TY - THES A1 - Anjana Vaman, Vamadevan Sujatha T1 - LASP1, a newly identified melanocytic protein with a possible role in melanin release, but not in melanoma progression T1 - LASP1, ein neu identifiziertes melanozytischen Protein mit einer möglichen Rolle bei der Freisetzung von Melanin, jedoch nicht in Melanomprogression N2 - LIM and SH3 protein 1 (LASP1) is a nucleocytoplasmic scaffolding protein. LASP1 interacts with various cytoskeletal proteins via its domain structure and is known to participate in physiological processes of cells. In the present study, a detailed investigation of the expression pattern of LASP1 protein in normal skin, melanocytic nevi and melanoma was carried out and the melanocyte–specific function of LASP1 was analyzed. LASP1 protein was identified in stratum basale of skin epidermis and a very high level was detected in nevi, the benign tumor of melanocyte. In the highly proliferative basal cells, an additional distinct nuclear localization of the protein was noted. In different tumor entities, an elevated LASP1 expression and nuclear localization, correlated positively with malignancy and tumor grade. However, LASP1 level was determined to be very low in melanoma and even reduced in metastases. Melanoma is distinguished as the first tumor tested to date – that displayed an absence of elevated LASP1 expression. In addition no significant relation was observed between LASP1 protein expression and clinicopathological parameters in melanoma. The epidermal melanin unit of skin comprises of melanocytes and keratinocytes. Melanocytes are specialized cells that synthesize the photo protective coloring pigment, melanin inside unique organelles called melanosomes. The presence of LASP1 in melanocytes is reported for the first time through this study and the existence was confirmed by immunoblotting analysis in cultured normal human epidermal melanocyte (NHEM) and in melanoma cell lines, along with the immunohistostaining imaging in normal skin and in melanocytic nevi. LASP1 depletion in MaMel2 cells revealed a moderate increase in the intracellular melanin level independently of de novo melanogenesis, pointing to a partial hindrance in melanin release. Immunofluorescence images of NHEM and MaMel2 cells visualized co-localization of LASP1 with dynamin and tyrosinase concomitant with melanosomes at the dendrite tips of the cells. Melanosome isolation experiments by sucrose density gradient centrifugation clearly demonstrated the presence of LASP1 and the melanosome specific markers tyrosinase and TRP1 in late stage melanosomes. The study identified LASP1 and dynamin as novel binding partners in melanocytes and provides first evidence for the existence of LASP1 and dynamin (a protein well–known for its involvement in vesicle formation and budding) in melanosomes. Co-localization of LASP1 and dynamin along the dendrites and at the tips of the melanocytes indicates a potential participation of the two proteins in the membrane vesicle fission at the plasma membrane. In summary, a possible involvement of LASP1 in the actin–dynamin mediated membrane fission and exocytosis of melanin laden melanosome vesicles into the extracellular matrix is suggested. N2 - LIM und SH3 protein 1 (LASP1) ist ein nukleozytoplasmatischen Gerüstprotein. LASP1 interagiert über seine Domänenstruktur mit verschiedenen Zytoskelettproteinen und ist an physiologischen Prozessen wie Migration und Zellproliferation beteiligt. In der vorliegenden Studie wurde eine detaillierte Untersuchung des Expressionsmusters von LASP1 in normale Haut, Nävi und Melanom durchgeführt und die Melanozyten-spezifische Funktion des Proteins analysiert. LASP1 konnte durch immunhistologische Färbungen im Stratum basale der Epidermis und in hoher Konzentration in Nävi (gutartige Tumore der Melanozyten) nachgewiesen werden, während die Expression in Melanom und Metastasen sehr gering ist. Auch wurde kein signifikanter Zusammenhang zwischen der LASP1 Proteinexpression in Melanomen und den klinisch-pathologischen Parametern bei 58 Patienten festgestellt. Dies steht im Gegensatz zu allen bisher getesteten Tumoren (u.a. Brust, HCC und Medulloblastom), bei der eine erhöhte LASP1 Expression in den Tumoren beobachtet wurde, die mit dem Tumorgrad korrelierte. Die hochproliferativen Basalzellen der Epidermis bestehen aus Keratinozyten und Melanozyten und weisen, im Gegensatz zu Nävi und Melanomzellen, eine deutliche Kernlokalisation des LASP1 Proteins auf. Melanozyten sind spezialisierte Zellen, die das UV-Schutzfarbpigment Melanin in einzigartigen Organellen, genannt Melanosomen, synthetisieren. Die Expression von LASP1 in diesen Melanozyten konnte zum ersten Mal in dieser Studie nachgewiesen werden. Immunfluoreszenzaufnahmen und Western Blots mit kultivierten normalen menschlichen epidermalen Melanozyten (NHEM) und Melanom-Zelllinien bestätigen die LASP1 Expression. Funktionelle Experimente mit LASP1 depletierten Zellen zeigen eine erhöhte Melaninkonzentration, die unabhängig von der de novo Melanogenese ist. Immunfluoreszenaufnahmen visualisieren eine Ko-Lokalisation von LASP1 mit Tyrosinase an den Melanosomen in den Zellausläufern von pigmentierten MaMel2 Zellen. Eine Auftrennung der einzelnen Melanosomenstadien durch Saccharose-Dichtegradienten-Zentrifugation erlauben die Detektion von LASP1 mit Dynamin, TRP1 und Tyrosinase in späten Stadium IV Melanosomen. Die vorliegende Studie liefert den ersten Beweis für die Existenz von Dynamin (einem für die Vesikelbildung essentiellem Protein) in Melanosomen und identifiziert Dynamin als neuartigen Bindungspartner von LASP1 in Melanozyten. Die Ko-Lokalisierung LASP1 und Dynamin entlang der Dendriten und in den Spitzen der Melanozyten weist auf eine mögliche Beteiligung beider Proteine an der Melanosomen-Vesikel-Abspaltung an der Plasmamembran hin. Zusammenfassend lässt sich sagen, dass LASP1 an der Actin-Dynamin vermittelten Exocytose von Melanin-beladenen Melanosomvesikeln in die Extrazellulärmatrix beteiligt ist. KW - Melanom KW - Melanin KW - LASP1 KW - melanocytic nevi KW - melanoma cancer KW - Molekularbiologie KW - Melanin release Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-116316 ER - TY - JOUR A1 - Andronic, Joseph A1 - Shirakashi, Ryo A1 - Pickel, Simone U. A1 - Westerling, Katherine M. A1 - Klein, Teresa A1 - Holm, Thorge A1 - Sauer, Markus A1 - Sukhorukov, Vladimir L. T1 - Hypotonic Activation of the Myo-Inositol Transporter SLC5A3 in HEK293 Cells Probed by Cell Volumetry, Confocal and Super-Resolution Microscopy JF - PLoS One N2 - Swelling-activated pathways for myo-inositol, one of the most abundant organic osmolytes in mammalian cells, have not yet been identified. The present study explores the SLC5A3 protein as a possible transporter of myo-inositol in hyponically swollen HEK293 cells. To address this issue, we examined the relationship between the hypotonicity-induced changes in plasma membrane permeability to myo-inositol Pino [m/s] and expression/localization of SLC5A3. Pino values were determined by cell volumetry over a wide tonicity range (100–275 mOsm) in myo-inositol-substituted solutions. While being negligible under mild hypotonicity (200–275 mOsm), Pino grew rapidly at osmolalities below 200 mOsm to reach a maximum of ∼3 nm/s at 100–125 mOsm, as indicated by fast cell swelling due to myo-inositol influx. The increase in Pino resulted most likely from the hypotonicity-mediated incorporation of cytosolic SLC5A3 into the plasma membrane, as revealed by confocal fluorescence microscopy of cells expressing EGFP-tagged SLC5A3 and super-resolution imaging of immunostained SLC5A3 by direct stochastic optical reconstruction microscopy (dSTORM). dSTORM in hypotonic cells revealed a surface density of membrane-associated SLC5A3 proteins of 200–2000 localizations/μm2. Assuming SLC5A3 to be the major path for myo-inositol, a turnover rate of 80–800 myo-inositol molecules per second for a single transporter protein was estimated from combined volumetric and dSTORM data. Hypotonic stress also caused a significant upregulation of SLC5A3 gene expression as detected by semiquantitative RT-PCR and Western blot analysis. In summary, our data provide first evidence for swelling-mediated activation of SLC5A3 thus suggesting a functional role of this transporter in hypotonic volume regulation of mammalian cells. KW - electrolytes KW - isotonic KW - membrane proteins KW - cell membranes KW - hypotonic KW - hypotonic solutions KW - tonicity KW - permeability Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-126408 VL - 10 IS - 3 ER - TY - JOUR A1 - Andreatta, Marta A1 - Pauli, Paul T1 - Appetitive vs. aversive conditioning in humans JF - Frontiers in Behavioral Neuroscience N2 - In classical conditioning, an initially neutral stimulus (conditioned stimulus, CS) becomes associated with a biologically salient event (unconditioned stimulus, US), which might be pain (aversive conditioning) or food (appetitive conditioning). After a few associations, the CS is able to initiate either defensive or consummatory responses, respectively. Contrary to aversive conditioning, appetitive conditioning is rarely investigated in humans, although its importance for normal and pathological behaviors (e.g., obesity, addiction) is undeniable. The present study intents to translate animal findings on appetitive conditioning to humans using food as an US. Thirty-three participants were investigated between 8 and 10 am without breakfast in order to assure that they felt hungry. During two acquisition phases, one geometrical shape (avCS+) predicted an aversive US (painful electric shock), another shape (appCS+) predicted an appetitive US (chocolate or salty pretzel according to the participants' preference), and a third shape (CS) predicted neither US. In a extinction phase, these three shapes plus a novel shape (NEW) were presented again without US delivery. Valence and arousal ratings as well as startle and skin conductance (SCR) responses were collected as learning indices. We found successful aversive and appetitive conditioning. On the one hand, the avCS+ was rated as more negative and more arousing than the CS and induced startle potentiation and enhanced SCR. On the other hand, the appCS+ was rated more positive than the CS and induced startle attenuation and larger SCR. In summary, we successfully confirmed animal findings in (hungry) humans by demonstrating appetitive learning and normal aversive learning. KW - extinction KW - attention KW - classical conditioning KW - skin conductance response KW - punishment KW - startle reflex KW - reward KW - fear KW - startle KW - model Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-148614 VL - 9 IS - 128 ER - TY - JOUR A1 - Andersen, Jens Peter A1 - Bøgsted, Martin A1 - Dybkær, Karen A1 - Mellqvist, Ulf-Henrik A1 - Morgan, Gareth J. A1 - Goldschmidt, Hartmut A1 - Dimopoulos, Meletios A. A1 - Einsele, Hermann A1 - San Miguel, Jesús A1 - Palumbo, Antonio A1 - Sonneveld, Pieter A1 - Johnsen, Hans Erik T1 - Global myeloma research clusters, output, and citations: a bibliometric mapping and clustering analysis JF - PLoS ONE N2 - Background International collaborative research is a mechanism for improving the development of disease-specific therapies and for improving health at the population level. However, limited data are available to assess the trends in research output related to orphan diseases. Methods and Findings We used bibliometric mapping and clustering methods to illustrate the level of fragmentation in myeloma research and the development of collaborative efforts. Publication data from Thomson Reuters Web of Science were retrieved for 2005-2009 and followed until 2013. We created a database of multiple myeloma publications, and we analysed impact and co-authorship density to identify scientific collaborations, developments, and international key players over time. The global annual publication volume for studies on multiple myeloma increased from 1,144 in 2005 to 1,628 in 2009, which represents a 43% increase. This increase is high compared to the 24% and 14% increases observed for lymphoma and leukaemia. The major proportion (> 90% of publications) was from the US and EU over the study period. The output and impact in terms of citations, identified several successful groups with a large number of intra-cluster collaborations in the US and EU. The US-based myeloma clusters clearly stand out as the most productive and highly cited, and the European Myeloma Network members exhibited a doubling of collaborative publications from 2005 to 2009, still increasing up to 2013. Conclusion and Perspective Multiple myeloma research output has increased substantially in the past decade. The fragmented European myeloma research activities based on national or regional groups are progressing, but they require a broad range of targeted research investments to improve multiple myeloma health care. KW - multiparametric flow cytometry KW - multiple myeloma KW - consensus statement KW - European experts KW - disorders KW - therapy KW - network Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-144214 VL - 10 IS - 1 ER - TY - JOUR A1 - Ammar, Mohamed Raafet A1 - Thahouly, Tamou A1 - Hanauer, André A1 - Stegner, David A1 - Nieswandt, Bernhard A1 - Vitale, Nicolas T1 - PLD1 participates in BDNF-induced signalling in cortical neurons JF - Scientific Reports N2 - The brain-derived neurotrophic factor BDNF plays a critical role in neuronal development and the induction of L-LTP at glutamatergic synapses in several brain regions. However, the cellular and