%FD4DFF7DFD245227A8FD4DFFFD26527DFD4DFF7DFD245227A8FD4DFFFD04 %8258FD12827C5282A7FD0FFF83A87DA87D7D837E7DA87DA183A87DA8CFFD %525227525252275252527DFD4DFF7DFD245227A8FD4DFFFD26527DFD4DFF There are Pogo detection and correction algorithms and … %%EndData It was installed in its underground cavern at the LHC during the period 2004 to 2008. %5227522752275227527DFD4DFFFD255227A8FD4DFF525227525252275252 %52277C587CFD0482A8FD09FF52FD06FFC2A1FD28FF7C8282825E8282825E %755E825E8258A8FD08FFA852FD06FF9AC9FD22FFA87DFFFFFFA88382825D %%+ 0.3255 0.4431 0.5373 0.1961 (Global Malt) %550000005500000055555555770000007700000077777777880000008800 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- %000088888888AA000000AA000000AAAAAAAABB000000BB000000BBBBBBBB Tuning of layered materials: Studies of CrAuTe4, PdSn4 and WTe2, Na Hyun Jo. %%PageOrigin:0 0 Transition radiation detector gives particle ID. 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. %7DFD04A87D7DA87DFFA8A87D7D527DA8A87DA87DA8A8FD0BFF99CAFFFFFF %3333663333993333CC3333FF3366003366333366663366993366CC3366FF %7DA87D514B7DFD27FFC2CAFD1DFF52FD24FF52525227277D27517DFD05FF Intermediate system is a large silicon strip tracker •Four barrel layers and 9 disk layers contain 61 m2 of silicon with 6.2M channels. %AI5_NumLayers: 1 Growth, characterization and study of critical rare-earth poor/free magnetic materials, Tej Nath Lamichhane. %7D7DFD0AFFA8FFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFF %A8FD47FFA8277D527D5252527D5252527D5252527D5252527D5252527D52 %FFA852FD06FF9AC9FD54FFA8A8FD06FFC9CFFD0DFF52FD06FFC2C9FD54FF %CCFF00CCFF33CCFF66CCFF99CCFFCCCCFFFFFF0033FF0066FF0099FF00CC %!PS-Adobe-3.0 Transition radiation detector gives particle ID. %82A8FD09FF52FD20FFA8FFFFFFA8FFA8FFFFFFA8A8FD04FF7C8227F8F827 %A883828258FD13827C8283FD12FFA8FFFFFFA9A9FFFFC9FD0EFF52FD06FF %7DA8527DA8527D272752FF27FFA82727A85252A87D27527D52277D7DA87D [E��� 1x ��"���\3�&���}�@HwQ����qKG It is 44 m long and 25 m in diameter. %%DocumentProcessColors: Cyan Magenta Yellow Black :���v[b. In addition to measurements of Stan-dard Model processes such as vector-boson and top-quark production, the properties of the newly %%BoundingBox: 33 160 588 775 The ATLAS detector site www.atlas.ch provides a comprehensive presentation of the detector and its physics. %4DFF52522752525227525252275252522752525227525252275252522752 %FFC2CAFFFFA85E8282825D7CFD04F827825E828282A8FD09FF52FD1EFFA8 %FFA8FFFFFFA8FD0DFF52A8FD72FF7D7DFD72FF7DA8FD1DFFA8FD54FF7D7D %%For: (Steve Horvath) (Atlas) %52FF527DA87D2752A87D527D527D275252A8527D277D5252277DFF272727 —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. %A87DA8A8A87DA8A8A87DA8A8A87DA8A8A8527D5252527D7D2752A87DA87D %522752272727F8A8A8A827527D52A8A8F8527DA8A87D2727FF27522752F8 %A883A87DFD13FF7DFFFFFF7EFFFFFFA1FD0DFFA852FD06FF9AC9FD24FFA8 K�F��u�Mz)�c�~�R�`�HhjP����D� ��t��L|��k$1я��Z�hzt����Ĉ �"��GBK���3=�V?