Download citation. luminosity of 4:6 fb 1, collected with the ATLAS detector. %%For: (Steve Horvath) (Atlas) Data were collected in December 2009 using a minimum-bi %0000330000660000990000CC0033000033330033660033990033CC0033FF 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 %27FF7DF8FF52A8F852A87D527D52FFFF7D52FF27277DFF7D527D7DFD0452 ATLAS at LBNL The ATLAS Detector. %7DA87D514B7DFD27FFC2CAFD1DFF52FD24FF52525227277D27517DFD05FF %AI5_ArtSize: 612 792 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 1.1 Inner Detector For example, Atlas currently uses extensive RD-180 engine health checks that occur prior to liftoff. 1.1 Inner Detector 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. <> %FD05FFA16876FD0CFF27F852FD05FF6E6FA17D522727525252272727A8FD It is 44 m long and 25 m in diameter. PDF. %8288828282888282828882828288FD04822D7C52525182A7FD0EFFA88288 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. %5252277DA87D277D52FF527D527D5227A8FF277D277DFFA87DFF7DFF2752 %6699CC6699FF66CC0066CC3366CC6666CC9966CCCC66CCFF66FF0066FF33 %C9C3C9C3C9C9BCC9FD22FFA8A8FD04FF7C82587C5858577C82825E828282 %CCFF00CCFF33CCFF66CCFF99CCFFCCCCFFFFFF0033FF0066FF0099FF00CC 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 … %A87DFFFFA8A85882588258825882588282825E8282825D58F8F85252F827 The reconstruction of tracks, leptons, photons, missing energy and jets is investigated, together with the performance of b-tagging and the trigger. %00FF9900FFCC3300003300333300663300993300CC3300FF333300333333 A detailed study is presented of the expected performance of the ATLAS detector. %%BoundingBox: 33 160 588 775 %58A8FD08FFA852FD06FF9AC9FD23FF7DA87DA87D58587C587C587C587C58 %09FF9AC9FD1AFFA8A87D7D7DFFA8FFFFFFA8FD06FF7D7DFD11FF7D7D7D52 The Editors also warmly thank Michèle Jouhet and Isabelle Canon %524C457D527D2752525227A8527D7DFF527D2727A8FF52A852FF7D7D527D %7DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8 ��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$X��|_��c;�s�'N Z�����x`��%1�xC��o�Q���(�m�~�q�J���|��76�h� az`M�� \�"��R��������m��J5퍓�ڹͷ�ɝO���W'��͗�O��lo�M���>���;)Y|߈/�第$tq�w5=�K����Bf(B6r��܃�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������ %%EndData 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��! The measurement probes The measurement probes the QCD sector of the Standard Model at high energy, in a region where b-quark mass %522752275227522752275227FD0D527DFD4DFF7DFD245227A8FD4DFFFD04 %FF66CCFF66FFFF9900FF9933FF9966FF9999FF99CCFF99FFFFCC00FFCC33 %%BeginData: 11229 Hex Bytes The detector itself is a many-layered instrument designed to detect some of the tiniest yet most energetic particles ever created on earth. %FFFFFFA8FFFFFFA8FD04FFA87DFD11FF52A8FD09FFA8A87DA8A8A87DA87D %5DFD1582588283FD0AFFC2CAFFFFA858825E828258F827F8F8278282825E The effect of in-time as well as out-of-time pile-up is simulated using minimum-bias events 12 m 10 8 6 4. 