%CFFD0DFF52FD06FFC3C9FD54FFA8FD07FFA1FD0DFFA852FD06FF9AC9FD54 %8282825E8282825E8282825D82828257A8FD0EFF7D8282825D7C272DFD04 ATLAS is one of two general-purpose detectors at the Large Hadron Collider (LHC). %0099CC0099FF00CC0000CC3300CC6600CC9900CCCC00CCFF00FF3300FF66 Transition radiation detector gives particle ID. %A8FFA8FFFFFFA8FFFFFFA8FFFFA8FFFFA8FD05FFA8FDFCFFFDFCFFFDFCFF ATLAS at LBNL The ATLAS Detector. K�F��u�Mz)�c�~�R��HhjP����D� ��t��L|��k$1я��Z�hzt����Ĉ �"��GBK���3=�V?�G�JK9���Yx5v�&�8 %5DFD1582588283FD0AFFC2CAFFFFA858825E828258F827F8F8278282825E 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 … For example, Atlas currently uses extensive RD-180 engine health checks that occur prior to liftoff. Thin gap chambers Cathode strip chambers Resistive plate chambers. %%Title: (WIRE ATLAS SCB TO NCE BD20.pdf) * c. DIN- DIN is the Detector Input. %A2A1CAA1CAFD0EFF52FD06FFC2A1FD24FF7EFFFFFF7C822727275827825D %6699CC6699FF66CC0066CC3366CC6666CC9966CCCC66CCFF66FF0066FF33 %06FF9AC9FD27FFA8838227F8277D27F8525858FD0E82A7FD0EFFA8FD0482 %FD06FF7D7DFD11FF7D277D7D7DF8527D52277DFFA8FD10FFA87D27527D7D 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. %1BFF7D7DFD28FFC2C9FD1DFFA87D7DA8A8A87DA8A8A87DA8A8FF52FD1CFF Intermediate system is a large silicon strip tracker •Four barrel layers and 9 disk layers contain 61 m2 of silicon with 6.2M channels. The tracking modules and the trigger system are of most relevance for the presented measurements. 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��! %%PageOrigin:0 0 %585252F827277C7DFFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FD06FFA9A9FD %AI3_TemplateBox: 306.5 395.5 306.5 395.5 In addition to measurements of Stan-dard Model processes such as vector-boson and top-quark production, the properties of the newly %52525227527DFD4DFF7DFD2552A8FD4DFFFD26527DFD4DFFFD255227A8FD 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. %A87E847EA87E847EA87E847EA87D7E7EA85AFFFFFFA1FD0DFFA852FD06FF The measurement probes The measurement probes the QCD sector of the Standard Model at high energy, in a region where b-quark mass A detailed understanding of %825D8282825D8282825D8282825D82828257525152F82757A8FD0EFF7D82 %A8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DFD04A8FD0AFF %AI7_Thumbnail: 116 128 8 %5E8282825D825D82F87C5EA7FD0AFF99CACAFF7D827B828182756F6F6F6E %27527DA87DA87D7D7DA8A1FD0DFFA87DFD06FF9ACAFD53FFA87D7DFD05FF %F8F827F8275D82828257A8FD08FFA852FD06FF9AC9FD22FFA8A8FD04FF83 H��Wko�� �A�0@�b,�z� %%+ 0.8 0 1 0 (Global Green) •Will assume some Unfamiliarity with the baseline ATLAS detector and will review the Inner tracker systems. %A87DA8A8A87DA87DA87DA852A87DA8A8A87DA8A8A87DA8A8A87DA8A87D52 %825E825D825E825D8258585758F82757A7CACFA8FFCACFA8FFCACFA8FFCA It is connected to the insulated rail detector lead, (or the detector lead from the Atlas Block Detector Board (BDB), (Item #233). %755E825E8258A8FD08FFA852FD06FF9AC9FD22FFA87DFFFFFFA88382825D %8282828382595888827C82888282A8FD09FF52FD06FFC3C9FD28FF7C825D %9AC9FD25FFA8FFA8A9A8FFA8A9A8FFA8A9A8FFA8A9A8FFA8A9A8FFA9FFA9 The ATLAS detector. %9966CC9966FF9999009999339999669999999999CC9999FF99CC0099CC33 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 %0000330000660000990000CC0033000033330033660033990033CC0033FF %%HiResBoundingBox: 33.1875 160.6563 587.2725 774.1597 x��)�ƒcZ�����-�L��u=l�Z�����P����y4r3\E�wE��.