�G�JK9���Yx5v�&�8 Search for the Lepton Flavor Violating decay Z → eμ with the ATLAS detector at the LHC, Hai Jiang. %A87DA8A8A87DA87DA87DA852A87DA8A8A87DA8A8A87DA8A8A87DA8A87D52 %DD000000DD000000DDDDDDDDEE000000EE000000EEEEEEEE0000000000FF %0000330000660000990000CC0033000033330033660033990033CC0033FF %%AI8_CreatorVersion: 11.0.0 ��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�( ao�_���hO4����c>����,�൛��hCb�R�`��K���ӡ�V�#]�=iM��Iځ4����(-C�3Ģ{T��T�*��_%�"2!I�9RE�Nl��e3 ��l� %CC9966CC9999CC99CCCC99FFCCCC00CCCC33CCCC66CCCC99CCCCCCCCCCFF %09FF9AC9FD1AFFA8A87D7D7DFFA8FFFFFFA8FD06FF7D7DFD11FF7D7D7D52 %FFFFA85E88828282A04B754B756F9F7BA07BA0A0C9C3C9C3C9C3C9C3C976 %AI3_ColorUsage: Color This analysis was not unusual for Atlas, as the building blocks of an EDS system for Atlas are flying today. %527D52277DFF277D527DA87D527D52FF2752277D527D7D7D52527D7D527D •Will describe the Novel Next Gen tracking sensors at the end.. 2 0 0 Radiation shield. %FFCC66FFCC99FFCCCCFFCCFFFFFF33FFFF66FFFF99FFFFCC110000001100 %5D8258A8FD08FFA852FD06FF9AC9FD28FF835E82588258825882827C8282 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. ATLAS at LBNL The ATLAS Detector. %27FFC3C9FD2BFF7DA8FD19FFA852527D27FD27FF9AC9FD2BFF7D7DFD1AFF %FD06FF7D7DFD11FF7D277D7D7DF8527D52277DFFA8FD10FFA87D27527D7D The reconstruction of tracks, leptons, photons, missing energy and jets is investigated, together with the performance of b-tagging and the trigger. %FFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8 %AI3_DocumentPreview: None %5E8282825127F827F827F82751828282A8FD09FF52FD06FFC2C9FD28FF7C %57825882585E57827B82578257A8FD08FFA852FD06FF9AC9FD27FFA88382 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. 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 %522752525227525252275252522752525227525252275252522752525227 The physics %58A8FD08FFA852FD06FF9AC9FD23FF7DA87DA87D58587C587C587C587C58 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. %825E825D825E825D8258585758F82757A7CACFA8FFCACFA8FFCACFA8FFCA %CC33CCCC33FFCC6600CC6633CC6666CC6699CC66CCCC66FFCC9900CC9933 A detailed understanding of %FF835E27FD05F8828288828282888282587C7C8252272782A7FD0AFFC2CA b. DOUT- DOUT is the optional Detector Output. Abstract. %AI3_TemplateBox: 306.5 395.5 306.5 395.5 %825D8252FD04F8275E82828258A8FD08FFA852FD1FFFFD0452277D7D7DFF %9966CC9966FF9999009999339999669999999999CC9999FF99CC0099CC33 %F8518258825D8282825D8282825D82828257A8FD0EFF7D825E825D7CF87C The ATLAS detector weighs 7,000 tonnes, similar to the weight of the Eiffel Tower. %7DA87DFFFFA882828288FD068251FD0582A8FD09FF52FD06FFC2A1FD22FF %8282825DFD0B825D82827C828283FD0AFFC3BBC2BCBC9999999F9876F827 %A87DFFFFA8A85882588258825882588282825E8282825D58F8F85252F827 %FFA852527DFD27FF9AC9FD1AFFA8FFFFFFA8FD0CFF7D7DFD1AFFFD0452FD %AI5_ArtSize: 612 792 %000011111111220000002200000022222222440000004400000044444444 x��)�ƒcZ�����-�L��u=l�Z�����P����y4r3\E�wE��.�PJ$�É��_o�;Uˁi���?�Q!&�� ~�+��/#˿[U���! %FD2FFFA8A8FFFFA9A8FFFFC9CFFD0DFF52FD06FFC2C9FD24FF7E847EA97E %522752275227522752275227FD0D527DFD4DFF7DFD245227A8FD4DFFFD04 %8288828282888282828882828288FD04822D7C52525182A7FD0EFFA88288 %6666006666336666666666996666CC6666FF669900669933669966669999 It is used to connect an auxiliary piece of equipment, (no more than +5VDC), such as an LED or relay. %FF9AC9FD54FFA8FD07FFC9FD0EFF52FD06FFC2A1FD54FF7DFD07FFA1FD0D %F87D275227F8527D52525227277D275227F827A8FD0BFFC2CAFFFFFFFD04 %AI5_OpenViewLayers: 7 %CFA8FFCAFF7DCACAFF7DA8CACFA0FD0DFFA852FD06FF9AC9FD24FFA9FFFF %FD05FFA16876FD0CFF27F852FD05FF6E6FA17D522727525252272727A8FD %A8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DFD04A8FD0AFF %FD28FFC3C9FD1DFF52FD2AFF527DFD28FF99CAFD1CFFA852FD2AFF7D7DFD %52527D5252527D5252527D5252527D5252527D27A8FD45FF7D7DFD2BFF7D Track storm activity by adding the lightning detector to your AcuRite Atlas Weather Sensor. %577DA8A8A852525227FD0552A8FF7D8282825E8282825D82582758828282 A detailed study is presented of the expected performance of the ATLAS detector. In addition to measurements of Stan-dard Model processes such as vector-boson and top-quark production, the properties of the newly %52FFA852FF52FFF852277D5252527DA8F8A8FF275252FF27275252277DA8 '��� ������:o��� TUߙ�Jtw��c~�z��du��Z�bʤV����G� }�����a��U#��:���=�Ȫ)�e}3�F�?4eq�9��7����?��Ra�]'�a�D]$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�������|����$7�ȥ��!������B�ɯ�V��*g)��FB;j�PYs5֤fj0�����ی޺�6SVO?���3�8��ˋ���^���S~v�{���F�ύ�NL�g(��ޙQ�;{�g((?4�?,�Wuyqe��p?����&���X�~,�F�"/��;$LO��m�ow�Z�j�?�). 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. %FF9AC9FD28FF838227F8525882587CFD09827C517C5127F87CA7FFCFFFCA 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. The detector itself is a many-layered instrument designed to detect some of the tiniest yet most energetic particles ever created on earth. %FD09FF52FD06FFC2C9FD28FF7C8257825D8257825D8257825E825D825D7C %%BeginData: 11229 Hex Bytes %7D7D7D837D7D7D837D837D837D7D7DFD09FFA852FD2AFFA8A8FFFFFFA883 Data were collected in December 2009 using a minimum-bi ATLAS Upgrade 3 This Talk •Will be somewhat reductionist in starting with Silicon and emerging with an ATLAS Upgrade. %5DFD1582588283FD0AFFC2CAFFFFA858825E828258F827F8F8278282825E %28FFC2CAFD1DFF52FD2AFF2752A8FD27FF99CAFD1CFFA852FD24FFA87DA8 Copy link Link copied. 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��0trs*�NH5�_���k尿;=Ȫ�1�_��U+����Ejp~zh��o����_���z�C[I�i�e�nVc��ߟj���m�N *��A��?�z�_�#}K�KCݦ�W�����?7�����LǪ:=��PM�Ø�5IL蝧���b���0j�f|2� The physics The ATLAS Detector is a particle physics experiment that explores the frontiers of the Standard Model (SM) of Physics. The first measurements from proton–proton collisions recorded with the ATLAS detector at the LHC are presented. %AI5_TargetResolution: 800 %FFA852FD06FF9AC9FD27FFA8835E27F852587C7C82828882828288828282 %0066000066330066660066990066CC0066FF009900009933009966009999 %A87E847EA87E847EA87E847EA87D7E7EA85AFFFFFFA1FD0DFFA852FD06FF %FFFFFFA8FFFFFFA8FD04FFA87DFD11FF52A8FD09FFA8A87DA8A8A87DA87D %AI5_ArtFlags: 0 0 0 1 0 0 1 0 0 %7DFD4DFF7DFD0B527D527D7DA8FD047D527D7D7DFD0C5227A8FD4DFFFD0E %%+ 1 0.5 0 0 (Global Night) %3399003399333399663399993399CC3399FF33CC0033CC3333CC6633CC99 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 %52527D7D7D2752527D527D52A8A8A87DA8A8A87DA89AA17DA8A8A87DA8A8 Download citation. the detector and collide in ATLAS, which creates new particles that are detected. %AI7_Thumbnail: 116 128 8 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 … 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. %82825D8282825D8282825D8251585158587C57A8FD0EFF7D8281825D8251 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 Particles ever created on earth of layered materials: Studies of CrAuTe4, PdSn4 and WTe2, Na Hyun.. 46M long, 25m in diameter, and then for the presented measurements presented measurements was! 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