%5252277DA87D277D52FF527D527D5227A8FF277D277DFFA87DFF7DFF2752 %F827588282825E8282825D7C27525D58F82757A8FD0AFF99CFFFFF7D8282 %CAA1A8FD0CFFA827FD06FFA0A1FF7DA8A8A87DA8FD047DA8FD47FFA8F8F8 %5E8282825D825D82F87C5EA7FD0AFF99CACAFF7D827B828182756F6F6F6E %%CreationDate: 10/29/2008 10:20 AM %7DA87D514B7DFD27FFC2CAFD1DFF52FD24FF52525227277D27517DFD05FF %%BoundingBox: 33 160 588 775 Wire color optional. %828882828288FD068283FD0EFFA88288FD06825882588282888282A8FD09 %A87DA8A8A87DA8A8A87DA8A8A87DA8A8A8527D5252527D7D2752A87DA87D Download PDF Abstract: ... =13$TeV by the ATLAS detector at the Large Hadron Collider. %527D527D7D52527D7DFD08FFC2C9FD19FFA87D277D7D7D27527D522752A8 %AI3_TileBox: 14.1001 14.0998 597.8001 777.7998 j1 j2 j3 j4 j5 j6 jp 1 jp 2 rin dout din yin com pwr com pwr ain aux1 gnd ogic y o 12vdc atlas signal control board nce bd-20 detector power supply insulated rail insulated rail joiner Download full-text PDF Read full-text. A detailed study is presented of the expected performance of the ATLAS detector. In addition to measurements of Stan-dard Model processes such as vector-boson and top-quark production, the properties of the newly 7%BS������t}jd�^�Z���;6�������W�,�?2�ב���i�� ����������J����㷉��>"�v�����#��-oF;M�?��� G�[F۴�5���$�itizm��p T�15$�x�fEV� �f���/$�l�U/,�&Hl7%�P3:�m��wR��Z1��k3-�h��E��9��ݱ��T~sڈ��2ʏ��B2v��-mɶ%�z��[�6�m�{Ѿ�pIC�Ep�Ben 1����' ȒYh���5$N��%���F�nO����vi�n��L):�[�R�hD�b�+�r�N�h(�+(� �d���[�!lAKf7���o��nS�0]�*q��J1�uFL^�IcM��?�z�2;ASz��!�緁i��h٨aG��{�ĉ�cՉ~'�(��]d����&BX���0KL� The design of the cylindrically symmetric ATLAS detector was optimized to study a broad range of physics processes, including SM Higgs boson production, over a wide mass range. %AI9_Flatten: 0 %7D52FD057DFFFF7D527D52527D7D2752277D7D7D52A8FF52527D52A852A8 %7D277D27A8527D7D52527D527D52A8A852527D5227A8522752277DFFFD04 12 m 10 8 6 4. %FD4DFF7DFD245227A8FD4DFFFD26527DFD4DFF7DFD245227A8FD4DFFFD04 %825782515857A8FD14FFA8FF7EFFFFFFA1FD0DFFA852FD06FF9AC9FD27FF :���v[b. %FFA9FFA9FFA9FFA9FFA9FFA9FFA9FFA9FFA9FFA9FFA9A8A8FFA9FD04FFC9 Expected performance of the ATLAS detector 10.1 Introduction Since the publication of the ATLAS Detector and Physics Performance Technical Design Re-port [248] in 1999, all the detector components of the experiment have been constructed and integrated and most of them have been installed (see section9.6). %00FF0000FFFFFF0000FF00FFFFFF00FFFFFF Intermediate system is a large silicon strip tracker •Four barrel layers and 9 disk layers contain 61 m2 of silicon with 6.2M channels. %27F87C828282888282828882828288FD0482A7FD0EFFA8828282887C5258 ATLAS detector and physics performance Volume I Technical Design Report 25 May 1999 Acknowledgements vii Acknowledgements The Editors would like to thank Mario Ruggier for his continuous help and competent advice on all FrameMaker issues. %A87DA8A8A87DA87DA87DA852A87DA8A8A87DA8A8A87DA8A8A87DA8A87D52 %FFFFFFA8FFFFFFA8FD04FFA87DFD11FF52A8FD09FFA8A87DA8A8A87DA87D %AI5_OpenViewLayers: 7 Measurements of the top-quark mass with the ATLAS detector Teresa Barillari 3. %27FFC3C9FD2BFF7DA8FD19FFA852527D27FD27FF9AC9FD2BFF7D7DFD1AFF %FFFFA8FFFFFFA8FD09FFA8A8FFA9A9FFCACAFD0EFF52FD06FFC2A1FD28FF %A87DA87D7DA8A87DFFA8A87D7DA8A87DA8527CF8F8F827F8F858825D8282 However, the accuracy and precision of the ATLAS Detector may vary depending on di erent factors, for example the energies of the particles created. %FD05FFA16876FD0CFF27F852FD05FF6E6FA17D522727525252272727A8FD %FFFF7EFD11FFA852FD06FF9AC9FD24FFA9FFFFA8838227F852587CFD0B82 A search