2026
|
| 44. | C. S. Kern, X Yang, G. Zamborlini, S. Mearini, M. Jugovac, V. Feyer, U. De Giovannini, A. Rubio, S. Soubatch, M. G. Ramsey F. S. Tautz, P. Puschnig Circular dichroism in the photoelectron angular distribution of achiral molecules Journal Article In: Phys. Rev. Research, vol. 8, iss. 023275, 2026. @article{Kern2026,
title = {Circular dichroism in the photoelectron angular distribution of achiral molecules},
author = {C. S. Kern and X Yang and G. Zamborlini and S. Mearini and M. Jugovac and V. Feyer and U. De Giovannini and A. Rubio and S. Soubatch and M. G. Ramsey F. S. Tautz and P. Puschnig},
url = {https://journals.aps.org/prresearch/abstract/10.1103/6bkb-4rm3},
doi = {10.1103/6bkb-4rm3},
year = {2026},
date = {2026-06-11},
journal = {Phys. Rev. Research},
volume = {8},
issue = { 023275},
abstract = {Circular dichroism in the angular distribution (CDAD) is the effect that the angular intensity distribution of photoemitted electrons depends on the handedness of the incident circularly polarized light. The origin of CDAD can be manifold, including intrinsic properties of the system under study, such as chirality, spin-orbit interaction, or quantum-geometrical properties, but CDAD can also originate from final-state effects influenced by the experimental geometry. For example, CDAD has been reported for achiral organic molecules at the interface to metallic substrates. For this latter case, we investigate two prototypical 𝜋
-conjugated molecules, namely, tetracene and pentacene, whose frontier orbitals have a similar shape but exhibit distinctly different symmetries. By comparing experimental CDAD momentum maps with simulations within time-dependent density functional theory, we show how the final state of the photoelectron must be regarded as the source of the CDAD in such otherwise achiral and quantum-geometrically trivial systems. We gain additional insight into the mechanism by employing a simple scattering model for the final state, which allows us to decompose the CDAD signal into partial wave contributions.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Circular dichroism in the angular distribution (CDAD) is the effect that the angular intensity distribution of photoemitted electrons depends on the handedness of the incident circularly polarized light. The origin of CDAD can be manifold, including intrinsic properties of the system under study, such as chirality, spin-orbit interaction, or quantum-geometrical properties, but CDAD can also originate from final-state effects influenced by the experimental geometry. For example, CDAD has been reported for achiral organic molecules at the interface to metallic substrates. For this latter case, we investigate two prototypical 𝜋
-conjugated molecules, namely, tetracene and pentacene, whose frontier orbitals have a similar shape but exhibit distinctly different symmetries. By comparing experimental CDAD momentum maps with simulations within time-dependent density functional theory, we show how the final state of the photoelectron must be regarded as the source of the CDAD in such otherwise achiral and quantum-geometrically trivial systems. We gain additional insight into the mechanism by employing a simple scattering model for the final state, which allows us to decompose the CDAD signal into partial wave contributions. |
| 43. | G. Inzani, V. Eggers, M. Meierhofer, L. Münster, J. Helml, R. Wallauer, S. Zajusch, S. Ito, L. Machtl, H. Yin, C. Kumpf, F. C. Bocquet, C. Bao, J. Güdde, F. S. Tautz, R. Huber, U. Höfer Direct subcycle momentum-resolved observation of Landau-Zener-Majorana transitions in lightwave-driven graphene Conference vol. 14077, 2026. @conference{Inzani2026,
title = {Direct subcycle momentum-resolved observation of Landau-Zener-Majorana transitions in lightwave-driven graphene},
author = {G. Inzani and V. Eggers and M. Meierhofer and L. Münster and J. Helml and R. Wallauer and S. Zajusch and S. Ito and L. Machtl and H. Yin and C. Kumpf and F. C. Bocquet and C. Bao and J. Güdde and F. S. Tautz and R. Huber and U. Höfer},
url = {https://www.spiedigitallibrary.org/conference-proceedings-of-spie/14077/3099485/Direct-subcycle-momentum-resolved-observation-of-Landau-Zener-Majorana-transitions/10.1117/12.3099485.full},
doi = {10.1117/12.3099485},
year = {2026},
date = {2026-05-26},
volume = {14077},
abstract = {Understanding electron motion driven by the carrier field of light is central to the development of lightwave electronics. In this work, we directly observe field-driven Landau-Zener-Majorana transitions in graphene with sub-cycle band-structure videography. Our experimental approach combines photoemission momentum microscopy with strong phase-stable few-cycle mid-infrared pump pulses and ultrashort extreme-ultraviolet probe pulses, enabling field-resolved measurements of carrier dynamics throughout the entire Brillouin zone. Time-resolved measurements around a Dirac point of graphene reveal the evolution of the electron distribution during the optical cycle: carriers accelerate away from the Fermi level and are displaced along the Dirac cone. This creates an asymmetric occupation which generates an ultrafast current. The transient two-dimensional carrier distribution encodes the signature of Landau-Zener-Majorana transitions and uncovers electron-electron and electron-phonon scattering pathways. Access to the full two-dimensional momentum space with subcycle resolution provides key insights into the physical phenomena dictating coherent light–matter interaction. This methodology opens new opportunities for exploring strong-field phenomena in solids, including inter- and intraband dynamics, Bloch oscillations, and Floquet-Bloch states. },
keywords = {},
pubstate = {published},
tppubtype = {conference}
}
Understanding electron motion driven by the carrier field of light is central to the development of lightwave electronics. In this work, we directly observe field-driven Landau-Zener-Majorana transitions in graphene with sub-cycle band-structure videography. Our experimental approach combines photoemission momentum microscopy with strong phase-stable few-cycle mid-infrared pump pulses and ultrashort extreme-ultraviolet probe pulses, enabling field-resolved measurements of carrier dynamics throughout the entire Brillouin zone. Time-resolved measurements around a Dirac point of graphene reveal the evolution of the electron distribution during the optical cycle: carriers accelerate away from the Fermi level and are displaced along the Dirac cone. This creates an asymmetric occupation which generates an ultrafast current. The transient two-dimensional carrier distribution encodes the signature of Landau-Zener-Majorana transitions and uncovers electron-electron and electron-phonon scattering pathways. Access to the full two-dimensional momentum space with subcycle resolution provides key insights into the physical phenomena dictating coherent light–matter interaction. This methodology opens new opportunities for exploring strong-field phenomena in solids, including inter- and intraband dynamics, Bloch oscillations, and Floquet-Bloch states. |
| 42. | S. Mearini, F. Auer, M. Laßhofer, A. Windischbacher, D. Brandstetter, D. Baranowski, Y. Y. Grisan Qiu, I. Cojocariu, M. Jugovac, M. Sterrer, G. Zamborlini, V. Feyer, C. M. Schneider Single Ni Atoms Drive Carboxyl Deprotonation in Metal–Organic Chains Journal Article In: ACS Nano, vol. 20, iss. 16, pp. 12596–12603, 2026. @article{Mearini2026,
title = {Single Ni Atoms Drive Carboxyl Deprotonation in Metal–Organic Chains},
author = {S. Mearini and F. Auer and M. Laßhofer and A. Windischbacher and D. Brandstetter and D. Baranowski and Y. Y. Grisan Qiu and I. Cojocariu and M. Jugovac and M. Sterrer and G. Zamborlini and V. Feyer and C. M. Schneider},
url = {https://pubs.acs.org/doi/10.1021/acsnano.6c01444},
doi = {10.1021/acsnano.6c01444},
year = {2026},
date = {2026-04-17},
journal = {ACS Nano},
volume = {20},
issue = {16},
pages = {12596–12603},
abstract = {Understanding how charge transfer and ligand activation processes govern metal–organic coordination at surfaces is crucial for controlling on-surface synthesis and the formation of low-dimensional architectures. Here, we show that Ni promotes the deprotonation of the carboxyl groups of terephthalic acid (TPA) on Ag(100), leading to the formation of linear metal–organic coordination chains. Scanning tunneling microscopy reveals that these chains emerge from preassembled hydrogen-bonded TPA stripes. X-ray photoelectron spectroscopy identifies stabilization of the Ni centers in the Ni(I) oxidation state through a single-electron charge transfer process, accompanied by the formation of deprotonated carboxylate species. Valence band spectroscopy reveals a coordination-induced electronic reorganization between Ni and TPA through the emergence of hybrid states, in agreement with complementary theoretical modeling. Together, these findings identify charge-transfer-driven deprotonation as the central mechanism governing the formation of linear metal–organic chains.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Understanding how charge transfer and ligand activation processes govern metal–organic coordination at surfaces is crucial for controlling on-surface synthesis and the formation of low-dimensional architectures. Here, we show that Ni promotes the deprotonation of the carboxyl groups of terephthalic acid (TPA) on Ag(100), leading to the formation of linear metal–organic coordination chains. Scanning tunneling microscopy reveals that these chains emerge from preassembled hydrogen-bonded TPA stripes. X-ray photoelectron spectroscopy identifies stabilization of the Ni centers in the Ni(I) oxidation state through a single-electron charge transfer process, accompanied by the formation of deprotonated carboxylate species. Valence band spectroscopy reveals a coordination-induced electronic reorganization between Ni and TPA through the emergence of hybrid states, in agreement with complementary theoretical modeling. Together, these findings identify charge-transfer-driven deprotonation as the central mechanism governing the formation of linear metal–organic chains. |
| 41. | M. Stettner, S. Kaidisch, Andrey V. Matetskiy, E. Fackelman, S. Soubatch, C. Kumpf, F. C. Bocquet, M. G. Ramsey, P. Puschnig, F. S. Tautz Tracing the film structure of an organic semiconductor with photoemission orbital tomography Journal Article Forthcoming In: arXiv:2603.06204 [cond-mat.mtrl-sci], Forthcoming. @article{Stettner2026,
title = {Tracing the film structure of an organic semiconductor with photoemission orbital tomography},
author = {M. Stettner and S. Kaidisch and Andrey V. Matetskiy and E. Fackelman and S. Soubatch and C. Kumpf and F. C. Bocquet and M. G. Ramsey and P. Puschnig and F. S. Tautz},
url = {https://arxiv.org/abs/2603.06204},
doi = {10.48550/arXiv.2603.06204},
year = {2026},
date = {2026-03-06},
journal = {arXiv:2603.06204 [cond-mat.mtrl-sci]},
keywords = {},
pubstate = {forthcoming},
tppubtype = {article}
}
|
| 40. | D. M. Janas, M. S. Arndt, J. E. Nitschke, L. Sternemann, V. Mischke, V. Feyer, I. Cojocariu, D. Baranowski, A. Sala, A. Windischbacher, P. Puschnig, J. Dreiser, S. Ponzoni, G. Zamborlini, M. Cinchetti Spin-Selective Interface Engineering in Oxide–Ferromagnetic Junctions via Atomic-Scale Oxygen Control Journal Article In: Advanced Science, vol. 13, iss. 25, no. e23165, 2026. @article{Janas2026,
title = {Spin-Selective Interface Engineering in Oxide–Ferromagnetic Junctions via Atomic-Scale Oxygen Control},
author = {D. M. Janas and M. S. Arndt and J. E. Nitschke and L. Sternemann and V. Mischke and V. Feyer and I. Cojocariu and D. Baranowski and A. Sala and A. Windischbacher and P. Puschnig and J. Dreiser and S. Ponzoni and G. Zamborlini and M. Cinchetti},
url = {https://advanced.onlinelibrary.wiley.com/doi/10.1002/advs.202523165},
doi = {10.1002/advs.202523165},
year = {2026},
date = {2026-02-20},
journal = {Advanced Science},
volume = {13},
number = {e23165},
issue = {25},
