1,695 research outputs found

    Topographic and electronic contrast of the graphene moir\'e on Ir(111) probed by scanning tunneling microscopy and non-contact atomic force microscopy

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    Epitaxial graphene grown on transition metal surfaces typically exhibits a moir\'e pattern due to the lattice mismatch between graphene and the underlying metal surface. We use both scanning tunneling microscopy (STM) and atomic force microscopy (AFM) experiments to probe the electronic and topographic contrast of the graphene moir\'e on the Ir(111) surface. While STM topography is influenced by the local density of states close to the Fermi energy and the local tunneling barrier height, AFM is capable of yielding the 'true' surface topography once the background force arising from the van der Waals (vdW) interaction between the tip and the substrate is taken into account. We observe a moir\'e corrugation of 35±\pm10 pm, where the graphene-Ir(111) distance is the smallest in the areas where the graphene honeycomb is atop the underlying iridium atoms and larger on the fcc or hcp threefold hollow sites.Comment: revised versio

    Anisotropic excitonic effects in the energy loss function of hexagonal boron nitride

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    We demonstrate that the valence energy-loss function of hexagonal boron nitride (hBN) displays a strong anisotropy in shape, excitation energy and dispersion for momentum transfer q parallel or perpendicular to the hBN layers. This is manifested by e.g. an energy shift of 0.7 eV that cannot be captured by single-particle approaches and is a demonstration of a strong anisotropy in the two-body electron-hole interaction. Furthermore, for in-plane directions of q we observe a splitting of the -plasmon in the M direction that is absent in the K direction and this can be traced back to band-structure effects.Comment: 10 pages, 4 figure

    Electrode thickness measurement of a Si(Li) detector for the SIXA array

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    Cathode electrodes of the Si(Li) detector elements of the SIXA X-ray spectrometer array are formed by gold-palladium alloy contact layers. The equivalent thickness of gold in one element was measured by observing the characteristic L-shell X-rays of gold excited by monochromatised synchrotron radiation with photon energies above the L3 absorption edge of gold. The results obtained at 4 different photon energies below the L2 edge yield an average value of 22.4(35) nm which is consistent with the earlier result extracted from detection efficiency measurements. PACS: 29.40.Wk; 85.30.De; 07.85.Nc; 95.55.Ka Keywords: Si(Li) detectors, X-ray spectrometers, X-ray fluorescence, detector calibration, gold electrodes, synchrotron radiationComment: 10 pages, 4 PostScript figures, uses elsart.sty, submitted to Nucl. Instrum. Meth.

    X-ray Raman scattering study of aligned polyfluorene

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    We present a non-resonant inelastic x-ray scattering study at the carbon K-edge on aligned poly[9,9-bis(2-ethylhexyl)-fluorene-2,7-diyl] and show that the x-ray Raman scattering technique can be used as a practical alternative to x-ray absorption measurements. We demonstrate that this novel method can be applied to studies on aligned π\pi-conjugated polymers complementing diffraction and optical studies. Combining the experimental data and a very recently proposed theoretical scheme we demonstrate a unique property of x-ray Raman scattering by performing the symmetry decomposition on the density of unoccupied electronic states into ss- and pp-type symmetry contributions.Comment: 19 pages, 8 figure

    Inelastic X-ray scattering in correlated (Mott) insulators

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    We calculate the inelastic light scattering from X-rays, which allows the photon to transfer both energy and momentum to the strongly correlated charge excitations. We find that the charge transfer peak and the low energy peak both broaden and disperse through the Brillouin zone similar to what is seen in experiments in materials like Ca_2 Cu O_2 Cl_2.Comment: 5 pages Revtex4, 6 figure

    Sukupolvien ketju : Suuret ikäluokat ja sukupolvien välinen vuorovaikutus Suomessa

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    Tutkimuksessa selvitään sukulaisten välistä vuorovaikutusta sekä avunantoa suomalaisissa perheissä ja suvuissa. Tutkimuskohteena on kolme perhesukupolvea: suuret ikäluokat, heidän aikuiset lapsensa ja vanhempansa, joista on kerätty laaja postikysely-, lomakehaastattelu- ja teemahaastatteluaineisto. Tutkimuskysymysten muodostamisessa ja tulosten tarkastelussa hyödynnetään aikaisempaa sosiologista sukupolvi- ja perhetutkimusta sekä evoluutioteorian esittämiä vastavuoroisuutta ja altruismia koskevia teorioita ja tuloksia. Tutkimuksessa kysytään, miten eri sukupolvet auttavat toisiaan, millaisia sukupolvikohtaisia eroja auttamiskäytännöissä esiintyy ja mitkä taustatekijät selittävät auttamista. Lisäksi selvitetään sukulaisten auttamisasenteita ja tyytyväisyyttä saatuun apuun sekä auttamiseen liittyviä ristiriitoja. Näiden ohella tarkastellaan, miten sukupolvien väliset sosiaaliset suhteet kytkeytyvät auttamiskäytäntöihin. Tutkimustulokset osoittavat, että sukulaisapu on tärkeä tekijä ihmisten välisessä vuorovaikutuksessa. Ihmiset ovat eniten yhteydessä biologisiin sukulaisiinsa, auttavat heitä eniten ja saavat heiltä eniten apua. Mitä keskeisemmästä avun muodosta on kysymys, sitä tärkeämpiä lähisukulaiset ovat. Toisaalta apua annetaan useille eri sukulaisille, mutta avun nettovirta kulkee sukulinjassa vanhemmilta nuoremmille polville. Keskeinen tulos onkin se, että suuret ikäluokat antavat apua enemmän lapsilleen kuin vanhemmilleen. Sukupolvien väliset erot auttamisessa liittyvät yleensä vastaajien ikään tai elämänvaiheeseen. Vastaajat ovat tavallisesti saaneet pyytäessään apua ja ovat yleensä myös tyytyväisiä saamaansa apuun. Sukulaisten auttaminen onkin valtaosalle itsestään selvää riippumatta siitä, koetaanko sitä varsinaisesti velvollisuudeksi. Huolimatta siitä, että sukulaisten auttaminen on runsasta, vain harvat mieltävät esimerkiksi vanhusten auttamisen yksinomaan perheen velvollisuudeksi.11,00 euro

