119225792
Performance of jet substructure techniques for large-R jets in proton-proton collisions at $ \sqrt{s}=7 $ TeV using the ATLAS detector
A bstractThis paper presents the application of a variety of techniques to study jet substructure. The performance of various modified jet algorithms, or jet grooming techniques, for several jet types and event topologies is investigated for jets with transverse momentum larger than 300 GeV. Properties of jets subjected to the mass-drop filtering, trimming, and pruning algorithms are found to have a reduced sensitivity to multiple proton-proton interactions, are more stable at high luminosity and improve the physics potential of searches for heavy boosted objects. Studies of the expected discrimination power of jet mass and jet substructure observables in searches for new physics are also presented. Event samples enriched in boosted W and Z bosons and top-quark pairs are used to study both the individual jet invariant mass scales and the efficacy of algorithms to tag boosted hadronic objects. The analyses presented use the full 2011 ATLAS dataset, corresponding to an integrated luminosity of 4.7 ± 0.1 fb−1 from proton-proton collisions produced by the Large Hadron Collider at a centre-of-mass energy of $ \sqrt{s}=7 $ TeV.

118500591
Measurement of moments of the hadronic-mass and energy spectrum in inclusive semileptonic anti-B ---> X(c) l- anti-nu decays
125358056
Evidence for the $B^0 \to \rho^0 \rho^0$ decay and implications for the CKM angle $\alpha$
We search for the decays B0->rho0rho0, B0->rho0f0, and B0->f0f0 in a sample of about 348 million Upsilon(4S)->BBbar decays collected with the BABAR detector at the PEP-II asymmetric-energy e+e- collider at SLAC. We find evidence for B0->rho0rho0 with 3.0 sigma significance and measure the branching fraction B = (1.16 +0.37-0.36 +-0.27) 10^{-6} and longitudinal polarization fraction f_L = 0.86 +0.11-0.13 +-0.05. As a consequence, the uncertainty on the CKM unitarity angle alpha due to penguin contributions in B->rhorho decays is estimated to be 18 degrees at 1 sigma level. We also set upper limits on the B0->rho0f0 and B0->f0f0 decay rates. All results are preliminary.
53073574
The ATLAS High Level Trigger Steering
The High Level Trigger (HLT) of the ATLAS experiment at the Large Hadron Collider receives events which pass the LVL1 trigger at ~75 kHz and has to reduce the rate to ~200 Hz while retaining the most interesting physics. It is a software trigger and performs the reduction in two stages: the LVL2 trigger and the Event Filter (EF). At the heart of the HLT is the Steering software. To minimise processing time and data transfers it implements the novel event selection strategies of seeded, step-wise reconstruction and early rejection. The HLT is seeded by regions of interest identified at LVL1. These and the static configuration determine which algorithms are run to reconstruct event data and test the validity of trigger signatures. The decision to reject the event or continue is based on the valid signatures, taking into account pre-scale and pass-through. After the EF, event classification tags are assigned for streaming purposes. Several powerful new features for commissioning and operation have been added: comprehensive monitoring is now built in to the framework; for validation and debugging, reconstructed data can be written out; the steering is integrated with the new configuration (presented separately), and topological and global triggers have been added. This paper will present details of the final design and its implementation, the principles behind it, and the requirements and constraints it is subject to. The experience gained from technical runs with realistic trigger menus will be described.