abstract = {Atomic-scale control of oxide–ferromagnet interfaces is crucial for optimizing spintronic heterostructures, yet interfacial oxygen remains difficult to control and verify. Here, we deterministically tune the prototypical MgO/Fe(100) interface from oxygen-free terminations to fully intercalated oxygen layers by reactive growth under controlled O2 exposure, while preserving epitaxy. Momentum-resolved photoemission identifies oxygen-dependent fingerprints in k-space that originate from the buried interface and persist up to a thickness of 8 layers of MgO. Insights from complementary spectroscopic methods link these k-space signatures to interfacial chemistry, structural order, work-function shifts, and an oxygen-induced interface resonance within the MgO gap that alters the tunneling response. The combined results define a calibrated growth protocol that allows reproducibly preparing and identifying three distinct terminations — oxygen-free, partially oxidized, and oxygen-intercalated — and enables post-growth conversion even in thicker films. Complementary spin-resolved experiments reveal that oxygen-free interfaces exhibit pronounced suppression of minority-spin spectral weight at the Fermi level, consistent with coherent spin filtering across crystalline MgO, whereas oxygen intercalation reduces the spin contrast at EF. By turning interfacial oxygen from an uncontrolled variable into a measurable, adjustable parameter, our approach establishes MgO/Fe(100) as a benchmark platform for optimizing spintronic functionality in oxide/metal junctions.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Atomic-scale control of oxide–ferromagnet interfaces is crucial for optimizing spintronic heterostructures, yet interfacial oxygen remains difficult to control and verify. Here, we deterministically tune the prototypical MgO/Fe(100) interface from oxygen-free terminations to fully intercalated oxygen layers by reactive growth under controlled O2 exposure, while preserving epitaxy. Momentum-resolved photoemission identifies oxygen-dependent fingerprints in k-space that originate from the buried interface and persist up to a thickness of 8 layers of MgO. Insights from complementary spectroscopic methods link these k-space signatures to interfacial chemistry, structural order, work-function shifts, and an oxygen-induced interface resonance within the MgO gap that alters the tunneling response. The combined results define a calibrated growth protocol that allows reproducibly preparing and identifying three distinct terminations — oxygen-free, partially oxidized, and oxygen-intercalated — and enables post-growth conversion even in thicker films. Complementary spin-resolved experiments reveal that oxygen-free interfaces exhibit pronounced suppression of minority-spin spectral weight at the Fermi level, consistent with coherent spin filtering across crystalline MgO, whereas oxygen intercalation reduces the spin contrast at EF. By turning interfacial oxygen from an uncontrolled variable into a measurable, adjustable parameter, our approach establishes MgO/Fe(100) as a benchmark platform for optimizing spintronic functionality in oxide/metal junctions. |
| 39. | V. Eggers, G. Inzani, M. Meierhofer, L. Münster, J. Helml, R. Wallauer, S. Zajusch, S. Ito, L. Machtl, H. Yin, C. Kumpf, F. C. Bocquet, C. Bao, J. Güdde, F. S. Tautz, R. Huber, U. Höfer Subcycle videography of lightwave-driven Landau-Zener-Majorana transitions in graphene Journal Article Forthcoming In: arXiv:2602.12844 [cond-mat.mes-hall], Forthcoming. @article{Eggers2026,
title = {Subcycle videography of lightwave-driven Landau-Zener-Majorana transitions in graphene},
author = {V. Eggers and G. Inzani and M. Meierhofer and L. Münster and J. Helml and R. Wallauer and S. Zajusch and S. Ito and L. Machtl and H. Yin and C. Kumpf and F. C. Bocquet and C. Bao and J. Güdde and F. S. Tautz and R. Huber and U. Höfer},
url = {https://arxiv.org/abs/2602.12844},
doi = {10.48550/arXiv.2602.12844},
year = {2026},
date = {2026-02-13},
journal = {arXiv:2602.12844 [cond-mat.mes-hall]},
abstract = {Strong light fields have unlocked previously unthinkable possibilities to tailor coherent electron trajectories, engineer band structures and shape emergent phases of matter all-optically. Unravelling the underlying quantum mechanisms requires a visualisation of the lightwave-driven electron motion directly in the band structure. While photoelectron momentum microscopy has imaged optically excited electrons averaged over many cycles of light, actual subcycle band-structure videography has been limited to small electron momenta. Yet lightwave-driven elementary processes in quantum materials often occur throughout momentum space. Here, we introduce attosecond-precision, subcycle band-structure videography covering the entire first Brillouin zone (BZ) and visualize one of the most fundamental but notoriously elusive strong-field processes: non-adiabatic Landau-Zener-Majorana (LZM) tunnelling. The interplay of field-driven acceleration within the Dirac-like band structure of graphene and periodic LZM interband tunnelling manifest in a coherent displacement and distortion of the momentum distribution at the BZ edge. The extremely non-thermal electron distributions also allow us to disentangle competing scattering processes and assess their impact on coherent electronic control through electron redistribution and thermalization. Our panoramic view of strong-field-driven electron motion in quantum materials lays the foundation for a microscopic understanding of some of the most discussed light-driven phenomena in condensed matter physics. },
keywords = {},
pubstate = {forthcoming},
tppubtype = {article}
}
Strong light fields have unlocked previously unthinkable possibilities to tailor coherent electron trajectories, engineer band structures and shape emergent phases of matter all-optically. Unravelling the underlying quantum mechanisms requires a visualisation of the lightwave-driven electron motion directly in the band structure. While photoelectron momentum microscopy has imaged optically excited electrons averaged over many cycles of light, actual subcycle band-structure videography has been limited to small electron momenta. Yet lightwave-driven elementary processes in quantum materials often occur throughout momentum space. Here, we introduce attosecond-precision, subcycle band-structure videography covering the entire first Brillouin zone (BZ) and visualize one of the most fundamental but notoriously elusive strong-field processes: non-adiabatic Landau-Zener-Majorana (LZM) tunnelling. The interplay of field-driven acceleration within the Dirac-like band structure of graphene and periodic LZM interband tunnelling manifest in a coherent displacement and distortion of the momentum distribution at the BZ edge. The extremely non-thermal electron distributions also allow us to disentangle competing scattering processes and assess their impact on coherent electronic control through electron redistribution and thermalization. Our panoramic view of strong-field-driven electron motion in quantum materials lays the foundation for a microscopic understanding of some of the most discussed light-driven phenomena in condensed matter physics. |
| 38. | A. Haags, A. Reichmann, Z. Ruan, Q. Fan, L. Egger, H. Kirschner, T. Naumann, S. Werner, O. Kleykamp, J. Martinez Castro, F. Lüpke, F. C. Bocquet, C. Kumpf, S. Soubatch, A. Gottwald, G. Koller, M. G. Ramsey, M. Richter, J. Sundermeyer, P. Puschnig, J. M. Gottfried, F. S. Tautz, S. Wenzel Multi-Orbital Charge Transfer into Nonplanar Cycloarenes Revealed with CO-Functionalized STM Tips Journal Article In: The Journal of Physical Chemistry Letters, vol. 17, iss. 5, pp. 1296–1304, 2026. @article{Haags2026,
title = {Multi-Orbital Charge Transfer into Nonplanar Cycloarenes Revealed with CO-Functionalized STM Tips},
author = {A. Haags and A. Reichmann and Z. Ruan and Q. Fan and L. Egger and H. Kirschner and T. Naumann and S. Werner and O. Kleykamp and J. Martinez Castro and F. Lüpke and F. C. Bocquet and C. Kumpf and S. Soubatch and A. Gottwald and G. Koller and M. G. Ramsey and M. Richter and J. Sundermeyer and P. Puschnig and J. M. Gottfried and F. S. Tautz and S. Wenzel},
url = {https://pubs.acs.org/doi/10.1021/acs.jpclett.5c03268},
doi = {10.1021/acs.jpclett.5c03268},
year = {2026},
date = {2026-01-21},
journal = {The Journal of Physical Chemistry Letters},
volume = {17},
issue = {5},
pages = {1296–1304},
abstract = {On-surface synthesis enables the tunable preparation of diverse molecular systems with tailored properties. Recently, the highly selective synthesis of kekulene (>99%) on Cu(111) and isokekulene (92%) on Cu(110) from the same molecular precursor was demonstrated. Scanning tunneling microscopy (STM) with CO-functionalized tips can identify individual molecules based on their geometric structure at low coverage on Cu(110) but also reveals complex features arising from electronic contributions near the Fermi energy. Here, we investigate the origin of these features by simulating STM images based on a weighted sum of multiple molecular orbitals, for which we employ weights based on the calculated molecular-orbital projected density of states. This analysis provides direct experimental evidence for charge transfer from the surface into multiple formerly unoccupied molecular orbitals for single molecules of kekulene as well as isokekulene in its two nonplanar adsorption configurations. In comparison, the area-integrating photoemission orbital tomography technique confirms the charge transfer as well as the high selectivity for the formation of a full monolayer of predominantly isokekulene on Cu(110). Our STM-based approach is applicable to a wide range of adsorbed molecular systems and specifically also suited for strongly interacting surfaces, nonplanar molecules, and compounds accessible only in extremely low yields.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
On-surface synthesis enables the tunable preparation of diverse molecular systems with tailored properties. Recently, the highly selective synthesis of kekulene (>99%) on Cu(111) and isokekulene (92%) on Cu(110) from the same molecular precursor was demonstrated. Scanning tunneling microscopy (STM) with CO-functionalized tips can identify individual molecules based on their geometric structure at low coverage on Cu(110) but also reveals complex features arising from electronic contributions near the Fermi energy. Here, we investigate the origin of these features by simulating STM images based on a weighted sum of multiple molecular orbitals, for which we employ weights based on the calculated molecular-orbital projected density of states. This analysis provides direct experimental evidence for charge transfer from the surface into multiple formerly unoccupied molecular orbitals for single molecules of kekulene as well as isokekulene in its two nonplanar adsorption configurations. In comparison, the area-integrating photoemission orbital tomography technique confirms the charge transfer as well as the high selectivity for the formation of a full monolayer of predominantly isokekulene on Cu(110). Our STM-based approach is applicable to a wide range of adsorbed molecular systems and specifically also suited for strongly interacting surfaces, nonplanar molecules, and compounds accessible only in extremely low yields. |
| 37. | C. Bao, V. Eggers, M. Meierhofer, J. Helml, L. Münster, S. Ito, L. Machtl, S. Zajusch, G. Inzani, L. Wittmann, M. Liebich, R. Wallauer, U. Höfer, R. Huber Observation of an isolated flat band in the van der Waals crystal NbOCl2 Journal Article In: Communications Materials, vol. 7, no. 60, 2026. @article{Bao2026,
title = {Observation of an isolated flat band in the van der Waals crystal NbOCl2},
author = {C. Bao and V. Eggers and M. Meierhofer and J. Helml and L. Münster and S. Ito and L. Machtl and S. Zajusch and G. Inzani and L. Wittmann and M. Liebich and R. Wallauer and U. Höfer and R. Huber},
url = {https://www.nature.com/articles/s43246-025-01070-0},
doi = {10.1038/s43246-025-01070-0},
year = {2026},
date = {2026-01-10},
journal = {Communications Materials},
volume = {7},
number = {60},
