PPT-Sub electron noise readout for scientific CCDs

Research Techniques Seminar September 14 2010 Gustavo Cancelo CCD low noise readout Juan Estrada Ken Treptow Gullermo Fernandez Moroni Gustavo Cancelo Tom Diehl Kevin Kuk. Yuri . Levin (Monash University). 1. Example: creep noise. 2.. Formalism. 3.. Creep noise again . 4. Thermal deformations of mirrors. 5. Thermal noise. 6. . Opto. -mechanical displacements. 7. Discussion. Single Electron Source. Jin Zhang , Yury Sherkunov, Nicholas d’Ambrumenil, Boris Muzykantskii. University of Warwick, U.K.. Conference on Computational Physics 2009, Kaohsiung, 16. th. , Dec.. Single Electron Excitation. Jin . Zhang, . Y. Sherkunov, . N. d'Ambrumenil, B. Muzykantskii. Department of Physics, University of Warwick, Coventry, CV4 7AL, U.K. .. (See poster by Y. Sherkunov also). ABSTRACT. We . obtain the full counting statistics (FCS) of a quantum point contact (QPC) for the case when the contact transparency is . Sensor Requirements. Sensor requirements (consistent with IPHC development direction). ~2 cm x 2 cm (1 reticle) size.. Pixel size < 30 µm.. Integration time of ≤ 200 µs for L = 8 x 10. 27. cm. Single Electron Source. Jin Zhang , Yury Sherkunov, Nicholas d’Ambrumenil, Boris Muzykantskii. University of Warwick, U.K.. Conference on Computational Physics 2009, Kaohsiung, 16. th. , Dec.. Single Electron Excitation. ATLAS . LAr. Calorimeters. Summer Student Sessions . 13 August 2008. Chew . Soo. . Hoon. . University Of Malaya, Malaysia . (caseycsh@cern.ch). Jan Stark . LPSC, Grenoble, France . (stark@in2p3.fr). TileCal. ) at the LHC is used to measure the hadrons produced with polar angles >21. 0 . and the energy deposition of ~20MeV to ~1.3TeV in the detector cells. The total readout channels are ~10K and the required readout dynamic range is 16-bit. The front-end readout electronics of the ATLAS . Y. B. Sherkunov, Jin Zhang, N. d'Ambrumenil, B. Muzykantskii. Department of Physics, University of Warwick, Coventry, CV4 7AL, U.K. .. ABSTRACT. Controlled . injection of single electrons into a ballistic conductor is . Cameras For Microscopy Ryan McGorty 26 March 2013 Goals of this lecture Understand what prevents the ideal camera from being a realty Understand sources of noise in digital imaging Decipher meaning of camera specification sheets Secondary Electron D etector Ana Zehtabi Oskuie Introduction Secondary electron secondary electron detector The electron beam interaction with near surface specimen atoms will make a signal which results in the SEM image ), which can be not only directly used but also adapted to meet our special requirements. The size of this camera is architecture CCDs can be placed in the camera. The readout and digitization uses  . Advances in CCD Applications with Sub Electron Noise Techniques. Juan Estrada, Gustavo . Cancelo. . 07/19/2011. R&D Projects. General . CCD R&D will benefit the following projects:. DAMIC. Prigozhin. , . B. Burke, K. Ryu, . M. Zhu, M. Cooper, K. Johnson, W. . Hu, B. Felton. , M. Cook. , C. Stull, V. . Suntharalingam. 1 December 2016. Germanium CCDs for Large-Format SWIR and X-Ray Imaging. 9 November 2019. New Directions in Detector Development at MIT Lincoln Laboratory. MIT-LL Silicon Charge-Coupled Devices (CCDs). Astronomy & NEO Detection. Space Surveillance. Astronomy & Astrophysics.