CERN Accelerating science

CERN Document Server 143 records found  1 - 10próximoend  jump to record: Search took 0.78 seconds. 
1.
Performance of the ATLASPix1 pixel sensor prototype in ams aH18 CMOS technology for the ATLAS ITk upgrade / Kiehn, M (Geneva U.) ; Herkert, A (Heidelberg U.) ; Weber, A (Heidelberg U.) ; Schöning, A (Heidelberg U.) ; Miucci, A (U. Bern, AEC) ; Fehr, A (U. Bern, AEC) ; Blattgerste, C (Heidelberg U.) ; Grzesik, C (Mainz U., Inst. Phys.) ; Sultan, D M S (Geneva U.) ; Immig, D (Heidelberg U.) et al.
Monolithic active pixel sensors (MAPS) based on commercial high-voltage CMOS processes are an exciting technology that is considered as an option for the ATLAS Inner Tracker upgrade. Particles are detected using deep n-wells on a p-type substrate as sensor diodes with the depleted region extending into the silicon bulk. [...]
2019 - 7 p. - Published in : JINST 14 (2019) C08013
In : International Workshop on Semiconductor Pixel Detectors for Particles and Imaging (PIXEL2018), Taipei, Taiwan, 10 - 14 Dec 2018, pp.C08013
2.
Characterization of the demonstrator of the fast silicon monolithic ASIC for the TT-PET project / Paolozzi, Lorenzo (U. Geneva (main)) ; Bandi, Yves (Bern U.) ; Cardarelli, Roberto (INFN, Rome) ; Debieux, Stephane (U. Geneva (main)) ; Favre, Yannick (U. Geneva (main)) ; Ferrere, Didier (U. Geneva (main)) ; Forshaw, Dean (Bern U.) ; Hayakawa, Daiki (U. Geneva (main)) ; Iacobucci, Giuseppe (U. Geneva (main)) ; Kaynak, Mehmet (IHP, Frankfurt) et al.
The TT-PET collaboration is developing a small animal TOF-PET scanner based on monolithic silicon pixel sensors in SiGe BiCMOS technology. The demonstrator chip, a small-scale version of the final detector ASIC, consists of a 3 x 10 pixel matrix integrated with the front-end, a 50 ps binning TDC and read out logic. [...]
arXiv:1811.11114.- 2019-02-11 - 12 p. - Published in : JINST 14 (2019) P02009 Fulltext: 1811.11114 - PDF; fulltext1705474 - PDF; Fulltext from Publisher: PDF;
3.
DsTau: Study of tau neutrino production with 400 GeV protons from the CERN-SPS / DsTau Collaboration
In the DsTau experiment at the CERN SPS, an independent and direct way to measure tau neutrino production following high energy proton interactions was proposed. As the main source of tau neutrinos is a decay of Ds mesons, produced in proton-nucleus interactions, the project aims at measuring a differential cross section of this reaction. [...]
arXiv:1906.03487.- 2020-01-07 - 24 p. - Published in : JHEP 2001 (2020) 033 Article from SCOAP3: PDF; Fulltext: PDF;
4.
Charge collection characterisation with the Transient Current Technique of the ams H35DEMO CMOS detector after proton irradiation / Anders, J. (U. Bern, AEC) ; Benoit, M. (Geneva U.) ; Braccini, S. (U. Bern, AEC) ; Casanova, R. (Barcelona, IFAE) ; Chen, H. (Brookhaven) ; Chen, K. (Brookhaven) ; Di Bello, F.A. (Geneva U.) ; Fehr, A. (U. Bern, AEC) ; Ferrere, D. (Geneva U.) ; Forshaw, D. (U. Bern, AEC) et al.
This paper reports on the characterisation with Transient Current Technique measurements of the charge collection and depletion depth of a radiation-hard high-voltage CMOS pixel sensor produced at ams AG. Several substrate resistivities were tested before and after proton irradiation with two different sources: the 24 GeV Proton Synchrotron at CERN and the 16.7 MeV Cyclotron at Bern Inselspital..
arXiv:1807.09553.- 2018-10-01 - 14 p. - Published in : JINST 13 (2018) P10004 Fulltext: fulltext1683864 - PDF; 1807.09553 - PDF; Anders_2018_J._Inst._13_P10004 - PDF; Fulltext from Publisher: PDF;
5.
Production and Integration of the ATLAS Insertable B-Layer / ATLAS IBL Collaboration
During the shutdown of the CERN Large Hadron Collider in 2013-2014, an additional pixel layer was installed between the existing Pixel detector of the ATLAS experiment and a new, smaller radius beam pipe. The motivation for this new pixel layer, the Insertable B-Layer (IBL), was to maintain or improve the robustness and performance of the ATLAS tracking system, given the higher instantaneous and integrated luminosities realised following the shutdown. [...]
arXiv:1803.00844; FERMILAB-PUB-18-826-V.- 2018-05-16 - 90 p. - Published in : JINST 13 (2018) T05008 Fulltext: 1803.00844 - PDF; pdf - PDF; 915f919fb4ff01d19bc67dd5a6b9cd70 - PDF; Fulltext from Publisher: PDF; External link: Fermilab Library Server
6.
Test beam measurement of the first prototype of the fast silicon pixel monolithic detector for the TT-PET project / Paolozzi, L. ; Bandi, Y. ; Benoit, M. ; Cardarelli, R. ; Débieux, S. ; Forshaw, D. ; Hayakawa, D. ; Iacobucci, G. ; Kaynak, M. ; Miucci, A. et al.
