Diamond detector technology, status and perspectives Alexopoulos, A.; Artuso, M.; Bachmair, F. ...
Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment,
04/2019, Letnik:
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Detectors based on Chemical Vapor Deposition (CVD) diamond have been used extensively and successfully in beam conditions/beam loss monitors as the innermost detectors in the highest radiation areas ...of Large Hadron Collider (LHC) experiments. The startup of the LHC in 2015 brought a new milestone where the first polycrystalline CVD (pCVD) diamond pixel modules were installed in an LHC experiment and successfully began operation. The RD42 collaboration at CERN is leading the effort to develop polycrystalline CVD diamond as a material for tracking detectors operating in extreme radiation environments. The status of the RD42 project with emphasis on recent beam test results is presented.
•Successful operation of the first pCVD diamond planar pixel detector in the ATLAS experiment at the LHC.•Demonstration that the average signal pulse height of pCVD diamond detectors irradiated up to 5×014n∕cm2 is independent of the particle flux up to ∼20 MHz/cm2.•Successful fabrication and operation of the first pCVD diamond 3D pixel detector with 50 micron × 50 micron cells read out with CMS pixel electronics with 3 cell × 2 cell ganging into pixels to match the electronics.•Demonstration that in the pCVD diamond 3D pixel device the efficiency for a MIP was 99% when operating with a 1500 e threshold.
Chemical Vapour Deposition (CVD) diamond is being considered as a material for particle detectors in a harsh radiation environment. This article presents beam test results of 3D pixel detectors ...fabricated with poly-crystalline CVD diamonds. The cells of the devices had a size of 50µm×50µm with columns 2.6µm in diameter. The cells were ganged in a 3×2 and 5×1 pattern to match the layouts of the pixel read-out electronics currently used in the CMS and ATLAS experiments at the Large Hadron Collider, respectively. In beam tests, using tracks reconstructed with a high precision tracking telescope, a tracking efficiency of 99.3% was achieved. The efficiency of both devices plateaus at a bias voltage of 30V. Also irradiated poly-crystalline CVD diamond pad detectors were investigated. In high rate beam tests with particle fluxes up to 20MHz/cm2 and irradiations up to 8 ⋅ 1015n/cm2 it was shown that the pulse height of irradiated poly-crystalline CVD diamonds does not depend on flux to the O2%.
Results on radiation tolerance of diamond detectors Venturi, N.; Alexopoulos, A.; Artuso, M. ...
Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment,
04/2019, Letnik:
924, Številka:
C
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In sight of the luminosity increase of the High Luminosity-LHC (HL-LHC), most experiments at the CERN Large Hadron Collider (LHC) are planning upgrades for their innermost layers in the next 5–10 ...years. These upgrades will require more radiation tolerant technologies than exist today. Usage of Chemical Vapor Deposition (CVD) diamond as detector material is one of the potentially interesting technologies for the upgrade. CVD diamond has been used extensively in the beam condition monitors of BaBar, Belle, CDF and all LHC experiments. Measurements of the radiation tolerance of the highest quality polycrystalline CVD material for a range of proton energies, pions and neutrons obtained with this material are presented. In addition, new results on the evolution of various semiconductor parameters as a function of the dose rate are described.
A measurement of fiducial and differential cross-sections for Formula omitted production in proton-proton collisions at Formula omitted TeV with the ATLAS experiment at the Large Hadron Collider ...using data corresponding to an integrated luminosity of 36.1 Formula omitted is presented. Events with one electron and one muon are selected, corresponding to the decay of the diboson system as Formula omitted. To suppress top-quark background, events containing jets with a transverse momentum exceeding 35 GeV are not included in the measurement phase space. The fiducial cross-section, six differential distributions and the cross-section as a function of the jet-veto transverse momentum threshold are measured and compared with several theoretical predictions. Constraints on anomalous electroweak gauge boson self-interactions are also presented in the framework of a dimension-six effective field theory.
A search for excited electrons produced in pp collisions at Formula omitted = 13 Formula omitted via a contact interaction Formula omitted is presented. The search uses 36.1 fb Formula omitted of ...data collected in 2015 and 2016 by the ATLAS experiment at the Large Hadron Collider. Decays of the excited electron into an electron and a pair of quarks ( Formula omitted) are targeted in final states with two electrons and two hadronic jets, and decays via a gauge interaction into a neutrino and a Formula omitted boson ( Formula omitted) are probed in final states with an electron, missing transverse momentum, and a large-radius jet consistent with a hadronically decaying Formula omitted boson. No significant excess is observed over the expected backgrounds. Upper limits are calculated for the Formula omitted and Formula omitted production cross sections as a function of the excited electron mass Formula omitted at 95% confidence level. The limits are translated into lower bounds on the compositeness scale parameter Formula omitted of the model as a function of Formula omitted. For Formula omitted Formula omitted, the lower bound for Formula omitted is 11 Formula omitted. In the special case of Formula omitted, the values of Formula omitted Formula omitted are excluded. The presented limits on Formula omitted are more stringent than those obtained in previous searches.