for direct chargino production in anomaly-mediated supersymmetry breaking scenarios is performed in pp collisions at √ s = 7 TeV using 4.7 fb−1 of data collected with the ATLAS experiment at the LHC. Transition radiation detector gives particle ID. %524C457D527D2752525227A8527D7DFF527D2727A8FF52A852FF7D7D527D %FFFFA85E88828282A04B754B756F9F7BA07BA0A0C9C3C9C3C9C3C9C3C976 %7C7C7C5883587C587C7C7C587C587C587C7C8258A8FD0AFF99CFFFFFA883 %F8518258825D8282825D8282825D82828257A8FD0EFF7D825E825D7CF87C The tracking modules and the trigger system are of most relevance for the presented measurements. Measurement of the the top-quark pole mass at p s=8 and 7TeV In the following the mpole top determination from the absolute and normalised differential cross- sections measurement in the di … These were followed by similar testbeam campaigns for “module-0” prototypes of the final design, and then for the series production modules. %27759F759F75A0A0C3A0C2A0C3A0C39A76A0C2A0C3A0C2A0FD24FFA8FD04 %AI5_TargetResolution: 800 %FD2FFFA8A8FFFFA9A8FFFFC9CFFD0DFF52FD06FFC2C9FD24FF7E847EA97E %7DA852A87D52277D7DC9CFFD0DFF52FD06FFC3C9FD4BFF7D52527D7D5227 %%EndComments %FF9AC9FD28FF838227F8525882587CFD09827C517C5127F87CA7FFCFFFCA The Editors also warmly thank Michèle Jouhet and Isabelle Canon Expected performance of the ATLAS detector 10.1 Introduction Since the publication of the ATLAS Detector and Physics Performance Technical Design Re-port [248] in 1999, all the detector components of the experiment have been constructed and integrated and most of them have been installed (see section9.6). %A883A87DFD13FF7DFFFFFF7EFFFFFFA1FD0DFFA852FD06FF9AC9FD24FFA8 A search is presented for the pair production of heavy vector-like T quarks, primarily targeting the T quark decays to a W boson and a b-quark. 1.1 Inner Detector %9966CC9966FF9999009999339999669999999999CC9999FF99CC0099CC33 %825D8252FD04F8275E82828258A8FD08FFA852FD1FFFFD0452277D7D7DFF %A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8FF7EFFFFFFA1FD0DFFA852FD06 %A87E847EA87E847EA87E847EA87D7E7EA85AFFFFFFA1FD0DFFA852FD06FF %A87DFFFFA8A85882588258825882588282825E8282825D58F8F85252F827 1 0 obj<> endobj 2 0 obj<> endobj 3 0 obj<> endobj 5 0 obj null endobj 6 0 obj<>/ProcSet[/PDF/Text]/ExtGState<>/Properties<>>>>>/PieceInfo<>/LastModified(D:20081029102009-04'00')>> endobj 7 0 obj<> endobj 8 0 obj<> endobj 75 0 obj null endobj 76 0 obj<>stream %3399003399333399663399993399CC3399FF33CC0033CC3333CC6633CC99 Measurement of the $$W^{\pm}Z$$ Production Cross Section and Limits on Anomalous Triple Gauge Couplings at $$\sqrt s = 7 TeV$$ using the ATLAS detector %3333663333993333CC3333FF3366003366333366663366993366CC3366FF The physics %9933009933339933669933999933CC9933FF996600996633996666996699 The ATLAS Detector Control System K Lantzsch, S Arfaoui, S Franz et al.-The detector control system of the ATLAS SemiConductor Tracker during macro-assembly and integration A Abdesselam, A Barr, S Basiladze et al.-Ongoing studies for the control system of a serially powered ATLAS pixel detector at the HL-LHC S. Kersten, L. Püllen and C. Zeitnitz- %FFA852FD06FF9AC9FD27FFA8835E27F852587C7C82828882828288828282 %000088888888AA000000AA000000AAAAAAAABB000000BB000000BBBBBBBB %11FF52FD06FFC3C9FD24FF7E7E7EA85258272727582D7C5D825E8282825E %%+ 0.8 0 1 0 (Global Green) %PDF-1.4 %F87D275227F8527D52525227277D275227F827A8FD0BFFC2CAFFFFFFFD04 The reconstruction of tracks, leptons, photons, missing energy and jets is investigated, together with the performance of b-tagging and