmetry, Electronic Structure, and Charge Distribution in the <sup>1</sup>MLCT S<sub>1</sub> State
Four
photophysically interesting dimolybdenum paddlewheel compounds are
synthesized and characterized: <b>I</b> and <b>II</b> contain
amide ligand (<i>N</i>,3-diphenyl-2-propynamide), and <b>III</b> and <b>IV</b> contain thioamide ligand (<i>N</i>,3-diphenyl-2-propynethioamide). <b>I</b> and <b>III</b> are <i>trans</i>-Mo<sub>2</sub>L<sub>2</sub>(O<sub>2</sub>C-T<sup><i>i</i></sup>PB)<sub>2</sub>-type
compounds, and <b>II</b> and <b>IV</b> are Mo<sub>2</sub>L<sub>4</sub>-type compounds, where O<sub>2</sub>C-T<sup><i>i</i></sup>PB is 2,4,6-triisopropylbenzoate. <b>I</b>–<b>IV</b> display strong light absorption due to metal to ligand
charge transfer (MLCT) transitions from molybdenum to the amide/thioamide
ligands. Charge transfer dynamics in the MLCT excited states of <b>I</b>–<b>IV</b> have been examined using femtosecond
transient absorption (fs-TA) spectroscopy and femtosecond time-resolved
infrared (fs-TRIR) spectroscopy. The asymmetric amide/thioamide ligands
show two forms of regioarrangements in the paddlewheel compounds.
Analyses of the νÂ(Cî—¼C) bands in the fs-TRIR spectra of <b>I</b> and <b>II</b> show similar electron density distribution
over ligands in their <sup>1</sup>MLCT S<sub>1</sub> states where
only two amide ligands are involved and the transferred electron is
mainly localized on one of them. The fs-TRIR spectra of <b>III</b> and <b>IV</b>, however, show different charge distribution
patterns where the transferred electron is fully delocalized over
two thioamide ligands in <b>III</b> and partially delocalized
in <b>IV</b>. Fast interligand electron transfer (ILET) was
recognized as the explanation for the various charge distribution
patterns, and ILET was shown to be influenced by both the ligands
and the ligand arrangements
Femtosecond Study of Dimolybdenum Paddlewheel Compounds with Amide/Thioamide Ligands: Symmetry, Electronic Structure, and Charge Distribution in the <sup>1</sup>MLCT S<sub>1</sub> State
Four
photophysically interesting dimolybdenum paddlewheel compounds are
synthesized and characterized: <b>I</b> and <b>II</b> contain
amide ligand (<i>N</i>,3-diphenyl-2-propynamide), and <b>III</b> and <b>IV</b> contain thioamide ligand (<i>N</i>,3-diphenyl-2-propynethioamide). <b>I</b> and <b>III</b> are <i>trans</i>-Mo<sub>2</sub>L<sub>2</sub>(O<sub>2</sub>C-T<sup><i>i</i></sup>PB)<sub>2</sub>-type
compounds, and <b>II</b> and <b>IV</b> are Mo<sub>2</sub>L<sub>4</sub>-type compounds, where O<sub>2</sub>C-T<sup><i>i</i></sup>PB is 2,4,6-triisopropylbenzoate. <b>I</b>–<b>IV</b> display strong light absorption due to metal to ligand
charge transfer (MLCT) transitions from molybdenum to the amide/thioamide
ligands. Charge transfer dynamics in the MLCT excited states of <b>I</b>–<b>IV</b> have been examined using femtosecond
transient absorption (fs-TA) spectroscopy and femtosecond time-resolved
infrared (fs-TRIR) spectroscopy. The asymmetric amide/thioamide ligands
show two forms of regioarrangements in the paddlewheel compounds.
