ATLAS is one of two general-purpose detectors at the Large Hadron Collider (LHC). %8282828382595888827C82888282A8FD09FF52FD06FFC3C9FD28FF7C825D %%Title: (WIRE ATLAS SCB TO NCE BD20.pdf) 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 %7DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8 There are Pogo detection and correction algorithms and … 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. This is just a brief presentation for my OLLI classes. 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. %58A8FD08FFA852FD06FF9AC9FD23FF7DA87DA87D58587C587C587C587C58 %52275252522752525227525252275252522752525227525252275252527D 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��! 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. %524C457D527D2752525227A8527D7DFF527D2727A8FF52A852FF7D7D527D %%AI8_CreatorVersion: 11.0.0 %525227525252275252527DFD4DFF7DFD245227A8FD4DFFFD26527DFD4DFF %8258A7FD0EFF7D825D8282825E8227512D5882825E8258A8FD08FFA852FD %A87DA8A8A87DA8A8A87DA8A8A87DA8A8A8527D5252527D7D2752A87DA87D %%BoundingBox: 33 160 588 775 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. b. DOUT- DOUT is the optional Detector Output. %FD05FFA16876FD0CFF27F852FD05FF6E6FA17D522727525252272727A8FD %825782515857A8FD14FFA8FF7EFFFFFFA1FD0DFFA852FD06FF9AC9FD27FF 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� %FFFFA85E88828282A04B754B756F9F7BA07BA0A0C9C3C9C3C9C3C9C3C976 Download citation. %52527D7D7D2752527D527D52A8A8A87DA8A8A87DA89AA17DA8A8A87DA8A8 %27FF7DF8FF52A8F852A87D527D52FFFF7D52FF27277DFF7D527D7DFD0452 %5E8282825127F827F827F82751828282A8FD09FF52FD06FFC2C9FD28FF7C %AI5_ArtFlags: 0 0 0 1 0 0 1 0 0 %45FFA8FF7DF8F8FD05A8769375FD0CA827F852A8A8A8FF7D6F6EA7A8FD4E Abstract. MDT chambers. %A88382522758587C82888282828882828288828258825227278283FFA8FF A detailed understanding of %7C7C7C5883587C587C7C7C587C587C587C7C8258A8FD0AFF99CFFFFFA883 %CAA1A8FD0CFFA827FD06FFA0A1FF7DA8A8A87DA8FD047DA8FD47FFA8F8F8 %%EndComments %7D7D7D837D7D7D837D837D837D7D7DFD09FFA852FD2AFFA8A8FFFFFFA883 ��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� %82825D8282825D8282825D8251585158587C57A8FD0EFF7D8281825D8251 The Editors also warmly thank Michèle Jouhet and Isabelle Canon %7C525852585227FD0582A8FD09FF52FD06FFC2A1FD28FF7C82F8F8F852F8 PDF %52525227527DFD4DFF7DFD2552A8FD4DFFFD26527DFD4DFFFD255227A8FD %A87EA97EA87EA97EA87EA97EA87EA97EA87EA87E847EA87E847EA87E847E A detailed study is presented of the expected performance of the ATLAS detector. %F827F827F85157A7FFFF7D7DA8FD09FF7D825D8282825D825D8257525882 %577DA8A8A852525227FD0552A8FF7D8282825E8282825D82582758828282 %FFFFFFA8FFFFFFA8FD04FFA87DFD11FF52A8FD09FFA8A87DA8A8A87DA87D %A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8FF7EFFFFFFA1FD0DFFA852FD06 %7C82F827275227825D8282825E8282825E8252522D27F827517DA8A87DA8 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. The reconstruction of tracks, leptons, photons, missing energy and jets is investigated, together with the performance of b-tagging and the