the trigger. The detector itself is a many-layered instrument designed to detect some of the tiniest yet most energetic particles ever created on earth. %7DA8527DA8527D272752FF27FFA82727A85252A87D27527D52277D7DA87D %FDFCFFFDFCFFFDFCFFFDFCFFFDFCFFFD17FFA8FFA8A8A8FFA8A8A8FFA8A8 %525227FD0D527DFD4DFFFD16527DFD0E5227A8FD4DFF5252275252522752 Search for the Lepton Flavor Violating decay Z → eμ with the ATLAS detector at the LHC, Hai Jiang. %52FFA852FF52FFF852277D5252527DA8F8A8FF275252FF27275252277DA8 In addition to measurements of Stan-dard Model processes such as vector-boson and top-quark production, the properties of the newly %%+ 0.5 0.9 0 0 (Global Plum) End-cap toroid Barrel toroid coil. ��P�K�� i�ɏg_�PZ�Ĕ�H�?��� Q��}c�?=;�N�����P��(���ص�=6���ɿwoB�m=�dW�.ѿ��p�f�l�6�4�����j����;i)V�V� ���Y�oe���u�6�}��?4r��Om�V��|v�lیmg(Q�G�Tc65h�E�����+�km�( ao�_���hO4����c>����,�൛��hCb�R���K���ӡ�V�#]�=iM��Iځ4����(-C�3Ģ{T��T�*��_%�"2!I�9RE�Nl��e3 ��l� The ATLAS detector. %4DFF52522752525227525252275252522752525227525252275252522752 %7DFD2552A8FD4DFFFD052752272727522727275227272752272727522727 I don’t mean to slight the other general detector at CERN which is CMS, but I only thought that we would have time for one detector description in class. %FFA8FD07FFC9FD0EFF52FD06FFC2A1FD54FF7DFD07FFA1FD0DFFA852FD06 %522752275227522752275227FD0D527DFD4DFF7DFD245227A8FD4DFFFD04 The LBNL ATLAS group consists of LBNL staff, UC Berkeley Faculty, Postdoctoral fellows and students. %7DFD45FFA87DFD2BFF7DA8FD45FF7D7DFD2BFF7D7DFD45FFA87DFD2BFF7D Copy link Link copied. %%+ 0 0.25 0 0 (Global Pink) In these models, the lightest chargino is predicted to have a lifetime long enough to be detected in the tracking detectors of collider experiments. %7DA87DFFFFA882828288FD068251FD0582A8FD09FF52FD06FFC2A1FD22FF It forms part of the ATLAS collaboration operating at the Large Hadron Collider (LHC) at CERN.. QUICK LINKS: Thin gap chambers Cathode strip chambers Resistive plate chambers. %5DFD1582588283FD0AFFC2CAFFFFA858825E828258F827F8F8278282825E 2 0 0 Radiation shield. %755E825E8258A8FD08FFA852FD06FF9AC9FD22FFA87DFFFFFFA88382825D %FFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8 PDF %%BoundingBox: 33 160 588 775 %7DFD04A87D7DA87DFFA8A87D7D527DA8A87DA87DA8A8FD0BFF99CAFFFFFF %FFC2CAFFFFA85E8282825D7CFD04F827825E828282A8FD09FF52FD1EFFA8 %09FF52FD06FFC2A1FD28FF5882582D57825D825D8282825D8282825D825D %52FD2FFFC2C9FD19FFA87DFD0452A8FD0BFF52A8FD11FF7DA87D7D7DFD04 %7DFD28FFC2C9FD1DFF52FD2AFF527DFD28FF9AC9FD1CFFA852FD2AFF7D7D %A8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DFD04A8FD0AFF Page 147 Service Bulletin June 15, 1999 Clinitek?Atlas?Rack Sample Handler NEW PH4 TUBE DETECTOR and REFLECTOR (Non-Mandatory) Service Bulletin Number: RACK - 001 Note the following changes in your Rack Sample Handler Service Manual, then initial and date these notes: Old … %C2C9FD28FF7C82F8272758515251825D8282825D825E822D272751F82751 %527DFD28FF9AC9FD1CFFA8527D7D527D527D527D527D527D527DFD1CFF7D %FFCC66FFCC99FFCCCCFFCCFFFFFF33FFFF66FFFF99FFFFCC110000001100 %A2A1CAA1CAFD0EFF52FD06FFC2A1FD24FF7EFFFFFF7C822727275827825D %8282825E8282825E8282825E82828258525852272751A8FD0EFF7D585782 %FFA8FFFFFFA8FD0DFF52A8FD72FF7D7DFD72FF7DA8FD1DFFA8FD54FF7D7D %585252F827277C7DFFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FD06FFA9A9FD It is connected to the insulated rail detector lead, (or the detector lead from the Atlas Block Detector Board (BDB), (Item #233). x��)�ƒcZ�����-�L��u=l�Z�����P����y4r3\E�wE��.�PJ$�É��_o�;Uˁi���?�Q!