molecular mechanisms underlying these BDNF effects have not been firmly established. Using in vitro cultures of cortical neurons from knockout mice for Pld1 and Rsk2, BDNF was observed to induce a rapid RSK2-dependent activation of PLD and to stimulate BDNF ERK1/2-CREB and mTor-S6K signalling pathways, but these effects were greatly reduced in Pld1\(^{-/-}\) neurons. Furthermore, phospho-CREB did not accumulate in the nucleus, whereas overexpression of PLD1 amplified the BDNF-dependent nuclear recruitment of phospho-ERK1/2 and phospho-CREB. This BDNF retrograde signalling was prevented in cells silenced for the scaffolding protein PEA15, a protein which complexes with PLD1, ERK1/2, and RSK2 after BDNF treatment. Finally PLD1, ERK1/2, and RSK2 partially colocalized on endosomal structures, suggesting that these proteins are part of the molecular module responsible for BDNF signalling in cortical neurons. KW - phospholipase D KW - ERK map kinease KW - long-term potentation KW - brain KW - protein RSK2 KW - dendritic growth KW - neurite outgrowth KW - neurotrophic factor KW - coffin-lowry-syndrome KW - phosphatidic acid Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-139962 VL - 5 IS - 14778 ER - TY - THES A1 - Ames, Christopher T1 - Molecular Beam Epitaxy of 2D and 3D HgTe, a Topological Insulator T1 - Molekularstrahlepitaxie von 2D und 3D HgTe, ein topologischer Isolator N2 - In the present thesis the MBE growth and sample characterization of HgTe structures is investigated and discussed. Due to the first experimental discovery of the quantum Spin Hall effect (QSHE) in HgTe quantum wells, this material system attains a huge interest in the spintronics society. Because of the long history of growing Hg-based heterostructures here at the Experimentelle Physik III in Würzburg, there are very good requirements to analyze this material system more precisely and in new directions. Since in former days only doped HgTe quantum wells were grown, this thesis deals with the MBE growth in the (001) direction of undoped HgTe quantum wells, surface located quantum wells and three dimensional bulk layers. All Hg-based layers were grown on CdTe substrates which generate strain in the layer stack and provide therefore new physical effects. In the same time, the (001) CdTe growth was investigated on n-doped (001) GaAs:Si because the Japanese supplier of CdTe substrates had a supply bottleneck due to the Tohoku earthquake and its aftermath in 2011. After a short introduction of the material system, the experimental techniques were demonstrated and explained explicitly. After that, the experimental part of this thesis is displayed. So, the investigation of the (001) CdTe growth on (001) GaAs:Si is discussed in chapter 4. Firstly, the surface preparation of GaAs:Si by oxide desorption is explored and analyzed. Here, rapid thermal desorption of the GaAs oxide with following cool down in Zn atmosphere provides the best results for the CdTe due to small holes at the surface, while e.g. an atomic flat GaAs buffer deteriorates the CdTe growth quality. The following ZnTe layer supplies the (001) growth direction of the CdTe and exhibits best end results of the CdTe for 30 seconds growth time at a flux ratio of Zn/Te ~ 1/1.2. Without this ZnTe layer, CdTe will grow in the (111) direction. However, the main investigation is here the optimization of the MBE growth of CdTe. The substrate temperature, Cd/Te flux ratio and the growth time has to be adjusted systematically. Therefore, a complex growth process is developed and established. This optimized CdTe growth process results in a RMS roughness of around 2.5 nm and a FWHM value of the HRXRD w-scan of 150 arcsec. Compared to the literature, there is no lower FWHM value traceable for this growth direction. Furthermore, etch pit density measurements show that the surface crystallinity is matchable with the commercial CdTe substrates (around 1x10^4 cm^(-2)). However, this whole process is not completely perfect and offers still room for improvements. The growth of undoped HgTe quantum wells was also a new direction in research in contrast to the previous n-doped grown HgTe quantum wells. Here in chapter 5, the goal of very low carrier densities was achieved and therefore it is now possible to do transport experiments in the n - and p - region by tuning the gate voltage. To achieve this high sample quality, very precise growth of symmetric HgTe QWs and their HRXRD characterization is examined. Here, the quantum well thickness can now determined accurate to under 0.3 nm. Furthermore, the transport analysis of different quantum well thicknesses shows that the carrier density and mobility increase with rising HgTe layer thickness. However, it is found out that the band gap of the HgTe QW closes indirectly at a thickness of 11.6 nm. This is caused by the tensile strained growth on CdTe substrates. Moreover, surface quantum wells are studied. These quantum wells exhibit no or a very thin HgCdTe cap. Though, oxidization and contamination of the surface reduces here the carrier mobility immensely and a HgCdTe layer of around 5 nm provides the pleasing results for transport experiments with superconductors connected to the topological insulator [119]. A completely new achievement is the realization of MBE growth of HgTe quantum wells on CdTe/GaAs:Si substrates. This is attended by the optimization of the CdTe growth on GaAs:Si. It exposes that HgTe quantum wells grown in-situ on optimized CdTe/GaAs:Si show very nice transport data with clear Hall plateaus, SdH oscillations, low carrier densities and carrier mobilities up to 500 000 cm^2/Vs. Furthermore, a new oxide etching process is developed and analyzed which should serve as an alternative to the standard HCl process which generates volcano defects at some time. However, during the testing time the result does not differ in Nomarski, HRXRD, AFM and transport measurements. Here, long-time tests or etching and mounting in nitrogen atmosphere may provide new elaborate results. The main focus of this thesis is on the MBE growth and standard characterization of HgTe bulk layers and is discussed in chapter 6. Due to the tensile strained growth on lattice mismatched CdTe, HgTe bulk opens up a band gap of around 22 meV at the G-point and exhibits therefore its topological surface states. The analysis of surface condition, roughness, crystalline quality, carrier density and mobility via Nomarski, AFM, XPS, HRXRD and transport measurements is therefore included in this work. Layer thickness dependence of carrier density and mobility is identified for bulk layer grown directly on CdTe substrates. So, there is no clear correlation visible between HgTe layer thickness and carrier density or mobility. So, the carrier density is almost constant around 1x10^11 cm^(-2) at 0 V gate voltage. The carrier mobility of these bulk samples however scatters between 5 000 and 60 000 cm^2/Vs almost randomly. Further experiments should be made for a clearer understanding and therefore the avoidance of unusable bad samples.But, other topological insulator materials show much higher carrier densities and lower mobility values. For example, Bi2Se3 exhibits just density values around 1019 cm^(-2) and mobility values clearly below 5000 cm2/Vs. The carrier density however depends much on lithography and surface treatment after growth. Furthermore, the relaxation behavior and critical thickness of HgTe grown on CdTe is determined and is in very good agreement with theoretical prediction (d_c = 155 nm). The embedding of the HgTe bulk layer between HgCdTe layers created a further huge improvement. Similar to the quantum well structures the carrier mobility increases immensely while the carrier density levels at around 1x10^11 cm^(-2) at 0 V gate voltage as well. Additionally, the relaxation behavior and critical thickness of these barrier layers has to be determined. HgCdTe grown on commercial CdTe shows a behavior as predicted except the critical thickness which is slightly higher than expected (d_c = 850 nm). Otherwise, the relaxation of HgCdTe grown on CdTe/GaAs:Si occurs in two parts. The layer is fully strained up to 250 nm. Between 250 nm and 725 nm the HgCdTe film starts to relax randomly up to 10 %. The relaxation behavior for thicknesses larger than 725 nm occurs than linearly to the inverse layer thickness. A explanation is given due to rough interface conditions and crystalline defects of the CdTe/GaAs:Si compared to the commercial CdTe substrate. HRXRD and AFM data support this statement. Another point is that the HgCdTe barriers protect the active HgTe layer and because of the high carrier mobilities the Hall measurements provide new transport data which have to be interpreted more in detail in the future. In addition, HgTe bulk samples show very interesting transport data by gating the sample from the top and the back. It is now possible to manipulate the carrier densities of the top and bottom surface states almost separately. The back gate consisting of the n-doped GaAs substrate and the thick insulating CdTe buffer can tune the carrier density for Delta(n) ~ 3x10^11 cm^(-2). This is sufficient to tune the Fermi energy from the p-type into the n-type region [138]. In this thesis it is shown that strained HgTe bulk layers exhibit superior transport data by embedding between HgCdTe barrier layers. The n-doped GaAs can here serve as a back gate. Furthermore, MBE growth of high crystalline, undoped HgTe quantum wells shows also new and extended transport output. Finally, it is notable that due to the investigated CdTe growth on GaAs the Hg-based heterostructure MBE growth is partially independent from commercial suppliers. N2 - In der vorliegenden Dissertation wurde das MBE-Wachstum von HgTe Strukturen erforscht und die anschließende Probencharakterisierung durchgeführt und diskutiert. Durch die erste experimentelle Entdeckung des Quanten-Spin-Hall-Effekts (QSHE) in HgTe Quantentrögen hat dieses Materialsystem großes Interesse im Gebiet der Spintronics erfahren. Aufgrund der langen Wachstumshistorie von quecksilberbasierenden Heterostrukturen am Lehrstuhl Experimentelle Physik III der Universität Würzburg sind die Voraussetzungen ausgesprochen gut, um dieses Materialsystem sehr ausführlich und auch in neue Richtungen hin zu untersuchen. Da vor dieser Doktorarbeit fast ausschließlich dotierte HgTe Quantentröge auf verschiedenen Substratorientierungen gewachsen wurden, beschäftigte sich diese Dissertation nun mit dem MBE-Wachstum von undotierten HgTe Quantentrögen, oberflächennahen Quantentrögen und dreidimensionalen Volumenkristallen. Alle quecksilberbasierenden Schichten wurden hierzu auf CdTe Substraten gewachsen, welche tensile Verspannung in den Schichten erzeugten und lieferten daher neue physikalische Effekte. In der selben Zeit wurde weiterhin das Wachstum von (001) CdTe auf n-dotiertem (001) GaAs:Si erforscht, da der japanische Zulieferer der CdTe Substrate eine Lieferengpass hatte aufgrund des Tohoku Erdbebens und seinen verheerenden Folgen im Jahr 2011. Die Erforschung des MBE-Wachstums von (001) CdTe auf (001) GaAs:Si wird im Kapitel 4 behandelt. Zuerst wurde hier die Oberflächenvorbereitung des GaAs:Si Substrates durch thermische Desorption untersucht und ausgewertet. Es stellte sich heraus, dass schnelle, thermische Desorption des GaAs - Oxides mit anschließendem Abkühlen in Zn Atmosphäre die besten Ergebnisse für das spätere CdTe durch kleine Löcher an der Oberfläche liefert, während zum Beispiel ein glatter GaAs Puffer das CdTe Wachstum verschlechtert. Der folgende ZnTe Film verschafft die gewünschte (001) Wachstumsrichtung für CdTe und weist bei 30 Sekunden Wachstumszeit bei einem Flussverhältnis von Zn/Te ~ 1/1.2 die besten Endergebnisse für CdTe auf. Jedoch war die Haupterneuerung hier die Optimierung des CdTe Wachstums. Dafür wurde ein komplexer Wachstumsprozess entwickelt und etabliert. Dieser optimierte CdTe Wachstumsprozess lieferte Ergebnisse von einer RMS Rauigkeit von ungefähr 2.5 nm und FWHMWerte der HRXRD w-Scans von 150 arcsec. Die Defektätzdichte-Messung zeigte weiterhin, dass die Oberflächenkristallinität vergleichbar mit kommerziell erwerbbaren CdTe Substraten ist (um 1x10^4 cm^(-2)). Des Weiteren ist kein niedrigerer Wert für die Halbwertsbreite des w-Scans in der Literatur für diese Wachstumsrichtung aufgeführt. Dies spiricht ebenfalls für die hohe Qualität der Schichten. Jedoch ist dieser Wachstumsprozess noch nicht endgültig ausgereift und bietet weiterhin noch Platz für Verbesserungen. Das Wachstum von undotierten HgTe Quantentrögen war ebenso eine neue Forschungsrichtung im Gegensatz zu den dotierten HgTe Quantentrögen, die in der Vergangenheit gewachsen wurden. Das Ziel hierbei, die Ladungsträgerdichte zu verringern, wurde erreicht und daher ist es nun möglich, Transportexperimente sowohl im n- als auch im p-Regime durchzuführen, indem eine Gatespannung angelegt wird. Des Weiteren experimentierten andere Arbeitsgruppen mit diesen Quantentrögen, bei denen die Fermi Energie in der Bandlücke liegt [143]. Außerdem wurde das sehr präzise MBE Wachstum anhand von symmetrischen HgTe Quantentrögen und ihren HRXRD Charakterisierungen behandelt. Daher kann nun die Quantentrogdicke präzise auf 0,3 nm angegeben werden. Die Transportergebnisse von verschieden dicken Quantentrögen zeigten, dass die Ladungsträgerdichte und Beweglichkeit mit steigender HgTe Schichtdicke zunimmt. Jedoch wurde auch herausgefunden, dass sich die Bandlücke von HgTe Quantentrögen indirekt bei einer Dicke von 11.6 nm schließt. Dies wird