Grid Pix Field Simulations and precision needed for a module Peter Kluit, Jan Timmermans Prepared 16 May 2016.

Slides:



Advertisements
Similar presentations
Lyon Gantry Status TEC meeting Dec D. Contardo Module production in Lyon Rigidifier test on R4 Frame tolerance effect on assembly plates Short term.
Advertisements

CONDUCTORS + CAPACITORS
Phys 133 Chapter 26 Electric Field. Phys 133 Electric Field A creates field in space changes the environment B interacts with field New long range interaction.
Section 5.1 Introduction to Normal Distributions and the Standard Normal Distribution.
5-Minute Check on Activity 4-8 Click the mouse button or press the Space Bar to display the answers. 1.What point does a direct variation graph always.
Equipotential Lines = Contours of constant V
Capacitors1 THE NATURE OF CAPACITANCE All passive components have three electrical properties Resistance, capacitance and inductance Capacitance is a measure.
Capacitance Energy & Dielectrics
ECE 4339: Physical Principles of Solid State Devices
Probability Distributions
16 MULTIPLE INTEGRALS.
LIMITS 2. LIMITS 2.4 The Precise Definition of a Limit In this section, we will: Define a limit precisely.
Statistics for Managers Using Microsoft Excel, 4e © 2004 Prentice-Hall, Inc. Chap 6-1 Chapter 6 The Normal Distribution and Other Continuous Distributions.
Conductors are commonly used as places to store charge You can’t just “create” some positive charge somewhere, you have to have corresponding negative.
Capacitors II Physics 2415 Lecture 9 Michael Fowler, UVa.
JIT HW 25-9 Conductors are commonly used as places to store charge You can’t just “create” some positive charge somewhere, you have to have corresponding.
Depletion Region ECE Depletion Region As electrons diffuse from the n region into the p region and holes diffuse from the p region into the n region,
Shearing Stresses in Beams and Thin-Walled Members
ENE 311 Lecture 2. Diffusion Process The drift current is the transport of carriers when an electric field is applied. There is another important carrier.
Normality Notes page 138. The heights of the female students at RSH are normally distributed with a mean of 65 inches. What is the standard deviation.
Lecture 5 Method of images Energy stored in an electric field Principle of virtual work 1.
Engineering Mechanics: Statics
Correlation and Linear Regression. Evaluating Relations Between Interval Level Variables Up to now you have learned to evaluate differences between the.
Normal Distribution Introduction. Probability Density Functions.
Ch 9 pages Lecture 22 – Harmonic oscillator.
Wall survey: With and without TT7. The wall targets are hybrid targets made of precise uncoded targets (the pin targets) which enter in the hole of the.
Today 3/10  Plates if charge  E-Field  Potential  HW:“Plates of Charge” Due Thursday, 3/13  Lab: “Electric Deflection of Electrons”
1 ELEC 3105 Basic EM and Power Engineering Start Solutions to Poisson’s and/or Laplace’s.
Week of February 17 05Electric Field 1 Lecture 04 The Electric Field Chapter 22 - HRW.
Which of these configurations gives V = 0 at all points on the y-axis? 4) all of the above 5) none of the above 10. Equipotential Surfaces III 1) x +2.
CEE 262A H YDRODYNAMICS Lecture 15 Unsteady solutions to the Navier-Stokes equation.
21 April 2004LCWS 2004 Paris1 Readout of a TPC using the Medipix2 CMOS pixel sensor (detection of single electrons on a direct pixel segmented anode) NIKHEF:
Continuous Probability Distributions Statistics for Management and Economics Chapter 8.