�PJ$�É��_o�;Uˁi���?�Q!&�� ~�+��/#˿[U���! %%AI8_CreatorVersion: 11.0.0 For example, Atlas currently uses extensive RD-180 engine health checks that occur prior to liftoff. %8282825E8282825E8282825E82828258525852272751A8FD0EFF7D585782 %A87DA8A8A87DA8A8A87DA8A8A87DA8A8A8527D5252527D7D2752A87DA87D L1DDC's function is to concentrate the data from multiple front-end boards and transmit ATLAS Upgrade 3 This Talk •Will be somewhat reductionist in starting with Silicon and emerging with an ATLAS Upgrade. 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 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. 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. %6666006666336666666666996666CC6666FF669900669933669966669999 %52FF527DA87D2752A87D527D527D275252A8527D277D5252277DFF272727 %3333663333993333CC3333FF3366003366333366663366993366CC3366FF %27F87C5D8258A8FD08FFA852FD06FF9AC9FD28FF835DFD178283FD0EFFA8 %%+ 0.5 0.9 0 0 (Global Plum) %28FFC2CAFD1DFF52FD2AFF2752A8FD27FF99CAFD1CFFA852FD24FFA87DA8 %%+ 0.43 0.28 0 0 (Global Periwinkle) PDF. %7C82F827275227825D8282825E8282825E8252522D27F827517DA8A87DA8 stream This analysis was not unusual for Atlas, as the building blocks of an EDS system for Atlas are flying today. •Will describe the Novel Next Gen tracking sensors at the end.. %52FD2FFFC2C9FD19FFA87DFD0452A8FD0BFF52A8FD11FF7DA87D7D7DFD04 [E��� 1x ��"���\3�&���}�@HwQ����qKG %52525227527DFD4DFF7DFD2552A8FD4DFFFD0C5227525252275252522752 The first measurements from proton–proton collisions recorded with the ATLAS detector at the LHC are presented. luminosity of 4:6 fb 1, collected with the ATLAS detector. %7DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8 12 m 10 8 6 4. %527D527D7D52527D7DFD08FFC2C9FD19FFA87D277D7D7D27527D522752A8 %33CCCC33CCFF33FF0033FF3333FF6633FF9933FFCC33FFFF660000660033 %7D277D27A8527D7D52527D527D52A8A852527D5227A8522752277DFFFD04 %7DA87D514B7DFD27FFC2CAFD1DFF52FD24FF52525227277D27517DFD05FF %%DocumentProcessColors: Cyan Magenta Yellow Black Download citation. %%+ 1 0.5 0 0 (Global Night) %CC0000CC0033CC0066CC0099CC00CCCC00FFCC3300CC3333CC3366CC3399 %FFFFFFA8FFFFFFA8FD04FFA87DFD11FF52A8FD09FFA8A87DA8A8A87DA87D %57825882585E57827B82578257A8FD08FFA852FD06FF9AC9FD27FFA88382 z�w��]��h��w&1��nGQ�wN %A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8FF7EFFFFFFA1FD0DFFA852FD06 %%HiResBoundingBox: 33.1875 160.6563 587.2725 774.1597 %AI9_Flatten: 0 %000011111111220000002200000022222222440000004400000044444444 %7D7D7D837D7D7D837D837D837D7D7DFD09FFA852FD2AFFA8A8FFFFFFA883 %7D52FD057DFFFF7D527D52527D7D2752277D7D7D52A8FF52527D52A852A8 MDT chambers. %7DFD04A87D7DA87DFFA8A87D7D527DA8A87DA87DA8A8FD0BFF99CAFFFFFF %52527D7D7D2752527D527D52A8A8A87DA8A8A87DA89AA17DA8A8A87DA8A8 %DD000000DD000000DDDDDDDDEE000000EE000000EEEEEEEE0000000000FF 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. %66FF6666FF9966FFCC66FFFF9900009900339900669900999900CC9900FF %8288828282888282828882828288FD04822D7C52525182A7FD0EFFA88288 Growth, characterization and study of critical rare-earth poor/free magnetic materials, Tej Nath Lamichhane. %51512D825782828257A8FD08FFA852FD06FF9AC9FD27FFA883822DF827F8 