&�� ~�+��/#˿[U���! The search is based on 36.1 fb−1 of pp collisions at √ s = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. PDF. %5D8258A8FD08FFA852FD06FF9AC9FD28FF835E82588258825882827C8282 %000011111111220000002200000022222222440000004400000044444444 1.1 Inner Detector %7D7DFD0AFFA8FFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFF stream The datasets used correspond to integrated luminosities of approximately 4.8 fb−1 collected at √ s = 7TeV in 2011 and 5.8 fb−1 at √ %58FD068252F8F85227F8268283FFFFFF7DFD0AFFA85EFD09822DFD0582A8 '��� ������:o��� TUߙ�Jtw��c~�z��du��Z�bʤV����G� }�����a��U#��:���=�Ȫ)�e}3�F�?4eq�9��7����?��Ra�]'�a�D]$j��ܚ3 6�� ��vО�����//����W�l��J:Q�n��NL�+�F9�C3�����+lEY[i�be���Ж��-��V6���M� ^+��{�M�S}�ׅ���U�۾�L�J�v�J �[ ����9�R��U�� �\Yy�s�޼ueUH�^�}��!��$��J����Bۖ��� ��u���o���n�����_B��Q_d���9�C���F�C̦x���.kp�ą�����U������"8�>�負��I��{�ٷn�U�=4�T����䛾图��w0�\#+6��&�FeU� fm��y��+ScZ�[�7�?��������#�r��mF>�Mn�˧�s� �7Jp�qw�q�(b�.&���Z�˙�r��ν3 !��:���j氲5�&�}_u�:���Ҝx�d��f�O��'�\�Tl��4��j�������|����$7�ȥ��!������B�ɯ�V��*g)��FB;j�PYs5֤fj0�����ی޺�6SVO?���3�8��ˋ���^���S~v�{���F�ύ�NL�g(��ޙQ�;{�g((?4�?,�Wuyqe��p?����&���X�~,�F�"/��;$LO��m�ow�Z�j�?�). %527D52277DFF277D527DA87D527D52FF2752277D527D7D7D52527D7D527D This is just a brief presentation for my OLLI classes. %52FF527DA87D2752A87D527D527D275252A8527D277D5252277DFF272727 The ATLAS detector is designed to detect a vast array of signatures of various physics pro-cesses and excellent calibration and alignment of all detector components is paramount to achieve good performance and to fulﬁll the desired physics programme. %A8FD47FFA8277D527D5252527D5252527D5252527D5252527D5252527D52 A detailed understanding of %%PageOrigin:0 0 %52277D527D7D7D52527D7D527DFD0AFF52FD2AFFA8A8FD04FF7C82587C58 %27527DA87DA87D7D7DA8A1FD0DFFA87DFD06FF9ACAFD53FFA87D7DFD05FF %AI5_ArtFlags: 0 0 0 1 0 0 1 0 0 Data were collected in December 2009 using a minimum-bi %AI9_OpenToView: 72.5 533.5 2 1002 640 26 1 0 11 83 1 1 1 1 1 0 1 %F82027FD0582A8FD09FF52FD06FFC2A1FD22FFA8A8FD04FF588282825D82 %828282888282828882828288FD048258FD06F882A7FFFFFF7DA87DA87DA8 %6699CC6699FF66CC0066CC3366CC6666CC9966CCCC66CCFF66FF0066FF33 %00FF9900FFCC3300003300333300663300993300CC3300FF333300333333 %66FF6666FF9966FFCC66FFFF9900009900339900669900999900CC9900FF Search for new phenomena in events with same-charge leptons and b-jets in pp collisions at √s=13 TeV with the ATLAS detector.pdf 1,240 × 1,753, 57 pages; 1.29 MB The small wheel (sensor array) arrives at CERN 2.jpg 3,168 × 2,112; 2.85 MB %!PS-Adobe-3.0 MDT chambers. %%+ 1 0.5 0 0 (Global Night) endstream endobj 77 0 obj<>stream Copy link Link copied. %52275252522752525227525252275252522752525227525252275252527D %AI7_ImageSettings: 0 Stephanie Zimmermann (1973-2020) was a German physicist who worked on the ATLAS expriment at the Large Hadron Collider at CERN.As a researcher from the University of Freiburg, she was involved in the Muon Detector Control System activities, and she served as muon run-coordinator. %8282825E8282825E8282825D82828257A8FD0EFF7D8282825D7C272DFD04 %PDF-1.4 %���� %FFA8FFFFFFA8FD0FFFA8FFFFFFA8FFA8FFA8FFFFFFA8FFFFFFA8FFFFFFA8 %AI7_Thumbnail: 116 128 8 * c. DIN- DIN is the Detector Input. TLAS-CONF-2020-051 2020 ATLAS CONF Note ATLAS-CONF-2020-051 6thOctober2020 Search for displaced leptons in p s = 13 TeV pp collisions with the ATLAS detector TheATLASCollaboration %%Creator: Adobe Illustrator(R) 11.0 %52527D7D7D2752527D527D52A8A8A87DA8A8A87DA89AA17DA8A8A87DA8A8 %%+ 0.43 0.28 0 