durch das verspannte Wachstum auf CdTe Substraten verursacht. Überdies wurden oberflächennahe Quantentröge untersucht. Diese Quantentröge besitzen keine oder nur eine sehr dünne HgCdTe Deckschicht. Allerdings verringerte Oxidation und Oberflächenverschmutzung hier die Ladungsträgerbeweglichkeit dramatisch und eine HgCdTe Schicht von ungefähr 5 nm lieferte ansprechende Transportergebnisse für Supraleiter, die den topologischen Isolator kontaktieren. Eine komplett neue Errungenschaft war die Realisierung, via MBE, HgTe Quantentröge auf CdTe/GaAs:Si Substrate zu wachsen. Dies ging einher mit der Optimierung des CdTe Wachstums auf GaAs:Si. Es zeigte sich, dass HgTe Quantentröge, die in-situ auf optimierten CdTe/GaAs:Si gewachsen wurden, sehr schöne Transportergebnisse mit deutlichen Hall Quantisierungen, SdH Oszillationen, niedrigen Ladungsträgerdichten und Beweglichkeiten bis zu 500 000 cm^2/Vs erreichen. Des Weiteren wurde ein neues Oxidätzverfahren entwickelt und untersucht, welches als Alternative zum Standard-HCl-Prozess dienen sollte, da dieses manchmal vulkan-artige Defekte hervorruft. Jedoch ergab sich kein Unterschied in den Nomarski, HRXRD, AFM und Transportexperimenten. Hier könnten vielleicht Langzeittests oder Ätzen und Befestigen in Stickstoffatmosphäre neue, gewinnbringende Ergbnisse aufzeigen. Der Hauptfokus dieser Doktorarbeit lag auf dem MBE Wachstum und der Standardcharakterisierung von HgTe Volumenkristallen und wurde in Kapitel 6 diskutiert. Durch das tensil verpannte Wachstum auf CdTe entsteht für HgTe als Volumenkristall eine Bandlücke von ungefähr 22 meV am G Punkt und zeigt somit seine topologischen Oberflächenzustände. Die Analyse der Oberfächenbeschaffenheit, der Rauigkeit, der kristallinen Qualität, der Ladungsdrägerdichte und Beweglichkeit mit Hilfe von Nomarski, AFM, XPS, HRXRD und Transportmessungen ist in dieser Arbeit anzutreffen. Außerdem wurde die Schichtdickenabhängigkeit von Ladungsträgerdichte und Beweglichkeit von HgTe Volumenkristallen, die direkt auf CdTe Substraten gewachsen wurden, ermittelt worden. So erhöhte sich durchschnittlich die Dichte und Beweglichkeit mit zunehmender HgTe Schichtdicke, aber die Beweglichkeit ging selten über μ ~ 40 000 cm^2/Vs hinaus. Die Ladungsträgerdichte n hing jedoch sehr von der Litographie und der Behandlung der Oberfläche nach dem Wachstum ab. Des Weiteren wurde das Relaxationsverhalten und die kritische Dicke bestimmt, welches sehr gut mit den theoretischen Vorhersagen übereinstimmt (dc = 155 nm). Das Einbetten des HgTe Volumenkristalls in HgCdTe Schichten brachte eine weitere große Verbesserung mit sich. Ähnlich wie bei den Quantentrögen erhörte sich die Beweglichkeit μ immens, während sich die Ladungsträgerdichte bei ungefähr 1x10^11 cm^(-2) einpendelte. Zusätzlich wurde auch hier das Relaxationsverhalten und die kritische Schichtdicke dieser Barrierenschichten ermittelt. HgCdTe, gewachsen auf kommerziellen CdTe Substraten, zeigte ein Verhalten ähnlich zu dem Erwarteten mit der Ausnahme, dass die kritische Schichtdicke leicht höher ist als die Vorhergesagte (dc = 850 nm). Auf der anderen Seite findet die Relaxation von HgCdTe auf CdTe/GaAs:Si zweigeteilt ab. Bis 250 nm ist die Schicht noch voll verspannt. Zwischen 250 nm und 725 nm beginnt die HgCdTe Schicht willkürlich bis zu 10 % zu relaxieren. Das Relaxationsverhalten für Dicken über 725 nm findet dann wieder linear zur invers aufgetragenen Schichtdicke statt. Eine Erklärung wurde durch das raue Interface der Schichten und der Defekte im Kristall von CdTe/GaAs:Si gegeben, im Vergleich zu den kommerziellen CdTe Substraten. HRXRD und AFM Ergebnisse belegten diese Aussage. Die HgCdTe Barrieren schützen die aktive HgTe Schicht und daher liegen nach Hall Messungen aufgrund der hohen Ladungsträgerbeweglichkeiten neue Transportergbnisse vor, welche in der Zukunft ausführlicher interpretiert werden müssen. Darüber hinaus zeigten HgTe Volumenkristalle neue, interessante Transportergebnisse durch das gleichzeitige Benutzen eines Top- und Backgates. Es ist nun möglich, die Ladungsträger der oberen und unteren Oberflächenzustände nahezu getrennt zu verändern und zu ermitteln. Das Backgate, bestehend aus dem n-dotierten GaAs:Si Substrate und dem dicken isolierenden CdTe Puffer, kann die Ladungsträgerdichte um ungefähr Delta(n) ~ 3x10^11 cm^(-2) varieren. Das ist ausreichend, um die Fermi Energie vom p- in den n-Bereich einzustellen [138]. In dieser Dissertation wurde also gezeigt, dass verspannte HgTe Volumenkristalle durch das Einbetten in HgCdTe Barrieren neue Transportergebnisse liefern. Das n-dotierte GaAs konnte hierbei als Backgate genutzt werden. Des Weiteren zeigte das MBE Wachstum von hochkristallinen , undotiereten HgTe Quantentrögen ebenso neue und erweiterte Transportergebnisse. Zuletzt ist es bemerkenswert, dass durch das erforschte CdTe Wachstum auf GaAs das MBE Wachstum von quecksilberbasierenden Heterostrukturen auf CdTe Substraten teilweise unabhänigig ist von kommerziellen Zulieferbetrieben. KW - Quecksilbertellurid KW - Topologischer Isolator KW - MBE KW - HgTe KW - topological insulator KW - Molekularstrahlepitaxie Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-151136 ER - TY - JOUR A1 - Altenburger, Roland T1 - Cao, Juan: In der Sackgasse oder auf dem Weg zu einem neuen Paradigma? Die Erforschung des Romans Der Traum der roten Kammer (Rotologie) im 21. Jahrhundert (Lun Wen: Studien zur Geistesgeschichte und Literatur in China; 17). Wiesbaden: Harrassowitz Verlag, 2013. XII, 256 S. ISBN 978-3-447-06992-2 JF - Asiatische Studien - Études Asiatiques N2 - No abstract available. KW - Rezension Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-193941 SN - 0004-4717 SN - 2235-5871 N1 - Dieser Beitrag ist mit Zustimmung des Rechteinhabers aufgrund einer (DFG-geförderten) Allianz- bzw. Nationallizenz frei zugänglich. VL - 69 IS - 1 ER - TY - JOUR A1 - Alizadehrad, Davod A1 - Krüger, Timothy A1 - Engstler, Markus A1 - Stark, Holger T1 - Simulating the complex cell design of Trypanosoma brucei and its motility JF - PLOS Computational Biology N2 - The flagellate Trypanosoma brucei, which causes the sleeping sickness when infecting a mammalian host, goes through an intricate life cycle. It has a rather complex propulsion mechanism and swims in diverse microenvironments. These continuously exert selective pressure, to which the trypanosome adjusts with its architecture and behavior. As a result, the trypanosome assumes a diversity of complex morphotypes during its life cycle. However, although cell biology has detailed form and function of most of them, experimental data on the dynamic behavior and development of most morphotypes is lacking. Here we show that simulation science can predict intermediate cell designs by conducting specific and controlled modifications of an accurate, nature-inspired cell model, which we developed using information from live cell analyses. The cell models account for several important characteristics of the real trypanosomal morphotypes, such as the geometry and elastic properties of the cell body, and their swimming mechanism using an eukaryotic flagellum. We introduce an elastic network model for the cell body, including bending rigidity and simulate swimming in a fluid environment, using the mesoscale simulation technique called multi-particle collision dynamics. The in silico trypanosome of the bloodstream form displays the characteristic in vivo rotational and translational motility pattern that is crucial for survival and virulence in the vertebrate host. Moreover, our model accurately simulates the trypanosome's tumbling and backward motion. We show that the distinctive course of the attached flagellum around the cell body is one important aspect to produce the observed swimming behavior in a viscous fluid, and also required to reach the maximal swimming velocity. Changing details of the flagellar attachment generates less efficient swimmers. We also simulate different morphotypes that occur during the parasite's development in the tsetse fly, and predict a flagellar course we have not been able to measure in experiments so far. KW - multiparticle collision dynamics KW - human african trypanosomiasis KW - biology KW - cytoskeleton KW - flow KW - flagellar motility KW - tsetse fly KW - propulsion KW - cytokinesis KW - parasites Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-144610 VL - 11 IS - 1 ER - TY - CHAP A1 - Ali, Qasim A1 - Montenegro, Sergio T1 - A Simple Approach to Quadrocopter Formation Flying Test Setup for Education and Development T2 - INTED2015 Proceedings N2 - A simple test setup has been developed at Institute of Aerospace Information Technology, University of Würzburg, Germany to realize basic functionalities for formation flight of quadrocopters. The test environment is planned to be utilized for developing and validating the algorithms for formation flying capability in real environment as well as for education purpose. An already existing test bed for single quadrocopter was extended with necessary inter-communication and distributed control mechanism to test the algorithms for formation flights in 2 degrees of freedom (roll / pitch). This study encompasses the domain of communication, control engineering and embedded systems programming. Bluetooth protocol has been used for inter-communication between two quadrocopters. A simple approach of PID control in combination with Kalman filter has been exploited. MATLAB Instrument Control Toolbox has been used for data display, plotting and analysis. Plots can be drawn in real-time and received information can also be stored in the form of files for later use and analysis. The test setup has been developed indigenously and at considerably low cost. Emphasis has been placed on simplicity to facilitate students learning process. Several lessons have been learnt during the course of development of this setup. Proposed setup is quite flexible that can be modified as per changing requirements. KW - Flugkörper KW - Design and Development KW - Formation Flight KW - Instrument Control Toolbox KW - Quadrocopter KW - Unmanned Aerial Vehicle KW - Quadrocopter Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-114495 SN - 978-84-606-5763-7 SN - 2340-1079 SP - 2776 EP - 2784 PB - International Academy of Technology, Education and Development (IATED) ER - TY - JOUR A1 - Alavipanah, Sadroddin A1 - Wegmann, Martin A1 - Qureshi, Salman A1 - Weng, Qihao A1 - Koellner, Thomas T1 - The role of vegetation in mitigating urban land surface temperatures: a case study of Munich, Germany during the warm season JF - Sustainability N2 - The Urban Heat Island (UHI) is the phenomenon of altered increased temperatures in urban areas compared to their rural surroundings. UHIs grow and intensify under extreme hot periods, such as during heat waves, which can affect human health and also increase the demand for energy for cooling. This study applies remote sensing and land use/land cover (LULC) data to assess the cooling effect of varying urban vegetation cover, especially during extreme warm periods, in the city of Munich, Germany. To compute the relationship between Land Surface Temperature (LST) and Land Use Land Cover (LULC), MODIS eight-day interval LST data for the months of June, July and August from 2002 to 2012 and the Corine Land Cover (CLC) database were used. Due to similarities in the behavior of surface temperature of different CLCs, some classes were reclassified and combined to form two major, rather simplified, homogenized classes: one of built-up area and one of urban vegetation. The homogenized map was merged with the MODIS eight-day interval LST data to compute the relationship between them. The results revealed that (i) the cooling effect accrued from urban vegetation tended to be non-linear; and (ii) a remarkable and stronger cooling effect in terms of LST was identified in regions where the proportion of vegetation cover was between seventy and almost eighty percent per square kilometer. The results also demonstrated that LST within urban vegetation was affected by the temperature of the surrounding built-up and that during the well-known European 2003 heat wave, suburb areas were cooler from the core of the urbanized region. This study concluded that the optimum green space for obtaining the lowest temperature is a non-linear trend. This could support urban planning strategies to facilitate appropriate applications to mitigate heat-stress in urban area. KW - Surface Urban Heat Island (SUHI) KW - cities KW - buildings KW - Land Surface Temperature (LST) KW - urban vegetation KW - climate change KW - heat waves Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-143447 VL - 7 ER - TY - JOUR A1 - Afonso-Grunz, Fabian A1 - Hoffmeier, Klaus A1 - Müller, Sören A1 - Westermann, Alexander J. A1 - Rotter, Björn A1 - Vogel, Jörg A1 - Winter, Peter A1 - Kahl, Günter T1 - Dual 3'Seq using deepSuperSAGE uncovers transcriptomes of interacting Salmonella enterica Typhimurium and human host cells JF - BMC Genomics N2 - Background: The interaction of eukaryotic host and prokaryotic pathogen cells is linked to specific changes in the cellular proteome, and consequently to infection-related gene expression patterns of the involved cells. To simultaneously assess the transcriptomes of both organisms during their interaction we developed dual 3'Seq, a tag-based sequencing protocol that allows for exact quantification of differentially expressed transcripts in interacting pro-and eukaryotic cells without prior fixation or physical disruption of the interaction. Results: Human epithelial cells were infected with Salmonella enterica Typhimurium as a model system for invasion of the intestinal epithelium, and the transcriptional response of the infected host cells together with the differential expression of invading and intracellular pathogen cells was determined by dual 3'Seq coupled with the next-generation sequencing-based transcriptome profiling technique deepSuperSAGE (deep Serial Analysis of Gene Expression). Annotation to reference transcriptomes comprising the operon structure of the employed S. enterica Typhimurium strain allowed for in silico separation of the interacting cells including quantification of polycistronic RNAs. Eighty-nine percent of the known loci are found to be transcribed in prokaryotic cells prior or subsequent to infection of the host, while 75% of all protein-coding loci are represented in the polyadenylated transcriptomes of human host cells. Conclusions: Dual 3'Seq was alternatively coupled to MACE (Massive Analysis of cDNA ends) to assess the advantages and drawbacks of a library preparation procedure that allows for sequencing of longer fragments. Additionally, the identified expression patterns of both organisms were validated by qRT-PCR using three independent biological replicates, which confirmed that RELB along with NFKB1 and NFKB2 are involved in the initial immune response of epithelial cells after infection with S. enterica Typhimurium. KW - complete genome sequence KW - secretion systems KW - RNA-Seq KW - deepSuperSAGE KW - transcriptome KW - gene expression KW - serovar Typhimurium KW - human macrophages KW - epithelial cells KW - infection KW - SuperSAGE KW - receptors KW - Dual 3'seq KW - MACE KW - tag based KW - simultaneous KW - genome wide KW - gene expression profiling KW - host pathogen interaction KW - Salmonella enterica Typhimurium strain SL1344 Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-143230 VL - 16 IS - 323 ER - TY - JOUR A1 - Adolfi, Mateus C. A1 - Carreira, Ana C. O. A1 - Jesus, Lázaro W. O. A1 - Bogerd, Jan A1 - Funes, Rejane M. A1 - Schartl, Manfred A1 - Sogayar, Mari C. A1 - Borella, Maria I. T1 - Molecular cloning and expression analysis of dmrt1 and sox9 during gonad development and male reproductive cycle in the lambari fish, Astyanax altiparanae JF - Reproductive Biology and Endocrinology N2 - Background The dmrt1 and sox9 genes have a well conserved function related to testis formation in vertebrates, and the group of fish presents a great diversity of species and reproductive mechanisms. The lambari fish (Astyanax altiparanae) is an important Neotropical species, where studies on molecular level of sex determination and gonad maturation are scarce. Methods Here, we employed molecular cloning techniques to analyze the cDNA sequences of the dmrt1 and sox9 genes, and describe the expression pattern of those genes during development and the male reproductive cycle by qRT-PCR, and related to histology of the gonad. Results Phylogenetic analyses of predicted amino acid sequences of dmrt1 and sox9 clustered A. altiparanae in the Ostariophysi group, which is consistent with the morphological phylogeny of this species. Studies of the gonad development revealed that ovary formation occurred at 58 days after hatching (dah), 2 weeks earlier than testis formation. Expression studies of sox9 and dmrt1 in different tissues of adult males and females and during development revealed specific expression in the testis, indicating that both genes also have a male-specific role in the adult. During the period of gonad sex differentiation, dmrt1 seems to have a more significant role than sox9. During the male reproductive cycle dmrt1 and sox9 are down-regulated after spermiation, indicating a role of these genes in spermatogenesis. Conclusions For the first time the dmrt1 and sox9 were cloned in a Characiformes species. We show that both genes have a conserved structure and expression, evidencing their role in sex determination, sex differentiation and the male reproductive cycle in A. altiparanae. These findings contribute to a better understanding of the molecular mechanisms of sex determination and differentiation in fish. KW - spermatogenesis KW - SOX9 KW - DMRT1 KW - sex differentiation KW - teleostei Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-126486 VL - 13 IS - 2 ER - TY - JOUR A1 - Adelfinger, Marion A1 - Bessler, Simon A1 - Cecil, Alexander A1 - Langbein-Laugwitz, Johanna A1 - Frentzen, Alexa A1 - Gentschev, Ivaylo A1 - Szalay, Aladar A. T1 - Preclinical Testing Oncolytic Vaccinia Virus Strain GLV-5b451 Expressing an Anti-VEGF Single-Chain Antibody for Canine Cancer Therapy JF - Viruses N2 - Virotherapy on the basis of oncolytic vaccinia virus (VACV) strains is a novel approach for canine cancer therapy. Here we describe, for the first time, the characterization and the use of VACV strain GLV-5b451 expressing the anti-vascular endothelial growth factor (VEGF) single-chain antibody (scAb) GLAF-2 as therapeutic agent against different canine cancers. Cell culture data demonstrated that GLV-5b451 efficiently infected and destroyed all four tested canine cancer cell lines including: mammary carcinoma (MTH52c), mammary adenoma (ZMTH3), prostate carcinoma (CT1258), and soft tissue sarcoma (STSA-1). The GLV-5b451 virus-mediated production of GLAF-2 antibody was observed in all four cancer cell lines. In addition, this antibody specifically recognized canine VEGF. Finally, in canine soft tissue sarcoma (CSTS) xenografted mice, a single systemic administration of GLV-5b451 was found to be safe and led to anti-tumor effects resulting in the significant reduction and substantial long-term inhibition of tumor growth. A CD31-based immuno-staining showed significantly decreased neo-angiogenesis in GLV-5b451-treated tumors compared to the controls. In summary, these findings indicate that GLV-5b451 has potential for use as a therapeutic agent in the treatment of CSTS. KW - canine cancer therapy KW - canine soft tissue sarcoma (CSTS) KW - oncolytic virus KW - cancer KW - canine cancer cell lines KW - antibody production KW - angiogenesis Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-125705 VL - 7 ER - TY - JOUR A1 - Abda, Ebrahim M. A1 - Krysciak, Dagmar A1 - Krohn-Molt, Ines A1 - Mamat, Uwe A1 - Schmeisser, Christel A1 - Förstner, Konrad U. A1 - Schaible, Ulrich E. A1 - Kohi, Thomas A. A1 - Nieman, Stefan A1 - Streit, Wolfgang R. T1 - Phenotypic Heterogeneity Affects Stenotrophomonas maltophilia K279a Colony Morphotypes and \(\beta\)-Lactamase Expression JF - Frontiers in Microbiology N2 - Phenotypic heterogeneity at the cellular level in response to various stresses, e.g., antibiotic treatment has been reported for a number of bacteria. In a clonal population, cell-to-cell variation may result in phenotypic heterogeneity that is a mechanism to survive changing environments including antibiotic therapy. Stenotrophomonas rnaltophilia has been frequently isolated from cystic fibrosis patients, can cause numerous infections in other organs and tissues, and is difficult to treat due to antibiotic resistances. S. maltophilia K279a produces the Li and L2 beta-lactamases in response to beta-lactam treatment. Here we report that the patient isolate S. rnaltophilia K279a diverges into cellular subpopulations with distinct but reversible morphotypes of small and big colonies when challenged with ampicillin. This observation is consistent with the formation of elongated chains of bacteria during exponential growth phase and the occurrence of mainly rod-shaped cells in liquid media. RNA-seq analysis of small versus big colonies revealed differential regulation of at least seven genes among the colony morphotypes. Among those, bleu and bla(L2) were transcriptionally the most strongly upregulated genes. Promoter fusions of b/a(L1) and b/a(L2) genes indicated that expression of both genes is also subject to high levels of phenotypic heterogeneous expression on a single cell level. Additionally, the comE homolog was found to be differentially expressed in homogenously versus heterogeneously bla(L2) expressing cells as identified by RNA(seq) analysis. Overexpression of cornE in S. maltophilia K279a reduced the level of cells that were in a bla(L2)-ON mode to 1% or lower. Taken together, our data provide strong evidence that S. maltophilia K279a populations develop phenotypic heterogeneity in an ampicillin challenged model. This cellular variability is triggered by regulation networks including b/a(L1), b/a(L2), and comE. KW - xanthomonas maltophilia KW - gram-negative bacteria KW - RNA-seq KW - pseudomas aeruginosa KW - antibiotic resistance KW - colony morphotypes KW - beta-lactamases KW - K279a KW - Stenotrophomonas maltophilia KW - phenotypic heterogeneity KW - persister cells KW - streptococcus pneumoniae KW - nosocomial pathogen KW - membrane vesicles KW - sinorhizobium fredii NGR234 KW - red fluorescent protein KW - escherichia coli Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-136446 VL - 6 IS - 1373 ER - TY - JOUR T1 - Search for dark matter in events with heavy quarks and missing transverse momentum in pp collisions with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - This article reports on a search for dark matter pair production in association with bottom or top quarks in 20.3 fb\(^{−1}\) of pp collisions collected at \(\sqrt {s}\) = 8 TeV by the ATLAS detector at the LHC. Events with large missing transverse momentum are selected when produced in association with high-momentum jets of which one or more are identified as jets containing b-quarks. Final states with top quarks are selected by requiring a high jet multiplicity and in some cases a single lepton. The data are found to be consistent with the Standard Model expectations and limits are set on the mass scale of effective field theories that describe scalar and tensor interactions between dark matter and Standard Model particles. Limits on the dark-matter–nucleon cross-section for spin-independent and spin-dependent interactions are also provided. These limits are particularly strong for low-mass dark matter. Using a simplified model, constraints are set on the mass of dark matter and of a coloured mediator suitable to explain a possible signal of annihilating dark matter. KW - dark matter KW - proton-proton collision KW - ATLAS detector Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150089 VL - 75 IS - 2 ER - TY - JOUR T1 - Search for Higgs boson pair production in the b\(\overline{b}\)b\(\overline{b}\) final state from pp collisions at \(\sqrt {s}\) = 8 TeV with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - A search for Higgs boson pair production pp → hh is performed with 19.5 fb\(^{−1}\) of proton–proton collision data at \(\sqrt {s}\) = 8 TeV, which were recorded by the ATLAS detector at the Large Hadron Collider in 2012. The decay products of each Higgs boson are reconstructed as a high-momentum b\(\overline{b}\) system with either a pair of small-radius jets or a single large-radius jet, the latter exploiting jet substructure techniques and associated b-tagged track-jets. No evidence for resonant or non-resonant Higgs boson pair production is observed. The data are interpreted in the context of the Randall–Sundrum model with a warped extra dimension as well as the two-Higgs-doublet model. An upper limit on the cross-section for pp → G\(^{*}_{KK}\) → hh → b\(\overline{b}\)b\(\overline{b}\) of 3.2(2.3) fb is set for a Kaluza–Klein graviton G\(^{*}_{KK}\) mass of 1.0(1.5) TeV, at the 95 % confidence level. The search for non-resonant Standard Model hh production sets an observed 95 % confidence level upper limit on the production cross-section σ(pp → hh → b\(\overline{b}\)b\(\overline{b}\)) of 202 fb, compared to a Standard Model prediction of σ(pp → hh → b\(\overline{b}\)b\(\overline{b}\)) = 3.6±0.5 fb. KW - Higgs boson KW - proton-proton collision KW - ATLAS detector KW - pair production Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150119 VL - 75 IS - 9 ER - TY - JOUR T1 - Search for invisible decays of the Higgs boson produced in association with a hadronically decaying vector boson in pp collisions at \(\sqrt {s}\) = TeV with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - A search for Higgs boson decays to invisible particles is performed using 20.3 fb\(^{−1}\) of pp collision data at a centre-of-mass energy of 8 TeV recorded by the ATLAS detector at the Large Hadron Collider. The process considered is Higgs boson production in association with a vector boson (V = W or Z) that decays hadronically, resulting in events with two or more jets and large missing transverse momentum. No excess of candidates is observed in the data over the background expectation. The results are used to constrain VH production followed by H decaying to invisible particles for the Higgs boson mass range 115 < m\(_{H}\) < 300 GeV. The 95 % confidence-level observed upper limit on σ\(_{VH}\) × BR(H → inv.) varies from 1.6 pb at 115 GeV to 0.13 pb at 300 GeV. Assuming Standard Model production and including the gg → H contribution as signal, the results also lead to an observed upper limit of 78 % at 95 % confidence level on the branching ratio of Higgs bosons decays to invisible particles at a mass of 125 GeV. KW - Higgs boson KW - ATLAS detector KW - decays Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150126 VL - 75 IS - 7 ER - TY - JOUR T1 - Search for invisible particles produced in association with single-top-quarks in proton-proton collisions at \(\sqrt {s}\) = 8 TeV