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 %7DA852A87D52277D7DC9CFFD0DFF52FD06FFC3C9FD4BFF7D52527D7D5227 %27FFC3C9FD2BFF7DA8FD19FFA852527D27FD27FF9AC9FD2BFF7D7DFD1AFF 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 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 √ %99CC6699CC9999CCCC99CCFF99FF0099FF3399FF6699FF9999FFCC99FFFF 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). %%CMYKProcessColor: 0 0 0 1 (Global Black) %FFA8FFFFFFA8FD0FFFA8FFFFFFA8FFA8FFA8FFFFFFA8FFFFFFA8FFFFFFA8 The ATLAS detector is a general-purpose particle detector ... and the CTEQ6L1 PDF set. 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� It forms part of the ATLAS collaboration operating at the Large Hadron Collider (LHC) at CERN.. QUICK LINKS: %%EndData %AI5_ArtFlags: 0 0 0 1 0 0 1 0 0 %FD09FF52FD06FFC2C9FD28FF7C8257825D8257825D8257825E825D825D7C %%+ 0 0.5 1 0 (Global Orange) <> %27FF7DF8FF52A8F852A87D527D52FFFF7D52FF27277DFF7D527D7DFD0452 The ATLAS detector site www.atlas.ch provides a comprehensive presentation of the detector and its physics. %527D52277DFF277D527DA87D527D52FF2752277D527D7D7D52527D7D527D She was elected and served as ATLAS Run-Coordinator in 2012–2014. %8258FD12827C5282A7FD0FFF83A87DA87D7D837E7DA87DA183A87DA8CFFD It is used to connect an auxiliary piece of equipment, (no more than +5VDC), such as an LED or relay. Search for the Lepton Flavor Violating decay Z → eμ with the ATLAS detector at the LHC, Hai Jiang. 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. %7D52277DFD27FFC2C3FD2BFF52A8FD1BFF5252FD28FF9AC9FD2BFF52A8FD %52277D527D7D7D52527D7D527DFD0AFF52FD2AFFA8A8FD04FF7C82587C58 %FFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8 It is 44 m long and 25 m in diameter. %AI5_TargetResolution: 800 %7DFD2552A8FD4DFFFD052752272727522727275227272752272727522727 %FFFFA85E88828282A04B754B756F9F7BA07BA0A0C9C3C9C3C9C3C9C3C976 Intermediate system is a large silicon strip tracker •Four barrel layers and 9 disk layers contain 61 m2 of silicon with 6.2M channels. Download full-text PDF Read full-text. The effect of in-time as well as out-of-time pile-up is simulated using minimum-bias events Track storm activity by adding the lightning detector to your AcuRite Atlas Weather Sensor. Download full-text PDF Read full-text. %%+ 0.3255 0.4431 0.5373 0.1961 (Global Malt) %A8FD45FF7D7DFD2BFF7D7DFD45FFA87DFD2BFF52A8FD09FFA8A87DA8A8A8 Wire color optional. %AI5_NumLayers: 1 %!PS-Adobe-3.0 %AI3_ColorUsage: Color Download full-text PDF. %%BeginData: 11229 Hex Bytes 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. %828882828288FD068283FD0EFFA88288FD06825882588282888282A8FD09 %A8FFFFFFA8FFA8FFA1FD0DFFA852FD06FF9AC9FD4BFFA8A87DA87DA87D7D %0066000066330066660066990066CC0066FF009900009933009966009999 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. %AI7_ImageSettings: 0 %FD4DFF7DFD245227A8FD4DFFFD26527DFD4DFF7DFD245227A8FD4DFFFD04 %00FF9900FFCC3300003300333300663300993300CC3300FF333300333333 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. %FF66CCFF66FFFF9900FF9933FF9966FF9999FF99CCFF99FFFFCC00FFCC33 %7D7DFD0AFFA8FFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFF There are Pogo detection and correction algorithms and … %AI5_ArtSize: 612 792 Read