Deutsches Elektronen-Synchrotron DESY

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    Model-independent measurement of D0D^0-D0\overline{D}{}^0 mixing parameters in D0KS0π+πD^0\rightarrow K^0_{S}\pi^+\pi^- decays at Belle and Belle II

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    We perform a model-independent measurement of the D0D^0-D0\overline{D}{}^0 mixing parameters using samples of e+ee^+e^--collision data collected by the Belle and Belle II experiments that have integrated luminosities of 951 fb1951\ \text{fb}^{-1} and 408 fb1408\ \text{fb}^{-1}, respectively. Approximately 2.05×1062.05\times10^6 neutral DD mesons are reconstructed in the D0KS0π+πD^0\rightarrow K^0_{S}\pi^+\pi^- channel, with the neutral DD flavor tagged by the charge of the pion in the D+D0π+D^{*+}\rightarrow D^0\pi^+ decay. Assuming charge-parity symmetry, the mixing parameters are measured to be x=(4.0±1.7±0.4)×103 x = (4.0\pm1.7\pm0.4)\times 10^{-3} and y=(2.9±1.4±0.3)×103 y = (2.9\pm1.4\pm0.3)\times 10^{-3}, where the first uncertainties are statistical and the second systematic. The results are consistent with previous determinations

    Search for charged lepton flavor violating Z and Z' boson decays in proton-proton collisions at s\sqrt{s} = 13 TeV

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    A search for flavor violating decays of the Z boson to charged leptons is performed using data from proton-proton collisions at s\sqrt{s} = 13 TeV collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 138 fb1^{-1}. Each of the decays Z \to eμμ, Z \to eττ, and Z \toμτμτ is considered. The data are consistent with the backgrounds expected from standard model processes. For the Z \to eμμ channel the observed (expected) 95% confidence level upper limit on the branching fraction is 1.9 (2.0) ×\times 107^{-7}, which is the most stringent direct limit to date on this process; the corresponding limits for the Z \to eττ and Z \to μτμτ channels are 13.8 (11.4) ×\times 106^{-6} and 12.0 (5.3) ×\times 106^{-6}, respectively. Additionally, the eμμ final state is used to search for lepton flavor violating decays of Z' resonances in the mass range from 110 to 500 GeV. No significant excess is observed above the predicted background levels

    Annular x-ray optics offer improved resolution for radiation sensitive samples

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    To detect faint signals from weakly scattering samples, high-resolution x-ray microscopy typically requires a high photon flux. This exposes samples to high radiation doses and can cause radiation damage. In this work we propose the use of annular optics in scanning microscopy as an alternative to full-aperture optics. Annular optics act as high-pass filters that produce a stronger signal from edges. Compared to regular optics with the same numerical aperture, annular optics expose the sample to less dose while producing the same signal from small sample features. Annular optics benefit significantly from the high photon fluxes of the latest x-ray sources to compensate for their overall smaller cross section. Using numerical simulations, we show that annular optics offer superior optical performance for sample features close to the resolution limit of the optic

    High pressure structural and lattice dynamics study of αα-In2_2Se3_3

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    Layered αα-In2_2Se3_3 has been studied using a combined in situ synchrotron angle-dispersive powder x-ray diffraction and Raman spectroscopy study in a diamond anvil cell up to 60+ GPa, at room temperature. Helium, which remains fairly hydrostatic up to the highest pressure in this study, was used as the pressure-transmitting medium. The results from both experimental methods reveal a pressure-induced structural phase transition from αα-In2_2Se3_3 to a monoclinic ββ′-In2_2Se3_3 structure at ≈1 GPa, in agreement with previous studies. Based on our detailed measurements using both experimental techniques and the F–f formalism, the ββ′-In2_2Se3_3 structure remains stable up to 45 GPa, without a clear indication of a phase transition toward the previously reported ββ-In2_2Se3_3 phase. Above this pressure, 2_2Se3_3 adopts a disordered solid-solution-like orthorhombic structure, phase IV. The results are discussed in comparison with the relevant previous studies of αα-In2_2Se3_3 under pressure

    Timing Performance of the DESY Chip V2 in a 65 nm CIS Technology

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    Monolithic Active Pixel Sensors (MAPS) produced in CMOS image sensor (CIS) technology are a promising candidate for meeting the stringent requirements for vertex detectors at future lepton colliders. Recently, a 65 nm CIS process has become available to the high-energy physics community, offering enhanced integration density and lowered power consumption. In this context, the DESY Chip V2 was developed as a test chip, studying the performance and intricacies of this technology. The chip features a 2 × 2 pixel test structure with a pixel pitch of 35 × 25 μm2. In contrast to complementary prototypes that rely on reading out digitised data only, the frontend voltage output can be measured, providing deeper insight into the charge collection and frontend response.The work presented in this thesis covers the commissioning and integration of the DESY Chip V2 into existing frameworks, a charge calibration and a test beam campaign with the analysis of the recorded data. Special focus is placed on the time resolution and the interaction of the placement of n-wells with the charge collection