with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - A search for the production of single-top-quarks in association with missing energy is performed in proton–proton collisions at a centre-of-mass energy of \(\sqrt {s}\) =8 TeV with the ATLAS experiment at the large hadron collider using data collected in 2012, corresponding to an integrated luminosity of 20.3 fb\(^{−1}\). In this search, the W boson from the top quark is required to decay into an electron or a muon and a neutrino. No deviation from the standard model prediction is observed, and upper limits are set on the production cross-section for resonant and non-resonant production of an invisible exotic state in association with a right-handed top quark. In the case of resonant production, for a spin-0 resonance with a mass of 500 GeV, an effective coupling strength above 0.15 is excluded at 95 % confidence level for the top quark and an invisible spin-1/2 state with mass between 0 and 100 GeV. In the case of non-resonant production, an effective coupling strength above 0.2 is excluded at 95 % confidence level for the top quark and an invisible spin-1 state with mass between 0 and 657 GeV. KW - single-top-quarks KW - proton-proton collision KW - ATLAS detector Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150134 VL - 75 IS - 2 ER - TY - JOUR T1 - Search for metastable heavy charged particles with large ionisation energy loss in pp collisions at \(\sqrt {s}\) = 8 TeV using the ATLAS experiment JF - European Physical Journal C: Particles and Fields N2 - Many extensions of the Standard Model predict the existence of charged heavy long-lived particles, such as R-hadrons or charginos. These particles, if produced at the Large Hadron Collider, should be moving non-relativistically and are therefore identifiable through the measurement of an anomalously large specific energy loss in the ATLAS pixel detector. Measuring heavy long-lived particles through their track parameters in the vicinity of the interaction vertex provides sensitivity to metastable particles with lifetimes from 0.6 ns to 30 ns. A search for such particles with the ATLAS detector at the Large Hadron Collider is presented, based on a data sample corresponding to an integrated luminosity of 18.4 fb\(^{−1}\) of pp collisions at \(\sqrt {s}\) = 8 TeV. No significant deviation from the Standard Model background expectation is observed, and lifetime-dependent upper limits on R-hadrons and chargino production are set. Gluino R-hadrons with 10 ns lifetime and masses up to 1185 GeV are excluded at 95 % confidence level, and so are charginos with 15 ns lifetime and masses up to 482 GeV. KW - ATLAS detector KW - charged heavy long-lived particles KW - proton-proton collision Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150149 VL - 75 IS - 9 ER - TY - JOUR T1 - Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at \(\sqrt {s}\) = 8 TeV with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb\(^{−1}\) of \(\sqrt {s}\) = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between E\(^{miss}_{T}\) > 150 GeV and E\(^{miss}_{T}\) > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presented. KW - ATLAS detector KW - energetic jet KW - proton-proton collision Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150152 VL - 75 IS - 7 ER - TY - JOUR T1 - Measurement of the production and lepton charge asymmetry of bosons in Pb+Pb collisions at \(\sqrt {^{S}NN}\) with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - A measurement of W boson production in lead-lead collisions at \(\sqrt {^{S}NN}\)=2.76 TeV is presented. It is based on the analysis of data collected with the ATLAS detector at the LHC in 2011 corresponding to an integrated luminosity of 0.14 nb\(^{-1}\) and 0.15 nb\(^{-1}\) in the muon and electron decay channels, respectively. The differential production yields and lepton charge asymmetry are each measured as a function of the average number of participating nucleons ⟨N\(_{part}\)⟩ and absolute pseudorapidity of the charged lepton. The results are compared to predictions based on next-to-leading-order QCD calculations. These measurements are, in principle, sensitive to possible nuclear modifications to the parton distribution functions and also provide information on scaling of W boson production in multi-nucleon systems. KW - Higgs boson KW - lead-lead collision Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-149889 VL - 75 IS - 1 ER - TY - JOUR T1 - Search for resonant diboson production in the ℓℓq\(\overline{q}\) final state in pp collisions at \(\sqrt {s}\) = 8 TeV with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - This paper reports on a search for narrow resonances in diboson production in the ℓℓq\(\overline{q}\) final state using pp collision data corresponding to an integrated luminosity of 20 fb\(^{−1}\) collected at \(\sqrt {s}\) = 8 TeV with the ATLAS detector at the Large Hadron Collider. No significant excess of data events over the Standard Model expectation is observed. Upper limits at the 95 % confidence level are set on the production cross section times branching ratio for Kaluza–Klein gravitons predicted by the Randall–Sundrum model and for Extended Gauge Model W′ bosons. These results lead to the exclusion of mass values below 740 and 1590 GeV for the graviton and W′ boson respectively. KW - ATLAS detector KW - proton-proton collision KW - diboson production KW - resonances Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150171 VL - 75 IS - 2 ER - TY - JOUR T1 - Observation and measurements of the production of prompt and non-prompt J/ψ mesons in association with a Z boson in pp collisions at \(\sqrt {s}\)=8 TeV with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - The production of a Z boson in association with a J/ψ meson in proton–proton collisions probes the production mechanisms of quarkonium and heavy flavour in association with vector bosons, and allows studies of multiple parton scattering. Using 20.3fb\(^{−1}\) of data collected with the ATLAS experiment at the LHC in pp collisions at \(\sqrt {s}\) = 8 TeV, the first measurement of associated Z+J/ψ production is presented for both prompt and non-prompt J/ψ production, with both signatures having a significance in excess of 5σ. The inclusive production cross-sections for Z boson production (analysed in μ\(^{+}\)μ\(^{−}\) or e\(^{+}\)e\(^{−}\) decay modes) in association with prompt and non-prompt J/ψ(→μ\(^{+}\)μ\(^{−}\)) are measured relative to the inclusive production rate of Z bosons in the same fiducial volume to be (36.8±6.7±2.5)×10\(^{−7}\) and (65.8±9.2±4.2)×10\(^{−7}\) respectively. Normalised differential production cross-section ratios are also determined as a function of the J/ψ transverse momentum. The fraction of signal events arising from single and double parton scattering is estimated, and a lower limit of 5.3 (3.7)mb at 68 (95)% confidence level is placed on the effective cross-section regulating double parton interactions. KW - ATLAS detector KW - Z boson KW - proton-proton-collision Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-149970 VL - 75 IS - 5 ER - TY - JOUR T1 - Performance of the ATLAS muon trigger in pp collisions at \(\sqrt {s}\)= 8 TeV JF - European Physical Journal C: Particles and Fields N2 - The performance of the ATLAS muon trigger system is evaluated with proton–proton collision data collected in 2012 at the Large Hadron Collider at a centre-of-mass energy of 8 TeV. It is primarily evaluated using events containing a pair of muons from the decay of Z bosons. The efficiency of the single-muon trigger is measured for muons with transverse momentum 25 < p\(_{T}\) < 100GeV, with a statistical uncertainty of less than 0.01 % and a systematic uncertainty of 0.6 %. The pT range for efficiency determination is extended by using muons from decays of J/ψ mesons, W bosons, and top quarks. The muon trigger shows highly uniform and stable performance. The performance is compared to the prediction of a detailed simulation. KW - LHC KW - proton-proton-collistion Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150032 VL - 75 IS - 3 ER - TY - JOUR T1 - Search for W' → tb → qqbb decays in pp collisions at \(\sqrt {s}\) = 8 TeV with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - A search for a massive W′ gauge boson decaying to a top quark and a bottom quark is performed with the ATLAS detector in pp collisions at the LHC. The dataset was taken at a centre-of-mass energy of \(\sqrt {s}\) = 8 TeV and corresponds to 20.3 fb\(^{−1}\) of integrated luminosity. This analysis is done in the hadronic decay mode of the top quark, where novel jet substructure techniques are used to identify jets from high-momentum top quarks. This allows for a search for high-mass W′ bosons in the range 1.5–3.0  TeV. b-tagging is used to identify jets originating from b-quarks. The data are consistent with Standard Model background-only expectations, and upper limits at 95 % confidence level are set on the W′ → tb cross section times branching ratio ranging from 0.16 pb to 0.33 pb for left-handed W′ bosons, and ranging from 0.10 pb to 0.21 pb for W′ bosons with purely right-handed couplings. Upper limits at 95 % confidence level are set on the W′-boson coupling to tb as a function of the W′ mass using an effective field theory approach, which is independent of details of particular models predicting a W′ boson. KW - ATLAS detector KW - proton-proton collision Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150068 VL - 75 IS - 4 ER - TY - JOUR T1 - Determination of spin and parity of the Higgs boson in the WW\(^{*}\)→eνμν decay channel with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - Studies of the spin and parity quantum numbers of the Higgs boson in the WW\(^{*}\)→eνμν final state are presented, based on proton–proton collision data collected by the ATLAS detector at the Large Hadron Collider, corresponding to an integrated luminosity of 20.3 fb\(^{-1}\) at a centre-of-mass energy of \(\sqrt {s}\)=8 TeV. The Standard Model spin-parity J\(^{CP}\)=0\(^{++}\) hypothesis is compared with alternative hypotheses for both spin and CP. The case where the observed resonance is a mixture of the Standard-Model-like Higgs boson and CP-even (J\(^{CP}\)=0\(^{++}\)) or CP-odd (J\(^{CP}\)=0\(^{+-}\)) Higgs boson in scenarios beyond the Standard Model is also studied. The data are found to be consistent with the Standard Model prediction and limits are placed on alternative spin and CP hypotheses, including CP mixing in different scenarios. KW - Higgs boson KW - spin KW - parity Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-149632 VL - 75 IS - 5 ER - TY - BOOK ED - Hornung, Christoph ED - Lambrecht, Gabriella-Maria ED - Sendner, Annika T1 - Kommunikation und Repräsentation in den romanischen Kulturen. Festschrift für Gerhard Penzkofer N2 - Diese Festschrift ehrt den Romanisten und Slawisten Gerhard Penzkofer anlässlich seines 65. Geburtstags. Kolleginnen und Kollegen sowie Schülerinnen und Schüler, die Gerhard Penzkofer auf seinem bisherigen Weg unter anderem in München, Bamberg und Würzburg sowohl fachlich als auch persönlich nahestanden, publizieren hier Beiträge, die von seinen Forschungen inspiriert sind. Im Zentrum dieser Untersuchungen, die den italienischen, französischen und spanischen Sprachraum umschließen, steht das Verhältnis von Kommunikation und Repräsentation. Dabei umfassen die Beiträge Aspekte, die historisch vom Mittelalter bis zum 20. Jahrhundert und thematisch von der mittelalterlichen Exempelsammlung bis zur postdiktatorialen Geschichtskonstruktion reichen. KW - Kommunikation KW - Repräsentation KW - Spanische Literatur KW - Französische Literatur KW - Italienische Literatur KW - Kommunikation KW - Literatur KW - Geschichte KW - Repräsentation KW - Romanische Sprachen KW - communication KW - spanish literature KW - french literature KW - italian literature Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-152021 UR - https://www.avm-verlag.de/detailview?no=5477-055 SN - 9783954770557 PB - AVM.edition CY - München ER - TY - JOUR T1 - einBlick - Ausgabe 32 - 22. September 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-119034 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 32/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 13 - 14. April 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-112041 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 13/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 11 - 24. März 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wuerzburg KW - Wurzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-111540 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 11/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 08 - 03. März 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-110786 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 8/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 14 - 21. April 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-112240 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 14/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 15 - 28. April 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-112404 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 15/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 06 - 17. Februar 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wuerzburg KW - Wurzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-109607 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 6/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 07 - 24. Februar 