104358197
Measurement of $\cos_{2beta}$ in $B^0 \to D^{(*)}$ 0 h0 decays with a time-dependent Dalitz plot analysis of $D^0 \to K^0_{s} \pi^{+} \pi^{-}$
We report a preliminary measurement of $\cos2\beta$ in $B^0\to D^{(*)0}h^0$ decays with a time-dependent Dalitz plot analysis of $D^0\to K_S\pi^+\pi^-$, where $h^0$ is a light neutral meson such as $\pi^0$, $\eta$, $\eta'$ or $\omega$. The strong phase variation on the Dalitz plot allows the access to the angle $\beta$ with only a two-fold ambiguity ($\beta+\pi$). Using $311\times 10^{6}$ $B\bar{B}$ pairs collected at the Babar detector, we obtain $\cos2\beta = 0.54 \pm 0.54 \pm 0.08 \pm 0.18$, $\sin2\beta = 0.45 \pm 0.36 \pm 0.05 \pm 0.07$, and $|\lambda| = 0.975^{+0.093}_{-0.085} \pm 0.012 \pm 0.002 $, where the first errors are statistical, the second are experimental systematic uncertainties, and the third are the signal Dalitz model uncertainties. This measurement favors the solution of $\beta= 22^\circ$ over $68^\circ$ at an 87% confidence level.
209834301
Search for supersymmetry in events with photons, bottom quarks, and missing transverse momentum in proton–proton collisions at a centre-of-mass energy of 7 TeV with the ATLAS detector
A search has been performed for the experimental signature of an isolated photon with high transverse momentum, at least one jet identified as originating from a bottom quark, and high missing transverse momentum. Such a final state may originate from supersymmetric models with gauge-mediated supersymmetry breaking in events in which one of a pair of higgsino-like neutralinos decays into a photon and a gravitino while the other decays into a Higgs boson and a gravitino. The search is performed using the full dataset of 7 TeV proton–proton collisions recorded with the ATLAS detector at the LHC in 2011, corresponding to an integrated luminosity of 4.7 fb−1. A total of 7 candidate events are observed while 7.5±2.2 events are expected from the Standard Model background. The results of the search are interpreted in the context of general gauge mediation to exclude certain regions of a benchmark plane for higgsino-like neutralino production.
120101281
The Mu3e Experiment
Abstract The Mu3e experiment is designed to search for charged lepton flavour violation in the process μ + → e + e − e + with a branching ratio sensitivity of 10 − 16 . This requires a detector capable of coping with rates of up to 2 ⋅ 10 9 muons/s whilst being able to reduce backgrounds from accidental coincidences and the process μ + → e + e − e + ν ¯ μ ν e to below the 10 − 16 level. The use of 50 μ m thin high-voltage monolithic active pixel sensors in conjunction with an innovative tracking concept provide the momentum and position resolution necessary, whilst the timing resolution is provided by a combination of scintillating fibres and tiles. The recently approved Mu3e experiment will be located at the Paul Scherrer Institute in Switzerland and is currently preparing for detector construction.
125611661
Measurement of diffractive Φ meson photoproduction at HERA with the H1 fast track trigger
A new measurement of diffractive φ meson photoproduction is performed with the H1 experiment at the electron-proton collider HERA. In the kinematic range 30 < Wγp < 90 GeV and 0.2 < |t| < 1.5 GeV, cross sections are determined double differentially in Wγp and t. From these data, the pomeron trajectory in elastic φ meson photoproduction is determined to be α(t) = 1.15 ± 0.05(stat.) −0.03(syst.) + t · (0.16 ± 0.09(stat.) −0.02(syst.))GeV−2. A combined fit with data from fixed target experiments and the ZEUS collaboration yields the most precise trajectory measurement using φ mesons to date, α(t) = 1.122 ± 0.008 + t · (0.150 ± 0.017) GeV. The spin density matrix elements, which provide information on the helicity structure of the interaction, are extracted using measurements of angular distributions of the φ meson decay products and are found to be in agreement with expectations from s-channel helicity conservation. The presented cross section measurement was made possible by the Fast Track Trigger (FTT). This new trigger based on signals from selected wire layers of the H1 central drift chamber provides