The TT-PET collaboration is developing a PET scanner for small animals with 30 ps time-of-flight resolution and sub-millimetre 3D detection granularity. The sensitive element of the scanner is a monolithic silicon pixel detector based on state-of-the-art SiGe BiCMOS technology. [...]
arXiv:1802.01319.- 2018-04-12 - 11 p. - Published in : JINST 13 (2018) P04015 Fulltext: pdf - PDF; arXiv:1802.01319 - PDF; 1802.01319 - PDF; Fulltext from Publisher: PDF;
7.
Amplitude analysis of the decay $\overline{B}^0 \to K_{S}^0 \pi^+ \pi^-$ and first observation of the CP asymmetry in $\overline{B}^0 \to K^{*}(892)^- \pi^+$ / LHCb Collaboration
The time-integrated Dalitz plot of the three-body hadronic charmless decay ${{\overline{B}}^0 \to K_{\mathrm{\scriptscriptstyle S}}^0 \pi^+ \pi^-}$ is studied using a $pp$ collision data sample recorded with the LHCb detector, corresponding to an integrated luminosity of $3.0\;\mathrm{fb}^{-1}$. The decay amplitude is described with an isobar model. [...]
arXiv:1712.09320; LHCB-PAPER-2017-033; CERN-EP-2017-317.- 2018-06-27 - 10 p. - Published in : Phys. Rev. Lett. 120 (2018) 261801 Article from SCOAP3: PDF; Fulltext: PDF; Fulltext from Publisher: PDF; External link: Figures, tables and other information
8.
Measurement of branching fractions of charmless four-body $\Lambda_b^0$ and $\Xi_b^0$ decays / LHCb Collaboration
A search for charmless four-body decays of $\Lambda_{b}^{0}$ and $\Xi_{b}^{0}$ baryons with a proton and three charged mesons (either kaons or pions) in the final state is performed. The data sample used was recorded in 2011 and 2012 with the LHCb experiment and corresponds to an integrated luminosity of 3 fb$^{-1}$. [...]
arXiv:1711.05490; CERN-EP-2017-278; LHCB-PAPER-2017-034; LHCB-PAPER-2017-034.- Geneva : CERN, 2018-02-16 - 25 p. - Published in : JHEP 02 (2018) 098 Article from SCOAP3: PDF; Fulltext: PDF; Related data file(s): ZIP; External link: Figures, tables and other information
9.
Measurement of the ratio of branching fractions $\mathcal{B}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$ / LHCb Collaboration
A measurement is reported of the ratio of branching fractions $\mathcal{R}(J/\psi)=\mathcal{B}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)/\mathcal{B}(B_c^+\,\to\,J/\psi \mu^+\nu_\mu)$, where the $\tau^+$ lepton is identified in the decay mode $\tau^+\,\to\,\mu^+\nu_\mu\overline{\nu}_\tau$. This analysis uses a sample of proton-proton collision data corresponding to 3.0$\mathrm{\,fb}^{-1}$ of integrated luminosity recorded with the LHCb experiment at center-of-mass energies $7\,\mathrm{TeV}$ and $8\,\mathrm{TeV}$. [...]
arXiv:1711.05623; LHCB-PAPER-2017-035; CERN-EP-2017-275; LHCB-PAPER-2017-035.- Geneva : CERN, 2018-03-27 - 10 p. - Published in : Phys. Rev. Lett. 120 (2018) 121801 Article from SCOAP3: PDF; Fulltext: PDF; Fulltext from Publisher: PDF; Related data file(s): ZIP; Supplementary information: ZIP; External link: Figures, tables and other information
10.
First observation of $B^{+} \to D_s^{+}K^{+}K^{-}$ decays and a search for $B^{+} \to D_s^{+}\phi$ decays / LHCb Collaboration
A search for $B^{+} \to D_s^{+}K^{+}K^{-}$ decays is performed using $pp$ collision data corresponding to an integrated luminosity of 4.8 fb$^{-1}$, collected at centre-of-mass energies of 7, 8 and 13$\,$TeV with the LHCb experiment. A significant signal is observed for the first time and the branching fraction is determined to be \begin{equation*} \mathcal{B}(B^{+} \to D_s^{+}K^{+}K^{-} ) = (7.1 \pm 0.5 \pm 0.6 \pm 0.7) \times 10^{-6}, \end{equation*} where the first uncertainty is statistical, the second systematic and the third due to the uncertainty on the branching fraction of the normalisation mode $B^{+} \to D_s^{+} \overline{\kern -0.2em D}^{0}$. [...]
arXiv:1711.05637; LHCB-PAPER-2017-032; CERN-EP-2017-289; LHCB-PAPER-2017-032.- Geneva : CERN, 2018-01-26 - 22 p. - Published in : JHEP 01 (2018) 131 Article from SCOAP3: PDF; Fulltext: PDF; Related data file(s): ZIP; External link: Figures, tables and other information

CERN Document Server : 143 records found   1 - 10próximoend  jump to record:
Veja também: nomes de autores similares
11 Forshaw, D
2 Forshaw, D C
9 Forshaw, D.C.
3 Forshaw, Dean
129 Forshaw, Dean Charles
Interested in being notified about new results for this query?
Set up a personal email alert or subscribe to the RSS feed.
Haven't found what you were looking for? Try your search on other servers:
Forshaw, D. em Amazon
Forshaw, D. em CERN EDMS
Forshaw, D. em CERN Intranet
Forshaw, D. em CiteSeer
Forshaw, D. em Google Books
Forshaw, D. em Google Scholar
Forshaw, D. em Google Web
Forshaw, D. em IEC
Forshaw, D. em IHS
Forshaw, D. em INSPIRE
Forshaw, D. em ISO
Forshaw, D. em KISS Books/Journals
Forshaw, D. em KISS Preprints
Forshaw, D. em NEBIS
Forshaw, D. em SLAC Library Catalog
Forshaw, D. em Scirus