TY - JOUR A1 - Tempel, Jean-Sebastian A1 - Veit, Tempel A1 - Assmann, Marc A1 - Kreilkamp, Lars Erik A1 - Höfling, Sven A1 - Kamp, Martin A1 - Forchel, Alfred A1 - Bayer, Manfred T1 - Temperature dependence of pulsed polariton lasing in a GaAs microcavity JF - New Journal of Physics N2 - The second-order correlation function g\(^2\)(\(\tau\) = 0), input-output curves and pulse duration of the emission from a microcavity exciton-polariton system subsequent to picosecond-pulsed excitation are measured for different temperatures. At low temperatures a two-threshold behaviour emerges, which has been attributed to the onset of polariton lasing and conventional lasing at the first and the second threshold, respectively. We observe that polariton lasing is stable up to temperatures comparable with the exciton binding energy. At higher temperatures a single threshold displays the direct transition from thermal emission to photon lasing. KW - semiconductor microavity KW - quantized vortices KW - cavity polaritons KW - room temperature KW - excitons KW - time Y1 - 2012 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-134022 VL - 14 IS - 083014 ER - TY - JOUR A1 - Aad, G. A1 - Abbott, B. A1 - Abdallah, J. A1 - Abdel Khalek, S. A1 - Abdelalim, A. A. T1 - Search for the Standard Model Higgs boson in the H→WW(⋆)→ℓνℓνH→WW(⋆)→ℓνℓν decay mode with 4.7 fb\(^{−1}\) of ATLAS data at \(\sqrt{s}\)=7 TeV JF - Physics Letters B N2 - A search for the Standard Model Higgs boson in the H→WW(⋆)→ℓνℓνH→WW(⋆)→ℓνℓν (ℓ=e,μℓ=e,μ) decay mode is presented. The search is performed using proton–proton collision data corresponding to an integrated luminosity of 4.7 fb\(^{−1}\) at a centre-of-mass energy of 7 TeV collected during 2011 with the ATLAS detector at the Large Hadron Collider. No significant excess of events over the expected background is observed. An upper bound is placed on the Higgs boson production cross section as a function of its mass. A Standard Model Higgs boson with mass in the range between 133 GeV and 261 GeV is excluded at 95% confidence level, while the expected exclusion range is from 127 GeV to 233 GeV. KW - ATLAS KW - LHC KW - Higgs KW - WW Y1 - 2012 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-127307 VL - 761 IS - 1 ER - TY - JOUR A1 - Margapoti, E. A1 - Alves, F. M. A1 - Mahapatra, S. A1 - Lopez-Richard, V. A1 - Worschech, L. A1 - Brunner, K. A1 - Qu, F. A1 - Destefani, C. A1 - Menendez-Proupin, E. A1 - Bougerol, C. A1 - Forchel, A. A1 - Marques, G. E. T1 - Paramagnetic shift in thermally annealed Cd\(_x\)Zn\(_{1-x}\)Se quantum dots JF - New Journal of Physics N2 - The photoluminescence of annealed Cd\(_x\)Zn\(_{1-x}\)Se quantum dots (QDs) under the influence of an external magnetic field has been studied in this paper. Post-growth annealing was performed for different annealing times. Above a critical annealing time, the QD luminescence shows a pronounced red-shift of the Zeeman split magnetic subcomponents. This observation is in contrast to the blue-shift caused by the diamagnetic behavior that is usually observed in non-magnetic QDs. We attribute our finding to the paramagnetism caused by the mixing of heavy and light hole states. Hence, post-growth thermal annealing treatment might be employed to render undoped epitaxial QDs intrinsically magnetic in a controlled manner. Two theoretical models were developed: a few-particle model to account for excitonic complex effects and a multiband calculation that describes the valence band hybridization. Contrasting the two models allowed us to unambiguously elucidate the nature of such an effect. KW - semiconductors Y1 - 2012 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-133294 VL - 14 IS - 043038 ER - TY - JOUR A1 - Wild, J. M. A1 - Marshall, H. A1 - Bock, M. A1 - Schad, L. R. A1 - Jakob, P. M. A1 - Puderbach, M. A1 - Molinari, F. A1 - Van Beek, E. J. R. A1 - Biederer, J. T1 - MRI of the lung (1/3): methods JF - Insights into Imaging N2 - Proton magnetic resonance imaging (MRI) has recently emerged as a clinical tool to image the lungs. This paper outlines the current technical aspects of MRI pulse sequences, radiofrequency (RF) coils and MRI system requirements needed for imaging the pulmonary parenchyma and vasculature. Lung MRI techniques are presented as a “technical toolkit”, from which MR protocols will be composed in the subsequent papers for comprehensive imaging of lung disease and function (parts 2 and 3). This paper is pitched at MR scientists, technicians and radiologists who are interested in understanding and establishing lung MRI methods. Images from a 1.5 T scanner are used for illustration of the sequences and methods that are highlighted. Main Messages • Outline of the hardware and pulse sequence requirements for proton lung MRI • Overview of pulse sequences for lung parenchyma, vascular and functional imaging with protons • Demonstration of the pulse-sequence building blocks for clinical lung MRI protocols KW - MRI KW - lung KW - proton Y1 - 2012 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124238 VL - 3 IS - 4 ER - TY - JOUR A1 - Aad, G. A1 - Abbott, B. A1 - Abdallah, J. A1 - Abdelalim, A. A. A1 - Abdesselam, A. T1 - Electron performance measurements with the ATLAS detector using the 2010 LHC proton-proton collision data JF - The European Physical Journal C N2 - Detailed measurements of the electron performance of the ATLAS detector at the LHC are reported, using decays of the Z, W and J/ψ particles. Data collected in 2010 at s√=7 TeV are used, corresponding to an integrated luminosity of almost 40 pb\(^{−1}\). The inter-alignment of the inner detector and the electromagnetic calorimeter, the determination of the electron energy scale and resolution, and the performance in terms of response uniformity and linearity are discussed. The electron identification, reconstruction and trigger efficiencies, as well as the charge misidentification probability, are also presented. KW - electromagnetic calorimeter KW - Atlas detector KW - calorimeter Y1 - 2012 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-127313 VL - 72 IS - 1909 ER - TY - JOUR A1 - Reiter, Theresa A1 - Gensler, Daniel A1 - Ritter, Oliver A1 - Weiss, Ingo A1 - Geistert, Wolfgang A1 - Kaufmann, Ralf A1 - Hoffmeister, Sabine A1 - Friedrich, Michael T. A1 - Wintzheimer, Stefan A1 - Düring, Markus A1 - Nordbeck, Peter A1 - Jakob, Peter M. A1 - Ladd, Mark E. A1 - Quick, Harald H. A1 - Bauer, Wolfgang R. T1 - Direct cooling of the catheter tip increases safety for CMR-guided electrophysiological procedures JF - Journal of Cardiovascular Magnetic Resonance N2 - Background: One of the safety concerns when performing electrophysiological (EP) procedures under magnetic resonance (MR) guidance is the risk of passive tissue heating due to the EP catheter being exposed to the radiofrequency (RF) field of the RF transmitting body coil. Ablation procedures that use catheters with irrigated tips are well established therapeutic options for the treatment of cardiac arrhythmias and when used in a modified mode might offer an additional system for suppressing passive catheter heating. Methods: A two-step approach was chosen. Firstly, tests on passive catheter heating were performed in a 1.5 T Avanto system (Siemens Healthcare Sector, Erlangen, Germany) using a ASTM Phantom in order to determine a possible maximum temperature rise. Secondly, a phantom was designed for simulation of the interface between blood and the vascular wall. The MR-RF induced temperature rise was simulated by catheter tip heating via a standard ablation generator. Power levels from 1 to 6 W were selected. Ablation duration was 120 s with no tip irrigation during the first 60 s and irrigation at rates from 2 ml/min to 35 ml/min for the remaining 60 s (Biotronik Qiona Pump, Berlin, Germany). The temperature was measured with fluoroscopic sensors (Luxtron, Santa Barbara, CA, USA) at a distance of 0 mm, 2 mm, 4 mm, and 6 mm from the catheter tip. Results: A maximum temperature rise of 22.4 degrees C at the catheter tip was documented in the MR scanner. This temperature rise is equivalent to the heating effect of an ablator's power output of 6 W at a contact force of the weight of 90 g (0.883 N). The catheter tip irrigation was able to limit the temperature rise to less than 2 degrees C for the majority of examined power levels, and for all examined power levels the residual temperature rise was less than 8 degrees C. Conclusion: Up to a maximum of 22.4 degrees C, the temperature rise at the tissue surface can be entirely suppressed by using the catheter's own irrigation system. The irrigated tip system can be used to increase MR safety of EP catheters by suppressing the effects of unwanted passive catheter heating due to RF exposure from the MR scanner. KW - EP Procedures KW - radiofrequency ablation KW - contact force KW - lesion size KW - MRI KW - temperature KW - tissue KW - wires KW - model KW - ablation KW - safety KW - catheter tip KW - MR guidance Y1 - 2012 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-134927 VL - 14 IS - 12 ER - TY - JOUR A1 - Wiessner, M. A1 - Rodriguez Lastra, N. S. A1 - Ziroff, J. A1 - Forster, F. A1 - Puschnig, P. A1 - Dössel, L. A1 - Müllen, K. A1 - Schöll, A. A1 - Reinert, F. T1 - Different views on the electronic structure of nanoscale graphene: aromatic molecule versus quantum dot JF - New Journal of Physics N2 - Graphene's peculiar electronic band structure makes it of interest for new electronic and spintronic approaches. However, potential applications suffer from quantization effects when the spatial extension reaches the nanoscale. We show by photoelectron spectroscopy on nanoscaled model systems (disc-shaped, planar polyacenes) that the two-dimensional band structure is transformed into discrete states which follow the momentum dependence of the graphene Bloch states. Based on a simple model of quantum wells, we show how the band structure of graphene emerges from localized states, and we compare this result with ab initio calculations which describe the orbital structure. KW - well KW - confinement KW - states KW - Ag(111) KW - photoemission KW - vicinal surfaces KW - coronene KW - energy KW - films KW - nanographenes Y1 - 2012 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-130184 VL - 14 IS - 113008 ER -