0 (Global Periwinkle) %522752525227525252275252522752525227525252275252522752525227 The ATLAS detector [1] is a multi-purpose apparatus designed to study a wide range of physics processes at the Large Hadron Collider (LHC) [2] at CERN. z�w��]��h��w&1��nGQ�wN %%CMYKProcessColor: 0 0 0 1 (Global Black) PDF. For example, Atlas currently uses extensive RD-180 engine health checks that occur prior to liftoff. %522752525227525252275252522752525227525252275252522752525227 %550000005500000055555555770000007700000077777777880000008800 %AI5_ArtSize: 612 792 %�쏢 %C2A1FD24FF7EFFFFFFA8A883A87DA883A87DA883A87DA883A87DA883A87D —The Level-1 Data Driver Card (L1DDC) is designed to fulfill the needs of the New Small Wheel, which will be used in the upgraded ATLAS experiment detectors. K�F��u�Mz)�c�~�R��HhjP����D� ��t��L|��k$1я��Z�hzt����Ĉ �"��GBK���3=�V?�G�JK9���Yx5v�&�8 PDF. the detector and collide in ATLAS, which creates new particles that are detected. 7μu&��.�e-U��VTu�S}m��3��R�v2e� ������]�O����&��V�X��dɌ#��n�7�p�����A"���}����.�ӿwZ �I#����._|$#? %A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8527DFD04A87D %A1A1CAA1CAA1CAA1CAA1CAA1C9A1CAA1CAA1CAA1CAA1CA77A1A1C9A8FD0D %FFCFFFCAFFCFFFCAFFCAFFCAFFCAFFCAFFCFA2A8FFCAC9FD0EFF52FD06FF %7D527D52527D527D7D7D277DA827527DFD05527D277DA8A8527D52A87D7D It is used to connect an auxiliary piece of equipment, (no more than +5VDC), such as an LED or relay. %7D7D7D837D7D7D837D837D837D7D7DFD09FFA852FD2AFFA8A8FFFFFFA883 %A87EA97EA87EA97EA87EA97EA87EA97EA87EA87E847EA87E847EA87E847E ATLAS Pixel Detector , Apr 13 2005 6 of 46 The ATLAS Inner Tracking Detector: Outermost system uses gas-filled 4mm straws • Contains 420K electronics channels. Download citation. ATLAS Upgrade 3 This Talk •Will be somewhat reductionist in starting with Silicon and emerging with an ATLAS Upgrade. ATLAS Toroidal Muon Spectrometer. %51512D825782828257A8FD08FFA852FD06FF9AC9FD27FFA883822DF827F8 %6600666600996600CC6600FF6633006633336633666633996633CC6633FF %57825882585E57827B82578257A8FD08FFA852FD06FF9AC9FD27FFA88382 %0099CC0099FF00CC0000CC3300CC6600CC9900CCCC00CCFF00FF3300FF66 %7C525852585227FD0582A8FD09FF52FD06FFC2A1FD28FF7C82F8F8F852F8 •Will not defend the upgrade based on expected Physics. It was installed in its underground cavern at the LHC during the period 2004 to 2008. %CC0000CC0033CC0066CC0099CC00CCCC00FFCC3300CC3333CC3366CC3399 %52525227527DFD4DFF7DFD2552A8FD4DFFFD26527DFD4DFFFD255227A8FD There are Pogo detection and correction algorithms and … %277D7D7D277D52A87DA8525252A8FFFFFFA8FFFFFFA8FFFFFFA8FD05FFA8 %%+ 0 1 1 0 (Global Red) Download citation. %FD0AFFA8FFFFFFA8FFFFFFA8FD07FFA8FFA87DA8FFFFFFA8FFFFFFA8FFFF %525227525252275252527DFD4DFF7DFD245227A8FD4DFFFD26527DFD4DFF %A8FD45FF7D7DFD2BFF7D7DFD45FFA87DFD2BFF52A8FD09FFA8A87DA8A8A8 Read full-text. 2 ATLAS detector The ATLAS detector covers almost the whole solid angle around the collision point with layers of tracking detectors, calorimeters and muon chambers. %5D825D7CF8272727262727585D8258A8FD08FFA852FD06FF9AC9FD28FF83 %7D52277DFD27FFC2C3FD2BFF52A8FD1BFF5252FD28FF9AC9FD2BFF52A8FD %27F87C5D8258A8FD08FFA852FD06FF9AC9FD28FF835DFD178283FD0EFFA8 %82825D8282825D8282825D8251585158587C57A8FD0EFF7D8281825D8251 For example, Atlas currently uses extensive RD-180 engine health checks that occur prior to liftoff. %09FF9AC9FD1AFFA8A87D7D7DFFA8FFFFFFA8FD06FF7D7DFD11FF7D7D7D52 %27FF7DF8FF52A8F852A87D527D52FFFF7D52FF27277DFF7D527D7DFD0452 Transition radiation detector gives particle ID. %FF66CCFF66FFFF9900FF9933FF9966FF9999FF99CCFF99FFFFCC00FFCC33 %FFA8FD05FFA8FFFFA8A8FFFFFFA8FD06FFA8A8FD07FFA8FD05FFA8FFA8FF %27522727275227272752FD04277DFD08FFFF %CFA8FFCAFF7DCACAFF7DA8CACFA0FD0DFFA852FD06FF9AC9FD24FFA9FFFF The entire detector weighs 7000 metric tons. x��][sݶ~ׯ8O���� �|Lb��4�\��Ndɒ�X�#�I�__ܱ~��H�L�d(� ���]]5bW�����������'���������_N��5�����f�ٙ�8��jT�����ǡ��f�7��Q���ߝݜ�w�g?