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Search Results: 1 - 10 of 475024 matches for " E. D. L. Rienks "
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Electron-phonon coupling in potassium-doped graphene: Angle-resolved photoemission spectroscopy
M. Bianchi,E. D. L. Rienks,S. Lizzit,A. Baraldi,R. Balog,L. Hornekaer,Ph. Hofmann
Physics , 2009, DOI: 10.1103/PhysRevB.81.041403
Abstract: The electron-phonon coupling in potassium-doped graphene on Ir(111) is studied via the renormalization of the pi* band near the Fermi level, using angle-resolved photoemission spectroscopy. The renormalization is found to be fairly weak and almost isotropic, with a mass enhancement parameter of lambda= 0.28(6) for both the K-M and the K-G direction. These results are found to agree well with recent first principles calculations.
Band dispersion in the deep 1s core level of graphene
S. Lizzit,G. Zampieri,L. Petaccia,R. Larciprete,P. Lacovig,E. D. L. Rienks,A. Baraldi,Ph. Hofmann
Physics , 2010, DOI: 10.1038/NPHYS1615
Abstract: Chemical bonding in molecules and solids arises from the overlap of valence electron wave functions, forming extended molecular orbitals and dispersing Bloch states, respectively. Core electrons with high binding energies, on the other hand, are localized to their respective atoms and their wave functions do not overlap significantly. Here we report the observation of band formation and considerable dispersion (up to 60 meV) in the $1s$ core level of the carbon atoms forming graphene, despite the high C $1s$ binding energy of $\approx$ 284 eV. Due to a Young's double slit-like interference effect, a situation arises in which only the bonding or only the anti-bonding states is observed for a given photoemission geometry.
The high-energy anomaly in ARPES spectra of the cuprates-many body or matrix element effect?
E. D. L. Rienks,M. ?rr?l,M. Lindroos,F. Roth,W. Tabis,G. Yu,M. Greven,J. Fink
Physics , 2013, DOI: 10.1103/PhysRevLett.113.137001
Abstract: We used polarization-dependent angle-resolved photoemission spectroscopy (ARPES) to study the high-energy anomaly (HEA) in the dispersion of Nd2-xCexCuO4, (x=0.123). We have found that at particular photon energies the anomalous, waterfalllike dispersion gives way to a broad, continuous band. This suggests that the HEA is a matrix element effect: it arises due to a suppression of the intensity of the broadened quasi-particle band in a narrow momentum range. We confirm this interpretation experimentally, by showing that the HEA appears when the matrix element is suppressed deliberately by changing the light polarization. Calculations of the matrix element using atomic wave functions and simulation of the ARPES intensity with one-step model calculations provide further proof for this scenario. The possibility to detect the full quasi-particle dispersion further allows us to extract the high-energy self-energy function near the center and at the edge of the Brillouin zone.
Anisotropic effect of warping on the lifetime broadening of topological surface states in angle-resolved photoemission from Bi$_2$Te$_3$
J. Sánchez-Barriga,M. R. Scholz,E. Golias,E. Rienks,D. Marchenko,A. Varykhalov,L. V. Yashina,O. Rader
Physics , 2015, DOI: 10.1103/PhysRevB.90.195413
Abstract: We analyze the strong hexagonal warping of the Dirac cone of Bi$_2$Te$_3$ by angle-resolved photoemission. Along $\overline{\Gamma}$$\overline{\rm M}$, the dispersion deviates from a linear behavior meaning that the Dirac cone is warped outwards and not inwards. We show that this introduces an anisotropy in the lifetime broadening of the topological surface state which is larger along $\overline{\Gamma}$$\overline{\rm K}$. The result is not consistent with nesting. Based on the theoretically predicted behavior of the ground-state spin texture of a strongly warped Dirac cone, we propose spin-dependent scattering processes as explanation for the anisotropic scattering rates. These results could help paving the way for optimizing future spintronic devices using topological insulators and controlling surface-scattering processes via external gate voltages.
Electronic structure and quantum criticality in Ba(Fe$_{1-x-y}$Co$_{x}$Mn$_{y}$)$_{2}$As$_{2}$, an ARPES study
E. D. L. Rienks,T. Wolf,K. Koepernik,I. Avigo,P. Hlawenka,C. Lupulescu,T. Arion,F. Roth,W. Eberhardt,U. Bovensiepen,J. Fink
Physics , 2013, DOI: 10.1209/0295-5075/103/47004
Abstract: We used angle-resolved photoemission spectroscopy (ARPES) and density functional theory calculations to study the electronic structure of Ba(Fe1-x-yCoxMny)2As2 for x=0.06 and 0<=y <=0.07. From ARPES we derive that the substitution of Fe by Mn does not lead to hole doping, indicating a localization of the induced holes. An evaluation of the measured spectral function does not indicate a diverging effective mass or scattering rate near optimal doping. Thus the present ARPES results indicate a continuous evolution of the quasiparticle interaction and therefore question previous quantum critical scenarios.
Unusual band renormalization in the simplest iron based superconductor
J. Maletz,V. B. Zabolotnyy,D. V. Evtushinsky,S. Thirupathaiah,A. U. B. Wolter,L. Harnagea,A. N. Yaresko,A. N. Vasiliev,D. A. Chareev,E. D. L. Rienks,B. Büchner,S. V. Borisenko
Physics , 2013, DOI: 10.1103/PhysRevB.89.220506
Abstract: The electronic structure of the iron chalcogenide superconductor FeSe_{1-x} was investigated by high- resolution angle-resolved photoemission spectroscopy (ARPES). The results were compared to DFT calculations showing some significant differences between the experimental electronic structure of FeSe_{1-x}, DFT calculations and existing data on FeSe_{x}Te_{1-x}. The bands undergo a pronounced orbital dependent renormalization, different from what was observed for FeSe_{x}Te_{1-x} and any other pnictides.