information to the first three trigger levels of the H1 experiment. The first level performs a coarse two-dimensional track reconstruction within 2 μs, whilst the second trigger level reconstructs the event vertex along the beam line, performs a precise three-dimensional track fit and determines invariant masses of track pairs in 20 μs. The third trigger level reconstructs final states from up to 48 tracks and allows for particle identification using information from the calorimeter and the muon system within 100 μs. Zusammenfassung Mit dem H1-Experiment am Elektron-Proton-Beschleuniger HERA wird eine neue Messung diffraktiver φ-Meson-Photoproduktion durchgeführt. Im kinematischen Bereich 30 < Wγp < 90 GeV und 0.2 < |t| < 1.5 GeV werden Wirkungsquerschnitte doppeltdifferenziell in Wγp und t gemessen. Aus diesen Daten bestimmt sich die PomeronTrajektorie in elastischer φ-Meson-Photoproduktion zu α(t) = 1.15 ± 0.05(stat.) −0.03(syst.) + t · (0.16 ± 0.09(stat.) −0.02(syst.))GeV−2. Eine gemeinsame Anpassung mit Daten von Experimenten mit ruhendem Target und der ZEUS-Kollaboration liefert die bisher genaueste Messung der Trajektorie mit Hilfe von φ-Mesonen: α(t) = 1.122 ± 0.008 + t · (0.150 ± 0.017) GeV. Aus der Messung der Winkelverteilung der φ-Meson-Zerfallsprodukte werden drei Elemente der Spindichtematrix bestimmt. Diese sind verträglich mit s-Kanal-Helizitätserhaltung. Die vorliegende Messung wurde durch den schnellen Spurtrigger (Fast Track Trigger, FTT) ermöglicht. Dieser neue Trigger leitet aus Signalen von ausgewählten Drahtlagen der zentralen Spurkammer von H1 Informationen für die ersten drei Triggerstufen des H1 Experimentes ab. Auf der ersten Stufe wird innert 2 μs eine grobe, zweidimensionale Spurrekonstruktion durchgeführt. In 20 μs rekonstruiert die zweite Stufe den EreignisVertex entlang der Strahllinie, führt eine präzise, dreidimensionale Spuranpassung durch und bestimmt die invariante Masse von Spurpaaren. Auf der dritten Stufe werden innert 100 μs aus bis zu 48 Spuren Endzustände rekonstruiert und mit Hilfe von Informationen aus dem Kalorimeter und dem Myon-System Teilchen identifiziert.
62237714
Partial wave analysis using graphics processing units
Partial wave analysis is an important tool for determining resonance properties in hadron spectroscopy. For large data samples however, the un-binned likelihood fits employed are computationally very expensive. At the Beijing Spectrometer (BES) III experiment, an increase in statistics compared to earlier experiments of up to two orders of magnitude is expected. In order to allow for a timely analysis of these datasets, additional computing power with short turnover times has to be made available. It turns out that graphics processing units (GPUs) originally developed for 3D computer games have an architecture of massively parallel single instruction multiple data floating point units that is almost ideally suited for the algorithms employed in partial wave analysis. We have implemented a framework for tensor manipulation and partial wave fits called GPUPWA. The user writes a program in pure C++ whilst the GPUPWA classes handle computations on the GPU, memory transfers, caching and other technical details. In conjunction with a recent graphics processor, the framework provides a speed-up of the partial wave fit by more than two orders of magnitude compared to legacy FORTRAN code.
119183835
A Tracker for the Mu3e Experiment based on High-Voltage Monolithic Active Pixel Sensors
The Mu3e experiment searches for the lepton flavour violating decay + ! e + e e + , aiming for a branching fraction sensitivity of 10 16 . This requires an excellent momentum resolution for low energy electrons, high rate capability and a large acceptance. In order to minimize multiple scattering, the amount of material has to be as small as possible. These challenges can be met with a tracker built from high-voltage monolithic active pixel sensors (HV-MAPS), which can be thinned to 50 µm and which incorporate the complete read-out electronics on the sensor chip. To further minimise material, the sensors are supported by a mechanical structure built from 25 m thick Kapton foil and cooled with gaseous helium.