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 physics In addition to measurements of Stan-dard Model processes such as vector-boson and top-quark production, the properties of the newly Copy link Link copied. %FDFCFFFDFCFFFDFCFFFDFCFFFDFCFFFD17FFA8FFA8A8A8FFA8A8A8FFA8A8 %A8A8FFFFA8FFFFA8FFA8FFA8FFA8FFFFFFA8FFFFA8A8FD07FFA8FFA8FFA8 %CAA1A8FD0CFFA827FD06FFA0A1FF7DA8A8A87DA8FD047DA8FD47FFA8F8F8 %A87DA8A8A87DA87DA87DA852A87DA8A8A87DA8A8A87DA8A8A87DA8A87D52 Download full-text PDF Read full-text. %FD09FF52FD06FFC2C9FD28FF7C8257825D8257825D8257825E825D825D7C The ATLAS detector. %FFC2CAFFFFA85E8282825D7CFD04F827825E828282A8FD09FF52FD1EFFA8 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. This analysis was not unusual for Atlas, as the building blocks of an EDS system for Atlas are flying today. Download full-text PDF. %7DA87DFFFFA882828288FD068251FD0582A8FD09FF52FD06FFC2A1FD22FF •Will not defend the upgrade based on expected Physics. %FFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8 For example, Atlas currently uses extensive RD-180 engine health checks that occur prior to liftoff. Download citation. %A2A1CAA1CAFD0EFF52FD06FFC2A1FD24FF7EFFFFFF7C822727275827825D %828882828288FD068283FD0EFFA88288FD06825882588282888282A8FD09 * c. DIN- DIN is the Detector Input. %9966CC9966FF9999009999339999669999999999CC9999FF99CC0099CC33 Download PDF Abstract: ... =13$ TeV by the ATLAS detector at the Large Hadron Collider. %7D52277DFD27FFC2C3FD2BFF52A8FD1BFF5252FD28FF9AC9FD2BFF52A8FD %5226515127277CA1CAA7CAC9CAA7CAC9CAA7CAC9CAA7CAC9CAA7A7A1CAC9 %AI5_FileFormat 7.0 Track storm activity by adding the lightning detector to your AcuRite Atlas Weather Sensor. %277D7D7D277D52A87DA8525252A8FFFFFFA8FFFFFFA8FFFFFFA8FD05FFA8 %A8FD047DA8A87DA8FD057DA87DFD09FFA852FD2AFFA87DFD05FFA8272752 %CC33CCCC33FFCC6600CC6633CC6666CC6699CC66CCCC66FFCC9900CC9933 %7D7D7D837D7D7D837D837D837D7D7DFD09FFA852FD2AFFA8A8FFFFFFA883 '��� ������: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�?�). x��)�ƒcZ�����-�L��u=l�Z�����P����y4r3\E�wE��.�PJ$�É��_o�;Uˁi���?�Q!&�� ~�+��/#˿[U���! %�쏢 %A1A1CAA1CAA1CAA1CAA1CAA1C9A1CAA1CAA1CAA1CAA1CA77A1A1C9A8FD0D 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. %AI5_OpenViewLayers: 7 PDF. %7DFD4DFF7DFD0B527D527D7DA8FD047D527D7D7DFD0C5227A8FD4DFFFD0E %7D527D52527D527D7D7D277DA827527DFD05527D277DA8A8527D52A87D7D •Will assume some Unfamiliarity with the baseline ATLAS detector and will review the Inner tracker systems. 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. However, the accuracy and precision of the ATLAS Detector may vary depending on di erent factors, for example the energies of the particles created. %3399003399333399663399993399CC3399FF33CC0033CC3333CC6633CC99 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. %522752525227525252275252522752525227525252275252522752525227 End-cap toroid Barrel toroid coil. %825E825D825E825D8258585758F82757A7CACFA8FFCACFA8FFCACFA8FFCA %FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFF %527D527D7D52527D7DFD08FFC2C9FD19FFA87D277D7D7D27527D522752A8 %A8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DFD04A8FD0AFF %FFA852FD06FF9AC9FD54FFA8A8FD06FFC9CFFD0DFF52FD06FFC2C9FD54FF %FFA8A87DFFA8FFA8835E27F82752F8F8FD09825858588252F8278283FD0A %%+ 0.43 0.28 0 0 (Global Periwinkle) %%CMYKProcessColor: 0 0 0 1 (Global Black) %27FFC3C9FD2BFF7DA8FD19FFA852527D27FD27FF9AC9FD2BFF7D7DFD1AFF %522752272727F8A8A8A827527D52A8A8F8527DA8A87D2727FF27522752F8 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. Transition radiation detector gives particle ID. 2 0 0 Radiation shield. %%HiResBoundingBox: 33.1875 160.6563 587.2725 774.1597 %27F87C5D8258A8FD08FFA852FD06FF9AC9FD28FF835DFD178283FD0EFFA8 %82825D8282825D8282825D8251585158587C57A8FD0EFF7D8281825D8251 %828282577C5851F827517DFD04A87DA8A8A87DA8A8A87DA8A8A87DA87DFF %7C82F827275227825D8282825E8282825E8252522D27F827517DA8A87DA8 %A87DA87D7DA8A87DFFA8A87D7DA8A87DA8527CF8F8F827F8F858825D8282 %825D8252FD04F8275E82828258A8FD08FFA852FD1FFFFD0452277D7D7DFF %%+ 0.33 0 0.73 0 (Global Lime) %6666006666336666666666996666CC6666FF669900669933669966669999 %A8FD45FF7D7DFD2BFF7D7DFD45FFA87DFD2BFF52A8FD09FFA8A87DA8A8A8 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. 7μu&��.�e-U��VTu�S}m��3��R�v2e� �����`�]�O����&��V�X��dɌ#��n�7�p�����A"���}����.�ӿwZ �I#����._|$#? %PDF-1.4 %���� The ATLAS Detector is a particle physics experiment that explores the frontiers of the Standard Model (SM) of Physics. %%+ 0.5 0.9 0 0 (Global Plum) %FF52FD06FFC3C9FD28FF7C82FD06F8585D578282825E8282825D8282825D 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� Read full-text. %%+ 0 1 1 0 (Global Red) Thin gap chambers Cathode strip chambers Resistive plate chambers. %585252F827277C7DFFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FD06FFA9A9FD %06FF9AC9FD27FFA8838227F8277D27F8525858FD0E82A7FD0EFFA8FD0482 %FFCC66FFCC99FFCCCCFFCCFFFFFF33FFFF66FFFF99FFFFCC110000001100 Read full-text. H��Wko�� �A�0@�b,�z� This analysis was not unusual for Atlas, as the building blocks of an EDS system for Atlas are flying today. %%+ 0 0.25 0 0 (Global Pink) %7D277D27A8527D7D52527D527D52A8A852527D5227A8522752277DFFFD04 The entire detector weighs 7000 metric tons. %550000005500000055555555770000007700000077777777880000008800 It was installed in its underground cavern at the LHC during the period 2004 to 2008. %52FFA852FF52FFF852277D5252527DA8F8A8FF275252FF27275252277DA8 %%Creator: Adobe Illustrator(R) 11.0 %825D8282825D8282825D8282825D82828257525152F82757A8FD0EFF7D82 %52275252522752525227525252275252522752525227525252275252527D These were followed by similar testbeam campaigns for “module-0” prototypes of the final design, and then for the series production modules. For all samples, the EvtGen v1.2.0 program [19] is used for properties of the bottom and charm hadron decays. %52525227527DFD4DFF7DFD2552A8FD4DFFFD26527DFD4DFFFD255227A8FD %0099CC0099FF00CC0000CC3300CC6600CC9900CCCC00CCFF00FF3300FF66 %A883828258FD13827C8283FD12FFA8FFFFFFA9A9FFFFC9FD0EFF52FD06FF %7DFD04A87D7DA87DFFA8A87D7D527DA8A87DA87DA8A8FD0BFF99CAFFFFFF 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). 