abstract = {Dispersionless electronic bands lead to an extremely high density of states and suppressed kinetic energy, thereby increasing electronic correlations and instabilities that can shape emergent ordered states, such as excitonic, ferromagnetic, and superconducting phases. A flat band that extends over the entire momentum space and is well isolated from other dispersive bands is, therefore, particularly interesting. Here, the band structure of the van der Waals crystal NbOCl2 is revealed by utilizing photoelectron momentum microscopy. We directly map out an electronic band that is flat throughout the entire Brillouin zone and features a width of only ~ 100 meV. This band is well isolated from both the conduction and remote valence bands. Moreover, the quasiparticle band gap shows a high tunability upon the deposition of cesium atoms on the surface. By combining the single-particle band structure with the optical transmission spectrum, the optical gap is identified. The fully isolated flat band in a van der Waals crystal provides a qualitatively new testbed for exploring flat-band physics.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Dispersionless electronic bands lead to an extremely high density of states and suppressed kinetic energy, thereby increasing electronic correlations and instabilities that can shape emergent ordered states, such as excitonic, ferromagnetic, and superconducting phases. A flat band that extends over the entire momentum space and is well isolated from other dispersive bands is, therefore, particularly interesting. Here, the band structure of the van der Waals crystal NbOCl2 is revealed by utilizing photoelectron momentum microscopy. We directly map out an electronic band that is flat throughout the entire Brillouin zone and features a width of only ~ 100 meV. This band is well isolated from both the conduction and remote valence bands. Moreover, the quasiparticle band gap shows a high tunability upon the deposition of cesium atoms on the surface. By combining the single-particle band structure with the optical transmission spectrum, the optical gap is identified. The fully isolated flat band in a van der Waals crystal provides a qualitatively new testbed for exploring flat-band physics. |
2025
|
| 36. | M. Theilen, S. Kaidisch, M. Stettner, S. Zajusch, E. Fackelman, A. Adamkiewicz, R. Wallauer, A. Windischbacher, C. S. Kern, M. G. Ramsey, F. C. Bocquet, S. Soubatch, F. S. Tautz, U. Höfer, P. Puschnig Observing the spatial and temporal evolution of exciton wave functions Journal Article Forthcoming In: arXiv:2511.23001 [cond-mat.mtrl-sci], Forthcoming. @article{Theilen2025,
title = {Observing the spatial and temporal evolution of exciton wave functions},
author = {M. Theilen and S. Kaidisch and M. Stettner and S. Zajusch and E. Fackelman and A. Adamkiewicz and R. Wallauer and A. Windischbacher and C. S. Kern and M. G. Ramsey and F. C. Bocquet and S. Soubatch and F. S. Tautz and U. Höfer and P. Puschnig},
url = {https://arxiv.org/abs/2511.23001},
doi = {10.48550/arXiv.2511.23001},
year = {2025},
date = {2025-11-28},
urldate = {2025-11-28},
journal = { arXiv:2511.23001 [cond-mat.mtrl-sci]},
abstract = {Excitons, the correlated electron-hole pairs governing optical and transport properties in organic semiconductors, have long resisted direct experimental access to their full quantum-mechanical wave functions. Here, we use femtosecond time-resolved photoemission orbital tomography (trPOT), combining high-harmonic probe pulses with time- and momentum-resolved photoelectron spectroscopy, to directly image the momentum-space distribution and ultrafast dynamics of excitons in -sexithiophene thin films. We introduce a quantitative model that enables reconstruction of the exciton wave function in real space, including both its spatial extent and its internal phase structure. The reconstructed wave function reveals coherent delocalization across approximately three molecular units and exhibits a characteristic phase modulation, consistent with ab initio calculations within the framework of many-body perturbation theory. Time-resolved measurements further show a % contraction of the exciton radius within 400 fs, providing direct evidence of self-trapping driven by exciton-phonon coupling. These results establish trPOT as a general and experimentally accessible approach for resolving exciton wave functions -- with spatial, phase, and temporal sensitivity -- in a broad class of molecular and low-dimensional materials. },
keywords = {},
pubstate = {forthcoming},
tppubtype = {article}
}
Excitons, the correlated electron-hole pairs governing optical and transport properties in organic semiconductors, have long resisted direct experimental access to their full quantum-mechanical wave functions. Here, we use femtosecond time-resolved photoemission orbital tomography (trPOT), combining high-harmonic probe pulses with time- and momentum-resolved photoelectron spectroscopy, to directly image the momentum-space distribution and ultrafast dynamics of excitons in -sexithiophene thin films. We introduce a quantitative model that enables reconstruction of the exciton wave function in real space, including both its spatial extent and its internal phase structure. The reconstructed wave function reveals coherent delocalization across approximately three molecular units and exhibits a characteristic phase modulation, consistent with ab initio calculations within the framework of many-body perturbation theory. Time-resolved measurements further show a % contraction of the exciton radius within 400 fs, providing direct evidence of self-trapping driven by exciton-phonon coupling. These results establish trPOT as a general and experimentally accessible approach for resolving exciton wave functions -- with spatial, phase, and temporal sensitivity -- in a broad class of molecular and low-dimensional materials. |
| 35. | S. Kaidisch, A. Kleiner, S. Refaely-Abramson, P. Puschnig, C. S. Kern Photoemission tomography of excitons in 2D systems: momentum-space signatures of correlated electron-hole wave functions Journal Article Forthcoming In: arXiv:2511.14956 [cond-mat.mtrl-sci], Forthcoming. @article{Kaidisch2025_arxiv,
title = {Photoemission tomography of excitons in 2D systems: momentum-space signatures of correlated electron-hole wave functions},
author = {S. Kaidisch and A. Kleiner and S. Refaely-Abramson and P. Puschnig and C. S. Kern},
url = {https://arxiv.org/abs/2511.14956},
doi = {10.48550/arXiv.2511.14956},
year = {2025},
date = {2025-11-18},
urldate = {2025-11-18},
journal = { arXiv:2511.14956 [cond-mat.mtrl-sci]},
abstract = {The momentum-space signatures of excitons can be experimentally accessed through time-resolved (pump-probe) photoelectron spectroscopy. In this work, we develop a computational framework for exciton photoemission orbital tomography (exPOT) in periodic systems, enabling the simulation and interpretation of experimental observables within many-body perturbation theory. By connecting the +Bethe-Salpeter Equation (BSE) approach to photoemission tomography, our formalism captures exciton photoemission in periodic systems, explicitly incorporating photoemission matrix element effects induced by the probe pulse. The correlated nature of electrons and holes introduces distinct consequences for excitonic photoemission, including a dependence on pump pulse polarization. Using the prototypical two-dimensional material hexagonal boron nitride, we demonstrate these effects and show how our framework extends to excitons with finite center-of-mass momentum, making it well-suited to studying momentum-dark excitons. This provides valuable insights into the microscopic nature of excitonic phenomena in quantum materials. },
keywords = {},
pubstate = {forthcoming},
tppubtype = {article}
}
The momentum-space signatures of excitons can be experimentally accessed through time-resolved (pump-probe) photoelectron spectroscopy. In this work, we develop a computational framework for exciton photoemission orbital tomography (exPOT) in periodic systems, enabling the simulation and interpretation of experimental observables within many-body perturbation theory. By connecting the +Bethe-Salpeter Equation (BSE) approach to photoemission tomography, our formalism captures exciton photoemission in periodic systems, explicitly incorporating photoemission matrix element effects induced by the probe pulse. The correlated nature of electrons and holes introduces distinct consequences for excitonic photoemission, including a dependence on pump pulse polarization. Using the prototypical two-dimensional material hexagonal boron nitride, we demonstrate these effects and show how our framework extends to excitons with finite center-of-mass momentum, making it well-suited to studying momentum-dark excitons. This provides valuable insights into the microscopic nature of excitonic phenomena in quantum materials. |
| 34. | W. Bennecke, I. Gonzalez Oliva, J. P. Bange, P. Werner, D. Schmitt, M. Merboldt, A. M. Seiler, K. Watanabe, T. Taniguchi, D. Steil, R. T. Weitz, P. Puschnig, C. Draxl, G. S. M. Jansen, M. Reutzel, S. Mathias Hybrid Frenkel–Wannier excitons facilitate ultrafast energy transfer at a 2D–organic interface Journal Article In: Nature Physics, vol. 21, pp. 1973–1980, 2025. @article{Bennecke2025,
title = {Hybrid Frenkel–Wannier excitons facilitate ultrafast energy transfer at a 2D–organic interface},
author = {W. Bennecke and I. Gonzalez Oliva and J. P. Bange and P. Werner and D. Schmitt and M. Merboldt and A. M. Seiler and K. Watanabe and T. Taniguchi and D. Steil and R. T. Weitz and P. Puschnig and C. Draxl and G. S. M. Jansen and M. Reutzel and S. Mathias },
url = {https://www.nature.com/articles/s41567-025-03075-5},
doi = {10.1038/s41567-025-03075-5},
year = {2025},
date = {2025-10-29},
journal = {Nature Physics},
volume = {21},
pages = {1973–1980},
abstract = {Two-dimensional transition metal dichalcogenides and organic semiconductors have emerged as promising material platforms for optoelectronic devices. Combining the two is predicted to yield emergent properties while retaining the advantages of each. In organic semiconductors, the optoelectronic response is typically dominated by localized Frenkel-type excitons, whereas transition metal dichalcogenides host delocalized Wannier-type excitons. However, much less is known about the characteristics of excitons at hybrid interfaces between these materials, which determine the possible energy- and charge-transfer pathways. Here we identify a hybrid exciton at one such interface using ultrafast momentum microscopy and many-body perturbation theory. We show that this hybrid exciton, formed predominantly via resonant Förster energy transfer, has both Frenkel- and Wannier-type contributions: intralayer electron–hole transitions within the organic semiconductor layer and interlayer transitions across the interface give rise to an exciton wavefunction with mixed character. This work advances our understanding of charge and energy transfer processes across 2D–organic heterostructures.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Two-dimensional transition metal dichalcogenides and organic semiconductors have emerged as promising material platforms for optoelectronic devices. Combining the two is predicted to yield emergent properties while retaining the advantages of each. In organic semiconductors, the optoelectronic response is typically dominated by localized Frenkel-type excitons, whereas transition metal dichalcogenides host delocalized Wannier-type excitons. However, much less is known about the characteristics of excitons at hybrid interfaces between these materials, which determine the possible energy- and charge-transfer pathways. Here we identify a hybrid exciton at one such interface using ultrafast momentum microscopy and many-body perturbation theory. We show that this hybrid exciton, formed predominantly via resonant Förster energy transfer, has both Frenkel- and Wannier-type contributions: intralayer electron–hole transitions within the organic semiconductor layer and interlayer transitions across the interface give rise to an exciton wavefunction with mixed character. This work advances our understanding of charge and energy transfer processes across 2D–organic heterostructures. |
| 33. | D. Brandstetter, S. Mearini, A. Windischbacher, Y. Y. Grisan Qiu, D. Baranowski, V. Feyer, C. M. Schneider, P. Puschnig Revealing the Character of Coordination Bonding in 2D Metal–Organic Frameworks Journal Article In: Advanced Science, vol. 12, iss. 47, no. e10414, 2025. @article{Brandstetter2025,
title = {Revealing the Character of Coordination Bonding in 2D Metal–Organic Frameworks},
author = {D. Brandstetter and S. Mearini and A. Windischbacher and Y. Y. Grisan Qiu and D. Baranowski and V. Feyer and C. M. Schneider and P. Puschnig},
url = {https://advanced.onlinelibrary.wiley.com/doi/10.1002/advs.202510414},
doi = {10.1002/advs.202510414},
year = {2025},
date = {2025-10-07},
journal = {Advanced Science},
volume = {12},
number = {e10414},
issue = {47},
abstract = {In this contribution, the coordination bond is investigated in a 2D metal–organic framework consisting of nickel and 7,7,8,8-tetracyanoquinodimethane (TCNQ) on a Ag(100) substrate. Using angle-resolved photoemission experiments supported by density functional theory calculations, the bonding is characterized as a result of the hybridisation between the ligand orbitals and the metal d-states. Unambiguous experimental fingerprints are presented for such a mechanism by revealing the splitting in energy of the frontier molecular orbitals into sets of bonding/antibonding states in the 2D metal–organic framework. Furthermore, a qualitative analysis of the energy level alignment is given for the transition metal inside the coordination environment and discuss the role of the network structure on the formation of such hybrid states.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