This paper presents measurements of the Formula omitted and Formula omitted cross-sections and the associated charge asymmetry as a function of the absolute pseudorapidity of the decay muon. The data ...were collected in proton-proton collisions at a centre-of-mass energy of 8 Formula omitted with the ATLAS experiment at the LHC and correspond to a total integrated luminosity of Formula omitted. The precision of the cross-section measurements varies between 0.8 and 1.5% as a function of the pseudorapidity, excluding the 1.9% uncertainty on the integrated luminosity. The charge asymmetry is measured with an uncertainty between 0.002 and 0.003. The results are compared with predictions based on next-to-next-to-leading-order calculations with various parton distribution functions and have the sensitivity to discriminate between them.
Searches for scalar leptoquarks pair-produced in proton-proton collisions at Formula omitted TeV at the Large Hadron Collider are performed by the ATLAS experiment. A data set corresponding to an ...integrated luminosity of 36.1 fb Formula omitted is used. Final states containing two electrons or two muons and two or more jets are studied, as are states with one electron or muon, missing transverse momentum and two or more jets. No statistically significant excess above the Standard Model expectation is observed. The observed and expected lower limits on the leptoquark mass at 95% confidence level extend up to 1.29 TeV and 1.23 TeV for first- and second-generation leptoquarks, respectively, as postulated in the minimal Buchmüller-Rückl-Wyler model, assuming a branching ratio into a charged lepton and a quark of 50%. In addition, measurements of particle-level fiducial and differential cross sections are presented for the Formula omitted, Formula omitted and Formula omitted processes in several regions related to the search control regions. Predictions from a range of generators are compared with the measurements, and good agreement is seen for many of the observables. However, the predictions for the Formula omitted measurements in observables sensitive to jet energies disagree with the data.
A study of the decays Bs0 → μ+μ− and B0 → μ+μ− has been performed using 26.3 fb−1 of 13 TeV LHC proton-proton collision data collected with the ATLAS detector in 2015 and 2016. Since the detector ...resolution in μ+μ− invariant mass is comparable to the Bs0-B0 mass difference, a single fit determines the signal yields for both decay modes. This results in a measurement of the branching fraction ℬBs0→μ+μ−=3.2−1.0+1.1×10−9\ \mathrm{\mathcal{B}}\left({B}_s^0\to {\mu}^{+}{\mu}^{-}\right)=\left({3.2}_{-1.0}^{+1.1}\right)\times {10}^{-9} \ and an upper limit ℬB0→μ+μ−<4.3×10−10\ \mathrm{\mathcal{B}}\left({B}^0\to {\mu}^{+}{\mu}^{-}\right)<4.3\times {10}^{-10} \ at 95% confidence level. The result is combined with the Run 1 ATLAS result, yielding ℬBs0→μ+μ−=2.8−0.7+0.8×10−9\ \mathrm{\mathcal{B}}\left({B}_s^0\to {\mu}^{+}{\mu}^{-}\right)=\left({2.8}_{-0.7}^{+0.8}\right)\times {10}^{-9} \ and ℬB0→μ+μ−<2.1×10−10\ \mathrm{\mathcal{B}}\left({B}^0\to {\mu}^{+}{\mu}^{-}\right)<2.1\times {10}^{-10} \ at 95% confidence level. The combined result is consistent with the Standard Model prediction within 2.4 standard deviations in the ℬB0→μ+μ−−ℬBs0→μ+μ−\ \mathrm{\mathcal{B}}\left({B}^0\to {\mu}^{+}{\mu}^{-}\right)-\mathrm{\mathcal{B}}\left({B}_s^0\to {\mu}^{+}{\mu}^{-}\right) \ plane.
Algorithms used for the reconstruction and identification of electrons in the central region of the ATLAS detector at the Large Hadron Collider (LHC) are presented in this paper; these algorithms are ...used in ATLAS physics analyses that involve electrons in the final state and which are based on the 2015 and 2016 proton-proton collision data produced by the LHC at Formula omitted = 13 Formula omitted. The performance of the electron reconstruction, identification, isolation, and charge identification algorithms is evaluated in data and in simulated samples using electrons from Formula omitted and Formula omitted decays. Typical examples of combinations of electron reconstruction, identification, and isolation operating points used in ATLAS physics analyses are shown.
Inclusive and differential cross-sections for the production of a top-quark pair in association with a photon are measured with proton-proton collision data corresponding to an integrated luminosity ...of 36.1 Formula omitted, collected by the ATLAS detector at the LHC in 2015 and 2016 at a centre-of-mass energy of 13 Formula omitted. The measurements are performed in single-lepton and dilepton final states in a fiducial volume. Events with exactly one photon, one or two leptons, a channel-dependent minimum number of jets, and at least one b-jet are selected. Neural network algorithms are used to separate the signal from the backgrounds. The fiducial cross-sections are measured to be Formula omitted and Formula omitted for the single-lepton and dilepton channels, respectively. The differential cross-sections are measured as a function of photon transverse momentum, photon absolute pseudorapidity, and angular distance between the photon and its closest lepton in both channels, as well as azimuthal opening angle and absolute pseudorapidity difference between the two leptons in the dilepton channel. All measurements are in agreement with the theoretical predictions.
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