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wuerzburg KW - Wurzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-109996 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 7/2015 ER - TY - JOUR T1 - Campus Uni Würzburg März 2015 N2 - Studieren mit Erfolg und Spaß - Die Universität Würzburg bietet vielfältige Studiengänge und spannende Forschungsprojekte KW - Universität Würzburg Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-111863 UR - http://www.presse.uni-wuerzburg.de/publikationen/campus/ VL - 03/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 12 - 07. April 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-111896 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 12/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 10 - 17. März 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-111505 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 10/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 43 - 08. Dezember 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124571 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 43/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 44 - 15. Dezember 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124581 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 44/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 45 - 22. Dezember 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124599 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 45/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 33 - 29. September 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124448 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 33/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 34 - 06. Oktober 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124454 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 34/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 35 - 13. Oktober 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124475 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 35/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 36 - 20. Oktober 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124486 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 36/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 37 - 27. Oktober 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124491 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 37/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 38 - 03. November 2015 N2 - einBlick - Ausgabe 37 - 27. Oktober 2015 KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124510 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 38/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 39 - 10. November 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124526 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 39/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 40 - 17. November 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124534 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 40/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 41 - 24. November 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124547 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 41/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 42 - 01. Dezember 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-124552 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 42/2015 ER - TY - JOUR ED - Bobineau, Julien ED - Callsen, Berit ED - Gold, Martina ED - Goldmann, Julius ED - Hesselbach, Robert ED - Hornung, Christoph ED - Ravasio, Paola T1 - promptus - Würzburger Beiträge zur Romanistik. Band 1 T2 - promptus - Würzburger Beiträge zur Romanistik N2 - Die Zeitschrift promptus – Würzburger Beiträge zur Romanistik richtet sich an alle NachwuchswissenschaftlerInnen im Bereich der romanistischen Sprach- und Literaturwissenschaft sowie der Fachdidaktik. Das Ziel der Zeitschrift ist die Förderung der romanistischen Forschung im Allgemeinen und des wissenschaftlichen Nachwuchses der Romanistik im Besonderen. Sie versteht sich damit als Impulsgeber für junge romanistische Forschung, ohne sich dabei thematisch zu beschränken. KW - Romanistik KW - Literaturwissenschaft KW - Sprachwissenschaft Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-139436 SN - 2510-2613 VL - 1/2015 ER - TY - JOUR T1 - Centrality and rapidity dependence of inclusive jet production in \(\sqrt{^SNN}\)=5.02 TeV proton–lead collisions with the ATLAS detector JF - Physics Letters B N2 - Measurements of the centrality and rapidity dependence of inclusive jet production in \(\sqrt{^SNN}\)=5.02 TeV proton–lead (p+Pb) collisions and the jet cross-section in \(\sqrt{s}\)=2.76 TeV proton–proton collisions are presented. These quantities are measured in datasets corresponding to an integrated luminosity of 27.8 nb\(^{−1}\) and 4.0 pb\(^{−1}\), respectively, recorded with the ATLAS detector at the Large Hadron Collider in 2013. The p+Pb collision centrality was characterised using the total transverse energy measured in the pseudorapidity interval −4.9<η<−3.2 in the direction of the lead beam. Results are presented for the double-differential per-collision yields as a function of jet rapidity and transverse momentum (\(p_T\)) for minimum-bias and centrality-selected p+Pb collisions, and are compared to the jet rate from the geometric expectation. The total jet yield in minimum-bias events is slightly enhanced above the expectation in a \(p_T\)-dependent manner but is consistent with the expectation within uncertainties. The ratios of jet spectra from different centrality selections show a strong modification of jet production at all \(p_T\) at forward rapidities and for large \(p_T\) at mid-rapidity, which manifests as a suppression of the jet yield in central events and an enhancement in peripheral events. These effects imply that the factorisation between hard and soft processes is violated at an unexpected level in proton–nucleus collisions. Furthermore, the modifications at forward rapidities are found to be a function of the total jet energy only, implying that the violations may have a simple dependence on the hard parton–parton kinematics. KW - jet production KW - proton-lead collision Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-139857 VL - 748 ER - TY - JOUR T1 - Search for s-channel single top-quark production in proton–proton collisions at \(\sqrt{s}\)=8 TeV with the ATLAS detector JF - Physics Letters B N2 - This Letter presents a search at the LHC for s-channel single top-quark production in proton–proton collisions at a centre-of-mass energy of 8 TeV. The analyzed data set was recorded by the ATLAS detector and corresponds to an integrated luminosity of 20.3 fb\(^{−1}\). Selected events contain one charged lepton, large missing transverse momentum and exactly two b-tagged jets. A multivariate event classifier based on boosted decision trees is developed to discriminate s-channel single top-quark events from the main background contributions. The signal extraction is based on a binned maximum-likelihood fit of the output classifier distribution. The analysis leads to an upper limit on the s-channel single top-quark production cross-section of 14.6 pb at the 95% confidence level. The fit gives a cross-section of σs=5.0±4.3 pb, consistent with the Standard Model expectation. KW - s-Channel KW - electroweak production KW - top-quark KW - ATLAS Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-139869 VL - 740 ER - TY - JOUR T1 - Search for \(W′→t\overline {b}\) in the lepton plus jets final state in proton–proton collisions at a centre-of-mass energy of \(\sqrt {s}\)=8 TeV with the ATLAS detector JF - Physics Letters B N2 - A search for new charged massive gauge bosons, called W′W′, is performed with the ATLAS detector at the LHC, in proton–proton collisions at a centre-of-mass energy of \(\sqrt {s}\)=8 TeV, using a dataset corresponding to an integrated luminosity of 20.3 fb\(^{−1}\). This analysis searches for W′W′ bosons in the \(W′→t\overline{b}\) decay channel in final states with electrons or muons, using a multivariate method based on boosted decision trees. The search covers masses between 0.5 and 3.0 TeV, for right-handed or left-handed W′W′ bosons. No significant deviation from the Standard Model expectation is observed and limits are set on the \(W′→t\overline{b}\) cross-section times branching ratio and on the W′W′-boson effective couplings as a function of the W′W′-boson mass using the CL\(_s\) procedure. For a left-handed (right-handed) W′W′ boson, masses below 1.70 (1.92) TeV are excluded at 95% confidence level. KW - boson Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-138262 VL - 743 ER - TY - JOUR T1 - Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in pp collisions at \(\sqrt{2}\)=8 TeV JF - Physics Letters B N2 - The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3 fb−120.3 fb\(^{−1}\) of data collected in proton–proton collisions at \(\sqrt{2}\)=8 TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeV to 900 GeV, and a long-lived neutral particle mass from 10 GeV to 150 GeV. KW - new physics KW - long-lived neutral particle KW - high-energy collider experiment Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-136099 VL - 743 ER - TY - JOUR T1 - Search for H→γγH→γγ produced in association with top quarks and constraints on the Yukawa coupling between the top quark and the Higgs boson using data taken at 7 TeV and 8 TeV with the ATLAS detector JF - Physics Letters B N2 - A search is performed for Higgs bosons produced in association with top quarks using the diphoton decay mode of the Higgs boson. Selection requirements are optimized separately for leptonic and fully hadronic final states from the top quark decays. The dataset used corresponds to an integrated luminosity of 4.5 fb\(^{−1}\) of proton–proton collisions at a center-of-mass energy of 7 TeV and 20.3 fb−120.3 fb\(^{−1}\) at 8 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. No significant excess over the background prediction is observed and upper limits are set on the \(t\overline{t}H\) production cross section. The observed exclusion upper limit at 95% confidence level is 6.7 times the predicted Standard Model cross section value. In addition, limits are set on the strength of the Yukawa coupling between the top quark and the Higgs boson, taking into account the dependence of the \(t\overline{t}H\) and tH   cross sections as well as the H→γγH→γγ branching fraction on the Yukawa coupling. Lower and upper limits at 95% confidence level are set at −1.3 and +8.0 times the Yukawa coupling strength in the Standard Model. KW - Higgs boson KW - diphoton decay KW - top quark KW - Yukawa coupling Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-136100 VL - 740 ER - TY - JOUR T1 - einBlick - Ausgabe 24 - 30. Juni 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wuerzburg KW - Wurzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-115011 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 24/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 27 - 21. Juli 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-116386 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 27/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 26 - 14. Juli 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-115763 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 26/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 28 - 28. Juli 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-116936 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 28/2015 ER - TY - GEN T1 - Jahresbericht 2013 T1 - Annual report 2013 N2 - Jahresbericht 2013 des Rechenzentrums der Universität Würzburg N2 - Annual Report 2013 of the Computer Center, University of Wuerzburg T3 - Jahresbericht des Rechenzentrums der Universität Würzburg - 2013 KW - Jahresbericht KW - Annual report KW - Computer Center University of Wuerzburg KW - Rechenzentrum Universität Würzburg Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-113847 ER - TY - JOUR T1 - einBlick - Ausgabe 16 - 05. Mai 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-113994 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 16/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 17 - 12. Mai 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-114006 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 17/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 25 - 07. Juli 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-115417 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 25/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 23 - 23. Juni 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wuerzburg KW - Wurzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-114751 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 23/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 21 - 09. Juni 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wuerzburg KW - Wurzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-114562 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 21/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 22 - 16. Juni 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wuerzburg KW - Wurzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-114576 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 22/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 18 - 19. Mai 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-114017 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 18/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 19 - 26. Mai 