Analyses of the νÂ(Cî—¼C) bands in the fs-TRIR spectra of <b>I</b> and <b>II</b> show similar electron density distribution
over ligands in their <sup>1</sup>MLCT S<sub>1</sub> states where
only two amide ligands are involved and the transferred electron is
mainly localized on one of them. The fs-TRIR spectra of <b>III</b> and <b>IV</b>, however, show different charge distribution
patterns where the transferred electron is fully delocalized over
two thioamide ligands in <b>III</b> and partially delocalized
in <b>IV</b>. Fast interligand electron transfer (ILET) was
recognized as the explanation for the various charge distribution
patterns, and ILET was shown to be influenced by both the ligands
and the ligand arrangements
Synthesis, Structure, and Photophysical Properties of Mo<sub>2</sub>(NN)<sub>4</sub> and Mo<sub>2</sub>(NN)<sub>2</sub>(T<sup><i>i</i></sup>PB)<sub>2</sub>, Where NN = <i>N</i>,<i>N</i>′‑Diphenylphenylpropiolamidinate and T<sup><i>i</i></sup>PB = 2,4,6-Triisopropylbenzoate
Two
dimolybdenum compounds featuring amidinate ligands with a Cî—¼C
bond, Mo<sub>2</sub>(NN)<sub>4</sub> (<b>I</b>), where NN = <i>N</i>,<i>N</i>′-diphenylphenylpropiolamidinate,
and <i>trans</i>-Mo<sub>2</sub>(NN)<sub>2</sub>(T<sup><i>i</i></sup>PB)<sub>2</sub> (<b>II</b>), where T<sup><i>i</i></sup>PB = 2,4,6-triisopropylbenzoate, have been prepared
and structurally characterized by single-crystal X-ray crystallography.
Together with Mo<sub>2</sub>(DAniF)<sub>4</sub> (<b>III</b>),
where DAniF = N,N′-bisÂ(<i>p</i>-anisyl)Âformamidinate,
all three compounds have been studied with steady-state UV–vis,
IR, and time-resolved spectroscopy methods. <b>I</b> and <b>II</b> display intense metal to ligand charge transfer (MLCT).
Singlet state (S<sub>1</sub>) lifetimes of <b>I</b>–<b>III</b> are determined to be 0.7, 19.1, and 2.0 ps, respectively.
All three compounds have long-lived triplet state (T<sub>1</sub>)
lifetimes around 100 μs. In femtosecond time-resolved infrared
(fs-TRIR) experiments, one νÂ(Cî—¼C) band is observed at
the S<sub>1</sub> state for <b>I</b> but two for <b>II</b>, which indicate different patterns of charge distribution. The electron
would have to be localized on one NN ligand in <b>I</b> and
partially delocalized over two NN ligands in <b>II</b> to account
for the observations. The result is a standard showcase of excited-state
mixed valence in coordination compounds
Electronic and Spectroscopic Properties of Avobenzone Derivatives Attached to Mo<sub>2</sub> Quadruple Bonds: Suppression of the Photochemical Enol-to-Keto Transformation
From
the reactions between Mo<sub>2</sub>(T<sup><i>i</i></sup>PB)<sub>4</sub>, where T<sup><i>i</i></sup>PB is
2,4,6-triisopropylbenzoate, and 2 equiv of the acids 4-formylbenzoic
acid, HBzald; 4-(3-oxo-3-phenylpropanoyl)Âbenzoic acid, HAvo; and 4-(2,2-difluoro-6-phenyl-2<i>H</i>-1λ<sup>3</sup>,3,2λ<sup>4</sup>-dioxaborinin-4-yl)Âbenzoic
acid, HAvoBF<sub>2</sub>, the compounds Mo<sub>2</sub>(T<sup><i>i</i></sup>PB)<sub>2</sub>(Bzald)<sub>2</sub>, <b>I</b>; Mo<sub>2</sub>(T<sup><i>i</i></sup>PB)<sub>2</sub>(Avo)<sub>2</sub>, <b>II</b>; and Mo<sub>2</sub>(T<sup><i>i</i></sup>PB)<sub>2</sub>(AvoBF<sub>2</sub>)<sub>2</sub>, <b>III</b>, have been isolated. Compounds <b>I</b> and <b>II</b> are red, and compound <b>III</b> is blue. The new compounds
have been characterized by <sup>1</sup>H NMR, MALDI-TOF MS, steady-state
absorption and emission spectroscopies, and femtosecond and nanosecond
time-resolved transient absorption and infrared spectroscopies. Electronic
structure calculations employing density functional theory and time-dependent
density functional theory have been carried out to aid in the interpretation
of these data. These compounds have strong metal-to-ligand charge
transfer, MLCT, and transitions in the visible region of their spectra,
and these comprise the S<sub>1</sub> states having lifetimes ∼5–15
