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Fumanal M, Daniel C, Gindensperger E. Excited-state dynamics of [Mn(im)(CO) 3(phen)] +: PhotoCORM, catalyst, luminescent probe? J Chem Phys 2021; 154:154102. [PMID: 33887929 DOI: 10.1063/5.0044108] [Citation(s) in RCA: 5] [Impact Index Per Article: 1.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 02/07/2023] Open
Abstract
Mn(I) α-diimine carbonyl complexes have shown promise in the development of luminescent CO release materials (photoCORMs) for diagnostic and medical applications due to their ability to balance the energy of the low-lying metal-to-ligand charge transfer (MLCT) and metal-centered (MC) states. In this work, the excited state dynamics of [Mn(im)(CO)3(phen)]+ (im = imidazole; phen = 1,10-phenanthroline) is investigated by means of wavepacket propagation on the potential energy surfaces associated with the 11 low-lying Sn singlet excited states within a vibronic coupling model in a (quasi)-diabatic representation including 16 nuclear degrees of freedom. The results show that the early time photophysics (<400 fs) is controlled by the interaction between two MC dissociative states, namely, S5 and S11, with the lowest S1-S3 MLCT bound states. In particular, the presence of S1/S5 and S2/S11 crossings within the diabatic picture along the Mn-COaxial dissociative coordinate (qMn-COaxial) favors a two-stepwise population of the dissociative states, at about 60-70 fs (S11) and 160-180 fs (S5), which reaches about 10% within 200 fs. The one-dimensional reduced densities associated with the dissociative states along qMn-COaxial as a function of time clearly point to concurrent primary processes, namely, CO release vs entrapping into the S1 and S2 potential wells of the lowest luminescent MLCT states within 400 fs, characteristics of luminescent photoCORM.
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Affiliation(s)
- Maria Fumanal
- Laboratoire de Chimie Quantique, Institut de Chimie Strasbourg, UMR-7177 CNRS/Université de Strasbourg, 1 Rue Blaise Pascal BP 296/R8, F-67008 Strasbourg, France
| | - Chantal Daniel
- Laboratoire de Chimie Quantique, Institut de Chimie Strasbourg, UMR-7177 CNRS/Université de Strasbourg, 1 Rue Blaise Pascal BP 296/R8, F-67008 Strasbourg, France
| | - Etienne Gindensperger
- Laboratoire de Chimie Quantique, Institut de Chimie Strasbourg, UMR-7177 CNRS/Université de Strasbourg, 1 Rue Blaise Pascal BP 296/R8, F-67008 Strasbourg, France
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10
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Zobel JP, Bokareva OS, Zimmer P, Wölper C, Bauer M, González L. Intersystem Crossing and Triplet Dynamics in an Iron(II) N-Heterocyclic Carbene Photosensitizer. Inorg Chem 2020; 59:14666-14678. [PMID: 32869981 PMCID: PMC7581298 DOI: 10.1021/acs.inorgchem.0c02147] [Citation(s) in RCA: 19] [Impact Index Per Article: 4.8] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/05/2023]
Abstract
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The electronic excited
states of the iron(II) complex [FeII(tpy)(pyz-NHC)]2+ [tpy = 2,2′:6′,2″-terpyridine; pyz-NHC
= 1,1′-bis(2,6-diisopropylphenyl)pyrazinyldiimidazolium-2,2′-diylidene]
and their relaxation pathways have been theoretically investigated.
To this purpose, trajectory surface-hopping simulations within a linear
vibronic coupling model including a 244-dimensional potential energy
surface (PES) with 20 singlet and 20 triplet coupled states have been
used. The simulations show that, after excitation to the lowest-energy
absorption band of predominant metal-to-ligand charge-transfer character
involving the tpy ligand, almost 80% of the population undergoes intersystem
crossing to the triplet manifold in about 50 fs, while the remaining
20% decays through internal conversion to the electronic ground state
in about 300 fs. The population transferred to the triplet states
is found to deactivate into two different regions of the PESs, one
where the static dipole moment is small and shows increased metal-centered
character and another with a large static dipole moment, where the
electron density is transferred from the tpy to pyz-NHC ligand. Coherent
oscillations of 400 fs are observed between these two sets of triplet
populations, until the mixture equilibrates to a ratio of 60:40. Finally,
the importance of selecting suitable normal modes is highlighted—a
choice that can be far from straightforward in transition-metal complexes
with hundreds of degrees of freedom. Trajectory
surface-hopping simulations with a linear vibronic coupling model
reveal the competition of major intersystem crossing versus minor
internal conversion dynamics in an iron(II) N-heterocyclic carbene
dye. The triplet population bifurcates into two regions of the potential
energy surfaces, characterized by small and large static dipole moments
due to different electronic character and showing coherent oscillations
of 400 fs until both triplet populations coexist in a mixture of 60:40.