    Azimuthal anisotropies of charged particles with high transverse momentum in Pb+Pb collisions at sNN=5.02\sqrt{s_{_\text{NN}}} = 5.02 TeV with the ATLAS detector

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    A measurement is presented of elliptic (v2v_2) and triangular (v3v_3) azimuthal anisotropy coefficients for charged particles produced in Pb+Pb collisions at sNN=5.02\sqrt{s_{_\text{NN}}} = 5.02 TeV using a dataset corresponding to an integrated luminosity of 0.440.44 nb1^{-1} collected with the ATLAS detector at the LHC in 2018. The values of v2v_2 and v3v_3 are measured for charged particles over a wide range of transverse momentum (pTp_\text{T}), 1-400 GeV, and Pb+Pb collision centrality, 0-60%, using the scalar product and multi-particle cumulant methods. These methods are sensitive to event-by-event fluctuations and non-flow effects in the measurements of azimuthal anisotropies. Positive values of v2v_2 are observed up to a pTp_{\text{T}} of approximately 100 GeV from both methods across all centrality intervals. Positive values of v3v_3 are observed up to approximately 25 GeV using both methods, though the application of the three-subevent technique to the multi-particle cumulant method leads to significant changes at the highest pTp_{\text{T}}. At high pTp_{\text{T}} (pT10p_{\text{T}} \gtrapprox 10 GeV), charged particles are dominantly from jet fragmentation. These jets, and hence the measurements presented here, are sensitive to the path-length dependence of parton energy loss in the quark-gluon plasma produced in Pb+Pb collisions

    The kinetics of nsp7-11 polyprotein processing and impact on complexation with nsp16 among human coronaviruses

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    In severe-acute respiratory syndrome coronavirus 2 (SARS-CoV-2) infection, polyproteins (pp1a/pp1ab) are processed into non-structural proteins (nsps), which largely form the replication/transcription complex (RTC). The polyprotein processing and complex formation is critical and offers potential therapeutic targets. However, the interplay of polyprotein processing and RTC-assembly are poorly understood. Here, we studied two key aspects: The influence of the pp1a terminal nsp11 on the order of polyprotein processing by viral main protease Mpro and the influence of polyprotein processing on core enzyme complex formation. We established a method based on native MS to determine rate constants k considering the structural environment. This enabled us to quantify the multi-reaction kinetics of coronavirus polyprotein processing for the first time. Our results serve as a blueprint for other multi-cleavage reactions. Further, it offers a detailed and quantifiable perspective to the dynamic reactions of SARS-CoV-2 polyprotein processing, which is required for development of novel antivirals

    Observation of a cross-section enhancement near the ttˉt\bar{t} production threshold in s\sqrt{s} =13 TeV pp collisions with the ATLAS detector

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    A measurement is presented of ttˉt\bar{t} production in the invariant-mass region near the pair production threshold,mttˉm_{t\bar{t}}∼345GeV, in final states with two charged leptons and multiple jets. The measurement is based on 140fb1^{-1} of proton–proton collision data collected at s\sqrt{s}=13TeV with the ATLAS detector. The data are compared to two models of ttˉt\bar{t} production: a baseline model including only perturbative QCD (pQCD) predictions for the hard process, and an extended model that, in addition to the pQCD predictions, incorporates state-of-the-art Monte Carlo simulations of colour-singlet quasi-bound-state formation near the ttˉt\bar{t} threshold. The agreement between the data and the models is quantified via a profile-likelihood fit to the reconstructed mttˉm_{t\bar{t}} distributions, in bins of two angular observables sensitive to spin-correlations in the ttˉt\bar{t} system. An excess of events is observed over the baseline pQCD prediction, with an observed significance of 7.7 standard deviations. This excess is consistent with the formation of colour-singlet, S-wave, quasi-bound ttˉt\bar{t} states as predicted by non-relativistic QCD, and corresponds to an observed cross-section of 9.0±\pm1.3pb

    Radio emission from airplanes as observed with RNO-G

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    This paper describes how intentional and unintentional radioemission from airplanes is recorded with the Radio NeutrinoObservatory Greenland (RNO-G). We characterize the receivedsignals and define a procedure to extract a clean set of impulsivesignals. These signals are highly suitable for instrumentcalibration, also for future experiments. A set of signals is usedto probe the timing precision of RNO-G in-situ, which is found tomatch expectations. We also discuss the impact of these signals onthe ability to detect neutrinos with RNO-G

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