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-114021 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 19/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 20 - 02. Juni 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-114140 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 20/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 09 - 10. März 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-110911 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 9/2015 ER - TY - GEN T1 - RückBLICK - Der Jahresbericht 2014 der Julius-Maximilians-Universität Würzburg N2 - Die Entwicklung der Universität Würzburg im Jahr 2014. N2 - Annual Report of the University of Würzburg, 2014. T3 - Blick : die Jahrbücher der Julius-Maximilians-Universität Würzburg - 2014 KW - Würzburg KW - Universität KW - Bericht KW - Wuerzburg KW - Wurzburg KW - annual report KW - University KW - Jahresbericht Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-110008 UR - http://www.presse.uni-wuerzburg.de/publikationen/ VL - 2014 ER - TY - JOUR T1 - einBlick - Ausgabe 04 - 03. Februar 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-108967 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 4/2015 ER - TY - JOUR T1 - Campus Uni Würzburg September 2015 T2 - Campus Uni Würzburg N2 - Forschung im Fokus: Nicht nur in den Naturwissenschaften wird an der Uni Würzburg geforscht. Ob Geschichte, Germanistik oder Informatik – viele Fächer bieten spannende Angebote. KW - Universität Würzburg Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-118734 UR - http://www.presse.uni-wuerzburg.de/publikationen/campus/ VL - 09/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 31 - 15. September 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-118745 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 31/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 29 - 01. September 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-118546 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 29/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 30 - 08. September 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-118620 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 30/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 01 - 13. Januar 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wuerzburg KW - Wurzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-108310 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 1/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 05 - 10. Februar 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wuerzburg KW - Wurzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-109364 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 5/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 02 - 20. Januar 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-108646 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 2/2015 ER - TY - JOUR T1 - einBlick - Ausgabe 03 - 27. Januar 2015 N2 - Nachrichten aus der Julius-Maximilians-Universität Würzburg KW - Würzburg KW - Universität KW - Wurzburg KW - Wuerzburg KW - University Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-108716 UR - http://www.presse.uni-wuerzburg.de/einblick/ VL - 3/2015 ER - TY - JOUR T1 - Search for production of WW/WZ resonances decaying to a lepton, neutrino and jets in pp collisions at \(\sqrt {s}\)= 8 TeV with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - A search is presented for narrow diboson resonances decaying to WW or WZ in the final state where one W boson decays leptonically (to an electron or a muon plus a neutrino) and the other W/Z boson decays hadronically. The analysis is performed using an integrated luminosity of 20.3 fb\(^{−1}\) of pp collisions at \(\sqrt {s}\) = 8 TeV collected by the ATLAS detector at the large hadron collider. No evidence for resonant diboson production is observed, and resonance masses below 700 and 1490 GeV are excluded at 95 % confidence level for the spin-2 Randall–Sundrum bulk graviton G\(^{*}\) with coupling constant of 1.0 and the extended gauge model W′ boson respectively. KW - ATLAS detector KW - W boson KW - Z boson KW - proton-proton collision Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150164 VL - 75 IS - 5 ER - TY - JOUR T1 - Measurement of the top-quark mass in the fully hadronic decay channel from ATLAS data at \(\sqrt {s}\)=7TeV JF - European Physical Journal C: Particles and Fields N2 - The mass of the top quark is measured in a data set corresponding to 4.6  fb\(^{-1}\) of proton–proton collisions with centre-of-mass energy \(\sqrt {s}\)=7 TeV collected by the ATLAS detector at the LHC. Events consistent with hadronic decays of top–antitop quark pairs with at least six jets in the final state are selected. The substantial background from multijet production is modelled with data-driven methods that utilise the number of identified b-quark jets and the transverse momentum of the sixth leading jet, which have minimal correlation. The top-quark mass is obtained from template fits to the ratio of three-jet to dijet mass. The three-jet mass is calculated from the three jets produced in a top-quark decay. Using these three jets the dijet mass is obtained from the two jets produced in the W boson decay. The top-quark mass obtained from this fit is thus less sensitive to the uncertainty in the energy measurement of the jets. A binned likelihood fit yields a top-quark mass of m\(_{t}\)= 175.1 ± 1.4 (stat.) ± 1.2 (syst.) GeV. KW - ATLAS KW - proton–proton collisions KW - top-quark mass KW - fully hadronic KW - LHC Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-149905 VL - 75 IS - 4 ER - TY - JOUR T1 - Campus Uni Würzburg Juni 2015 N2 - Der Weg in die Wissenschaft - Jura, Germanistik, Informatik? Die Auswahl spannender Studiengänge an der Uni Würzburg ist riesig. Experten helfen dir, das Richtige zu finden. KW - Universität Würzburg Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-118350 UR - http://www.presse.uni-wuerzburg.de/publikationen/campus/ VL - 06/2015 ER - TY - JOUR T1 - Measurements of the W production cross sections in association with jets with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - This paper presents cross sections for the production of a W boson in association with jets, measured in proton–proton collisions at \(\sqrt {s}\) = 7 TeV with the ATLAS experiment at the large hadron collider. With an integrated luminosity of 4.6 fb\(^{−1}\), this data set allows for an exploration of a large kinematic range, including jet production up to a transverse momentum of 1 TeV and multiplicities up to seven associated jets. The production cross sections for W bosons are measured in both the electron and muon decay channels. Differential cross sections for many observables are also presented including measurements of the jet observables such as the rapidities and the transverse momenta as well as measurements of event observables such as the scalar sums of the transverse momenta of the jets. The measurements are compared to numerous QCD predictions including next-to-leading-order perturbative calculations, resummation calculations and Monte Carlo generators. KW - ATLAS detector KW - W boson KW - proton-prton-collision Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-149925 VL - 75 IS - 2 ER - TY - JOUR T1 - Constraints on the off-shell Higgs boson signal strength in the high-mass ZZ and WW final states with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - Measurements of the ZZ and WW final states in the mass range above the 2m\(_Z\) and 2m\(_W\) thresholds provide a unique opportunity to measure the off-shell coupling strength of the Higgs boson. This paper presents constraints on the off-shell Higgs boson event yields normalised to the Standard Model prediction (signal strength) in the ZZ→4ℓ, ZZ→2ℓ2ν and WW→eνμν final states. The result is based on pp collision data collected by the ATLAS experiment at the LHC, corresponding to an integrated luminosity of 20.3 fb\(^{-1}\) at a collision energy of \(\sqrt {s}\)=8 TeV. Using the CL\(_S\) method, the observed 95 % confidence level (CL) upper limit on the off-shell signal strength is in the range 5.1–8.6, with an expected range of 6.7–11.0. In each case the range is determined by varying the unknown gg→ZZ and gg→WW background K-factor from higher-order quantum chromodynamics corrections between half and twice the value of the known signal K-factor. Assuming the relevant Higgs boson couplings are independent of the energy scale of the Higgs boson production, a combination with the on-shell measurements yields an observed (expected) 95 % CL upper limit on Γ\(_H\)/Γ\(^{SM}_{H}\) in the range 4.5–7.5 (6.5–11.2) using the same variations of the background K-factor. Assuming that the unknown gg→VV background K-factor is equal to the signal K-factor, this translates into an observed (expected) 95 % CL upper limit on the Higgs boson total width of 22.7 (33.0) MeV. KW - Higgs boson KW - coupling strength Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-149615 VL - 75 IS - 7 ER - TY - JOUR T1 - Measurement of transverse energy–energy correlations in multi-jet events in pp collisions at \(\sqrt {s}\)=7 TeV using the ATLAS detector and determination of the strong coupling constant αs(m\(_{Z}\)) JF - Physics Letters B N2 - High transverse momentum jets produced in pp collisions at a centre of mass energy of 7 TeV are used to measure the transverse energy–energy correlation function and its associated azimuthal asymmetry. The data were recorded with the ATLAS detector at the LHC in the year 2011 and correspond to an integrated luminosity of 158 pb\(^{-1}\). The selection criteria demand the average transverse momentum of the two leading jets in an event to be larger than 250 GeV. The data at detector level are well described by Monte Carlo event generators. They are unfolded to the particle level and compared with theoretical calculations at next-to-leading-order accuracy. The agreement between data and theory is good and provides a precision test of perturbative Quantum Chromodynamics at large momentum transfers. From this comparison, the strong coupling constant given at the Z   boson mass is determined to be αs(m\(_{Z}\))=0.1173±0.0010 (exp.) \(^{+0.0065}_{−0.0026}\) (theo.). KW - physics KW - high transverse momentum jets KW - transverse energy–energy correlation function Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-143398 VL - 750 ER - TY - JOUR T1 - Measurement of three-jet production cross-sections in pp collisions at 7 TeV centre-of-mass energy using the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - Double-differential three-jet production cross-sections are measured in proton–proton collisions at a centre-of-mass energy of \(\sqrt {s}\) = 7 TeV using the ATLAS detector at the large hadron collider. The measurements are presented as a function of the three-jet mass (m\(_{jjj}\)), in bins of the sum of the absolute rapidity separations between the three leading jets (|Y\(^{*}\)|). Invariant masses extending up to 5 TeV are reached for 8 < |Y\(^{*}\)| < 10. These measurements use a sample of data recorded using the ATLAS detector in 2011, which corresponds to an integrated luminosity of 4.51 fb\(^{-1}\). Jets are identified using the anti-k\(_{t}\) algorithm with two different jet radius parameters, R = 0.4 and R = 0.6. The dominant uncertainty in these measurements comes from the jet energy scale. Next-to-leading-order QCD calculations corrected to account for non-perturbative effects are compared to the measurements. Good agreement is found between the data and the theoretical predictions based on most of the available sets of parton distribution functions, over the full kinematic range, covering almost seven orders of magnitude in the measured cross-section values. KW - proton-proton-collisions KW - ATLAS detector Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-149918 VL - 75 IS - 5 ER - TY - JOUR T1 - Measurement of the top quark mass in the t\(\overline{t}\)→ lepton+jets and t\(\overline{t}\)→ dilepton channels using \(\sqrt {s}\)=7 TeV ATLAS data JF - European Physical Journal C: Particles and Fields N2 - The top quark mass was measured in the channels t\(\overline{t}\) → lepton+jets and t\(\overline{t}\) → dilepton (lepton = e,μ) based on ATLAS data recorded in 2011. The data were taken at the LHC with a proton–proton centre-of-mass energy of \(\sqrt {s}\) = 7 TeV and correspond to an integrated luminosity of 4.6 fb\(^{-1}\). The t\(\overline{t}\) → lepton+jets analysis uses a three-dimensional template technique which determines the top quark mass together with a global jet energy scale factor (JSF), and a relative b-to-light-jet energy scale factor(bJSF), where the terms b-jets and light-jets refer to jets originating from b-quarks and u, d, c, s-quarks or gluons, respectively. The analysis of the t\(\overline{t}\) → dilepton channel exploits a one-dimensional template method using the m\(_{lb}\) observable, defined as the average invariant mass of the two lepton+b-jet pairs in each event. The top quark mass is measured to be 172.33±0.75(stat + JSF + bJSF)±1.02(syst) GeV, and 173.79 ± 0.54(stat) ± 1.30(syst) GeV in the t\(\overline{t}\) → lepton+jets and t\(\overline{t}\) → dilepton channels, respectively. The combination of the two results yields m\(_{top}\) =172.99 ± 0.48(stat) ± 0.78(syst) GeV, with a total uncertainty of 0.91 GeV. KW - top quark mass Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-149890 VL - 75 IS - 7 ER - TY - JOUR T1 - Search for supersymmetry in events containing a same-flavour