ps. The triplet states are Mo<sub>2</sub>δδ* with lifetimes
in the microseconds. The spectroscopic properties of <b>I</b> and <b>II</b> are similar, whereas the planarity of the ligand
in <b>III</b> greatly lowers the energy of the MLCT and enhances
the intensity of the time-resolved spectra. The Mo<sub>2</sub> unit
shifts the ground state equilibrium entirely to the enol form and
quenches the degradation pathways of the avobenzone moiety
Electronic and Spectroscopic Properties of Avobenzone Derivatives Attached to Mo<sub>2</sub> Quadruple Bonds: Suppression of the Photochemical Enol-to-Keto Transformation
From
the reactions between Mo<sub>2</sub>(T<sup><i>i</i></sup>PB)<sub>4</sub>, where T<sup><i>i</i></sup>PB is
2,4,6-triisopropylbenzoate, and 2 equiv of the acids 4-formylbenzoic
acid, HBzald; 4-(3-oxo-3-phenylpropanoyl)Âbenzoic acid, HAvo; and 4-(2,2-difluoro-6-phenyl-2<i>H</i>-1λ<sup>3</sup>,3,2λ<sup>4</sup>-dioxaborinin-4-yl)Âbenzoic
acid, HAvoBF<sub>2</sub>, the compounds Mo<sub>2</sub>(T<sup><i>i</i></sup>PB)<sub>2</sub>(Bzald)<sub>2</sub>, <b>I</b>; Mo<sub>2</sub>(T<sup><i>i</i></sup>PB)<sub>2</sub>(Avo)<sub>2</sub>, <b>II</b>; and Mo<sub>2</sub>(T<sup><i>i</i></sup>PB)<sub>2</sub>(AvoBF<sub>2</sub>)<sub>2</sub>, <b>III</b>, have been isolated. Compounds <b>I</b> and <b>II</b> are red, and compound <b>III</b> is blue. The new compounds
have been characterized by <sup>1</sup>H NMR, MALDI-TOF MS, steady-state
absorption and emission spectroscopies, and femtosecond and nanosecond
time-resolved transient absorption and infrared spectroscopies. Electronic
structure calculations employing density functional theory and time-dependent
density functional theory have been carried out to aid in the interpretation
of these data. These compounds have strong metal-to-ligand charge
transfer, MLCT, and transitions in the visible region of their spectra,
and these comprise the S<sub>1</sub> states having lifetimes ∼5–15
ps. The triplet states are Mo<sub>2</sub>δδ* with lifetimes
in the microseconds. The spectroscopic properties of <b>I</b> and <b>II</b> are similar, whereas the planarity of the ligand
in <b>III</b> greatly lowers the energy of the MLCT and enhances
the intensity of the time-resolved spectra. The Mo<sub>2</sub> unit
shifts the ground state equilibrium entirely to the enol form and
quenches the degradation pathways of the avobenzone moiety
Probing Interligand Electron Transfer in the <sup>1</sup>MLCT S<sub>1</sub> Excited State of <i>trans</i>-Mo<sub>2</sub>L<sub>2</sub>L′<sub>2</sub> Compounds: A Comparative Study of Auxiliary Ligands and Solvents
The interligand charge
dynamics of the lowest singlet metal-to-ligand
charge-transfer states (<sup>1</sup>MLCT S<sub>1</sub> states) of
a series of quadruply bonded <i>trans</i>-Mo<sub>2</sub>(NN)<sub>2</sub>(O<sub>2</sub>C–X)<sub>2</sub> paddlewheel
compounds are investigated, where NN is a π-accepting phenylpropiolamidinate
ligand and O<sub>2</sub>C–X (X = Me, <sup><i>t</i></sup>Bu, T<sup><i>i</i></sup>PB, or CF<sub>3</sub>) is
an auxiliary carboxylate ligand. The compounds show strong light absorption
in the visible region due to MLCT transitions from the Mo<sub>2</sub> center to the NN ligands. The transferred electron density was followed
by femtosecond time-resolved infrared (fs-TRIR) spectroscopy with
vibrational reporters such as the ethynyl groups on the NN ligands.
The observed fs-TRIR spectra show that these compounds have asymmetric <sup>1</sup>MLCT S<sub>1</sub> excited states where the transferred electron
mainly resides on a single NN ligand. The presence of interligand
electron transfer (ILET) is suggested to explain the shape of the
νÂ(Cî—¼C) bands and the influence of auxiliary ligands and
solvents on the interligand electronic coupling. The ILET in the <sup>1</sup>MLCT S<sub>1</sub> state is shown to be sensitive to the functional
groups on the auxiliary ligands while being less responsive to changes
in solvents