����:)v5����.���n�vw���:�����Ӄ��0trs*�NH5�_���k尿;=Ȫ�1�_��U+����Ejp~zh��o����_���z�C[I�i�e�nVc��ߟj���m�N *��A��?�z�_�#}K�KCݦ�W�����?7�����LǪ:=��PM�Ø�5IL蝧���b���0j�f|2� Measurement of the $$W^{\pm}Z$$ Production Cross Section and Limits on Anomalous Triple Gauge Couplings at $$\sqrt s = 7 TeV$$ using the ATLAS detector %F8F827F8275D82828257A8FD08FFA852FD06FF9AC9FD22FFA8A8FD04FF83 The measurement probes The measurement probes the QCD sector of the Standard Model at high energy, in a region where b-quark mass It investigates a wide range of physics, from the search for the Higgs boson to extra dimensions and particles that could make up dark matter.Although it has the same scientific goals as the CMS experiment, it uses different technical solutions and a different magnet-system design. Abstract. The ATLAS detector at the CERN Large Hadron Collider is an apparatus of unprecedented complexity, designed to probe physics in proton-proton collisions at centre-of-mass energies up to 14 TeV. Download full-text PDF. %%+ 0.46 0 0 0 (Global Blue) %%+ 0 0 1 0 (Global Yellow) %33CCCC33CCFF33FF0033FF3333FF6633FF9933FFCC33FFFF660000660033 %52527D5252527D5252527D5252527D5252527D27A8FD45FF7D7DFD2BFF7D The ATLAS detector [1] is a multi-purpose apparatus designed to study a wide range of physics processes at the Large Hadron Collider (LHC) [2] at CERN. %0000330000660000990000CC0033000033330033660033990033CC0033FF %FF52FD06FFC3C9FD28FF7C82FD06F8585D578282825E8282825D8282825D The analysis is performed in the detector fiducial phase-space region, defined by the presence of two same-sign leptons, electron or muon, and at least two jets with a large invariant mass and rapidity difference. •Will assume some Unfamiliarity with the baseline ATLAS detector and will review the Inner tracker systems. This analysis was not unusual for Atlas, as the building blocks of an EDS system for Atlas are flying today. endstream endobj 78 0 obj 15636 endobj 79 0 obj<>stream %0066000066330066660066990066CC0066FF009900009933009966009999 %CC9966CC9999CC99CCCC99FFCCCC00CCCC33CCCC66CCCC99CCCCCCCCCCFF Read full-text. %A8FFFFFFA8FFA8FFA1FD0DFFA852FD06FF9AC9FD4BFFA8A87DA87DA87D7D Download full-text PDF Read full-text. %A8FD047DA8A87DA8FD057DA87DFD09FFA852FD2AFFA87DFD05FFA8272752 ATLAS is one of two general-purpose detectors at the Large Hadron Collider (LHC). %522752272727F8A8A8A827527D52A8A8F8527DA8A87D2727FF27522752F8 Track storm activity by adding the lightning detector to your AcuRite Atlas Weather Sensor. For all samples, the EvtGen v1.2.0 program [19] is used for properties of the bottom and charm hadron decays. Intermediate system is a large silicon strip tracker •Four barrel layers and 9 disk layers contain 61 m2 of silicon with 6.2M channels. %7DFD4DFF7DFD0B527D527D7DA8FD047D527D7D7DFD0C5227A8FD4DFFFD0E %525227527D7DA8FFA8FF7D7DA8A87DA8A87D275252522752525227525252 %AI5_NumLayers: 1 ATLAS has the dimensions of a cylinder, 46m long, 25m in diameter, and sits in a cavern 100m below ground. This analysis was not unusual for Atlas, as the building blocks of an EDS system for Atlas are flying today. %8258FD12827C5282A7FD0FFF83A87DA87D7D837E7DA87DA183A87DA8CFFD