full-text. %%For: (Steve Horvath) (Atlas) %F8518258825D8282825D8282825D82828257A8FD0EFF7D825E825D7CF87C %C9C3C9C3C9C9BCC9FD22FFA8A8FD04FF7C82587C5858577C82825E828282 %FFA9FFA9FFA9FFA9FFA9FFA9FFA9FFA9FFA9FFA9FFA9A8A8FFA9FD04FFC9 %F87D275227F8527D52525227277D275227F827A8FD0BFFC2CAFFFFFFFD04 %525227525252275252527DFD4DFF7DFD245227A8FD4DFFFD26527DFD4DFF A detailed understanding of 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- %5252277DA87D277D52FF527D527D5227A8FF277D277DFFA87DFF7DFF2752 2 0 0 Radiation shield. %27522727275227272752FD04277DFD08FFFF %%BoundingBox: 33 160 588 775 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. %27F87C828282888282828882828288FD0482A7FD0EFFA8828282887C5258 There are Pogo detection and correction algorithms and … %82A8FD09FF52FD20FFA8FFFFFFA8FFA8FFFFFFA8A8FD04FF7C8227F8F827 %7DA8527DA8527D272752FF27FFA82727A85252A87D27527D52277D7DA87D %FFC2CAFFFFA85E8282825D7CFD04F827825E828282A8FD09FF52FD1EFFA8 The physics %A1A1CAA1CAA1CAA1CAA1CAA1C9A1CAA1CAA1CAA1CAA1CA77A1A1C9A8FD0D 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). %PDF-1.4 ��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������ %%CreationDate: 10/29/2008 10:20 AM In these models, the lightest chargino is predicted to have a lifetime long enough to be detected in the tracking detectors of collider experiments. %550000005500000055555555770000007700000077777777880000008800 %A8FD047DA8A87DA8FD057DA87DFD09FFA852FD2AFFA87DFD05FFA8272752 %27759F759F75A0A0C3A0C2A0C3A0C39A76A0C2A0C3A0C2A0FD24FFA8FD04 %525227FD0D527DFD4DFFFD16527DFD0E5227A8FD4DFF5252275252522752 %AI5_FileFormat 7.0 Download citation. endstream endobj 78 0 obj 15636 endobj 79 0 obj<>stream %%Creator: Adobe Illustrator(R) 11.0 PDF. %FD0AFFA8FFFFFFA8FFFFFFA8FD07FFA8FFA87DA8FFFFFFA8FFFFFFA8FFFF %FFCFFFCAFFCFFFCAFFCAFFCAFFCAFFCAFFCFA2A8FFCAC9FD0EFF52FD06FF b. DOUT- DOUT is the optional Detector Output. %09FF9AC9FD1AFFA8A87D7D7DFFA8FFFFFFA8FD06FF7D7DFD11FF7D7D7D52 %825782515857A8FD14FFA8FF7EFFFFFFA1FD0DFFA852FD06FF9AC9FD27FF %FD05FFA16876FD0CFF27F852FD05FF6E6FA17D522727525252272727A8FD %277D7D7D277D52A87DA8525252A8FFFFFFA8FFFFFFA8FFFFFFA8FD05FFA8 The physics The detector itself is a many-layered instrument designed to detect some of the tiniest yet most energetic particles ever created on earth. %58A8FD08FFA852FD06FF9AC9FD23FF7DA87DA87D58587C587C587C587C58 %7DFD28FFC2C9FD1DFF52FD2AFF527DFD28FF9AC9FD1CFFA852FD2AFF7D7D %%+ 0 1 1 0 (Global Red) %52FFA852FF52FFF852277D5252527DA8F8A8FF275252FF27275252277DA8 %%+ 0.46 0 0 0 (Global Blue) %C2C9FD28FF7C82F8272758515251825D8282825D825E822D272751F82751 %FF835E27FD05F8828288828282888282587C7C8252272782A7FD0AFFC2CA %825D8252FD04F8275E82828258A8FD08FFA852FD1FFFFD0452277D7D7DFF %A87DFFFFA8A85882588258825882588282825E8282825D58F8F85252F827 The ATLAS Detector is a particle physics experiment that explores the frontiers of the Standard Model (SM) of Physics. %828282577C5851F827517DFD04A87DA8A8A87DA8A8A87DA8A8A87DA87DFF %%+ 1 1 1 1 ([Registration]) %5D825D7CF8272727262727585D8258A8FD08FFA852FD06FF9AC9FD28FF83 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. %FFFFA8FFFFFFA8FD09FFA8A8FFA9A9FFCACAFD0EFF52FD06FFC2A1FD28FF %58FD068252F8F85227F8268283FFFFFF7DFD0AFFA85EFD09822DFD0582A8 Download PDF Abstract: ... =13$TeV by the ATLAS detector at the Large Hadron Collider. It was installed in its underground cavern at the LHC during the period 2004 to 2008. Data were collected in December 2009 using a minimum-bi A detailed study is presented of the expected performance of the ATLAS detector. Copy link Link copied. ATLAS has the dimensions of a cylinder, 46m long, 25m in diameter, and sits in a cavern 100m below ground. For all samples, the EvtGen v1.2.0 program [19] is used for properties of the bottom and charm hadron decays. ��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� %FFA852FD06FF9AC9FD27FFA8835E27F852587C7C82828882828288828282 However, the accuracy and precision of the ATLAS Detector may vary depending on di erent factors, for example the energies of the particles created. %45FFA8FF7DF8F8FD05A8769375FD0CA827F852A8A8A8FF7D6F6EA7A8FD4E %5226515127277CA1CAA7CAC9CAA7CAC9CAA7CAC9CAA7CAC9CAA7A7A1CAC9 %4DFF52522752525227525252275252522752525227525252275252522752 the detector and collide in ATLAS, which creates new particles that are detected. %FF9AC9FD28FF838227F8525882587CFD09827C517C5127F87CA7FFCFFFCA Tuning of layered materials: Studies of CrAuTe4, PdSn4 and WTe2, Na Hyun Jo. The Editors also warmly thank Michèle Jouhet and Isabelle Canon %828282888282828882828288FD048258FD06F882A7FFFFFF7DA87DA87DA8 %5E8282825127F827F827F82751828282A8FD09FF52FD06FFC2C9FD28FF7C In addition to measurements of Stan-dard Model processes such as vector-boson and top-quark production, the properties of the newly The reconstruction of tracks, leptons, photons, missing energy and jets is investigated, together with the performance of b-tagging and the trigger. This analysis was not unusual for Atlas, as the building blocks of an EDS system for Atlas are flying today. 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. %�쏢 PDF. %FFA852527DFD27FF9AC9FD1AFFA8FFFFFFA8FD0CFF7D7DFD1AFFFD0452FD %522752272727F8A8A8A827527D52A8A8F8527DA8A87D2727FF27522752F8 %F827588282825E8282825D7C27525D58F82757A8FD0AFF99CFFFFF7D8282 %AI9_OpenToView: 72.5 533.5 2 1002 640 26 1 0 11 83 1 1 1 1 1 0 1 %9933009933339933669933999933CC9933FF996600996633996666996699 Measurements of the top-quark mass with the ATLAS detector Teresa Barillari 3. 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 … •Will not defend the upgrade based on expected Physics. %CFA8FFCAFF7DCACAFF7DA8CACFA0FD0DFFA852FD06FF9AC9FD24FFA9FFFF %A8FD47FFA8277D527D5252527D5252527D5252527D5252527D5252527D52 %FF3300FF3333FF3366FF3399FF33CCFF33FFFF6600FF6633FF6666FF6699 %A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8527DFD04A87D These were followed by similar testbeam campaigns for “module-0” prototypes of the final design, and then for the series production modules. %FFFF7EFD11FFA852FD06FF9AC9FD24FFA9FFFFA8838227F852587CFD0B82 A detailed study is presented of the expected performance of the ATLAS detector. %6600666600996600CC6600FF6633006633336633666633996633CC6633FF %%EndComments %7DFD45FFA87DFD2BFF7DA8FD45FF7D7DFD2BFF7D7DFD45FFA87DFD2BFF7D %AI5_RulerUnits: 0 5 0 obj %AI9_ColorModel: 2 %FF9AC9FD54FFA8FD07FFC9FD0EFF52FD06FFC2A1FD54FF7DFD07FFA1FD0D %FD05FF52A8FD11FFFD077DA87D7D7DFD15FFA8FFA8FFFFFFA8FFFFFFA8FD %52275252522752525227525252275252522752525227525252275252527D %C2A1FD24FF7EFFFFFFA8A883A87DA883A87DA883A87DA883A87DA883A87D %00FF0000FFFFFF0000FF00FFFFFF00FFFFFF —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. 