In this contribution, the coordination bond is investigated in a 2D metal–organic framework consisting of nickel and 7,7,8,8-tetracyanoquinodimethane (TCNQ) on a Ag(100) substrate. Using angle-resolved photoemission experiments supported by density functional theory calculations, the bonding is characterized as a result of the hybridisation between the ligand orbitals and the metal d-states. Unambiguous experimental fingerprints are presented for such a mechanism by revealing the splitting in energy of the frontier molecular orbitals into sets of bonding/antibonding states in the 2D metal–organic framework. Furthermore, a qualitative analysis of the energy level alignment is given for the transition metal inside the coordination environment and discuss the role of the network structure on the formation of such hybrid states. |
| 32. | J. Brandhoff, R. K. Berger, F. Otto, M. Schaal, L. Brill, O. T. Hofmann, P. Puschnig, T. Fritz, R. Forker When Aromaticity Falls Short in Molecule–Surface Interactions Journal Article In: The Journal of Physical Chemistry C, vol. 129, iss. 46, 2025. @article{Brandhoff2025,
title = {When Aromaticity Falls Short in Molecule–Surface Interactions},
author = {J. Brandhoff and R. K. Berger and F. Otto and M. Schaal and L. Brill and O. T. Hofmann and P. Puschnig and T. Fritz and R. Forker},
url = {https://pubs.acs.org/doi/full/10.1021/acs.jpcc.5c05441},
doi = {10.1021/acs.jpcc.5c05441},
year = {2025},
date = {2025-09-26},
urldate = {2025-09-26},
journal = {The Journal of Physical Chemistry C},
volume = {129},
issue = {46},
abstract = {Aromaticity is one of the most important concepts in organic chemistry. There are cases in which a molecule undergoes changes to increase its aromaticity. This higher aromaticity comes with an energetic gain and is commonly referred to as aromatic stabilization. Previously, it has been reported that some molecules undergo such a stabilization when adsorbing on a surface, which has been identified as the reason for charge transfer into the molecular π-system. Utilizing photoemission orbital tomography and density functional theory, we investigate changes in the molecular π-system upon adsorption and elucidate the influence on the aromaticity. We demonstrate how the energetic gain from an aromatic stabilization on surfaces can be outweighed by hybridization. Uncovering a mechanism in which the molecular π-system forms dative bonds with the surface, our study reveals that the concept of aromatic stabilization on surfaces has been incomplete so far.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Aromaticity is one of the most important concepts in organic chemistry. There are cases in which a molecule undergoes changes to increase its aromaticity. This higher aromaticity comes with an energetic gain and is commonly referred to as aromatic stabilization. Previously, it has been reported that some molecules undergo such a stabilization when adsorbing on a surface, which has been identified as the reason for charge transfer into the molecular π-system. Utilizing photoemission orbital tomography and density functional theory, we investigate changes in the molecular π-system upon adsorption and elucidate the influence on the aromaticity. We demonstrate how the energetic gain from an aromatic stabilization on surfaces can be outweighed by hybridization. Uncovering a mechanism in which the molecular π-system forms dative bonds with the surface, our study reveals that the concept of aromatic stabilization on surfaces has been incomplete so far. |
| 31. | C. S. Kern, X. Yang, G. Zamborlini, S. Mearini, M. Jugovac, V. Feyer, U. De Giovannini, A. Rubio, S. Soubatch, M. G. Ramsey, F. S. Tautz, P. Puschnig Circular dichroism in the photoelectron angular distribution of achiral molecules Journal Article Forthcoming In: arXiv:2507.12113 [cond-mat.mtrl-sci], Forthcoming. @article{Kern2025,
title = {Circular dichroism in the photoelectron angular distribution of achiral molecules},
author = {C. S. Kern and X. Yang and G. Zamborlini and S. Mearini and M. Jugovac and V. Feyer and U. De Giovannini and A. Rubio and S. Soubatch and M. G. Ramsey and F. S. Tautz and P. Puschnig},
url = {https://arxiv.org/abs/2507.12113},
doi = {10.48550/arXiv.2507.12113},
year = {2025},
date = {2025-07-16},
urldate = {2025-07-16},
journal = {arXiv:2507.12113 [cond-mat.mtrl-sci]},
keywords = {},
pubstate = {forthcoming},
tppubtype = {article}
}
|
| 30. | M. Zirwick, N. Kainbacher, J. B. Bauer, M. S. Wagner, P. Puschnig, T. Chassé, H. F. Bettinger, H. Peisert Highly Ordered Single Domain Peri-Tetracene Monolayers on Ag(110) Journal Article In: The Journal of Physical Chemistry C, vol. 129, iss. 17, pp. 8447–8454, 2025. @article{Zirwick2025,
title = {Highly Ordered Single Domain Peri-Tetracene Monolayers on Ag(110)},
author = {M. Zirwick and N. Kainbacher and J. B. Bauer and M. S. Wagner and P. Puschnig and T. Chassé and H. F. Bettinger and H. Peisert},
url = {https://pubs.acs.org/doi/10.1021/acs.jpcc.5c01482},
doi = {10.1021/acs.jpcc.5c01482},
year = {2025},
date = {2025-04-15},
urldate = {2025-04-15},
journal = {The Journal of Physical Chemistry C},
volume = {129},
issue = {17},
pages = {8447–8454},
abstract = {The on-surface reaction of 1,1’-bitetracene (Bi4A) to peri-tetracene (tetrabenzo[bc,ef,kl,no]coronene) (4-PA) on Cu(110) and Ag(110) is studied by photoemission, scanning tunneling microscopy (STM) and low energy electron diffraction (LEED). Density functional theory (DFT) computations suggest that the Ag(110) substrate is well suited for the formation of large-area 4-PA monolayers with a preferential adsorption alignment of 4-PA molecules along the [11̅0] direction. The experiments confirm the formation of 4-PA and presence of large highly ordered 4-PA domains. Two distinct phases emerge, growing seamlessly over large areas and even spanning step edges. Evidence for charge transfer from the substrate to the molecule was found, resulting in a filling of the lowest unoccupied molecular orbital (LUMO) of 4-PA.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
The on-surface reaction of 1,1’-bitetracene (Bi4A) to peri-tetracene (tetrabenzo[bc,ef,kl,no]coronene) (4-PA) on Cu(110) and Ag(110) is studied by photoemission, scanning tunneling microscopy (STM) and low energy electron diffraction (LEED). Density functional theory (DFT) computations suggest that the Ag(110) substrate is well suited for the formation of large-area 4-PA monolayers with a preferential adsorption alignment of 4-PA molecules along the [11̅0] direction. The experiments confirm the formation of 4-PA and presence of large highly ordered 4-PA domains. Two distinct phases emerge, growing seamlessly over large areas and even spanning step edges. Evidence for charge transfer from the substrate to the molecule was found, resulting in a filling of the lowest unoccupied molecular orbital (LUMO) of 4-PA. |
| 29. | A. Haags, D. Brandstetter, X. Yang, L. Egger, H. Kirschner, A. Gottwald, M. Richter, G. Koller, F. C. Bocquet, C. Wagner, M. G. Ramsey, S. Soubatch, P. Puschnig, F. S. Tautz Tomographic identification of all molecular orbitals in a wide binding-energy range Journal Article In: Phys. Rev. B, vol. 111, no. 16, 2025, ISSN: 2469-9969. @article{Haags2025b,
title = {Tomographic identification of all molecular orbitals in a wide binding-energy range},
author = {A. Haags and D. Brandstetter and X. Yang and L. Egger and H. Kirschner and A. Gottwald and M. Richter and G. Koller and F. C. Bocquet and C. Wagner and M. G. Ramsey and S. Soubatch and P. Puschnig and F. S. Tautz},
doi = {10.1103/physrevb.111.165402},
issn = {2469-9969},
year = {2025},
date = {2025-04-00},
urldate = {2025-04-00},
journal = {Phys. Rev. B},
volume = {111},
number = {16},
publisher = {American Physical Society (APS)},
abstract = {<jats:p>In the past decade, photoemission orbital tomography (POT) has evolved into a powerful tool to investigate the electronic structure of organic molecules adsorbed on surfaces. Here we show that POT allows for the comprehensive experimental identification of all molecular orbitals in a substantial binding energy range of more than 10 eV. Making use of the angular distribution of photoelectrons as a function of binding-energy, we exemplify this by extracting an orbital-resolved projected density of states for 15 <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mi>π</a:mi></a:math> and 23 <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:mi>σ</b:mi></b:math> orbitals from the experimental data of the prototypical organic molecule bisanthene (<c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:mrow><c:msub><c:mi mathvariant="normal">C</c:mi><c:mn>28</c:mn></c:msub><c:msub><c:mi mathvariant="normal">H</c:mi><c:mn>14</c:mn></c:msub></c:mrow></c:math>) on a Cu(110) surface. These experimental results for an essentially complete set of orbitals within the given binding-energy range serve as stringent benchmarks for electronic structure methods, which we illustrate by performing density functional calculations employing four frequently used exchange-correlation functionals. By computing the respective molecular-orbital-projected densities of states, a one-to-one comparison with experimental data for an unprecedented number of 38 orbital energies became possible. The quantitative analysis of our data reveals that the range-separated hybrid functional HSE performs best for the investigated organic/metal interface. At a more fundamental level, the remarkable agreement between the experimental and the Kohn-Sham orbital energies over a binding-energy range larger than 10 eV suggests that—perhaps unexpectedly—Kohn-Sham orbitals approximate Dyson orbitals, which would rigorously account for the electron extraction process in photoemission spectroscopy but are notoriously difficult to compute, in a much better way than previously thought.</jats:p>
<jats:sec>
<jats:title/>
<jats:supplementary-material>
<jats:permissions>
<jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement>
<jats:copyright-year>2025</jats:copyright-year>
</jats:permissions>
</jats:supplementary-material>
</jats:sec>},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
<jats:p>In the past decade, photoemission orbital tomography (POT) has evolved into a powerful tool to investigate the electronic structure of organic molecules adsorbed on surfaces. Here we show that POT allows for the comprehensive experimental identification of all molecular orbitals in a substantial binding energy range of more than 10 eV. Making use of the angular distribution of photoelectrons as a function of binding-energy, we exemplify this by extracting an orbital-resolved projected density of states for 15 <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mi>π</a:mi></a:math> and 23 <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:mi>σ</b:mi></b:math> orbitals from the experimental data of the prototypical organic molecule bisanthene (<c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:mrow><c:msub><c:mi mathvariant="normal">C</c:mi><c:mn>28</c:mn></c:msub><c:msub><c:mi mathvariant="normal">H</c:mi><c:mn>14</c:mn></c:msub></c:mrow></c:math>) on a Cu(110) surface. These experimental results for an essentially complete set of orbitals within the given binding-energy range serve as stringent benchmarks for electronic structure methods, which we illustrate by performing density functional calculations employing four frequently used exchange-correlation functionals. By computing the respective molecular-orbital-projected densities of states, a one-to-one comparison with experimental data for an unprecedented number of 38 orbital energies became possible. The quantitative analysis of our data reveals that the range-separated hybrid functional HSE performs best for the investigated organic/metal interface. At a more fundamental level, the remarkable agreement between the experimental and the Kohn-Sham orbital energies over a binding-energy range larger than 10 eV suggests that—perhaps unexpectedly—Kohn-Sham orbitals approximate Dyson orbitals, which would rigorously account for the electron extraction process in photoemission spectroscopy but are notoriously difficult to compute, in a much better way than previously thought.</jats:p>
<jats:sec>
<jats:title/>
<jats:supplementary-material>
<jats:permissions>
<jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement>
<jats:copyright-year>2025</jats:copyright-year>