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 %FF9AC9FD54FFA8FD07FFC9FD0EFF52FD06FFC2A1FD54FF7DFD07FFA1FD0D %09FF52FD06FFC2A1FD28FF5882582D57825D825D8282825D8282825D825D 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 %4DFF52522752525227525252275252522752525227525252275252522752 The ATLAS detector is a general-purpose particle detector ... and the CTEQ6L1 PDF set. ATLAS Upgrade 3 This Talk •Will be somewhat reductionist in starting with Silicon and emerging with an ATLAS Upgrade. %99CC6699CC9999CCCC99CCFF99FF0099FF3399FF6699FF9999FFCC99FFFF %FFA8FD05FFA8FFFFA8A8FFFFFFA8FD06FFA8A8FD07FFA8FD05FFA8FFA8FF %FF835E27FD05F8828288828282888282587C7C8252272782A7FD0AFFC2CA Intermediate system is a large silicon strip tracker •Four barrel layers and 9 disk layers contain 61 m2 of silicon with 6.2M channels. %828282888282828882828288FD048258FD06F882A7FFFFFF7DA87DA87DA8 %27F87C828282888282828882828288FD0482A7FD0EFFA8828282887C5258 %AI9_OpenToView: 72.5 533.5 2 1002 640 26 1 0 11 83 1 1 1 1 1 0 1 %FD2FFFA8A8FFFFA9A8FFFFC9CFFD0DFF52FD06FFC2C9FD24FF7E847EA97E %%+ 0 0.5 1 0 (Global Orange) 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���/$�l�U/,�&Hl7%�P3:�m��wR��Z1��k3-�h��E��9��ݱ��T~sڈ��2ʏ��B2v��-mɶ%�z��[�6�m�{Ѿ�pIC�Ep�Ben 1����' ȒYh���5$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� %7DFD45FFA87DFD2BFF7DA8FD45FF7D7DFD2BFF7D7DFD45FFA87DFD2BFF7D %8282825E8282825E8282825E82828258525852272751A8FD0EFF7D585782 %52527D7D7D2752527D527D52A8A8A87DA8A8A87DA89AA17DA8A8A87DA8A8 %%+ 0.46 0 0 0 (Global Blue) %FD28FFC3C9FD1DFF52FD2AFF527DFD28FF99CAFD1CFFA852FD2AFF7D7DFD She was elected and served as ATLAS Run-Coordinator in 2012–2014. %%+ 1 0.5 0 0 (Global Night) %A8FFFFFFA8FFA8FFA1FD0DFFA852FD06FF9AC9FD4BFFA8A87DA87DA87D7D %FFA8FD07FFC9FD0EFF52FD06FFC2A1FD54FF7DFD07FFA1FD0DFFA852FD06 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. %A883A87DFD13FF7DFFFFFF7EFFFFFFA1FD0DFFA852FD06FF9AC9FD24FFA8 •Will describe the Novel Next Gen tracking sensors at the end.. %%BoundingBox: 33 160 588 775 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 √ %9933009933339933669933999933CC9933FF996600996633996666996699 %577DA8A8A852525227FD0552A8FF7D8282825E8282825D82582758828282 %%HiResBoundingBox: 33.1875 160.6563 587.2725 774.1597 %52277D527D7D7D52527D7D527DFD0AFF52FD2AFFA8A8FD04FF7C82587C58 %3333663333993333CC3333FF3366003366333366663366993366CC3366FF %%+ 0 0 1 0 (Global Yellow) %28FFC2CAFD1DFF52FD2AFF2752A8FD27FF99CAFD1CFFA852FD24FFA87DA8 %825D825D5827525158F82757A7FD0AFF99CAFFFF7D825D82828251FD04F8 %7DA852A87D52277D7DC9CFFD0DFF52FD06FFC3C9FD4BFF7D52527D7D5227 In addition to measurements of Stan-dard Model processes such as vector-boson and top-quark production, the properties of the newly %%PageOrigin:0 0 A detailed understanding of 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. Growth, characterization and study of critical rare-earth poor/free magnetic materials, Tej Nath Lamichhane. %AI3_TileBox: 14.1001 14.0998 597.8001 777.7998 %52527D5252527D5252527D5252527D5252527D27A8FD45FF7D7DFD2BFF7D %FFA852FD06FF9AC9FD27FFA8835E27F852587C7C82828882828288828282 %33CCCC33CCFF33FF0033FF3333FF6633FF9933FFCC33FFFF660000660033 %58FD068252F8F85227F8268283FFFFFF7DFD0AFFA85EFD09822DFD0582A8 %82A8FD09FF52FD20FFA8FFFFFFA8FFA8FFFFFFA8A8FD04FF7C8227F8F827 %FFFF7EFD11FFA852FD06FF9AC9FD24FFA9FFFFA8838227F852587CFD0B82 The first measurements from proton–proton collisions recorded with the ATLAS detector at the LHC are presented. PDF %27759F759F75A0A0C3A0C2A0C3A0C39A76A0C2A0C3A0C2A0FD24FFA8FD04 %%+ 0.3255 0.4431 0.5373 0.1961 (Global Malt) %7DFD28FFC2C9FD1DFF52FD2AFF527DFD28FF9AC9FD1CFFA852FD2AFF7D7D Abstract. %%+ 1 1 1 1 ([Registration]) The physics A detailed study is presented of the expected performance of the ATLAS detector. ATLAS has the dimensions of a cylinder, 46m long, 25m in diameter, and sits in a cavern 100m below ground. PDF. b. DOUT- DOUT is the optional Detector Output. Measurements of the top-quark mass with the ATLAS detector Teresa Barillari 3. %AI3_ColorUsage: Color %5E8282825D825D82F87C5EA7FD0AFF99CACAFF7D827B828182756F6F6F6E %755E825E8258A8FD08FFA852FD06FF9AC9FD22FFA87DFFFFFFA88382825D %C2A1FD24FF7EFFFFFFA8A883A87DA883A87DA883A87DA883A87DA883A87D K�F��u�Mz)�c�~�R�`�HhjP����D� ��t��L|��k$1я��Z�hzt����Ĉ �"��GBK���3=�V?�G�JK9���Yx5v�&�8 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 %1BFF7D7DFD28FFC2C9FD1DFFA87D7DA8A8A87DA8A8A87DA8A8FF52FD1CFF %AI7_GridSettings: 2.25 8 2.25 8 1 0 0.8 0.8 0.8 0.9 0.9 0.9 %7D52FD057DFFFF7D527D52527D7D2752277D7D7D52A8FF52527D52A852A8 %525227525252275252527DFD4DFF7DFD245227A8FD4DFFFD26527DFD4DFF 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. %5227522752275227527DFD4DFFFD255227A8FD4DFF525227525252275252 The ATLAS detector weighs 7,000 tonnes, similar to the weight of the Eiffel Tower. 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 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. %AI5_ArtFlags: 0 0 0 1 0 0 1 0 0 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. %8258FD12827C5282A7FD0FFF83A87DA87D7D837E7DA87DA183A87DA8CFFD %27522727275227272752FD04277DFD08FFFF 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 %FF5252275227522752275227522752275227522752275227522752272727 %FFCFFFCAFFCFFFCAFFCAFFCAFFCAFFCAFFCFA2A8FFCAC9FD0EFF52FD06FF Search for the Lepton Flavor Violating decay Z → eμ with the ATLAS detector at the LHC, Hai Jiang. %%Title: (WIRE ATLAS SCB TO NCE BD20.pdf) %527D52277DFF277D527DA87D527D52FF2752277D527D7D7D52527D7D527D It forms part of the ATLAS collaboration operating at the Large Hadron Collider (LHC) at CERN.. QUICK LINKS: %000011111111220000002200000022222222440000004400000044444444 endstream endobj 78 0 obj 15636 endobj 79 0 obj<>stream stream In these models, the lightest chargino is predicted to have a lifetime long enough to be detected in the tracking detectors of collider experiments. %7DFD2552A8FD4DFFFD052752272727522727275227272752272727522727 The tracking modules and the trigger system are of most relevance for the presented measurements. %525227FD0D527DFD4DFFFD16527DFD0E5227A8FD4DFF5252275252522752 MDT chambers. %%+ 0.8 0 1 0 (Global Green) %57825882585E57827B82578257A8FD08FFA852FD06FF9AC9FD27FFA88382 %A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8FF7EFFFFFFA1FD0DFFA852FD06 %AI3_TemplateBox: 306.5 395.5 306.5 395.5 %A87DA8A8A87DA8A8A87DA8A8A87DA8A8A8527D5252527D7D2752A87DA87D Transition radiation detector gives particle ID. %FF9AC9FD28FF838227F8525882587CFD09827C517C5127F87CA7FFCFFFCA %AI7_Thumbnail: 116 128 8 %FFA8FFFFFFA8FD0DFF52A8FD72FF7D7DFD72FF7DA8FD1DFFA8FD54FF7D7D Download full-text PDF. %52FF527DA87D2752A87D527D527D275252A8527D277D5252277DFF272727 ATLAS Toroidal Muon Spectrometer. 