HFT Geometry Considerations F.Videbæk BNL. Introduction This presentation is meant to be a living document, updated as more and better information becomes.

Slides:



Advertisements
Similar presentations
Aim: To understand and know the vocabulary for parts of a circle
Advertisements

FGT installation disks … viewed from the back (From West end looking in towards vertex). SSD cables go in the spaces above and below the rails on the left.
Shawlands Academy Department Of Technical Education
HFT Technical Overview September 26, HFT 2013 TPC FGT 2011 STAR Detectors Fast and Full azimuthal particle identification EMC+EEMC+FMS (-1 ≤ 
SURFACE AREA GEOMETRY 3D solid SOLID SHAPES AND THEIR FACES SOLID FIGURE Enclose a part of space COMPOSITE SOLID It is made by combining two or more.
ATLAS Pixel Detector BCM Signal Cable October 13, 2005 E. Anderssen, LBNL.
HFT PXL Mechanical WBS 1.2 March 2010 Howard Wieman LBNL 1.
Vertex Detector Cooling Bill Cooper Fermilab (Layer 5) (Layer 1) VXD.
1 Integration issues of FPCCD VTX Yasuhiro Sugimoto May 22,
Graphics Output Primitives Pixel Addressing and Fill Area Dr. M. Al-Mulhem Feb. 1, 2008.
L. Greiner 1IPHC meeting – September 5-6, 2011 STAR HFT Plans for the next year A short report on review results and plans for TPC – Time Projection.
HFT PXL Mechanical July 2010 Howard Wieman LBNL 1.
Polygons, Circles, and Solids
ACT Math Practice. Geometry and Trigonometry Placement Tests Primary content areas included in the Geometry Placement Test include: » Triangles (perimeter,
Performance of the DZero Layer 0 Detector Marvin Johnson For the DZero Silicon Group.
Hexagons & Hexagonal Prisms. Hexagons Hexagons are 6 sided shapes. Hexagons can be dimensioned in 2 different ways. 1. Across the faces. 2. Across the.
It is therefore drawn in the Front View
Hexagonal Pyramid cut at an angle #1
HFT & PXL geometry F.Videbæk Brookhaven National Laboratory 13/9/12.
SSD Operations Manual March 2014 SSD: 4 th layer of vertex detector Heavy Flavor Tracker Silicon Strip Detector – Operations Manual PXL Inserted from this.
Areas and Volume Area is a measure of the surface covered by a given shape Figures with straight sides (polygons) are easy to measure Square centimetres:
Dr. R. Ribeiro, Mechanical Engg. Dept. IITD
Engineering Division 1 Mechanical and Integration CD0 Walkthru, 19-Dec, 2007 Eric Anderssen, LBNL.
Math 10 GEOMETRY.
 Phones Cindy Ly 3A. Point  A point is a location without shape of size. It has no dimensions.  The silver button represents a “point” T.
Proving Relationships October Homework Quiz Page (c) Page (b) Page (a) Page (a)
ATLAS SLHC UPGRADE ENGINEERING – LIST OF DECISIONS which will affect the design of auxiliary systems layout and routing BASIC LAYOUT FOR BARREL and WHEELS.
Circle Properties An Arc is a fraction of the circumference A sector is a fraction of a circle. Two radii and an arc A B O 3 cm r = 3 cm d = 6 cm Arc AB.
ATLAS Pixel Detector BCM Signal Cable October 5, 2005 E. Anderssen, LBNL.
SLHC Pixel Layout Studies S. Dardin, M. Garcia-Sciveres, M. Gilchriese, N. Hartman LBNL November 4, 2008.
ATLAS Upgrade ID Barrel: Services around ‘outer cylinder’ TJF updated According to the drawing ‘Preparation outer cylinder volume reservation’
L. Greiner 1IPHC meeting – May 7, 2012 STAR HFT Plans for the next year A short report on HFT/PXL plans for post May 2012 TPC – Time Projection Chamber.
ACFA-7; Taipei, Nov 2004 H.Weerts status Si licon D etector Status H.Weerts Fermilab/Michigan State Univ. (Progress on Si-tracker layout)
f30 G1 G A a F B E C D T F A1 A G G1 B C G A 50 G1 A1
Projection of Planes Plane figures or surfaces have only two dimensions, viz. length & breadth. They do not have thickness. A plane figure, extended if.