</jats:permissions>
</jats:supplementary-material>
</jats:sec> |
| 28. | S. Mearini, D. Brandstetter, Y. Y. Grisan Qiu, D. Baranowski, I. Cojocariu, M. Jugovac, P. Gargiani, M. Valvidares, L. Schio, L. Floreano, A. Windischbacher, P. Puschnig, V. Feyer, C. M. Schneider Substrate Stabilized Charge Transfer Scheme In Coverage Controlled 2D Metal Organic Frameworks Journal Article In: Small, vol. 2500507, 2025. @article{Mearini2025,
title = {Substrate Stabilized Charge Transfer Scheme In Coverage Controlled 2D Metal Organic Frameworks},
author = {S. Mearini and D. Brandstetter and Y. Y. Grisan Qiu and D. Baranowski and I. Cojocariu and M. Jugovac and P. Gargiani and M. Valvidares and L. Schio and L. Floreano and A. Windischbacher and P. Puschnig and V. Feyer and C. M. Schneider},
url = {https://onlinelibrary.wiley.com/doi/10.1002/smll.202500507?af=R},
doi = {10.1002/smll.202500507},
year = {2025},
date = {2025-02-17},
urldate = {2025-02-17},
journal = {Small},
volume = {2500507},
abstract = {Recently, 2D metal-organic frameworks (2D MOFs), characterized by complexcharge transfer mechanisms, have emerged as a promising class of networksin the development of advanced materials with tailored electronic andmagnetic properties. Following the successful synthesis of a 2D MOF formedby nickel (Ni) linkers and 7,7,8,8-tetracyanoquinodimethane (TCNQ) ligands,this work investigates how the Ni-to-ligand ratio influences the electroniccharge redistribution in an Ag(100)-supported 2D MOF. The interplaybetween linker-ligand and substrate-MOF charge transfer processes leads to astable equilibrium, resulting in a robust electronic structure that remainsindependent of stoichiometric ratios. This stability is primarily based on theelectron transfer from the metal substrate, which compensates for chargeimbalances introduced by the metal-organic coordination across differentMOF configurations. Despite minor changes observed in the magneticresponse of the Ni centers, these findings emphasize the robustness of theelectronic structure, which remains largely unaffected by structural variations,highlighting the potential of these 2D MOFs for advanced applications inelectronics and spintronics.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Recently, 2D metal-organic frameworks (2D MOFs), characterized by complexcharge transfer mechanisms, have emerged as a promising class of networksin the development of advanced materials with tailored electronic andmagnetic properties. Following the successful synthesis of a 2D MOF formedby nickel (Ni) linkers and 7,7,8,8-tetracyanoquinodimethane (TCNQ) ligands,this work investigates how the Ni-to-ligand ratio influences the electroniccharge redistribution in an Ag(100)-supported 2D MOF. The interplaybetween linker-ligand and substrate-MOF charge transfer processes leads to astable equilibrium, resulting in a robust electronic structure that remainsindependent of stoichiometric ratios. This stability is primarily based on theelectron transfer from the metal substrate, which compensates for chargeimbalances introduced by the metal-organic coordination across differentMOF configurations. Despite minor changes observed in the magneticresponse of the Ni centers, these findings emphasize the robustness of theelectronic structure, which remains largely unaffected by structural variations,highlighting the potential of these 2D MOFs for advanced applications inelectronics and spintronics. |
| 27. | Y. Nakayama, F. C. Bocquet, R. Tsuruta, S. Soubatch, F. S. Tautz Anisotropic dispersion of excitonic bands of the single-crystal pentacene (001) surface as measured by low-energy angle-resolved high-resolution electron energy-loss spectroscopy Journal Article In: Journal of Electron Spectroscopy and Related Phenomena, vol. 279, iss. 147514, 2025. @article{Nakayama2025b,
title = {Anisotropic dispersion of excitonic bands of the single-crystal pentacene (001) surface as measured by low-energy angle-resolved high-resolution electron energy-loss spectroscopy},
author = {Y. Nakayama and F. C. Bocquet and R. Tsuruta and S. Soubatch and F. S. Tautz},
url = {https://www.sciencedirect.com/science/article/pii/S0368204825000015},
doi = {10.1016/j.elspec.2025.147514},
year = {2025},
date = {2025-01-31},
journal = {Journal of Electron Spectroscopy and Related Phenomena},
volume = {279},
issue = {147514},
abstract = {Low-energy high-resolution electron energy-loss spectroscopy (HREELS) is a useful technique for the charac-
terization of various excitation processes at solid surfaces. However, no successful work has been reported on
molecular single-crystal samples yet. In the present study, low-energy angle-resolved HREELS measurements
were conducted on single-crystal pentacene, an organic semiconductor. The results confirmed the excitonic
bands exhibiting energy–momentum dispersion and anisotropy of these depending on the surface crystallo-
graphic directions, corroborating the occurrence of exciton delocalization, contrary to the ordinary notion of the
Frenkel exciton for weakly interacting van der Waals molecular solids. The present results demonstrate that low-
energy angle-resolved HREELS is applicable to the precise examination of the excitonic characteristics of solid-
state surfaces, even for molecular semiconductor single crystals.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Low-energy high-resolution electron energy-loss spectroscopy (HREELS) is a useful technique for the charac-
terization of various excitation processes at solid surfaces. However, no successful work has been reported on
molecular single-crystal samples yet. In the present study, low-energy angle-resolved HREELS measurements
were conducted on single-crystal pentacene, an organic semiconductor. The results confirmed the excitonic
bands exhibiting energy–momentum dispersion and anisotropy of these depending on the surface crystallo-
graphic directions, corroborating the occurrence of exciton delocalization, contrary to the ordinary notion of the
Frenkel exciton for weakly interacting van der Waals molecular solids. The present results demonstrate that low-
energy angle-resolved HREELS is applicable to the precise examination of the excitonic characteristics of solid-
state surfaces, even for molecular semiconductor single crystals. |
| 26. | Y. Y. Grisan Qiu, D. Brandstetter, S. Mearini, D. Baranowski, I. Cojocariu, M. Jugovac, G. Zamborlini, P. Gargiani, M. Valvidares, A. Windischbacher, P. Puschnig, V. Feyer, C. M. Schneider Conformation-Driven Nickel Redox States and Magnetism in 2D Metal–organic Frameworks Journal Article In: Adv. Funct. Mater., vol. 2418186, 2025. @article{Qiu2025,
title = {Conformation-Driven Nickel Redox States and Magnetism in 2D Metal–organic Frameworks},
author = {Y. Y. Grisan Qiu and D. Brandstetter and S. Mearini and D. Baranowski and I. Cojocariu and M. Jugovac and G. Zamborlini and P. Gargiani and M. Valvidares and A. Windischbacher and P. Puschnig and V. Feyer and C. M. Schneider},
url = {https://advanced.onlinelibrary.wiley.com/doi/10.1002/adfm.202418186?af=R},
doi = {10.1002/adfm.202418186},
year = {2025},
date = {2025-01-29},
urldate = {2025-01-29},
journal = {Adv. Funct. Mater.},
volume = {2418186},
abstract = {2D metal–organic frameworks (2D MOFs) attract considerable attention because of their versatile properties and as potential candidates for single-atom catalysis, high-density information storage media or molecular electronics and spintronics devices. Their unique characteristics arise from an intricate interplay between the metal center, the surrounding ligands and the underlying substrate. Here, the intrinsic magnetic and electronic properties of a single-layer MOF on graphene is investigated with a combination of spectroscopic techniques and theoretical modeling. Taking advantage of the weak interaction between the MOF and graphene substrate, it is specifically focused on the influence of the coordination environment on these properties. Notably, two distinct coordination configurations are observed for the transition metal centers within the 2D MOF, and clarify how axial distortions in the ligand field affect the hybridization between the Ni 3d states and the π-symmetric molecular orbitals of 7,7,8,8-tetracyanoquinodimethane ligands, leading to the coexistence of two Ni redox states with different spin configurations. Furthermore, the transition from a nearly free-standing MOF is examined to metal-supported frameworks, elucidating the impact of substrate interactions on the electronic and magnetic properties. The findings advance the understanding of MOFs and offer insights into developing functional materials with tailored magnetic and electronic properties.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
2D metal–organic frameworks (2D MOFs) attract considerable attention because of their versatile properties and as potential candidates for single-atom catalysis, high-density information storage media or molecular electronics and spintronics devices. Their unique characteristics arise from an intricate interplay between the metal center, the surrounding ligands and the underlying substrate. Here, the intrinsic magnetic and electronic properties of a single-layer MOF on graphene is investigated with a combination of spectroscopic techniques and theoretical modeling. Taking advantage of the weak interaction between the MOF and graphene substrate, it is specifically focused on the influence of the coordination environment on these properties. Notably, two distinct coordination configurations are observed for the transition metal centers within the 2D MOF, and clarify how axial distortions in the ligand field affect the hybridization between the Ni 3d states and the π-symmetric molecular orbitals of 7,7,8,8-tetracyanoquinodimethane ligands, leading to the coexistence of two Ni redox states with different spin configurations. Furthermore, the transition from a nearly free-standing MOF is examined to metal-supported frameworks, elucidating the impact of substrate interactions on the electronic and magnetic properties. The findings advance the understanding of MOFs and offer insights into developing functional materials with tailored magnetic and electronic properties. |
| 25. | A. Haags, D. Brandstetter, X. Yang, L. Egger, H. Kirschner, A. Gottwald, M. Richter, G. Koller, F. C. Bocquet, C. Wagner, M. G. Ramsey, S. Soubatch, P. Puschnig, F. S. Tautz Tomographic identification of all molecular orbitals in a wide binding energy range Journal Article Forthcoming In: ArXiv, Forthcoming. @article{Haags2025,
title = {Tomographic identification of all molecular orbitals in a wide binding energy range},
author = {A. Haags and D. Brandstetter and X. Yang and L. Egger and H. Kirschner and A. Gottwald and M. Richter and G. Koller and F. C. Bocquet and C. Wagner and M. G. Ramsey and S. Soubatch and P. Puschnig and F. S. Tautz},
url = {https://arxiv.org/abs/2501.05287},
year = {2025},
date = {2025-01-09},
urldate = {2025-01-09},
journal = {ArXiv},
abstract = {In the past decade, photoemission orbital tomography (POT) has evolved into a powerful tool to investigate the electronic structure of organic molecules adsorbed on surfaces. Here we show that POT allows for the comprehensive experimental identification of all molecular orbitals in a substantial binding energy range, in the present case more than 10 eV. Making use of the angular distribution of photoelectrons as a function of binding energy, we exemplify this by extracting orbital-resolved partial densities of states (pDOS) for 15 π and 23 σ orbitals from the experimental photoemission intensities of the prototypical organic molecule bisanthene (C28H14) on a Cu(110) surface. In their entirety, these experimentally measured orbital-resolved pDOS for an essentially complete set of orbitals serve as a stringent benchmark for electronic structure methods, which we illustrate by performing density functional theory (DFT) calculations employing four frequently-used exchange-correlation functionals. By computing the respective molecular-orbital-projected densities of states of the bisanthene/Cu(110) interface, a one-to-one comparison with experimental data for an unprecedented number of 38 orbital energies becomes possible. The quantitative analysis of our data reveals that the range-separated hybrid functional HSE performs best for the investigated organic/metal interface. At a more fundamental level, the remarkable agreement between the experimental and the Kohn-Sham orbital energies over a binding energy range larger than 10,eV suggests that -- perhaps unexpectedly -- Kohn-Sham orbitals approximate Dyson orbitals, which would rigorously account for the electron extraction process in photoemission spectroscopy but are notoriously difficult to compute, in a much better way than previously thought. },