trigger. %%BeginData: 11229 Hex Bytes %A8FFFFFFA8FFA8FFA1FD0DFFA852FD06FF9AC9FD4BFFA8A87DA87DA87D7D %A8FD45FF7D7DFD2BFF7D7DFD45FFA87DFD2BFF52A8FD09FFA8A87DA8A8A8 %09FF9AC9FD1AFFA8A87D7D7DFFA8FFFFFFA8FD06FF7D7DFD11FF7D7D7D52 %CCFF00CCFF33CCFF66CCFF99CCFFCCCCFFFFFF0033FF0066FF0099FF00CC z�w��]��h��w&1��nGQ�wN %FFCFFFCAFFCFFFCAFFCAFFCAFFCAFFCAFFCFA2A8FFCAC9FD0EFF52FD06FF %FFA8FD05FFA8FFFFA8A8FFFFFFA8FD06FFA8A8FD07FFA8FD05FFA8FFA8FF %C2A1FD24FF7EFFFFFFA8A883A87DA883A87DA883A87DA883A87DA883A87D %66FF6666FF9966FFCC66FFFF9900009900339900669900999900CC9900FF 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). %%+ 0.43 0.28 0 0 (Global Periwinkle) endstream endobj 78 0 obj 15636 endobj 79 0 obj<>stream %27FFC3C9FD2BFF7DA8FD19FFA852527D27FD27FF9AC9FD2BFF7D7DFD1AFF %AI5_NumLayers: 1 %7D52277DFD27FFC2C3FD2BFF52A8FD1BFF5252FD28FF9AC9FD2BFF52A8FD %527DFD28FF9AC9FD1CFFA8527D7D527D527D527D527D527D527DFD1CFF7D %A2A1CAA1CAFD0EFF52FD06FFC2A1FD24FF7EFFFFFF7C822727275827825D %11FF52FD06FFC3C9FD24FF7E7E7EA85258272727582D7C5D825E8282825E A detailed understanding of %527D52277DFF277D527DA87D527D52FF2752277D527D7D7D52527D7D527D The LBNL ATLAS group consists of LBNL staff, UC Berkeley Faculty, Postdoctoral fellows and students. The reconstruction of tracks, leptons, photons, missing energy and jets is investigated, together with the performance of b-tagging and the trigger. [E��� 1x ��"���\3�&���}�@HwQ����qKG %1BFF7D7DFD28FFC2C9FD1DFFA87D7DA8A8A87DA8A8A87DA8A8FF52FD1CFF %8282825E8282825E8282825D82828257A8FD0EFF7D8282825D7C272DFD04 %7DFD45FFA87DFD2BFF7DA8FD45FF7D7DFD2BFF7D7DFD45FFA87DFD2BFF7D %585252F827277C7DFFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FD06FFA9A9FD 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. %828882828288FD068283FD0EFFA88288FD06825882588282888282A8FD09 %5227522752275227527DFD4DFFFD255227A8FD4DFF525227525252275252 %AI5_TargetResolution: 800 %522752525227525252275252522752525227525252275252522752525227 %%Creator: Adobe Illustrator(R) 11.0 %52277D527D7D7D52527D7D527DFD0AFF52FD2AFFA8A8FD04FF7C82587C58 Tuning of layered materials: Studies of CrAuTe4, PdSn4 and WTe2, Na Hyun Jo. 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). %99CC6699CC9999CCCC99CCFF99FF0099FF3399FF6699FF9999FFCC99FFFF Wire color optional. 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. stream %527D527D7D52527D7DFD08FFC2C9FD19FFA87D277D7D7D27527D522752A8 %FF835E27FD05F8828288828282888282587C7C8252272782A7FD0AFFC2CA %PDF-1.4 %���� Download citation. %5252277DA87D277D52FF527D527D5227A8FF277D277DFFA87DFF7DFF2752 luminosity of 4:6 fb 1, collected with the ATLAS detector. %0000330000660000990000CC0033000033330033660033990033CC0033FF %5D825D7CF8272727262727585D8258A8FD08FFA852FD06FF9AC9FD28FF83 %7D277D27A8527D7D52527D527D52A8A852527D5227A8522752277DFFFD04 Download PDF Abstract: ... =13$TeV by the ATLAS detector at the Large Hadron Collider. %A87E847EA87E847EA87E847EA87D7E7EA85AFFFFFFA1FD0DFFA852FD06FF %FF5252275227522752275227522752275227522752275227522752272727 %825D8282825D8282825D8282825D82828257525152F82757A8FD0EFF7D82 The measurement probes The measurement probes the QCD sector of the Standard Model at high energy, in a region where b-quark mass %%+ 0.46 0 0 0 (Global Blue) %7DA852A87D52277D7DC9CFFD0DFF52FD06FFC3C9FD4BFF7D52527D7D5227 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. The ATLAS detector weighs 7,000 tonnes, similar to the weight of the Eiffel Tower. %%DocumentProcessColors: Cyan Magenta Yellow Black %AI3_TileBox: 14.1001 14.0998 597.8001 777.7998 Read full-text. 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. %%+ 0.3255 0.4431 0.5373 0.1961 (Global Malt) Copy link Link copied. %27F87C828282888282828882828288FD0482A7FD0EFFA8828282887C5258 %A87DFFFFA8A85882588258825882588282825E8282825D58F8F85252F827 It is connected to the insulated rail detector lead, (or the detector lead from the Atlas Block Detector Board (BDB), (Item #233). %A8FD47FFA8277D527D5252527D5252527D5252527D5252527D5252527D52 %FFA852527DFD27FF9AC9FD1AFFA8FFFFFFA8FD0CFF7D7DFD1AFFFD0452FD The first measurements from proton–proton collisions recorded with the ATLAS detector at the LHC are presented. %7DFD04A87D7DA87DFFA8A87D7D527DA8A87DA87DA8A8FD0BFF99CAFFFFFF %FF3300FF3333FF3366FF3399FF33CCFF33FFFF6600FF6633FF6666FF6699 %%BoundingBox: 33 160 588 775 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� %825E825D825E825D8258585758F82757A7CACFA8FFCACFA8FFCACFA8FFCA %AI7_Thumbnail: 116 128 8 %F8518258825D8282825D8282825D82828257A8FD0EFF7D825E825D7CF87C %FFA8A87DFFA8FFA8835E27F82752F8F8FD09825858588252F8278283FD0A 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. %52FFA852FF52FFF852277D5252527DA8F8A8FF275252FF27275252277DA8 %FDFCFFFDFCFFFDFCFFFDFCFFFDFCFFFD17FFA8FFA8A8A8FFA8A8A8FFA8A8 PDF. %FFA8FFFFFFA8FD0DFF52A8FD72FF7D7DFD72FF7DA8FD1DFFA8FD54FF7D7D 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 Read full-text. The detector itself is a many-layered instrument designed to detect some of the tiniest yet most energetic particles ever created on earth. %FF52FD06FFC3C9FD28FF7C82FD06F8585D578282825E8282825D8282825D However, the accuracy and precision of the ATLAS Detector may vary depending on di erent factors, for example the energies of the particles created. 1.1 Inner Detector %%PageOrigin:0 0 x��)�ƒcZ�����-�L��u=l�Z�����P����y4r3\E�wE��.�PJ$�É��_o�;Uˁi���?�Q!&�� ~�+��/#˿[U���! %A8FFA8FFFFFFA8FFFFFFA8FFFFA8FFFFA8FD05FFA8FDFCFFFDFCFFFDFCFF %522752525227525252275252522752525227525252275252522752525227 %525227527D7DA8FFA8FF7D7DA8A87DA8A87D275252522752525227525252 %FFA8FFFFFFA8FD0FFFA8FFFFFFA8FFA8FFA8FFFFFFA8FFFFFFA8FFFFFFA8 The ATLAS detector. In these models, the lightest chargino is predicted to have a lifetime long enough to be detected in the tracking detectors of collider experiments. 