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. the detector and collide in ATLAS, which creates new particles that are detected. 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- 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. %FD06FF7D7DFD11FF7D277D7D7DF8527D52277DFFA8FD10FFA87D27527D7D There are Pogo detection and correction algorithms and … %11FF52FD06FFC3C9FD24FF7E7E7EA85258272727582D7C5D825E8282825E Copy link Link copied. %527DFD28FF9AC9FD1CFFA8527D7D527D527D527D527D527D527DFD1CFF7D %A88382522758587C82888282828882828288828258825227278283FFA8FF %F827588282825E8282825D7C27525D58F82757A8FD0AFF99CFFFFF7D8282 %7C7C7C5883587C587C7C7C587C587C587C7C8258A8FD0AFF99CFFFFFA883 %%DocumentProcessColors: Cyan Magenta Yellow Black %5E8282825127F827F827F82751828282A8FD09FF52FD06FFC2C9FD28FF7C %525227527D7DA8FFA8FF7D7DA8A87DA8A87D275252522752525227525252 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. The LBNL ATLAS group consists of LBNL staff, UC Berkeley Faculty, Postdoctoral fellows and students. %5D825D7CF8272727262727585D8258A8FD08FFA852FD06FF9AC9FD28FF83 %A8FFA8A8A8FFA8A8A8FFA8A8A8FFA8A8A8FFA8A8A8FFA8A8A8FFA8A8A8FF %FF3300FF3333FF3366FF3399FF33CCFF33FFFF6600FF6633FF6666FF6699 %AI9_ColorModel: 2 %AI5_TargetResolution: 800 %F8518258825D8282825D8282825D82828257A8FD0EFF7D825E825D7CF87C %8258A7FD0EFF7D825D8282825E8227512D5882825E8258A8FD08FFA852FD %CFFD0DFF52FD06FFC3C9FD54FFA8FD07FFA1FD0DFFA852FD06FF9AC9FD54 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. %AI5_NumLayers: 1 %66FF6666FF9966FFCC66FFFF9900009900339900669900999900CC9900FF %27527DA87DA87D7D7DA8A1FD0DFFA87DFD06FF9ACAFD53FFA87D7DFD05FF %45FFA8FF7DF8F8FD05A8769375FD0CA827F852A8A8A8FF7D6F6EA7A8FD4E %A87E847EA87E847EA87E847EA87D7E7EA85AFFFFFFA1FD0DFFA852FD06FF [E��� 1x ��"���\3�&���}�@HwQ����qKG %FD0AFFA8FFFFFFA8FFFFFFA8FD07FFA8FFA87DA8FFFFFFA8FFFFFFA8FFFF %FFFFA85E88828282A04B754B756F9F7BA07BA0A0C9C3C9C3C9C3C9C3C976 %8282825E8282825E8282825D82828257A8FD0EFF7D8282825D7C272DFD04 %825782515857A8FD14FFA8FF7EFFFFFFA1FD0DFFA852FD06FF9AC9FD27FF %A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8A8A87DA8527DFD04A87D %AI5_RulerUnits: 0 %522752525227525252275252522752525227525252275252522752525227 %FFFFA8FFFFFFA8FD09FFA8A8FFA9A9FFCACAFD0EFF52FD06FFC2A1FD28FF %0066000066330066660066990066CC0066FF009900009933009966009999 %AI3_DocumentPreview: None %CC9966CC9999CC99CCCC99FFCCCC00CCCC33CCCC66CCCC99CCCCCCCCCCFF 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 … 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 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. %CC0000CC0033CC0066CC0099CC00CCCC00FFCC3300CC3333CC3366CC3399 The ATLAS detector site www.atlas.ch provides a comprehensive presentation