keywords = {},
pubstate = {forthcoming},
tppubtype = {article}
}
In the past decade, photoemission orbital tomography (POT) has evolved into a powerful tool to investigate the electronic structure of organic molecules adsorbed on surfaces. Here we show that POT allows for the comprehensive experimental identification of all molecular orbitals in a substantial binding energy range, in the present case more than 10 eV. Making use of the angular distribution of photoelectrons as a function of binding energy, we exemplify this by extracting orbital-resolved partial densities of states (pDOS) for 15 π and 23 σ orbitals from the experimental photoemission intensities of the prototypical organic molecule bisanthene (C28H14) on a Cu(110) surface. In their entirety, these experimentally measured orbital-resolved pDOS for an essentially complete set of orbitals serve as a stringent benchmark for electronic structure methods, which we illustrate by performing density functional theory (DFT) calculations employing four frequently-used exchange-correlation functionals. By computing the respective molecular-orbital-projected densities of states of the bisanthene/Cu(110) interface, a one-to-one comparison with experimental data for an unprecedented number of 38 orbital energies becomes possible. The quantitative analysis of our data reveals that the range-separated hybrid functional HSE performs best for the investigated organic/metal interface. At a more fundamental level, the remarkable agreement between the experimental and the Kohn-Sham orbital energies over a binding energy range larger than 10,eV suggests that -- perhaps unexpectedly -- Kohn-Sham orbitals approximate Dyson orbitals, which would rigorously account for the electron extraction process in photoemission spectroscopy but are notoriously difficult to compute, in a much better way than previously thought. |
| 24. | P. Hurdax, M. Hollerer, C. S. Kern, P. Puschnig, M. Sterrer, M. G. Ramsey Integer Charge Transfer Model–PTCDA on MgO(001)/Ag(001) Probing the Transition from Single to Double Integer Charge Transfer Journal Article In: J. Phys. Chem. C, vol. 129, iss. 2, pp. 1553–1561, 2025, ISSN: 1932-7455. @article{Hurdax2025,
title = {Integer Charge Transfer Model–PTCDA on MgO(001)/Ag(001) Probing the Transition from Single to Double Integer Charge Transfer},
author = {P. Hurdax and M. Hollerer and C. S. Kern and P. Puschnig and M. Sterrer and M. G. Ramsey},
url = {https://pubs.acs.org/doi/10.1021/acs.jpcc.4c08104},
doi = {10.1021/acs.jpcc.4c08104},
issn = {1932-7455},
year = {2025},
date = {2025-01-08},
urldate = {2025-01-08},
journal = {J. Phys. Chem. C},
volume = {129},
issue = {2},
pages = {1553--1561},
publisher = {American Chemical Society (ACS)},
abstract = {For weakly interacting adsorbate/substrate systems, the integer charge transfer (ICT) model describes how charge transfer across interfaces depends on the substrate work function. In particular, work function regimes where no charge transfer occurs (vacuum level alignment) can be distinguished from regions where integer charge transfer by electron tunneling from substrate to adsorbate or vice versa takes place (Fermi level pinning). While the formation of singly integer charged molecular anions and cations of organic semiconductors on various substrates has been well described by this model, the double integer charging regime has so far remained unexplored and experimentally elusive. Here, we extend the integer charge transfer model to the transition from single to double integer charging. This was made possible by combining a molecular adsorbate with high electron affinity (Perylenetetracarboxylic-dianhydride (PTCDA)) with a substrate with tunable work function (ultrathin MgO(001) films on Ag(001)). Our results, obtained with scanning tunneling microscopy (STM), photoemission spectroscopy (PES), work function measurements and density function theory (DFT) calculations, show that after completing the single negative charging of all molecules in a PTCDA monolayer in the first Fermi level pinning regime, the system transitions to a vacuum level alignment regime for singly charged molecules when the substrate work function is reduced, and finally enters the second Fermi level pinning regime at very low substrate work function, in which the molecules become doubly negatively charged.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
For weakly interacting adsorbate/substrate systems, the integer charge transfer (ICT) model describes how charge transfer across interfaces depends on the substrate work function. In particular, work function regimes where no charge transfer occurs (vacuum level alignment) can be distinguished from regions where integer charge transfer by electron tunneling from substrate to adsorbate or vice versa takes place (Fermi level pinning). While the formation of singly integer charged molecular anions and cations of organic semiconductors on various substrates has been well described by this model, the double integer charging regime has so far remained unexplored and experimentally elusive. Here, we extend the integer charge transfer model to the transition from single to double integer charging. This was made possible by combining a molecular adsorbate with high electron affinity (Perylenetetracarboxylic-dianhydride (PTCDA)) with a substrate with tunable work function (ultrathin MgO(001) films on Ag(001)). Our results, obtained with scanning tunneling microscopy (STM), photoemission spectroscopy (PES), work function measurements and density function theory (DFT) calculations, show that after completing the single negative charging of all molecules in a PTCDA monolayer in the first Fermi level pinning regime, the system transitions to a vacuum level alignment regime for singly charged molecules when the substrate work function is reduced, and finally enters the second Fermi level pinning regime at very low substrate work function, in which the molecules become doubly negatively charged. |
2024
|
| 23. | M. Aeschlimann, J. P. Bange, M. Bauer, U. Bovensiepen, H.-J. Elmers, T. Fauster, L. Gierster, U. Höfer, R. Huber, A. Li, X. Li, S. Mathias, K. Morgenstern, H. Petek, M. Reutzel, K. Rossnagel, G. Schönhense, M. Scholz, B. Stadtmüller, J. Stähler, S. Tan, B. Wang, Z. Wang, M. Weinelt Time-resolved photoelectron spectroscopy at surfaces Journal Article In: Surface Science, vol. 753, iss. 122631, 2024. @article{Aeschlimann2025,
title = {Time-resolved photoelectron spectroscopy at surfaces},
author = {M. Aeschlimann and J. P. Bange and M. Bauer and U. Bovensiepen and H.-J. Elmers and T. Fauster and L. Gierster and U. Höfer and R. Huber and A. Li and X. Li and S. Mathias and K. Morgenstern and H. Petek and M. Reutzel and K. Rossnagel and G. Schönhense and M. Scholz and B. Stadtmüller and J. Stähler and S. Tan and B. Wang and Z. Wang and M. Weinelt},
url = {https://www.sciencedirect.com/science/article/pii/S0039602824001821},
doi = {10.1016/j.susc.2024.122631},
year = {2024},
date = {2024-11-26},
journal = {Surface Science},
volume = {753},
issue = {122631},
abstract = {Light is a preeminent spectroscopic tool for investigating the electronic structure of surfaces. Time-resolved photoelectron spectroscopy has mainly been developed in the last 30 years. It is therefore not surprising that the topic was hardly mentioned in the issue on “The first thirty years” of surface science. In the second thirty years, however, we have seen tremendous progress in the development of time-resolved photoelectron spectroscopy on surfaces. Femtosecond light pulses and advanced photoelectron detection schemes are increasingly being used to study the electronic structure and dynamics of occupied and unoccupied electronic states and dynamic processes such as the energy and momentum relaxation of electrons, charge transfer at interfaces and collective processes such as plasmonic excitation and optical field screening. Using spin- and time-resolved photoelectron spectroscopy, we were able to study ultrafast spin dynamics, electron–magnon scattering and spin structures in magnetic and topological materials. Light also provides photon energy as well as electric and magnetic fields that can influence molecular surface processes to steer surface photochemistry and hot-electron-driven catalysis. In addition, we can consider light as a chemical reagent that can alter the properties of matter by creating non-equilibrium states and ultrafast phase transitions in correlated materials through the coupling of electrons, phonons and spins. Electric fields have also been used to temporarily change the electronic structure. This opened up new methods and areas such as high harmonic generation, light wave electronics and attosecond physics. This overview certainly cannot cover all these interesting topics. But also as a testimony to the cohesion and constructive exchange in our ultrafast community, a number of colleagues have come together to share their expertise and views on the very vital field of dynamics at surfaces. Following the introduction, the interested reader will find a list of contributions and a brief summary in Section 1.3.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Light is a preeminent spectroscopic tool for investigating the electronic structure of surfaces. Time-resolved photoelectron spectroscopy has mainly been developed in the last 30 years. It is therefore not surprising that the topic was hardly mentioned in the issue on “The first thirty years” of surface science. In the second thirty years, however, we have seen tremendous progress in the development of time-resolved photoelectron spectroscopy on surfaces. Femtosecond light pulses and advanced photoelectron detection schemes are increasingly being used to study the electronic structure and dynamics of occupied and unoccupied electronic states and dynamic processes such as the energy and momentum relaxation of electrons, charge transfer at interfaces and collective processes such as plasmonic excitation and optical field screening. Using spin- and time-resolved photoelectron spectroscopy, we were able to study ultrafast spin dynamics, electron–magnon scattering and spin structures in magnetic and topological materials. Light also provides photon energy as well as electric and magnetic fields that can influence molecular surface processes to steer surface photochemistry and hot-electron-driven catalysis. In addition, we can consider light as a chemical reagent that can alter the properties of matter by creating non-equilibrium states and ultrafast phase transitions in correlated materials through the coupling of electrons, phonons and spins. Electric fields have also been used to temporarily change the electronic structure. This opened up new methods and areas such as high harmonic generation, light wave electronics and attosecond physics. This overview certainly cannot cover all these interesting topics. But also as a testimony to the cohesion and constructive exchange in our ultrafast community, a number of colleagues have come together to share their expertise and views on the very vital field of dynamics at surfaces. Following the introduction, the interested reader will find a list of contributions and a brief summary in Section 1.3. |
| 22. | S. Mearini, D. Baranowski, D. Brandstetter, A. Windischbacher, I. Cojocariu, P. Gargiani, M. Valvidares, L. Schio, L. Floreano, P. Puschnig, V. Feyer, C. M. Schneider Band Structure Engineering in 2D Metal–Organic Frameworks Journal Article In: Advanced Science, vol. 11, iss. 38, no. 2404667, 2024. @article{Mearini2024,
title = {Band Structure Engineering in 2D Metal–Organic Frameworks},
author = {S. Mearini and D. Baranowski and D. Brandstetter and A. Windischbacher and I. Cojocariu and P. Gargiani and M. Valvidares and L. Schio and L. Floreano and P. Puschnig and V. Feyer and C. M. Schneider},
url = {https://onlinelibrary.wiley.com/doi/10.1002/advs.202404667},
doi = {10.1002/advs.202404667},
year = {2024},
date = {2024-08-09},
urldate = {2024-08-09},
journal = {Advanced Science},
volume = {11},
number = {2404667},
issue = {38},