One-dimensional spin texture of Bi(441); Quantum Spin Hall properties without a topological insulator
M. Bianchi,F. Song,S. Cooil,A. F. Monsen,E. Wahlstrom,J. A. Miwa,E. D. L. Rienks,D. A. Evans,A. Strozecka,J. I. Pascual,M. Leandersson,T. Balasubramanian,Ph. Hofmann,J. W. Wells
Physics , 2015, DOI: 10.1103/PhysRevB.91.165307
Abstract: The high index (441) surface of bismuth has been studied using Scanning Tunnelling Microscopy (STM), Angle Resolved Photoemission Spectroscopy (APRES) and spin-resolved ARPES. The surface is strongly corrugated, exposing a regular array of (110)-like terraces. Two surface localised states are observed, both of which are linearly dispersing in one in-plane direction ($k_x$), and dispersionless in the orthogonal in-plane direction ($k_y$), and both of which have a Dirac-like crossing at $k_x$=0. Spin ARPES reveals a strong in-plane polarisation, consistent with Rashba-like spin-orbit coupling. One state has a strong out-of-plane spin component, which matches with the miscut angle, suggesting its {possible} origin as an edge-state. The electronic structure of Bi(441) has significant similarities with topological insulator surface states and is expected to support one dimensional Quantum Spin Hall-like coupled spin-charge transport properties with inhibited backscattering, without requiring a topological insulator bulk.
How chemical pressure affects the fundamental properties of rare-earth pnictides: an ARPES view
M. G. Holder,A. Jesche,P. Lombardo,R. Hayn,D. V. Vyalikh,K. Kummer,S. Danzenb?cher,C. Krellner,C. Geibel,E. D. L. Rienks,S. L. Molodtsov,C. Laubschat
Physics , 2012, DOI: 10.1103/PhysRevB.86.020506
Abstract: Angle-resolved photoelectron spectroscopy, supplemented by theoretical calculations has been applied to study the electronic structure of heavy-fermion material CeFePO, a homologue to the Fe-based high-temperature superconductors, and CeFeAs_0.7P_0.3O, where the applied chemical pressure results in a ferromagnetic order of the 4f moments. A comparative analysis reveals characteristic differences in the Fe-derived band structure for these materials, implying a rather different hybridization of valence electrons to the localized 4f orbitals. In particular, our results suggest that the ferromagnetism of Ce moments in CeFeAs_0.7P_0.3O is mediated mainly by Fe 3d_xz/yz orbitals, while the Kondo screening in CeFePO is instead due to a strong interaction of Fe 3d_3z^2-r^2 orbitals.
Dissimilarities between the electronic structure of chemically doped and chemically pressurized iron pnictides from an angle-resolved photoemission spectroscopy study
S. Thirupathaiah,E. D. L. Rienks,H. S. Jeevan,R. Ovsyannikov,E. Slooten,J. Kaas,E. van Heumen,S. de Jong,H. A. Duerr,K. Siemensmeyer,R. Follath,P. Gegenwart,M. S. Golden,J. Fink
Physics , 2010, DOI: 10.1103/PhysRevB.84.014531
Abstract: We have studied the electronic structure of EuFe2As2-xPx using high resolution angle-resolved photoemission spectroscopy. Upon substituting As with the isovalent P, which leads to a chemical pressure and to superconductivity, we observe a non-rigid-band like change of the electronic structure along the center of the Brillouin zone (BZ): an orbital and kz dependent increase or decrease in the size of the hole pockets near the Gamma - Z line. On the other hand, the diameter of the Fermi surface cylinders at the BZ corner forming electron pockets, hardly changes. This is in stark contrast to p and n-type doped iron pnictides where, on the basis of ARPES experiments, a more rigid-band like behavior has been proposed. These findings indicate that there are different ways in which the nesting conditions can be reduced causing the destabilization of the antiferromagnetic order and the appearance of the superconducting dome.
Samarium hexaboride: A trivial surface conductor
P. Hlawenka,K. Siemensmeyer,E. Weschke,A. Varykhalov,J. Sánchez-Barriga,N. Y. Shitsevalova,A. V. Dukhnenko,V. B. Filipov,S. Gabáni,K. Flachbart,O. Rader,E. D. L. Rienks
Physics , 2015,
Abstract: Recent theoretical and experimental studies suggest that SmB$_6$ is the first topological Kondo insulator: A material in which the interaction between localized and itinerant electrons renders the bulk insulating at low temperature, while topological surface states leave the surface metallic. While this would elegantly explain the material's puzzling conductivity, we find the experimentally observed candidates for both predicted topological surface states to be of trivial character instead: The surface state at $\bar{\Gamma}$ is very heavy and shallow with a mere $\sim 2$ meV binding energy. It exhibits large Rashba splitting which excludes a topological nature. We further demonstrate that the other metallic surface state, located at $\bar{X}$, is not an independent in-gap state as supposed previously, but part of a massive band with much higher binding energy (1.7 eV). We show that it remains metallic down to 1 K due to reduced hybridization with the energy-shifted surface 4$f$ level.
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