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. %FF5252275227522752275227522752275227522752275227522752272727 %5227522752275227527DFD4DFFFD255227A8FD4DFF525227525252275252 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. %8282825DFD0B825D82827C828283FD0AFFC3BBC2BCBC9999999F9876F827 %FD28FFC3C9FD1DFF52FD2AFF527DFD28FF99CAFD1CFFA852FD2AFF7D7DFD %000088888888AA000000AA000000AAAAAAAABB000000BB000000BBBBBBBB 7μu&��.�e-U��VTu�S}m��3��R�v2e� ������]�O����&��V�X��dɌ#��n�7�p�����A"���}����.�ӿwZ �I#����._|$#? 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. %7C525852585227FD0582A8FD09FF52FD06FFC2A1FD28FF7C82F8F8F852F8 %CC9966CC9999CC99CCCC99FFCCCC00CCCC33CCCC66CCCC99CCCCCCCCCCFF The ATLAS detector weighs 7,000 tonnes, similar to the weight of the Eiffel Tower. %522752525227525252275252522752525227525252275252522752525227 %09FF52FD06FFC2A1FD28FF5882582D57825D825D8282825D8282825D825D %AI5_OpenViewLayers: 7 %A87DA87D7DA8A87DFFA8A87D7DA8A87DA8527CF8F8F827F8F858825D8282 %%+ 0 0.25 0 0 (Global Pink) %525227527D7DA8FFA8FF7D7DA8A87DA8A87D275252522752525227525252 %FFA8FD07FFC9FD0EFF52FD06FFC2A1FD54FF7DFD07FFA1FD0DFFA852FD06 %A88382522758587C82888282828882828288828258825227278283FFA8FF 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. ATLAS Toroidal Muon Spectrometer. PDF This is just a brief presentation for my OLLI classes. %FDFCFFFDFCFFFDFCFFFDFCFFFDFCFFFD17FFA8FFA8A8A8FFA8A8A8FFA8A8 Transition radiation detector gives particle ID. %FFA8FD05FFA8FFFFA8A8FFFFFFA8FD06FFA8A8FD07FFA8FD05FFA8FFA8FF End-cap toroid Barrel toroid coil. Copy link Link copied. :���v[b. %52527D5252527D5252527D5252527D5252527D27A8FD45FF7D7DFD2BFF7D 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. %522752525227525252275252522752525227525252275252522752525227 %FF52FD06FFC3C9FD28FF7C82FD06F8585D578282825E8282825D8282825D 1.1 Inner Detector %3399003399333399663399993399CC3399FF33CC0033CC3333CC6633CC99 The LBNL ATLAS group consists of LBNL staff, UC Berkeley Faculty, Postdoctoral fellows and students. %A883828258FD13827C8283FD12FFA8FFFFFFA9A9FFFFC9FD0EFF52FD06FF %A8A8FFFFA8FFFFA8FFA8FFA8FFA8FFFFFFA8FFFFA8A8FD07FFA8FFA8FFA8 %CAA1A8FD0CFFA827FD06FFA0A1FF7DA8A8A87DA8FD047DA8FD47FFA8F8F8 %FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFF %524C457D527D2752525227A8527D7DFF527D2727A8FF52A852FF7D7D527D %522752275227522752275227FD0D527DFD4DFF7DFD245227A8FD4DFFFD04 The reconstruction of tracks, leptons, photons, missing energy and jets is investigated, together with the performance of b-tagging and the trigger. 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 %7DA87DFFFFA882828288FD068251FD0582A8FD09FF52FD06FFC2A1FD22FF %527DFD28FF9AC9FD1CFFA8527D7D527D527D527D527D527D527DFD1CFF7D %7C7C7C5883587C587C7C7C587C587C587C7C8258A8FD0AFF99CFFFFFA883 %CCFF00CCFF33CCFF66CCFF99CCFFCCCCFFFFFF0033FF0066FF0099FF00CC %11FF52FD06FFC3C9FD24FF7E7E7EA85258272727582D7C5D825E8282825E 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 bottom and charm Hadron decays proton–proton collisions recorded with the baseline detector. 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