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Affiliation(s)
- J Patrick Zobel
- Institute of Theoretical Chemistry, Faculty of Chemistry, University of Vienna, Währingerstraße 19, 1090 Vienna, Austria
| | - Olga S Bokareva
- Institute of Physics, Rostock University, Albert Einstein Straße 23-24, 18059 Rostock, Germany
| | - Peter Zimmer
- Faculty of Science, Chemistry Department and Center for Sustainable Systems Design (CSSD), Paderborn University, Warburger Straße 100, 33098 Paderborn, Germany
| | - Christoph Wölper
- Department for X-Ray Diffraction, Inorganic Chemistry, University of Duisburg-Essen, Universitätsstraße 7, D-45117 Essen, Germany
| | - Matthias Bauer
- Faculty of Science, Chemistry Department and Center for Sustainable Systems Design (CSSD), Paderborn University, Warburger Straße 100, 33098 Paderborn, Germany
| | - Leticia González
- Institute of Theoretical Chemistry, Faculty of Chemistry, University of Vienna, Währingerstraße 19, 1090 Vienna, Austria.,Vienna Research Platform on Accelerating Photoreaction Discovery, University of Vienna, Währingerstr. 19, 1090 Vienna, Austria
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13
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Kunnus K, Vacher M, Harlang TCB, Kjær KS, Haldrup K, Biasin E, van Driel TB, Pápai M, Chabera P, Liu Y, Tatsuno H, Timm C, Källman E, Delcey M, Hartsock RW, Reinhard ME, Koroidov S, Laursen MG, Hansen FB, Vester P, Christensen M, Sandberg L, Németh Z, Szemes DS, Bajnóczi É, Alonso-Mori R, Glownia JM, Nelson S, Sikorski M, Sokaras D, Lemke HT, Canton SE, Møller KB, Nielsen MM, Vankó G, Wärnmark K, Sundström V, Persson P, Lundberg M, Uhlig J, Gaffney KJ. Vibrational wavepacket dynamics in Fe carbene photosensitizer determined with femtosecond X-ray emission and scattering. Nat Commun 2020; 11:634. [PMID: 32005815 PMCID: PMC6994595 DOI: 10.1038/s41467-020-14468-w] [Citation(s) in RCA: 61] [Impact Index Per Article: 15.3] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/14/2019] [Accepted: 12/30/2019] [Indexed: 12/31/2022] Open
Abstract
The non-equilibrium dynamics of electrons and nuclei govern the function of photoactive materials. Disentangling these dynamics remains a critical goal for understanding photoactive materials. Here we investigate the photoinduced dynamics of the [Fe(bmip)2]2+ photosensitizer, where bmip = 2,6-bis(3-methyl-imidazole-1-ylidine)-pyridine, with simultaneous femtosecond-resolution Fe Kα and Kβ X-ray emission spectroscopy (XES) and X-ray solution scattering (XSS). This measurement shows temporal oscillations in the XES and XSS difference signals with the same 278 fs period oscillation. These oscillations originate from an Fe-ligand stretching vibrational wavepacket on a triplet metal-centered (3MC) excited state surface. This 3MC state is populated with a 110 fs time constant by 40% of the excited molecules while the rest relax to a 3MLCT excited state. The sensitivity of the Kα XES to molecular structure results from a 0.7% average Fe-ligand bond length shift between the 1 s and 2p core-ionized states surfaces.
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Affiliation(s)
- Kristjan Kunnus
- PULSE Institute, SLAC National Accelerator Laboratory, Stanford University, Menlo Park, CA, 94025, USA.