The reconstruction of tracks, leptons, photons, missing energy and jets is investigated, together with the performance of b-tagging and the trigger. A detailed understanding of %A8A8FFFFA8FFFFA8FFA8FFA8FFA8FFFFFFA8FFFFA8A8FD07FFA8FFA8FFA8 %825E825D825E825D8258585758F82757A7CACFA8FFCACFA8FFCACFA8FFCA %DD000000DD000000DDDDDDDDEE000000EE000000EEEEEEEE0000000000FF <> 5 0 obj %AI3_ColorUsage: Color %1BFF7D7DFD28FFC2C9FD1DFFA87D7DA8A8A87DA8A8A87DA8A8FF52FD1CFF This add-on allows AcuRite Atlas to detect lightning strikes within 25 miles (40 kilometers), track total strikes and estimate the distance of the most recent strike. H��Wko�� �A�0@�b,�z� %%HiResBoundingBox: 33.1875 160.6563 587.2725 774.1597 The ATLAS detector weighs 7,000 tonnes, similar to the weight of the Eiffel Tower. Model Higgs Boson with the ATLAS Detector at the LHC The ATLAS Collaboration Abstract A search for the Standard Model Higgs boson in proton-protoncollisions with the ATLAS detector at the LHC is presented. %825D825D5827525158F82757A7FD0AFF99CAFFFF7D825D82828251FD04F8 %7C82F827275227825D8282825E8282825E8252522D27F827517DA8A87DA8 •Will describe the Novel Next Gen tracking sensors at the end.. %8282828382595888827C82888282A8FD09FF52FD06FFC3C9FD28FF7C825D %%+ 0.33 0 0.73 0 (Global Lime) %FF3300FF3333FF3366FF3399FF33CCFF33FFFF6600FF6633FF6666FF6699 %5227522752275227527DFD4DFFFD255227A8FD4DFF525227525252275252 The ATLAS Detector is a particle physics experiment that explores the frontiers of the Standard Model (SM) of Physics. b. DOUT- DOUT is the optional Detector Output. She was elected and served as ATLAS Run-Coordinator in 2012–2014. %45FFA8FF7DF8F8FD05A8769375FD0CA827F852A8A8A8FF7D6F6EA7A8FD4E %28FFC2CAFD1DFF52FD2AFF2752A8FD27FF99CAFD1CFFA852FD24FFA87DA8 ATLAS Pixel Detector , Apr 13 2005 6 of 46 The ATLAS Inner Tracking Detector: Outermost system uses gas-filled 4mm straws • Contains 420K electronics channels. %F827F827F85157A7FFFF7D7DA8FD09FF7D825D8282825D825D8257525882 %06FF9AC9FD27FFA8838227F8277D27F8525858FD0E82A7FD0EFFA8FD0482 %9AC9FD25FFA8FFA8A9A8FFA8A9A8FFA8A9A8FFA8A9A8FFA8A9A8FFA9FFA9 Download full-text PDF. There are Pogo detection and correction algorithms and … ATLAS at LBNL The ATLAS Detector. %CC33CCCC33FFCC6600CC6633CC6666CC6699CC66CCCC66FFCC9900CC9933 %5226515127277CA1CAA7CAC9CAA7CAC9CAA7CAC9CAA7CAC9CAA7A7A1CAC9 %FF5252275227522752275227522752275227522752275227522752272727 %8282825DFD0B825D82827C828283FD0AFFC3BBC2BCBC9999999F9876F827 %5E8282825127F827F827F82751828282A8FD09FF52FD06FFC2C9FD28FF7C %%AI8_CreatorVersion: 11.0.0 %A8FFA8FFFFFFA8FFFFFFA8FFFFA8FFFFA8FD05FFA8FDFCFFFDFCFFFDFCFF %FD09FF52FD06FFC2C9FD28FF7C8257825D8257825D8257825E825D825D7C %FD06FF7D7DFD11FF7D277D7D7DF8527D52277DFFA8FD10FFA87D27527D7D %FD28FFC3C9FD1DFF52FD2AFF527DFD28FF99CAFD1CFFA852FD2AFF7D7DFD ��D�z;�����tP����ȢW��z}/II���� �A��o^�K���r����E��ȹ�x�.idީ��1bgYU}�5Zt�p��@ڊ/����l�R�7Fg����z��t~R�[����+�Uy{��벫$X��|_��c;�s�'N Z�����x��%1�xC��o�Q���(�m�~�q�J���|��76�h� azM�� \�"��R��������m��J5퍓�ڹͷ�ɝO���W'��͗�O��lo�M���>���;)Y|߈/�第$tq�w5=�K����Bf(B6r��܃�Qv,-Hn?�c^7� �s��R/yeK6=���~8�Խ���x��)�I��f����#A�s�Y��\�(s�W�nL�J�+��Q��v^˪���)��cv�^6�ײ�R�Yr���S]mt������ t�)LVa *|�y��F�U�^�aC0�r�"��� �m)���Vo���� p��B&\M:aw�hq�t3�E�����:��������a"g�3��������3�i#ƉT/�T�e��2x��"�&އԉ�b�f�ϋ�%�@�r���o9QS�j�����X�`_����#o?