DO NOW!!! (1 st ) 1.A rectangular prism has length 4 cm, width 5 cm, and height 9 cm. a) Find the area of the cross section parallel to the base. b) Find.
DIMENSIONING Sizing of drawings in Drafting has standards and guidelines.
17/02/03Designed by Barry Forbes Graphic Communication Hexagons & Hexagonal Prisms.
1 STAR HFT Pixel Detector Howard Wieman Lawrence Berkeley National Lab.
Mario Sitta 1 CERN – Mon. 7 Jul., 2008 Status of ITS v11Hybrid geometry Mario Sitta Univ. Piemonte Orient. & INFN Alessandria.
L. Greiner 1IPHC meeting – May 7, 2012 STAR HFT Plans for the next year A short report on HFT/PXL plans for post May 2012 TPC – Time Projection Chamber.
Simulations Report E. García, UIC. Run 1 Geometry Radiator (water) 1cm x 2cm x 2cm with optical properties Sensitive Volume (hit collector) acrylic (with.
TECH 104 – Technical Graphics Communication Introduction to Engineering Graphics Communication.
Year 9Dice. Select “New” Select “Metric” Standard (mm).ipt 1 2.
PRESENTATION ON INTERSECTION OF SOLIDS by Mr.Venkata Narayana Mr.A.S.Pavan Kumar Department of Mechanical Engineering SNIST.
Geometric Construction
Evgeny Kryshen (PNPI) Mikhail Ryzhinskiy (SPbSPU) Vladimir Nikulin (PNPI) Detailed geometry of MUCH detector in cbmroot Outline Motivation Realistic module.
F.Videbaek PXL geometry update. PXL ladder For realistic simulation it is essential to get the proper layout of ladders. Starting point 1.SW model 2.Material.
M. Deveaux, CBM-Collaboration-Meeting, 25 – 28. Feb 2008, GSI-Darmstadt Considerations on the material budget of the CBM Micro Vertex Detector. Outline:
TC Straw man for ATLAS ID for SLHC This layout is a result of the discussions in the GENOA ID upgrade workshop. Aim is to evolve this to include list of.
Hexagons & Hexagonal Prisms.
SiD Collaboration Meeting Highlights Tom Markiewicz/SLAC ILC BDS Meeting 08 May 2007.
R. Bradford 10 December, 2014 Sensor Details. Explanation Submitted some designs that will be included on the Novati/Tezzaron submission. Designs based.
Redesign of LumiCal mechanical structure W.Daniluk, E.Kielar, J.Kotula, K.Oliwa, Wojciech Wierba, L.Zawiejski Institute of Nuclear Physics PAN Cracow,
GEOMETRY!!!. Points  A point is an end of a line segment.  It is an exact location in space.   It is represented by a small dot. Point A A.
Three Ways to Draw a Threaded Bolt Even though they look different, they all mean the exact same thing. It is the CALL-OUT information that is critical.
1 IST development status  Seattle  Composite Design.
October 2014Silicon Pixel Tracker – Chris Damerell 1 Tracking sensor, one of 12,000, 8x8 cm 2, 2.56 Mpixels each Matching endcaps (only one layer shown)
Volume and Surface Area
Learning Aid: Technical Terms for Describing Drawings
Ampère’s Law Figure Arbitrary path enclosing a current, for Ampère’s law. The path is broken down into segments of equal length Δl.
Introduction to Engineering – E10
Additional muon stations for the Upgrade of the Elevator Regions in the ATLAS Muon Spectrometer. Integration issues Denis Diyakov, Alexander Seletskiy,
Ampère’s Law Figure Arbitrary path enclosing a current, for Ampère’s law. The path is broken down into segments of equal length Δl.
WG4 – Progress report R. Santoro and A. Tauro.
COORDINATE PLANE The plane containing the "x" axis and "y" axis.
DIMENSION PLACEMENT By: Muhammad Zahid.
BCM Overview Placement such that system is sensitive to all types of beam accidents. => 2 independent subsystems Halo losses inside the Pixel volume ie.
Cross Sections.
Presentation transcript:

HFT Geometry Considerations F.Videbæk BNL

Introduction This presentation is meant to be a living document, updated as more and better information becomes available. Version 2 December 9, 2011