of the detector and its physics. A detailed understanding of %8282828382595888827C82888282A8FD09FF52FD06FFC3C9FD28FF7C825D %52FD2FFFC2C9FD19FFA87DFD0452A8FD0BFF52A8FD11FF7DA87D7D7DFD04 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. %5D8258A8FD08FFA852FD06FF9AC9FD28FF835E82588258825882827C8282 %AI9_Flatten: 0 There are Pogo detection and correction algorithms and … %51512D825782828257A8FD08FFA852FD06FF9AC9FD27FFA883822DF827F8 :���v[b. %F82027FD0582A8FD09FF52FD06FFC2A1FD22FFA8A8FD04FF588282825D82 It is connected to the insulated rail detector lead, (or the detector lead from the Atlas Block Detector Board (BDB), (Item #233). %8282825DFD0B825D82827C828283FD0AFFC3BBC2BCBC9999999F9876F827 %7C525852585227FD0582A8FD09FF52FD06FFC2A1FD28FF7C82F8F8F852F8 %00FF0000FFFFFF0000FF00FFFFFF00FFFFFF %AI7_ImageSettings: 0 %%EndComments %FFA8FFFFFFA8FD0FFFA8FFFFFFA8FFA8FFA8FFFFFFA8FFFFFFA8FFFFFFA8 %52277C587CFD0482A8FD09FF52FD06FFC2A1FD28FF7C8282825E8282825E %CFA8FFCAFF7DCACAFF7DA8CACFA0FD0DFFA852FD06FF9AC9FD24FFA9FFFF %%AI8_CreatorVersion: 11.0.0 %FFA9FFA9FFA9FFA9FFA9FFA9FFA9FFA9FFA9FFA9FFA9A8A8FFA9FD04FFC9 %7DA8527DA8527D272752FF27FFA82727A85252A87D27527D52277D7DA87D %F8F827F8275D82828257A8FD08FFA852FD06FF9AC9FD22FFA8A8FD04FF83 The reconstruction of tracks, leptons, photons, missing energy and jets is investigated, together with the performance of b-tagging and the trigger. %FD05FF52A8FD11FFFD077DA87D7D7DFD15FFA8FFA8FFFFFFA8FFFFFFA8FD %DD000000DD000000DDDDDDDDEE000000EE000000EEEEEEEE0000000000FF %%CreationDate: 10/29/2008 10:20 AM %!PS-Adobe-3.0 %C2C9FD28FF7C82F8272758515251825D8282825D825E822D272751F82751 %A8FFA8FFFFFFA8FFFFFFA8FFFFA8FFFFA8FD05FFA8FDFCFFFDFCFFFDFCFF %F827F827F85157A7FFFF7D7DA8FD09FF7D825D8282825D825D8257525882 Wire color optional. %7D7DFD0AFFA8FFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFFFFA8FFFF %9AC9FD25FFA8FFA8A9A8FFA8A9A8FFA8A9A8FFA8A9A8FFA8A9A8FFA9FFA9 %6600666600996600CC6600FF6633006633336633666633996633CC6633FF %52525227527DFD4DFF7DFD2552A8FD4DFFFD0C5227525252275252522752 endstream endobj 77 0 obj<>stream This is just a brief presentation for my OLLI classes. %FD4DFF7DFD245227A8FD4DFFFD26527DFD4DFF7DFD245227A8FD4DFFFD04 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. %A87EA97EA87EA97EA87EA97EA87EA97EA87EA87E847EA87E847EA87E847E %000088888888AA000000AA000000AAAAAAAABB000000BB000000BBBBBBBB L1DDC's function is to concentrate the data from multiple front-end boards and transmit %FFA852527DFD27FF9AC9FD1AFFA8FFFFFFA8FD0CFF7D7DFD1AFFFD0452FD %A8FD47FFA8277D527D5252527D5252527D5252527D5252527D5252527D52 Tuning of layered materials: Studies of CrAuTe4, PdSn4 and WTe2, Na Hyun Jo. ��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� ATLAS is one of two general-purpose detectors at the Large Hadron Collider (LHC). 5 0 obj It is used to connect an auxiliary piece of equipment, (no more than +5VDC), such as an LED or relay. %F87D275227F8527D52525227277D275227F827A8FD0BFFC2CAFFFFFFFD04 z�w��]��h��w&1��nGQ�wN Download full-text PDF Read full-text. 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