    Inverse Modeling for MEG/EEG data

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    We provide an overview of the state-of-the-art for mathematical methods that are used to reconstruct brain activity from neurophysiological data. After a brief introduction on the mathematics of the forward problem, we discuss standard and recently proposed regularization methods, as well as Monte Carlo techniques for Bayesian inference. We classify the inverse methods based on the underlying source model, and discuss advantages and disadvantages. Finally we describe an application to the pre-surgical evaluation of epileptic patients.Comment: 15 pages, 1 figur

    Non-invasive detection of animal nerve impulses with an atomic magnetometer operating near quantum limited sensitivity

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    Magnetic fields generated by human and animal organs, such as the heart, brain and nervous system carry information useful for biological and medical purposes. These magnetic fields are most commonly detected using cryogenically-cooled superconducting magnetometers. Here we present the frst detection of action potentials from an animal nerve using an optical atomic magnetometer. Using an optimal design we are able to achieve the sensitivity dominated by the quantum shot noise of light and quantum projection noise of atomic spins. Such sensitivity allows us to measure the nerve impulse with a miniature room-temperature sensor which is a critical advantage for biomedical applications. Positioning the sensor at a distance of a few millimeters from the nerve, corresponding to the distance between the skin and nerves in biological studies, we detect the magnetic field generated by an action potential of a frog sciatic nerve. From the magnetic field measurements we determine the activity of the nerve and the temporal shape of the nerve impulse. This work opens new ways towards implementing optical magnetometers as practical devices for medical diagnostics.Comment: Main text with figures, and methods and supplementary informatio

    K -shell diagram and hypersatellite spectra of 4d transition elements

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    The K-shell diagram (K alpha(1,2) and K beta(1,3)) and hypersatellite (HS) (K-h alpha(1,2)) spectra of Y, Zr, Mo, and Pd have been measured with high energy-resolution using photoexcitation by 90 keV synchrotron radiation. Comparison of the measured and ab initio calculated HS spectra demonstrates the importance of quantum electrodynamical (QED) effects for the HS spectra. Phenomenological fits of the measured spectra by Voigt functions yield accurate values for the shift of the HS from the diagram lines, the splitting of the HS lines, and their intensity ratio. Good agreement with theory was found for all quantities except for the intensity ratio, which is dominated by the intermediacy of the coupling of the angular momenta. The observed deviations imply that our current understanding of the variation of the coupling scheme from LS to jj across the periodic table may require some revision.The K-shell diagram (K alpha(1,2) and K beta(1,3)) and hypersatellite (HS) (K-h alpha(1,2)) spectra of Y, Zr, Mo, and Pd have been measured with high energy-resolution using photoexcitation by 90 keV synchrotron radiation. Comparison of the measured and ab initio calculated HS spectra demonstrates the importance of quantum electrodynamical (QED) effects for the HS spectra. Phenomenological fits of the measured spectra by Voigt functions yield accurate values for the shift of the HS from the diagram lines, the splitting of the HS lines, and their intensity ratio. Good agreement with theory was found for all quantities except for the intensity ratio, which is dominated by the intermediacy of the coupling of the angular momenta. The observed deviations imply that our current understanding of the variation of the coupling scheme from LS to jj across the periodic table may require some revision.The K-shell diagram (K alpha(1,2) and K beta(1,3)) and hypersatellite (HS) (K-h alpha(1,2)) spectra of Y, Zr, Mo, and Pd have been measured with high energy-resolution using photoexcitation by 90 keV synchrotron radiation. Comparison of the measured and ab initio calculated HS spectra demonstrates the importance of quantum electrodynamical (QED) effects for the HS spectra. Phenomenological fits of the measured spectra by Voigt functions yield accurate values for the shift of the HS from the diagram lines, the splitting of the HS lines, and their intensity ratio. Good agreement with theory was found for all quantities except for the intensity ratio, which is dominated by the intermediacy of the coupling of the angular momenta. The observed deviations imply that our current understanding of the variation of the coupling scheme from LS to jj across the periodic table may require some revision.Peer reviewe

    Boron Nitride Monolayer: A Strain-Tunable Nanosensor

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    The influence of triaxial in-plane strain on the electronic properties of a hexagonal boron-nitride sheet is investigated using density functional theory. Different from graphene, the triaxial strain localizes the molecular orbitals of the boron-nitride flake in its center depending on the direction of the applied strain. The proposed technique for localizing the molecular orbitals that are close to the Fermi level in the center of boron nitride flakes can be used to actualize engineered nanosensors, for instance, to selectively detect gas molecules. We show that the central part of the strained flake adsorbs polar molecules more strongly as compared with an unstrained sheet.Comment: 20 pages, 9 figure
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