| | - Morgane Vacher
- Department of Chemistry - Ångström laboratory, Uppsala University, Box 538, 75121, Uppsala, Sweden
| | - Tobias C B Harlang
- Department of Chemical Physics, Lund University, P.O. Box 12 4, 22100, Lund, Sweden
- Department of Physics, Technical University of Denmark, DK-2800, Lyngby, Denmark
| | - Kasper S Kjær
- PULSE Institute, SLAC National Accelerator Laboratory, Stanford University, Menlo Park, CA, 94025, USA
- Department of Chemical Physics, Lund University, P.O. Box 12 4, 22100, Lund, Sweden
- Department of Physics, Technical University of Denmark, DK-2800, Lyngby, Denmark
| | - Kristoffer Haldrup
- Department of Physics, Technical University of Denmark, DK-2800, Lyngby, Denmark
| | - Elisa Biasin
- PULSE Institute, SLAC National Accelerator Laboratory, Stanford University, Menlo Park, CA, 94025, USA
- Department of Physics, Technical University of Denmark, DK-2800, Lyngby, Denmark
| | - Tim B van Driel
- LCLS, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - Mátyás Pápai
- Department of Chemistry, Technical University of Denmark, Kemitorvet 207, DK-2800, Kongens Lyngby, Denmark
| | - Pavel Chabera
- Department of Chemical Physics, Lund University, P.O. Box 12 4, 22100, Lund, Sweden
| | - Yizhu Liu
- Department of Chemical Physics, Lund University, P.O. Box 12 4, 22100, Lund, Sweden
- Centre for Analysis and Synthesis, Department of Chemistry, Lund University, P.O. Box 124, 22100, Lund, Sweden
| | - Hideyuki Tatsuno
- Department of Chemical Physics, Lund University, P.O. Box 12 4, 22100, Lund, Sweden
| | - Cornelia Timm
- Department of Chemical Physics, Lund University, P.O. Box 12 4, 22100, Lund, Sweden
| | - Erik Källman
- Department of Chemistry - Ångström laboratory, Uppsala University, Box 538, 75121, Uppsala, Sweden
| | - Mickaël Delcey
- Department of Chemistry - Ångström laboratory, Uppsala University, Box 538, 75121, Uppsala, Sweden
| | - Robert W Hartsock
- PULSE Institute, SLAC National Accelerator Laboratory, Stanford University, Menlo Park, CA, 94025, USA
| | - Marco E Reinhard
- PULSE Institute, SLAC National Accelerator Laboratory, Stanford University, Menlo Park, CA, 94025, USA
| | - Sergey Koroidov
- PULSE Institute, SLAC National Accelerator Laboratory, Stanford University, Menlo Park, CA, 94025, USA
| | - Mads G Laursen
- Department of Physics, Technical University of Denmark, DK-2800, Lyngby, Denmark
| | - Frederik B Hansen
- Department of Physics, Technical University of Denmark, DK-2800, Lyngby, Denmark
| | - Peter Vester
- Department of Physics, Technical University of Denmark, DK-2800, Lyngby, Denmark
| | - Morten Christensen
- Department of Physics, Technical University of Denmark, DK-2800, Lyngby, Denmark
| | - Lise Sandberg
- Department of Physics, Technical University of Denmark, DK-2800, Lyngby, Denmark
- University of Copenhagen, Niels Bohr Institute, Blegdamsvej 17, 2100, Copenhagen, Denmark
| | - Zoltán Németh
- Wigner Research Centre for Physics, Hungarian Academy of Sciences, P.O. Box 49, H-1525, Budapest, Hungary
| | - Dorottya Sárosiné Szemes
- Wigner Research Centre for Physics, Hungarian Academy of Sciences, P.O. Box 49, H-1525, Budapest, Hungary
| | - Éva Bajnóczi
- Wigner Research Centre for Physics, Hungarian Academy of Sciences, P.O. Box 49, H-1525, Budapest, Hungary
| | | | - James M Glownia
- LCLS, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - Silke Nelson
- LCLS, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - Marcin Sikorski
- LCLS, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | | | - Henrik T Lemke
- LCLS, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - Sophie E Canton
- ELI-ALPS, ELI-HU Non-Profit Ltd., Dugonics ter 13, Szeged, 6720, Hungary
- Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, D-22607, Hamburg, Germany
| | - Klaus B Møller
- Department of Chemistry, Technical University of Denmark, Kemitorvet 207, DK-2800, Kongens Lyngby, Denmark
| | - Martin M Nielsen
- Department of Physics, Technical University of Denmark, DK-2800, Lyngby, Denmark
| | - György Vankó
- Wigner Research Centre for Physics, Hungarian Academy of Sciences, P.O. Box 49, H-1525, Budapest, Hungary
| | - Kenneth Wärnmark
- Centre for Analysis and Synthesis, Department of Chemistry, Lund University, P.O. Box 124, 22100, Lund, Sweden
| | - Villy Sundström
- Department of Chemical Physics, Lund University, P.O. Box 12 4, 22100, Lund, Sweden
| | - Petter Persson
- Theoretical Chemistry Division, Lund University, P.O. Box 124, 22100, Lund, Sweden
| | - Marcus Lundberg
- Department of Chemistry - Ångström laboratory, Uppsala University, Box 538, 75121, Uppsala, Sweden
| | - Jens Uhlig
- Department of Chemical Physics, Lund University, P.O. Box 12 4, 22100, Lund, Sweden
| | - Kelly J Gaffney
- PULSE Institute, SLAC National Accelerator Laboratory, Stanford University, Menlo Park, CA, 94025, USA.
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