Tutorial for XFDTD Written by Cynthia Furse University of Utah.
CLIC_ILD vertex detector modules and stave Layout Mathieu Benoit 15/03/12 mini workshop on engineering aspects of the CLIC vertex detectors 1.
Electrostatics #5 Capacitance. Capacitance I. Define capacitance and a capacitor: Capacitance is defined as the ability of an object to store charge.
1 SCT Lorentz angle & Cluster Width Simulations From first principles Guang Hao Low (Summer Student) In consultation with Steve McMahon, Shaun Roe, Taka.
TPC ExB distortion at LHC-ALICE experiment Yasuto Hori for the ALICE-TPC collaboration Center for Nuclear Study, University of Tokyo 1.
Residuals Recall that the vertical distances from the points to the least-squares regression line are as small as possible.  Because those vertical distances.
SIAM M. Despeisse / 29 th January Toward a Gigatracker Front-end - Performance of the NINO LCO and HCO Matthieu Despeisse F. Osmic, S. Tiuraniemi,
Simulations and Probability An Internal Achievement Standard worth 2 Credits.
Geant4 Tracking Test (D. Lunesu)1 Daniela Lunesu, Stefano Magni Dario Menasce INFN Milano GEANT4 TRACING TESTs.
CLIC Beam Physics Working Group CLIC pre-alignment simulations Thomas Touzé BE/ABP-SU Update on the simulations of the CLIC pre-alignment.
Electric Field.
1 The Precise Definition of a Limit Section The Precise Definition of a Limit A geometric interpretation of limits can be given in terms of the.
Copyright © Cengage Learning. All rights reserved. 2 Limits and Derivatives.
INTRODUCTION Strain gauge measurement is a point strain measurement method developed in the USA c.a independently by E. Simmons and A. Ruge. It.
Straightness measurement
Peterson xBSM Optics, Beam Size Calibration1 xBSM Beam Size Calibration Dan Peterson CesrTA general meeting introduction to the optics.
Optimization of planar pixel detector. T. Habermann Planar pixel detectors L W H ground U.
Transmitted by the expert from GTB Informal Document No. GRE (64th GRE, 4-7 October 2010, agenda item 5(f)) Proposal for Amendments to Regulations.
Electrical Energy and Potential AP Physics 2. Electric Fields and WORK In order to bring two like charges near each other work must be done. In order.
G. Eigen, Paris, Introduction The SiPM response is non-linear and depends on operating voltage (V-V bd ) and temperature  SiPMs need monitoring.
CHAPTER 11 Mean and Standard Deviation. BOX AND WHISKER PLOTS  Worksheet on Interpreting and making a box and whisker plot in the calculator.
TE-MSC. 07/04/2016 Jose Ferradas TE-MSC-MDT Alejandro Carlon TE-MSC-MDT Juan Carlos Perez TE-MSC-MDT On behalf to MSC-MDT section and Coil working group.
Space Charge Effects and Induced Signals in Resistive Plate Chambers
Introduction to Functions of Several Variables
A proton and an electron are in a constant electric field created by oppositely charged plates. You release the proton from the positive side and the.
Grid Pix Field Simulations and precision needed for a module
Shear in Straight Members Shear Formula Shear Stresses in Beams
Analysis Test Beam Pixel TPC
Notes 4 ECE 3318 Applied Electricity and Magnetism Spring 2017
Numerical simulations on single mask conical GEMs
Depletion Region ECE 2204.
TPC Paul Colas Technical meeting, Lyon.
GG 450 February 19, 2008 Magnetic Anomalies.
Cubes Orthographic projections One and Two-point Perspective
Lines used in drafting are lines whose appearance and meaning are determined by international agreements. Geometric Lines.
Lattice (bounce) diagram
Chapter 23 Electric Field Phys 133.
Presentation transcript:

Grid Pix Field Simulations and precision needed for a module Peter Kluit, Jan Timmermans Prepared 16 May 2016

Introduction Aim is to simulate some possible different grid pix designs Current emphasis is on a simulation of the edge effects and the impact on E field deformations. The simulations uses the expressions for the E field for a rectangular plates of size a and b. In that case one has an analytic expression for the fields in Ex, Ey and Ez. The coordinate system is chosen thus that z is the drift field direction and xy defines the sensor plane. On the surfaces a charge is put. To define the ground planes mirror charges are put.

Introduction One can then simulate a grid pix sensor(s) with a grid of squared holes embedded in a homogeneous generated by two large parallel plates (so the TPC). See next slides for the – simplified - simulated geometry. The aim is to study the E field design for a module and the needed mechanical and electrical precision. Edge effects are essential for this as well as the so-called T structures that are needed to make the E field as constant as possible in order to reduce the deformations at the edges of the chips.

Geometry ∧ 550 mm ∨ TPC endplate x z Start with 2 sensors in x 128x0.055 mmguard is in the sensor plane and extends to 100x 550 mm “infinite plane” Ez field = 13 V/mm

Sensor definition 775 μm (z) -400 V Chip 700 μm (z) height Guard size Chip (x) 128*55 μm Note there is ground just below the grid at z = 700 μm. The grid is 75 μm above the grid. The ground under the Guard is at z = 0 The distance between the (2) chips in x is distChip it varies from 2 to 256 pixels. The ground in the empty area is at z =0. The sensor is not fully realistic, because the real grid doesnot extend till the edge of the chip. Also part of the area under the grid is not sensitive due to the presence of the dike. distChip/2 z

Results By calculating the field in the x and z directions starting from z = 550 mm till the sensor at z = 0.7 mm one can calculate the total deviation in the x coordinate, due to the presence of a non zero distance between the chips. If distChip = 0 the deviation is zero. The deviation has been fitted and is described by: double p1 = 1.25; double p2 = /(p0+0.11); double p3 = /(p0+0.11); double y0 = x (in mm); double y1 = x+2*p0; double f00 = p3/(1+p1*y0*y0+p2*sqrt(y0*y0)); double f11 = p3/(1+p1*y1*y1+p2*sqrt(y1*y1)); deviation (in microns) = f00-f11;

Results for distance between chips So empty zone == distChip Top curve corresponds to distChip = 2 pixels etc. x = x –distChip/2 So x = 0 always corresponds to the chip edge.

Interpretation of the Results One observes that even for small distance between the chips of 110 microns, there is a sizeable deviation that goes up to 250 microns. Part of the drifted electrons (at x = 0) will not end up on the sensor. For very small deformations (up to 20 microns) one has to stay 1 mm away from the chip edge. The other extreme (large distance): what happens if a chip is switched off or not presented. This is the 256 pixels case. This is not so different from having a 2 mm (40 pixels) gap between the chips. Note that we have a 2 mm gap due to the bonds. It shows that it is important to put e.g. a well designed T shaped structure to define the Electric field over the bonding area. If one puts a full T structure around the chip one can also compensate for the distortions that are introduced because of the fact that the grid field does not cover the full chip plus distance between the chips. A full structure will also limit the deviation in case a neighbor chip is switched off.

The impact of asymmetries The following three simulations were performed with a zero distance between the chips: 1)The voltage on the left chip is changed by 10% (40 V) 2)The distance of the grid to the chip is changed from 75 to 70 microns on the left chip. 3)The thickness of the left chip is changed from 700 to 800 microns As in the other simulations the total deviation is evaluated It may well be that we can and must reach better specifications than the variations listed above.

Results for asymmetries x = x –distChip/2 So x = 0 always corresponds to the chip edge.

Interpretation impact of asymmetries - The voltage of the grid can be regulated with a precision that is way better than 4 V. So no problem. - The 5 microns for the grid distance going from one grid to another is probably realistic. To realize 2 micron is maybe achievable. - The (z) height of the chip is pretty essential and from the plot it looks like we have to reach 10 microns (on the chip depth) to keep the deviations small enough. That might not be so easy.

T structure(s) around the edges of the sensor 775 μm (z) -400 V Chip 700 μm (z) height Guard size Chip (x) 256*55 μm Similar sensor structure but now we simulate 256 pixels The T structure is indicate on the left. The distance in z wrt grid is 500 μm. The size of the T is distChip (symmetrical around x = 0). The voltage is tuned to minimize the deviations. Simulations were done for distChip = 40 (80) pixels This allows to cover the space between the chips (no bonds). For the chip side that will be bonded one needs more space (80). distChip/2 z T structure 500 μm

Results for a T structure 40 pixels After tuning of the Voltage on the T structure, the deformations are reduced from 600 μm to max. 100 μm. Deformations at a distance of more than 1 mm from the edge of the grid are smaller than 50 μm. NB here x is not shifted and the chip edge is indicated

Results for a T structure 80 pixels After tuning of the Voltage on the T structure, the deformations are reduced from 650 μm to max. 140 μm. Deformations at a distance of more than 1 mm from the edge of the grid are smaller than 70 μm. NB here x is not shifted and the chip edge is indicated

What precision do we need for a module? Using the T structures of 40 and 80 pixels the deformations for a distance larger than say 5 pixels from the edge (dike) are max microns (slides 13 and 14). 1. The chip height must be controlled at the micron level to stay below microns (slide 10). 2.The distance of the grid wrt chip should be constant to better than 1 micron (averaged over chip, slide 10). 3. The voltage must be regulated to better than 4 V (1%). So no problem (slide 10). 4. The height of the T structure is now chosen to be mm. The height itself should be constant at the micron level (same as chip item 1 and slide 10). 5. The width of the T (top) and its placement wrt the chip should stay below 10 microns (slide 7). The first two items have to be ensured during the chip production process. Items 4,5 depend on the production of the T structure and 2,4,5 on the assembling (gluing) of the chips and T structure on the module.