abstract = {The design of 2D metal–organic frameworks (2D MOFs) takes advantage ofthe combination of the diverse electronic properties of simple organic ligandswith different transition metal (TM) centers. The strong directional nature ofthe coordinative bonds is the basis for the structural stability and the periodicarrangement of the TM cores in these architectures. Here, direct and clearevidence that 2D MOFs exhibit intriguing energy-dispersive electronic bandswith a hybrid character and distinct magnetic properties in the metal cores,resulting from the interactions between the TM electronic levels and theorganic ligand 𝝅-molecular orbitals, is reported. Importantly, a method toeffectively tune both the electronic structure of 2D MOFs and the magneticproperties of the metal cores by exploiting the electronic structure of distinctTMs is presented. Consequently, the ionization potential characteristic ofselected TMs, particularly the relative energy position and symmetry of the 3dstates, can be used to strategically engineer bands within specificmetal–organic frameworks. These findings not only provide a rationale forband structure engineering in 2D MOFs but also offer promisingopportunities for advanced material design.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
The design of 2D metal–organic frameworks (2D MOFs) takes advantage ofthe combination of the diverse electronic properties of simple organic ligandswith different transition metal (TM) centers. The strong directional nature ofthe coordinative bonds is the basis for the structural stability and the periodicarrangement of the TM cores in these architectures. Here, direct and clearevidence that 2D MOFs exhibit intriguing energy-dispersive electronic bandswith a hybrid character and distinct magnetic properties in the metal cores,resulting from the interactions between the TM electronic levels and theorganic ligand 𝝅-molecular orbitals, is reported. Importantly, a method toeffectively tune both the electronic structure of 2D MOFs and the magneticproperties of the metal cores by exploiting the electronic structure of distinctTMs is presented. Consequently, the ionization potential characteristic ofselected TMs, particularly the relative energy position and symmetry of the 3dstates, can be used to strategically engineer bands within specificmetal–organic frameworks. These findings not only provide a rationale forband structure engineering in 2D MOFs but also offer promisingopportunities for advanced material design. |
| 21. | D. Baranowski, M. Thaler, D. Brandstetter, A. Windischbacher, I. Cojocariu, S. Mearini, V. Chesnyak, L. Schio, L. Floreano, C. Gutiérrez Bolaños, P. Puschnig, L. L. Patera, V. Feyer, C. M. Schneider Emergence of Band Structure in a Two- Dimensional Metal−Organic Framework upon Hierarchical Self-Assembly Journal Article In: ACS Nano, vol. 18, pp. 19618−19627, 2024. @article{nokey,
title = {Emergence of Band Structure in a Two- Dimensional Metal−Organic Framework upon Hierarchical Self-Assembly},
author = {D. Baranowski and M. Thaler and D. Brandstetter and A. Windischbacher and I. Cojocariu and S. Mearini and V. Chesnyak and L. Schio and L. Floreano and C. Gutiérrez Bolaños and P. Puschnig and L. L. Patera and V. Feyer and C. M. Schneider},
url = {https://pubs.acs.org/doi/10.1021/acsnano.4c04191#},
doi = {10.1021/acsnano.4c04191},
year = {2024},
date = {2024-07-17},
urldate = {2024-07-17},
journal = {ACS Nano},
volume = {18},
pages = {19618−19627},
abstract = {Two-dimensional metal−organic frameworks (2D-MOFs) represent a category of atomically thin materials that combine the structural tunability of molecular systems with the crystalline structure characteristic of solids. The strong bonding between the organic linkers and transition metal centers is expected to result in delocalized electronic states. However, it remains largely unknown how the band structure in 2D-MOFs emerges through the coupling of electronic states in the building blocks. Here, we demonstrate the on-surface synthesis of a 2D-MOF exhibiting prominent π-conjugation. Through a combined experimental and theoretical approach, we provide direct evidence of band structure formation upon hierarchical self-assembly, going from metal−organic complexes to a conjugated two-dimensional framework. Additionally, we identify the robustly dispersive nature of the emerging hybrid states, irrespective of the metallic support type, highlighting the tunability of the band structure through charge transfer from the substrate. Our findings encourage the exploration of band-structure engineering in 2D-MOFs for potential applications in electronics and photonics.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Two-dimensional metal−organic frameworks (2D-MOFs) represent a category of atomically thin materials that combine the structural tunability of molecular systems with the crystalline structure characteristic of solids. The strong bonding between the organic linkers and transition metal centers is expected to result in delocalized electronic states. However, it remains largely unknown how the band structure in 2D-MOFs emerges through the coupling of electronic states in the building blocks. Here, we demonstrate the on-surface synthesis of a 2D-MOF exhibiting prominent π-conjugation. Through a combined experimental and theoretical approach, we provide direct evidence of band structure formation upon hierarchical self-assembly, going from metal−organic complexes to a conjugated two-dimensional framework. Additionally, we identify the robustly dispersive nature of the emerging hybrid states, irrespective of the metallic support type, highlighting the tunability of the band structure through charge transfer from the substrate. Our findings encourage the exploration of band-structure engineering in 2D-MOFs for potential applications in electronics and photonics. |
| 20. | W. Bennecke, A. Windischbacher, D. Schmitt, J. P. Bange, R. Hemm, C. S. Kern, G. D’Avino, X. Blase, D. Steil, S. Steil, M. Aeschlimann, B. Stadtmüller, M. Reutzel, P. Puschnig, G. S. M. Jansen, S. Mathias Disentangling the multiorbital contributions of excitons by photoemission exciton tomography Journal Article In: Nature Communications, vol. 15, no. 1804, pp. 10, 2024. @article{Bennecke2024,
title = {Disentangling the multiorbital contributions of excitons by photoemission exciton tomography},
author = {W. Bennecke and A. Windischbacher and D. Schmitt and J. P. Bange and R. Hemm and C. S. Kern and G. D’Avino and X. Blase and D. Steil and S. Steil and M. Aeschlimann and B. Stadtmüller and M. Reutzel and P. Puschnig and G. S. M. Jansen and S. Mathias},
url = {https://www.nature.com/articles/s41467-024-45973-x},
doi = {10.1038/s41467-024-45973-x},
year = {2024},
date = {2024-02-28},
urldate = {2024-02-28},
journal = {Nature Communications},
volume = {15},
number = {1804},
pages = {10},
abstract = {Excitons are realizations of a correlated many-particle wave function, specifi-cally consisting of electrons and holes in an entangled state. Excitons occurwidely in semiconductors and are dominant excitations in semiconductingorganic and low-dimensional quantum materials. To efficiently harness thestrong optical response and high tuneability of excitons in optoelectronics andin energy-transformation processes,access to the full wavefunction of theentangled state is critical, but has so far not been feasible. Here, we show howtime-resolved photoemission momentum microscopy can be used to gainaccess to the entangled wavefunction and to unravel the exciton’s multiorbitalelectron and hole contributions. For the prototypical organic semiconductorbuckminsterfullerene (C60), we exemplify the capabilities of exciton tomo-graphy and achieve unprecedented access to key properties of the entangledexciton state including localization, charge-transfer character, and ultrafastexciton formation and relaxation dynamics.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Excitons are realizations of a correlated many-particle wave function, specifi-cally consisting of electrons and holes in an entangled state. Excitons occurwidely in semiconductors and are dominant excitations in semiconductingorganic and low-dimensional quantum materials. To efficiently harness thestrong optical response and high tuneability of excitons in optoelectronics andin energy-transformation processes,access to the full wavefunction of theentangled state is critical, but has so far not been feasible. Here, we show howtime-resolved photoemission momentum microscopy can be used to gainaccess to the entangled wavefunction and to unravel the exciton’s multiorbitalelectron and hole contributions. For the prototypical organic semiconductorbuckminsterfullerene (C60), we exemplify the capabilities of exciton tomo-graphy and achieve unprecedented access to key properties of the entangledexciton state including localization, charge-transfer character, and ultrafastexciton formation and relaxation dynamics. |
| 19. | M. Klein, J. B. Bauer, N. Kainbacher, M. S. Wagner, K. Greulich, P. Haizmann, E. Giangrisostomi, R. Ovsyannikov, P. Puschnig, T. Chassé, H. F. Bettinger, H. Peisert Peri-Tetracene from 1,1′-Bitetracene: Zipping up Structurally Defined Graphene Nanoribbons Journal Article In: J. Phys. Chem. C, vol. 128, pp. 4048-4059, 2024. @article{Klein2024,
title = {Peri-Tetracene from 1,1′-Bitetracene: Zipping up Structurally Defined Graphene Nanoribbons},
author = {M. Klein and J. B. Bauer and N. Kainbacher and M. S. Wagner and K. Greulich and P. Haizmann and E. Giangrisostomi and R. Ovsyannikov and P. Puschnig and T. Chassé and H. F. Bettinger and H. Peisert},
doi = {10.1021/acs.jpcc.3c08182},
year = {2024},
date = {2024-02-22},
journal = {J. Phys. Chem. C},
volume = {128},
pages = {4048-4059},
abstract = {Polycyclicaromatichydrocarbons(PAHs) are promising molecules for a manifold of applications in organic electronics, spintronics, or energy storage devices. Among PAHs, particular attention has been focused on the synthesis and study of acenes and fused acenes, peri-acenes, allowing tuning of the highest occupied molecular orbital−lowest unoccupied molecular orbital (HOMO−LUMO) gap with the size of the conjugated system. As a starting point for the surface synthesis of larger PAHs, we synthesized a 1,1′-bitetracene for the first time. This precursor molecule consists of two tetracene units connected via the 1,1′-position with a torsion angle of 70°. The interface properties of the molecule before and after annealing on a Cu(111) surface are investigated. Using X-ray photoemission spectroscopy(XPS), angle-resolved photoelectron spectroscopy (ARPES), low-energy electron diffraction (LEED), and scanning-tunneling microscopy (STM), it is experimentally demonstrated that the tetracene units zip up with the help of heat forming peri-tetracene. These results and the exact adsorption geometry are in excellent agreement with calculations using density functionaltheory (DFT). Moreover, the calculations enable the identification of newly formed valence band states at the interface to Cu(111).},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Polycyclicaromatichydrocarbons(PAHs) are promising molecules for a manifold of applications in organic electronics, spintronics, or energy storage devices. Among PAHs, particular attention has been focused on the synthesis and study of acenes and fused acenes, peri-acenes, allowing tuning of the highest occupied molecular orbital−lowest unoccupied molecular orbital (HOMO−LUMO) gap with the size of the conjugated system. As a starting point for the surface synthesis of larger PAHs, we synthesized a 1,1′-bitetracene for the first time. This precursor molecule consists of two tetracene units connected via the 1,1′-position with a torsion angle of 70°. The interface properties of the molecule before and after annealing on a Cu(111) surface are investigated. Using X-ray photoemission spectroscopy(XPS), angle-resolved photoelectron spectroscopy (ARPES), low-energy electron diffraction (LEED), and scanning-tunneling microscopy (STM), it is experimentally demonstrated that the tetracene units zip up with the help of heat forming peri-tetracene. These results and the exact adsorption geometry are in excellent agreement with calculations using density functionaltheory (DFT). Moreover, the calculations enable the identification of newly formed valence band states at the interface to Cu(111). |
2023
|
| 18. | A. Adamkiewicz, M. Raths, M. Stettner, M. Theilen, L. Münster, S. Wenzel, M. Hutter, S. Soubatch, C. Kumpf, F. C. Bocquet, R. Wallauer, F. S. Tautz, U. Höfer Coherent and Incoherent Excitation Pathways in Time-Resolved Photoemission Orbital Tomography of CuPc/Cu(001)-2O Journal Article In: J.Phys. Chem. C, vol. 127, pp. 20411, 2023. @article{Adamkiewicz2023,
title = {Coherent and Incoherent Excitation Pathways in Time-Resolved Photoemission Orbital Tomography of CuPc/Cu(001)-2O},
author = {A. Adamkiewicz and M. Raths and M. Stettner and M. Theilen and L. Münster and S. Wenzel and M. Hutter and S. Soubatch and C. Kumpf and F. C. Bocquet and R. Wallauer and F. S. Tautz and U. Höfer},