Support Structure Overview

Schematic Layout

Current Geant View courtesy Spiros

As build

Supporting Structures XY cut OSC (r=21 cm) PST ~13 cm Beam Pipe

Details on cylinders OSC Outer Support Cylinder – CF ~ 800 micron; – Will support SSD for run14+ PST (Pixel Support Tube) – Isolate PXL from other part. Enables cooling of PXL – Install for engineering run 13. – Will support IST from run-14+ – CF ~ 800 Micro

OSC Flange region

Pixel Support Tube SW model

OSC

OSC Flange Diameter 432.4/2 Diameter 435.4/2

Material and Radiation Lengths OSC: – The nominal thickness is 1mm (cross check) of CF. The precise rd. length of CF depends on the compositions but is usually around 24 cm. – Thus 1 mm 1/240= 0.42 % rad length MSC (PST) – 800 microns = 0.33%

PXL material budget The nominal average thickness is 0.37 rad length (for Al based cable), but is clearly large at sector beam sides. Also the ladders are not perpendicular so incident angle goes from ~90 deg to ~ 60 deg. For the inner sector; slightly slanted for outer sector.

Beam Pipe material Assume the Beam Pipe is Be with a thickness of 0.8 mm, and an outer radius of 20 mm. Q: Have the as built dimensions been checked.

IST material The TDR claims ~ 1.1% overall. It would be important to look at the budget in the Si/CF foam area and in the APV/cooling tube area separately.

SSD material This should be accounted for in the current GSTAR, but also in the NIM article.

PXL ladder and support beam structures. First input is to understand the Sector layout and get it into GSTAR to study phi variation of radiation length, not just averages.

sector geometry based on ladder layout ph1.SLDPRT (Sketch2) The outer ladder positions are defined by placing the active edge of the pixel array (side opposite pad row) on an 80 mm radius and positioned 12 mm apart. The starting point for the first active region is placed mm from the vertical surface of the sector beam along the surface line of the active silicon. The side surfaces of the sector beams are defined by lines 1 mm inside and parallel to the vertical radial line and the 36 deg radial line. The ladder angle is defined by requiring a 1 mm overlap of the active regions for the phase 1 detector

The grey rectangles have the length of the active region of phase 1 detector and the thickness represents what was expected to be the ladder thickness. This is what is used to define the sector beam surface that the ladder gets bonded to. The ladder thickness ended up slightly different than the value here of mm, so the ladders will be off a little from the 80 mm radius circle. sector geometry based on ladder layout ph1.SLDPRT (Sketch2)

The inner ladder is positioned with the active edge next to the wire pads on a 25 mm radius circle. The angle is defined by a 1 mm overlap of the active region. There is an arbitrary offset from the sector beam side edge.

sector beam ph1.SLDPRT (Sketch1) The sector beam shape is linked to ladder layout ph1.SLDPRT (Sketch 2) The 6 longer straight lines are collinear with the inside rectangle edges. All the arcs but one have a 1.5 mm radius. All arc are tangent to joining lines. The 2 short lines are collinear with radius lines. 3 points are coincident with points in ladder layout ph1.SLDPRT (Sketch 2). This completely defines the shape. The beam material extends in from the sketch. ladder layout ph1.SLDPRT 1 2 3

The actual placement of the ladders in the model deviate a little from the ladder layout ph1.SLDPRT because the ladder thickness is not quite as specified in the layout. ladder layout thickness: mm ladder model thickness: mm

Approach Got all information from Howard how the geometry in SW is setup. Check with SW model. Extracted other info from there. Put this information into a root script that could generate cross section of geometry. i.e. picture from last week. Generated root Tgeo script that could be executed to generate geometry. See next two slides for output. Communicated with Jonathan and Jason

Cross section plots

Scripts The scripts are currently in ~videbaek/star (i.e. my BRAHMS area- since I use root v5.28 for daily work). Sector.C – Calculates based on general information the detailled information need to make the cross section plot and output Root TGeo.. Statements assembly.C – Embedded output from above program and executes a root macro the generate the root geometry, and draw this.

End view (Tgeo)

Sector ladder layout cm (CF beam) Cable Length cm ~20 cm Active Si (19.2*19.2 mm) cm

Current implemented (C.F. beams, Si, Beampipe)