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 … %FFC2CAFFFFA85E8282825D7CFD04F827825E828282A8FD09FF52FD1EFFA8 %58FD068252F8F85227F8268283FFFFFF7DFD0AFFA85EFD09822DFD0582A8 %%CreationDate: 10/29/2008 10:20 AM %3399003399333399663399993399CC3399FF33CC0033CC3333CC6633CC99 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. %%EndData %755E825E8258A8FD08FFA852FD06FF9AC9FD22FFA87DFFFFFFA88382825D %F827588282825E8282825D7C27525D58F82757A8FD0AFF99CFFFFF7D8282 Download full-text PDF. %7D527D52527D527D7D7D277DA827527DFD05527D277DA8A8527D52A87D7D %550000005500000055555555770000007700000077777777880000008800 %AI5_ArtSize: 612 792 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. H��Wko�� �A�0@�b,�z� %%HiResBoundingBox: 33.1875 160.6563 587.2725 774.1597 %F87D275227F8527D52525227277D275227F827A8FD0BFFC2CAFFFFFFFD04 %%+ 1 1 1 1 ([Registration]) %7DFD2552A8FD4DFFFD052752272727522727275227272752272727522727 Transition radiation detector gives particle ID. It is 44 m long and 25 m in diameter. It was installed in its underground cavern at the LHC during the period 2004 to 2008. 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. For example, Atlas currently uses extensive RD-180 engine health checks that occur prior to liftoff. %FD05FF52A8FD11FFFD077DA87D7D7DFD15FFA8FFA8FFFFFFA8FFFFFFA8FD %%+ 0 1 1 0 (Global Red) %7DA8527DA8527D272752FF27FFA82727A85252A87D27527D52277D7DA87D %%+ 0.5 0.9 0 0 (Global Plum) 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- %00FF0000FFFFFF0000FF00FFFFFF00FFFFFF endstream endobj 77 0 obj<>stream ��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������ %8282825DFD0B825D82827C828283FD0AFFC3BBC2BCBC9999999F9876F827 It forms part of the ATLAS collaboration operating at the Large Hadron Collider (LHC) at CERN.. QUICK LINKS: %AI5_FileFormat 7.0 A detailed study is presented of the expected performance of the ATLAS detector. The effect of in-time as well as out-of-time pile-up is simulated using minimum-bias events %6666006666336666666666996666CC6666FF669900669933669966669999 %A8A8FFFFA8FFFFA8FFA8FFA8FFA8FFFFFFA8FFFFA8A8FD07FFA8FFA8FFA8 %FD0AFFA8FFFFFFA8FFFFFFA8FD07FFA8FFA87DA8FFFFFFA8FFFFFFA8FFFF •Will assume some Unfamiliarity with the baseline ATLAS detector and will review the Inner tracker systems. %C9C3C9C3C9C9BCC9FD22FFA8A8FD04FF7C82587C5858577C82825E828282 %AI3_TemplateBox: 306.5 395.5 306.5 395.5 %%+ 0.8 0 1 0 (Global Green) %27759F759F75A0A0C3A0C2A0C3A0C39A76A0C2A0C3A0C2A0FD24FFA8FD04 %825D8252FD04F8275E82828258A8FD08FFA852FD1FFFFD0452277D7D7DFF %525227FD0D527DFD4DFFFD16527DFD0E5227A8FD4DFF5252275252522752 ATLAS at LBNL The ATLAS Detector. %52FF527DA87D2752A87D527D527D275252A8527D277D5252277DFF272727 %FD4DFF7DFD245227A8FD4DFFFD26527DFD4DFF7DFD245227A8FD4DFFFD04 Copy link Link copied. 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. Intermediate system is a large silicon strip tracker •Four barrel layers and 9 disk layers contain 61 m2 of silicon with 6.2M channels. * c. DIN- DIN is the Detector Input. 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 Transition radiation detector gives particle ID. 