doi = {10.1021/acs.jpcc.3c04859},
year = {2023},
date = {2023-10-09},
urldate = {2023-10-09},
journal = {J.Phys. Chem. C},
volume = {127},
pages = {20411},
abstract = {Time-resolved photoemission orbital tomography (tr-POT) offers unique possibilities for tracing molecular electron dynamics. The recorded pump-induced changes of the angle-resolved photoemission intensities allow one to characterize unoccupied molecular states in momentum space and to deduce the incoherent temporal evolution of their population. Here, we show for the example of CuPc/Cu(001)-2O that the method also gives access to the coherent regime and that different excitation pathways can be disentangled by a careful analysis of the time-dependent change of the photoemission momentum pattern. In particular, we demonstrate by varying photon energy and polarization of the pump light how the incoherent temporal evolution of the LUMO distribution can be distinguished from coherent contributions of the projected HOMO. Moreover, we report the selective excitation of molecules with a specific orientation at normal incidence by aligning the electric field of the pump light along the molecular axis.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Time-resolved photoemission orbital tomography (tr-POT) offers unique possibilities for tracing molecular electron dynamics. The recorded pump-induced changes of the angle-resolved photoemission intensities allow one to characterize unoccupied molecular states in momentum space and to deduce the incoherent temporal evolution of their population. Here, we show for the example of CuPc/Cu(001)-2O that the method also gives access to the coherent regime and that different excitation pathways can be disentangled by a careful analysis of the time-dependent change of the photoemission momentum pattern. In particular, we demonstrate by varying photon energy and polarization of the pump light how the incoherent temporal evolution of the LUMO distribution can be distinguished from coherent contributions of the projected HOMO. Moreover, we report the selective excitation of molecules with a specific orientation at normal incidence by aligning the electric field of the pump light along the molecular axis. |
| 17. | C. S. Kern, A. Windischbacher, P. Puschnig Photoemission orbital tomography for excitons in organic molecules Journal Article In: Phys. Rev. B, vol. 108, pp. 085132, 2023. @article{Kern2023,
title = {Photoemission orbital tomography for excitons in organic molecules},
author = {C. S. Kern and A. Windischbacher and P. Puschnig},
doi = {https://doi.org/10.1103/PhysRevB.108.085132},
year = {2023},
date = {2023-08-22},
urldate = {2023-08-22},
journal = {Phys. Rev. B},
volume = {108},
pages = {085132},
abstract = {Driven by recent developments in time-resolved photoemission spectroscopy, we extend the successful method of photoemission orbital tomography (POT) to excitons. Our theory retains the intuitive orbital picture of POT, while respecting both the entangled character of the exciton wave function and the energy conservation in the photoemission process. Analyzing results from three organic molecules, we classify generic exciton structures and give a simple interpretation in terms of natural transition orbitals. We validate our findings by directly simulating pump-probe experiments with time-dependent density functional theory.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Driven by recent developments in time-resolved photoemission spectroscopy, we extend the successful method of photoemission orbital tomography (POT) to excitons. Our theory retains the intuitive orbital picture of POT, while respecting both the entangled character of the exciton wave function and the energy conservation in the photoemission process. Analyzing results from three organic molecules, we classify generic exciton structures and give a simple interpretation in terms of natural transition orbitals. We validate our findings by directly simulating pump-probe experiments with time-dependent density functional theory. |
| 16. | C. S. Kern, A. Haags, L.Egger, X. Yang, H. Kirschner, S. Wolff, T. Seyller, A. Gottwald, M. Richter, U. De Giovannini, A. Rubio, M. G. Ramsey, F. C. Bocquet, Soubatch, F. S. Tautz, P. Puschnig, S. Moser Simple extension of the plane-wave final state in photoemission: Bringing understanding to the photon-energy dependence of two-dimensional materials Journal Article In: Phys. Rev. Research, vol. 5, iss. 033075, 2023. @article{Kern2023b,
title = {Simple extension of the plane-wave final state in photoemission: Bringing understanding to the photon-energy dependence of two-dimensional materials},
author = {C. S. Kern and A. Haags and L.Egger and X. Yang and H. Kirschner and S. Wolff and T. Seyller and A. Gottwald and M. Richter and U. De Giovannini and A. Rubio and M. G. Ramsey and F. C. Bocquet and Soubatch and F. S. Tautz and P. Puschnig and S. Moser},
url = {https://journals.aps.org/prresearch/abstract/10.1103/PhysRevResearch.5.033075},
doi = {10.1103/PhysRevResearch.5.033075},
year = {2023},
date = {2023-08-03},
journal = {Phys. Rev. Research},
volume = {5},
issue = {033075},
abstract = {Angle-resolved photoemission spectroscopy (ARPES) is a method that measures orbital and band structure contrast through the momentum distribution of photoelectrons. Its simplest interpretation is obtained in the plane-wave approximation, according to which photoelectrons propagate freely to the detector. The photoelectron momentum distribution is then essentially given by the Fourier transform of the real-space orbital. While the plane-wave approximation is remarkably successful in describing the momentum distributions of aromatic compounds, it generally fails to capture kinetic-energy-dependent final-state interference and dichroism effects. Focusing our present study on quasi-freestanding monolayer graphene as the archetypical two-dimensional (2D) material, we observe an exemplary 𝐸kin
-dependent modulation of, and a redistribution of spectral weight within, its characteristic horseshoe signature around the
‾‾‾
K
and
‾‾‾
K
′
points: both effects indeed cannot be rationalized by the plane-wave final state. Our data are, however, in remarkable agreement with ab initio time-dependent density functional simulations of a freestanding graphene layer and can be explained by a simple extension of the plane-wave final state, permitting the two dipole-allowed partial waves emitted from the C 2𝑝𝑧
orbitals to scatter in the potential of their immediate surroundings. Exploiting the absolute photon flux calibration of the Metrology Light Source, this scattered-wave approximation allows us to extract 𝐸kin
-dependent amplitudes and phases of both partial waves directly from photoemission data. The scattered-wave approximation thus represents a powerful yet intuitive refinement of the plane-wave final state in photoemission of 2D materials and beyond.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Angle-resolved photoemission spectroscopy (ARPES) is a method that measures orbital and band structure contrast through the momentum distribution of photoelectrons. Its simplest interpretation is obtained in the plane-wave approximation, according to which photoelectrons propagate freely to the detector. The photoelectron momentum distribution is then essentially given by the Fourier transform of the real-space orbital. While the plane-wave approximation is remarkably successful in describing the momentum distributions of aromatic compounds, it generally fails to capture kinetic-energy-dependent final-state interference and dichroism effects. Focusing our present study on quasi-freestanding monolayer graphene as the archetypical two-dimensional (2D) material, we observe an exemplary 𝐸kin
-dependent modulation of, and a redistribution of spectral weight within, its characteristic horseshoe signature around the
‾‾‾
K
and
‾‾‾
K
′
points: both effects indeed cannot be rationalized by the plane-wave final state. Our data are, however, in remarkable agreement with ab initio time-dependent density functional simulations of a freestanding graphene layer and can be explained by a simple extension of the plane-wave final state, permitting the two dipole-allowed partial waves emitted from the C 2𝑝𝑧
orbitals to scatter in the potential of their immediate surroundings. Exploiting the absolute photon flux calibration of the Metrology Light Source, this scattered-wave approximation allows us to extract 𝐸kin
-dependent amplitudes and phases of both partial waves directly from photoemission data. The scattered-wave approximation thus represents a powerful yet intuitive refinement of the plane-wave final state in photoemission of 2D materials and beyond. |
| 15. | S. Ito, M. Schüler, M. Meierhofer, S. Schlauderer, J. Freudenstein, R. Reimann, D. Afanasiev, K. A. Kokh, O. E. Tereshchenko, J. Güdde, M. A. Sentef, U. Höfer, R. Huber
Build-up and dephasing of Floquet-Bloch bands on subcycle timescales Journal Article In: Nature, vol. 616, pp. pages 696–701, 2023. @article{Ito2023,
title = {Build-up and dephasing of Floquet-Bloch bands on subcycle timescales},
author = {S. Ito and M. Schüler and M. Meierhofer and S. Schlauderer and J. Freudenstein and R. Reimann and D. Afanasiev and K. A. Kokh and O. E. Tereshchenko and J. Güdde and M. A. Sentef and U. Höfer and R. Huber
},
doi = {10.1038/s41586-023-05850-x},
year = {2023},
date = {2023-04-12},
urldate = {2023-04-12},
journal = {Nature},
volume = {616},
pages = {pages 696–701},
abstract = {Strong light fields have created opportunities to tailor novel functionalities of solids. Floquet–Bloch states can form under periodic driving of electrons and enable exotic quantum phases. On subcycle timescales, lightwaves can simultaneously drive intraband currents and interband transition, which enable high-harmonic generation and pave the way towards ultrafast electronics. Yet, the interplay of intraband and interband excitations and their relation to Floquet physics have been key open questions as dynamical aspects of Floquet states have remained elusive. Here we provide this link by visualizing the ultrafast build-up of Floquet–Bloch bands with time-resolved and angle-resolved photoemission spectroscopy. We drive surface states on a topological insulator with mid-infrared fields—strong enough for high-harmonic generation—and directly monitor the transient band structure with subcycle time resolution. Starting with strong intraband currents, we observe how Floquet sidebands emerge within a single optical cycle; intraband acceleration simultaneously proceeds in multiple sidebands until high-energy electrons scatter into bulk states and dissipation destroys the Floquet bands. Quantum non-equilibrium calculations explain the simultaneous occurrence of Floquet states with intraband and interband dynamics. Our joint experiment and theory study provides a direct time-domain view of Floquet physics and explores the fundamental frontiers of ultrafast band-structure engineering.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Strong light fields have created opportunities to tailor novel functionalities of solids. Floquet–Bloch states can form under periodic driving of electrons and enable exotic quantum phases. On subcycle timescales, lightwaves can simultaneously drive intraband currents and interband transition, which enable high-harmonic generation and pave the way towards ultrafast electronics. Yet, the interplay of intraband and interband excitations and their relation to Floquet physics have been key open questions as dynamical aspects of Floquet states have remained elusive. Here we provide this link by visualizing the ultrafast build-up of Floquet–Bloch bands with time-resolved and angle-resolved photoemission spectroscopy. We drive surface states on a topological insulator with mid-infrared fields—strong enough for high-harmonic generation—and directly monitor the transient band structure with subcycle time resolution. Starting with strong intraband currents, we observe how Floquet sidebands emerge within a single optical cycle; intraband acceleration simultaneously proceeds in multiple sidebands until high-energy electrons scatter into bulk states and dissipation destroys the Floquet bands. Quantum non-equilibrium calculations explain the simultaneous occurrence of Floquet states with intraband and interband dynamics. Our joint experiment and theory study provides a direct time-domain view of Floquet physics and explores the fundamental frontiers of ultrafast band-structure engineering. |