opposite-sign dilepton pair, jets, and large missing transverse momentum in \(\sqrt {s}\) = 8 TeV pp collisions with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - Two searches for supersymmetric particles in final states containing a same-flavour opposite-sign lepton pair, jets and large missing transverse momentum are presented. The proton–proton collision data used in these searches were collected at a centre-of-mass energy \(\sqrt {s}\) = 8 TeV by the ATLAS detector at the Large Hadron Collider and corresponds to an integrated luminosity of 20.3 fb\(^{−1}\). Two leptonic production mechanisms are considered: decays of squarks and gluinos with Z bosons in the final state, resulting in a peak in the dilepton invariant mass distribution around the Z-boson mass; and decays of neutralinos (e.g. \(\tilde{χ}\)\(^{0}_{2}\) → ℓ\(^{+}\)ℓ\(^{−}\)\(\tilde{χ}\)\(^{0}_{1}\)), resulting in a kinematic endpoint in the dilepton invariant mass distribution. For the former, an excess of events above the expected Standard Model background is observed, with a significance of three standard deviations. In the latter case, the data are well-described by the expected Standard Model background. The results from each channel are interpreted in the context of several supersymmetric models involving the production of squarks and gluinos. KW - ATLAS detector KW - supersymmetry KW - proton-proton collision Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150184 VL - 75 IS - 7 ER - TY - JOUR T1 - Two-particle Bose-Einstein correlations in pp collisions at \(\sqrt {s}\) = 0.9 and 7 TeV measured with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - The paper presents studies of Bose–Einstein Correlations (BEC) for pairs of like-sign charged particles measured in the kinematic range p\(_{T}\) > 100 MeV and |η| <  2.5 in proton collisions at centre-of-mass energies of 0.9 and 7 TeV with the ATLAS detector at the CERN Large Hadron Collider. The integrated luminosities are approximately 7 μb\(^{−1}\), 190 μb\(^{−1}\) and 12.4 nb\(^{−1}\) for 0.9 TeV, 7 TeV minimum-bias and 7 TeV high-multiplicity data samples, respectively. The multiplicity dependence of the BEC parameters characterizing the correlation strength and the correlation source size are investigated for charged-particle multiplicities of up to 240. A saturation effect in the multiplicity dependence of the correlation source size parameter is observed using the high-multiplicity 7 TeV data sample. The dependence of the BEC parameters on the average transverse momentum of the particle pair is also investigated. KW - ATLAS detector KW - proton-proton collision KW - Bose-Einstein Correlations Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150222 VL - 75 IS - 10 ER - TY - JOUR T1 - Search for a new resonance decaying to a W or Z boson and a Higgs boson in the ℓℓ/ℓν/νν+b\(\overline{b}\) final states with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - A search for a new resonance decaying to a W or Z boson and a Higgs boson in the ℓℓ/ℓν/νν+b\(\overline{b}\) final states is performed using 20.3 fb\(^{−1}\) of pp collision data recorded at \(\sqrt {s}\) = 8 TeV with the ATLAS detector at the Large Hadron Collider. The search is conducted by examining the WH / ZH invariant mass distribution for a localized excess. No significant deviation from the Standard Model background prediction is observed. The results are interpreted in terms of constraints on the Minimal Walking Technicolor model and on a simplified approach based on a phenomenological Lagrangian of Heavy Vector Triplets. KW - Higgs boson KW - W boson KW - Z boson KW - ATLAS detector Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150075 VL - 75 IS - 6 ER - TY - JOUR T1 - Measurement of the branching ratio Γ(Λ\(^0_b\)→ψ(2S)Λ\(^0\))/Γ(Λ\(^0_b\)→J/ψΛ\(^0\)) with the ATLAS detector JF - Physics Letters B N2 - An observation of the View the Λ\(^0_b\)→ψ(2S)Λ\(^0\) decay and a comparison of its branching fraction with that of the Λ\(^0_b\)→J/ψΛ\(^0\) decay has been made with the ATLAS detector in proton–proton collisions at \(\sqrt {s}\)=8 TeV at the LHC using an integrated luminosity of 20.6 fb\(^{-1}\). The J/ψJ/ψ and ψ(2S) mesons are reconstructed in their decays to a muon pair, while the Λ\(^0\)→pπ\(^-\) decay is exploited for the Λ\(^0\) baryon reconstruction. The Λ\(^0_b\) baryons are reconstructed with transverse momentum p\(_T\)>10 GeV pT>10 GeV and pseudorapidity |η|<2.1. The measured branching ratio of the Λ\(^0_b\)→ψ(2S)Λ\(^0\) and Λ\(^0_b\)→J/ψΛ\(^0\) decays is Γ(Λ\(^0_b\)→ψ(2S)Λ\(^0\))/Γ(Λ\(^0_b\)→J/ψΛ\(^0\))=0.501±0.033(stat)±0.019(syst), lower than the expectation from the covariant quark model. KW - physics KW - proton–proton collisions KW - Large Hadron Collider KW - decay Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-143375 VL - 751 ER - TY - JOUR T1 - Search for the associated production of the Higgs boson with a top quark pair in multilepton final states with the ATLAS detector JF - Physics Letters B N2 - A search for the associated production of the Higgs boson with a top quark pair is performed in multilepton final states using 20.3 fb\(^{−1}\) of proton–proton collision data recorded by the ATLAS experiment at \(\sqrt {s}\)=8 TeV at the Large Hadron Collider. Five final states, targeting the decays H→WW\(^{*}\), ττ, and ZZ\(^{*}\), are examined for the presence of the Standard Model (SM) Higgs boson: two same-charge light leptons (e or μ) without a hadronically decaying τ lepton; three light leptons; two same-charge light leptons with a hadronically decaying τ lepton; four light leptons; and one light lepton and two hadronically decaying τ leptons. No significant excess of events is observed above the background expectation. The best fit for the t\(\overline{t}\)H production cross section, assuming a Higgs boson mass of 125 GeV, is 2.1\(^{+1.4}_{-1.2}\) times the SM expectation, and the observed (expected) upper limit at the 95% confidence level is 4.7 (2.4) times the SM rate. The p-value for compatibility with the background-only hypothesis is 1.8σ; the expectation in the presence of a Standard Model signal is 0.9σ. KW - physics KW - associated production KW - Higgs boson Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-144231 VL - 749 ER - TY - JOUR T1 - Measurement of exclusive γγ→ℓ\(^{+}\)ℓ\(^{−}\) production in proton–proton collisions at \(\sqrt {s}\)=7 TeV with the ATLAS detector JF - Physics Letters B N2 - This Letter reports a measurement of the exclusive γγ→ℓ\(^{+}\)ℓ\(^{−}\) (ℓ=e, μℓ=e, μ) cross-section in proton–proton collisions at a centre-of-mass energy of 7 TeV by the ATLAS experiment at the LHC, based on an integrated luminosity of 4.6 fb\(^{−1}\). For the electron or muon pairs satisfying exclusive selection criteria, a fit to the dilepton acoplanarity distribution is used to extract the fiducial cross-sections. The cross-section in the electron channel is determined to be \(^{excl.}_{γγ→e^{+}e^{-}}\)=0.428 ± 0.035 (stat.) ± 0.018 (syst.) pb for a phase–space region with invariant mass of the electron pairs greater than 24 GeV, in which both electrons have transverse momentum p\(_{T}\)>12 GeV and pseudorapidity |η|<2.4. For muon pairs with invariant mass greater than 20 GeV, muon transverse momentum p\(_{T}\)>10 GeV and pseudorapidity |η|<2.4, the cross-section is determined to be \(^{excl.}_{γγ→μ^{+}μ^{-}}\) =0.628 ± 0.032 (stat.) ± 0.021 (syst.) pb. When proton absorptive effects due to the finite size of the proton are taken into account in the theory calculation, the measured cross-sections are found to be consistent with the theory prediction. KW - physics Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-144247 VL - 749 ER - TY - JOUR T1 - Measurement of colour flow with the jet pull angle in t\(\overline{t}\) events using the ATLAS detector at \(\sqrt {s}\)=8 TeV JF - Physics Letters B N2 - The distribution and orientation of energy inside jets is predicted to be an experimental handle on colour connections between the hard-scatter quarks and gluons initiating the jets. This Letter presents a measurement of the distribution of one such variable, the jet pull angle. The pull angle is measured for jets produced in t\(\overline{t}\) events with one W boson decaying leptonically and the other decaying to jets using 20.3 fb\(^{−1}\) of data recorded with the ATLAS detector at a centre-of-mass energy of \(\sqrt {s}\)=8 TeV at the LHC. The jet pull angle distribution is corrected for detector resolution and acceptance effects and is compared to various models. KW - physics KW - colour flow Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-144229 VL - 750 ER - TY - JOUR T1 - Measurement of the production of neighbouring jets in lead–lead collisions at =2.76 TeV with the ATLAS detector JF - Physics Letters B N2 - This Letter presents measurements of correlated production of nearby jets in Pb+Pb collisions at \(\sqrt S_{NN}\)=2.76 TeV using the ATLAS detector at the Large Hadron Collider. The measurement was performed using 0.14 nb\(^{-1}\) of data recorded in 2011. The production of correlated jet pairs was quantified using the rate, R\(_{ΔR}\), of “neighbouring” jets that accompany “test” jets within a given range of angular distance, ΔR , in the pseudorapidity–azimuthal angle plane. The jets were measured in the ATLAS calorimeter and were reconstructed using the anti-k\(_t\) algorithm with radius parameters d=0.2, 0.3, and 0.4. R\(_{ΔR}\) was measured in different Pb+Pb collision centrality bins, characterized by the total transverse energy measured in the forward calorimeters. A centrality dependence of R\(_{ΔR}\) is observed for all three jet radii with R\(_{ΔR}\) found to be lower in central collisions than in peripheral collisions. The ratios formed by the R\(_{ΔR}\) values in different centrality bins and the values in the 40–80% centrality bin are presented. KW - physics Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150448 VL - 751 SP - 376 EP - 395 ER - TY - JOUR T1 - Jet energy measurement and its systematic uncertainty in proton-proton collisions at \(\sqrt {s}\)=7 TeV with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - The jet energy scale (JES) and its systematic uncertainty are determined for jets measured with the ATLAS detector using proton–proton collision data with a centre-of-mass energy of \(\sqrt {s}\)=7 TeV corresponding to an integrated luminosity of 4.7 fb\(^{-1}\). Jets are reconstructed from energy deposits forming topological clusters of calorimeter cells using the anti-k\(_t\) algorithm with distance parameters R=0.4 or R=0.6, and are calibrated using MC simulations. A residual JES correction is applied to account for differences between data and MC simulations. This correction and its systematic uncertainty are estimated using a combination of in situ techniques exploiting the transverse momentum balance between a jet and a reference object such as a photon or a Z boson, for 20≤p\(^{jet}_{T}\)<1000 GeV and pseudorapidities |η|<4.5. The effect of multiple proton–proton interactions is corrected for, and an uncertainty is evaluated using in situ techniques. The smallest JES uncertainty of less than 1 % is found in the central calorimeter region (|η|<1.2) for jets with 55≤p\(^{jet}_{T}\)<500 GeV. For central jets at lower p\(_{T}\), the uncertainty is about 3 %. A consistent JES estimate is found using measurements of the calorimeter response of single hadrons in proton–proton collisions and test-beam data, which also provide the estimate for p\(^{jet}_{T}\)>1 TeV. The calibration of forward jets is derived from dijet p\(_{T}\) balance measurements. The resulting uncertainty reaches its largest value of 6 % for low-p\(_{T}\) jets at |η|=4.5. Additional JES uncertainties due to specific event topologies, such as close-by jets or selections of event samples with an enhanced content of jets originating from light quarks or gluons, are also discussed. The magnitude of these uncertainties depends on the event sample used in a given physics analysis, but typically amounts to 0.5–3 %. KW - jet energy scale KW - proton-proton-collision Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-149854 VL - 75 IS - 1 ER - TY - JOUR T1 - Search for direct pair production of a chargino and a neutralino decaying to the 125 GeV Higgs boson in \(\sqrt {s}\) = 8 TeV pp collisions with the ATLAS detector JF - European Physical Journal C: Particles and Fields N2 - A search is presented for the direct pair production of a chargino and a neutralino pp → \(\tilde{χ}\)\(^{±}_{1}\)\(\tilde{χ}\)\(^{0}_{2}\), where the chargino decays to the lightest neutralino and the W boson, \(\tilde{χ}\)\(^{±}_{1}\)→\(\tilde{χ}\)\(^{0}_{1}\)(W\(^{±}\)→ℓ\(^{±}\)ν), while the neutralino decays to the lightest neutralino and the 125 GeV Higgs boson, \(\tilde{χ}\)\(^{0}_{2}\)→\(\tilde{χ}\)\(^{0}_{1}\)(h→bb/γγ/ℓ\(^{±}\)νqq). The final states considered for the search have large missing transverse momentum, an isolated electron or muon, and one of the following: either two jets identified as originating from bottom quarks, or two photons, or a second electron or muon with the same electric charge. The analysis is based on 20.3 fb\(^{-1}\) of \(\sqrt {s}\) = 8 TeV proton–proton collision data delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with the Standard Model expectations, and limits are set in the context of a simplified supersymmetric model. KW - neutralino KW - chargino KW - proton-proton collision KW - Higgs boson KW - ATLAS detector Y1 - 2015 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150099 VL - 75 IS - 5 ER -