�nk8u۩�ά�I�����wC���S�������ᘬ���A��P�ak��\S�B�~��m��kC����͠J����F�0��! %%DocumentProcessColors: Cyan Magenta Yellow Black %AI7_GridSettings: 2.25 8 2.25 8 1 0 0.8 0.8 0.8 0.9 0.9 0.9 The road to stable data taking with the ATLAS detector began in the early 1990s, with beam testing of prototype designs for different detector subsystems. L1DDC's function is to concentrate the data from multiple front-end boards and transmit The ATLAS detector site www.atlas.ch provides a comprehensive presentation of the detector and its physics. %A8FFA8A8A8FFA8A8A8FFA8A8A8FFA8A8A8FFA8A8A8FFA8A8A8FFA8A8A8FF %CCFF00CCFF33CCFF66CCFF99CCFFCCCCFFFFFF0033FF0066FF0099FF00CC %52277C587CFD0482A8FD09FF52FD06FFC2A1FD28FF7C8282825E8282825E A detailed study is presented of the expected performance of the ATLAS detector. %FF9AC9FD54FFA8FD07FFC9FD0EFF52FD06FFC2A1FD54FF7DFD07FFA1FD0D %%+ 0.3255 0.4431 0.5373 0.1961 (Global Malt) %A883828258FD13827C8283FD12FFA8FFFFFFA9A9FFFFC9FD0EFF52FD06FF %%EndData Growth, characterization and study of critical rare-earth poor/free magnetic materials, Tej Nath Lamichhane. The first measurements from proton–proton collisions recorded with the ATLAS detector at the LHC are presented. The physics %%+ 0 0.5 1 0 (Global Orange) %AI3_DocumentPreview: None %FD05FF52A8FD11FFFD077DA87D7D7DFD15FFA8FFA8FFFFFFA8FFFFFFA8FD %AI5_FileFormat 7.0 %AI3_TemplateBox: 306.5 395.5 306.5 395.5 %8288828282888282828882828288FD04822D7C52525182A7FD0EFFA88288 %%BeginData: 11229 Hex Bytes Tuning of layered materials: Studies of CrAuTe4, PdSn4 and WTe2, Na Hyun Jo. The effect of in-time as well as out-of-time pile-up is simulated using minimum-bias events %FF835E27FD05F8828288828282888282587C7C8252272782A7FD0AFFC2CA %FFA852527DFD27FF9AC9FD1AFFA8FFFFFFA8FD0CFF7D7DFD1AFFFD0452FD %%HiResBoundingBox: 33.1875 160.6563 587.2725 774.1597 The ATLAS detector is a general-purpose particle detector ... and the CTEQ6L1 PDF set. %%For: (Steve Horvath) (Atlas) %%Title: (WIRE ATLAS SCB TO NCE BD20.pdf) %8258A7FD0EFF7D825D8282825E8227512D5882825E8258A8FD08FFA852FD %A88382522758587C82888282828882828288828258825227278283FFA8FF %577DA8A8A852525227FD0552A8FF7D8282825E8282825D82582758828282 %7DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8 The ATLAS detector is designed to detect a vast array of signatures of various physics pro-cesses and excellent calibration and alignment of all detector components is paramount to achieve good performance and to fulﬁll the desired physics programme. %FFA852FD06FF9AC9FD54FFA8A8FD06FFC9CFFD0DFF52FD06FFC2C9FD54FF %C9C3C9C3C9C9BCC9FD22FFA8A8FD04FF7C82587C5858577C82825E828282 %%+ 1 1 1 1 ([Registration]) It is 44 m long and 25 m in diameter. %828282577C5851F827517DFD04A87DA8A8A87DA8A8A87DA8A8A87DA87DFF %99CC6699CC9999CCCC99CCFF99FF0099FF3399FF6699FF9999FFCC99FFFF %FFA8A87DFFA8FFA8835E27F82752F8F8FD09825858588252F8278283FD0A %CFFD0DFF52FD06FFC3C9FD54FFA8FD07FFA1FD0DFFA852FD06FF9AC9FD54 %AI9_ColorModel: 2 %AI5_RulerUnits: 0 %82A8FD09FF52FD20FFA8FFFFFFA8FFA8FFFFFFA8A8FD04FF7C8227F8F827 [E��� 1x ��"���\3�&���}�@HwQ����qKG %FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFF j1 j2 j3 j4 j5 j6 jp 1 jp 2 rin dout din yin com pwr com pwr ain aux1 gnd ogic y o 12vdc atlas signal control board nce bd-20 detector power supply insulated rail insulated rail joiner %58A8FD08FFA852FD06FF9AC9FD23FF7DA87DA87D58587C587C587C587C58 luminosity of 4:6 fb 1, collected with the ATLAS detector. %52525227527DFD4DFF7DFD2552A8FD4DFFFD0C5227525252275252522752 %825D8282825D8282825D8282825D82828257525152F82757A8FD0EFF7D82 %6666006666336666666666996666CC6666FF669900669933669966669999 Craute4, PdSn4 and WTe2, Na Hyun Jo and study of critical poor/free... 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