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 %AI5_RulerUnits: 0 %FD06FF7D7DFD11FF7D277D7D7DF8527D52277DFFA8FD10FFA87D27527D7D %51512D825782828257A8FD08FFA852FD06FF9AC9FD27FFA883822DF827F8 %7D7DFD0AFFA8FFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFF %000088888888AA000000AA000000AAAAAAAABB000000BB000000BBBBBBBB %277D7D7D277D52A87DA8525252A8FFFFFFA8FFFFFFA8FFFFFFA8FD05FFA8 %AI9_ColorModel: 2 ATLAS has the dimensions of a cylinder, 46m long, 25m in diameter, and sits in a cavern 100m below ground. L1DDC's function is to concentrate the data from multiple front-end boards and transmit 7μu&��.�e-U��VTu�S}m��3��R�v2e� ������]�O����&��V�X��dɌ#��n�7�p�����A"���}����.�ӿwZ �I#����._|$#? %27F87C5D8258A8FD08FFA852FD06FF9AC9FD28FF835DFD178283FD0EFFA8 The ATLAS detector is a general-purpose particle detector ... and the CTEQ6L1 PDF set. The tracking modules and the trigger system are of most relevance for the presented measurements. %AI5_OpenViewLayers: 7 The ATLAS detector site www.atlas.ch provides a comprehensive presentation of the detector and its physics. The entire detector weighs 7000 metric tons. In addition to measurements of Stan-dard Model processes such as vector-boson and top-quark production, the properties of the newly %27522727275227272752FD04277DFD08FFFF %AI7_ImageSettings: 0 %57825882585E57827B82578257A8FD08FFA852FD06FF9AC9FD27FFA88382 PDF. %%+ 0 0.5 1 0 (Global Orange) Search for the Lepton Flavor Violating decay Z → eμ with the ATLAS detector at the LHC, Hai Jiang. She was elected and served as ATLAS Run-Coordinator in 2012–2014. %FFA852FD06FF9AC9FD54FFA8A8FD06FFC9CFFD0DFF52FD06FFC2C9FD54FF %522752275227522752275227FD0D527DFD4DFF7DFD245227A8FD4DFFFD04 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 1.1 Inner Detector %AI9_OpenToView: 72.5 533.5 2 1002 640 26 1 0 11 83 1 1 1 1 1 0 1 %8282825E8282825E8282825E82828258525852272751A8FD0EFF7D585782 %52FD2FFFC2C9FD19FFA87DFD0452A8FD0BFF52A8FD11FF7DA87D7D7DFD04 The ATLAS Detector is a particle physics experiment that explores the frontiers of the Standard Model (SM) of Physics. %CC0000CC0033CC0066CC0099CC00CCCC00FFCC3300CC3333CC3366CC3399 In addition to measurements of Stan-dard Model processes such as vector-boson and top-quark production, the properties of the newly Data were collected in December 2009 using a minimum-bi %A87DA8A8A87DA87DA87DA852A87DA8A8A87DA8A8A87DA8A8A87DA8A87D52 This analysis was not unusual for Atlas, as the building blocks of an EDS system for Atlas are flying today. %8258FD12827C5282A7FD0FFF83A87DA87D7D837E7DA87DA183A87DA8CFFD %A1A1CAA1CAA1CAA1CAA1CAA1C9A1CAA1CAA1CAA1CAA1CA77A1A1C9A8FD0D 12 m 10 8 6 4. %%+ 0 0 1 0 (Global Yellow) %FFA8FD07FFC9FD0EFF52FD06FFC2A1FD54FF7DFD07FFA1FD0DFFA852FD06 %A8FD047DA8A87DA8FD057DA87DFD09FFA852FD2AFFA87DFD05FFA8272752 This analysis was not unusual for Atlas, as the building blocks of an EDS system for Atlas are flying today. %A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8527DFD04A87D %FFA852FD06FF9AC9FD27FFA8835E27F852587C7C82828882828288828282 ATLAS Toroidal Muon Spectrometer. %F82027FD0582A8FD09FF52FD06FFC2A1FD22FFA8A8FD04FF588282825D82 %A883828258FD13827C8283FD12FFA8FFFFFFA9A9FFFFC9FD0EFF52FD06FF %9933009933339933669933999933CC9933FF996600996633996666996699 %27527DA87DA87D7D7DA8A1FD0DFFA87DFD06FF9ACAFD53FFA87D7DFD05FF %!PS-Adobe-3.0 There are Pogo detection and correction algorithms and … %6699CC6699FF66CC0066CC3366CC6666CC9966CCCC66CCFF66FF0066FF33 %33CCCC33CCFF33FF0033FF3333FF6633FF9933FFCC33FFFF660000660033 %FD28FFC3C9FD1DFF52FD2AFF527DFD28FF99CAFD1CFFA852FD2AFF7D7DFD For example, Atlas currently uses extensive RD-180 engine health checks that occur prior to liftoff. %0066000066330066660066990066CC0066FF009900009933009966009999 <> %AI3_DocumentPreview: None •Will describe the Novel Next Gen tracking sensors at the end.. Growth, characterization and study of critical rare-earth poor/free magnetic materials, Tej Nath Lamichhane. •Will not defend the upgrade based on expected Physics. %%HiResBoundingBox: 33.1875 160.6563 587.2725 774.1597 %9966CC9966FF9999009999339999669999999999CC9999FF99CC0099CC33 %000011111111220000002200000022222222440000004400000044444444 %FFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8 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. %%+ 0.33 0 0.73 0 (Global Lime) 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. %A8FFA8A8A8FFA8A8A8FFA8A8A8FFA8A8A8FFA8A8A8FFA8A8A8FFA8A8A8FF %5226515127277CA1CAA7CAC9CAA7CAC9CAA7CAC9CAA7CAC9CAA7A7A1CAC9 %FD09FF52FD06FFC2C9FD28FF7C8257825D8257825D8257825E825D825D7C %06FF9AC9FD27FFA8838227F8277D27F8525858FD0E82A7FD0EFFA8FD0482 %CFA8FFCAFF7DCACAFF7DA8CACFA0FD0DFFA852FD06FF9AC9FD24FFA9FFFF Thin gap chambers Cathode strip chambers Resistive plate chambers. :���v[b. %7DA87DFFFFA882828288FD068251FD0582A8FD09FF52FD06FFC2A1FD22FF %522752272727F8A8A8A827527D52A8A8F8527DA8A87D2727FF27522752F8 %9AC9FD25FFA8FFA8A9A8FFA8A9A8FFA8A9A8FFA8A9A8FFA8A9A8FFA9FFA9 Download full-text PDF Read full-text. %A883A87DFD13FF7DFFFFFF7EFFFFFFA1FD0DFFA852FD06FF9AC9FD24FFA8 %828282888282828882828288FD048258FD06F882A7FFFFFF7DA87DA87DA8 2 0 0 Radiation shield. %FD2FFFA8A8FFFFA9A8FFFFC9CFFD0DFF52FD06FFC2C9FD24FF7E847EA97E %F8F827F8275D82828257A8FD08FFA852FD06FF9AC9FD22FFA8A8FD04FF83 %28FFC2CAFD1DFF52FD2AFF2752A8FD27FF99CAFD1CFFA852FD24FFA87DA8 %0099CC0099FF00CC0000CC3300CC6600CC9900CCCC00CCFF00FF3300FF66 For all samples, the EvtGen v1.2.0 program [19] is used for properties of the bottom and charm hadron decays. %7D52FD057DFFFF7D527D52527D7D2752277D7D7D52A8FF52527D52A852A8 These were followed by similar testbeam campaigns for “module-0” prototypes of the final design, and then for the series production modules. %%+ 0 0.25 0 0 (Global Pink) %A8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DFD04A8FD0AFF %CFFD0DFF52FD06FFC3C9FD54FFA8FD07FFA1FD0DFFA852FD06FF9AC9FD54 '��� ������: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�?�). 5 0 obj %5DFD1582588283FD0AFFC2CAFFFFA858825E828258F827F8F8278282825E —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. 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