Charges Sensing Preamplifier & noise instrumentation examples1 A little example of noise measurement in time domain and frequency domain I acquired noise.

Slides:



Advertisements
Similar presentations
ECE410 Spring 2012 Lecture #32 AC Circuits I.
Advertisements

Specific requirements for analog electronics of a high counting rate TRD Vasile Catanescu NIHAM - Bucharest CBM 10th Collaboration Meeting Sept 25 – 28,
Sampling and quantization Seminary 2. Problem 2.1 Typical errors in reconstruction: Leaking and aliasing We have a transmission system with f s =8 kHz.
Noise. Noise is like a weed. Just as a weed is a plant where you do not wish it to be, noise is a signal where you do not wish it to be. The noise signal.
Microelectronics System Design for Chronic Brain Implants ECEN 5007 S. Johnson, V. Ganesan
Example Problem You are measuring the EEG of a patient and accidently choose two different types of electrodes for EEG lead. One of them has a source impedance.
NA62 front end Layout in DM option Jan Kaplon/Pierre Jarron.
NA62 front end architecture and performance Jan Kaplon/Pierre Jarron.
The Spectrum Jean Baptiste Fourier ( ) discovered a fundamental tenet of wave theory All periodic waves are composed of a series of sinusoidal.
The Spectrum n Jean Baptiste Fourier ( ) discovered a fundamental tenet of wave theory n All periodic waves are composed of a series of sinusoidal.
Introduction to Nanomechanics (Spring 2012) Martino Poggio.
Electronics for first beam tests of diamond sensors Presented by: Igor Emeliantchik NC PHEP, Minsk:Konstantin Afanaciev, Igor Emeliantchik Alexander Ignatenko.
Leakage & Hanning Windows
AC Waveform and AC Circuit Theory Md Shahabul Alam Dept: EEE.
Characterization of the electrical response of Micromegas detectors to spark processes. J.Galan CEA-Saclay/Irfu For the RD51 meeting.
Lecture 1 Signals in the Time and Frequency Domains
3/26/2003BAE of 10 Application of photodiodes A brief overview.
Recent results on wave-particle interactions as inferred from SCATHA RC Olsen University of Alabama, Huntsville Invited talk, XXIst General Assembly of.
Alternating Current Chapter 12. Generating AC (12-1)
.Compare bipolar and ON-OFF line codes in terms of spectrum efficiency, transperancy, error detection and timing.
APD, CSP and T-card Characteristics Toru Sugitate / Hiroshima University for PHOS FEE Review / PRR Meeting in Wuhan, China on.
L.Royer– Calice DESY – July 2010 Laurent ROYER, Samuel MANEN, Pascal GAY LPC Clermont-Ferrand R&D LPC Clermont-Fd dedicated to the.
Development of a Low Noise Preamplifier for the LEM read-out
Chapter 2. Fourier Representation of Signals and Systems
INC 112 Basic Circuit Analysis Week 13 Frequency Response.
to Electronics Summer 2009 Introduction to Electronics in HEP Experiments Philippe Farthouat CERN.
Alternating Current (AC) R, L, C in AC circuits
Lecture 13: Complex Numbers and Sinusoidal Analysis Nilsson & Riedel Appendix B, ENG17 (Sec. 2): Circuits I Spring May 13, 2014.
Contents Introduction ( P1-P4). Frequency modulation.(P5-P7) Frequency demodulation (P8-P14) FM using simulink implementation (P15 – P 17)
19.2 Graphs of Harmonic Motion pp Mr. Richter.
1 Development of the input circuit for GOSSIP vertex detector in 0.13 μm CMOS technology. Vladimir Gromov, Ruud Kluit, Harry van der Graaf. NIKHEF, Amsterdam,
EE 1270 Introduction to Electric Circuits Suketu Naik 0 EE 1270: Introduction to Electric Circuits Lecture 17: 1) Sinusoidal Source 2) Complex Numbers.
Ya Bao, South Bank University 1 Noise Richard Read, The Essence of Communications Theory, Chapter 3.
Michael Unrau, Institut für Kernphysik Analyse von Bolometersignalen der EDELWEISS Dark Matter Suche EDELWEISS dark matter searchFull InterDigitized detector.
INC 111 Basic Circuit Analysis Week 13 Frequency Response.
October, 2001CMS Tracker Electronics1 Module studies at IC OUTLINE laboratory setup description, APV I2C settings pulse shape studies (dependence on ISHA,
Preamplifiers : BGA 2003 (Silicon MMIC amplifier): In general, the function of a preamp is to amplify a low-level signal to line-level. DESCRIPTION: Silicon.
Electrons capture in the air instrumentation examples1 The subject: Medical Ionization Chambers are air filled ICs In the air, electrons are captured by.
A 128-channel event-driven readout ASIC for the R 3 B Tracker TWEPP 2015, Lisbon Lawrence Jones ASIC Design Group Science and Technology Facilities Council.
A complete DIY numerical shaper… … from scratch! instrumentation examples1 What do we need? The signal digitized at the output of a Charge Sensing Preamp.
N/  discrimination instrumentation examples1 The problem… Particles beam Active taget Scintillator neutron  activation decay time Concrete wall activation.
Hyper-Pure Germanium in Planar Configuration instrumentation examples1 A HP Ge is a cooled solid state detector LN2 Dewar HP Ge Charges Sensing Preamplifier.
Status of the ETL 9125FLB Photomultiplier Tubes Steve Bache UNC-Wilmington.
A Fast Monolithic Active Pixel Sensor with in Pixel level Reset Noise Suppression and Binary Outputs for Charged Particle Detection Y.Degerli 1 (Member,
Status of integrated preamplifiers for GERDA GERDA meeting – MPI Heidelberg, Feb 20-22, 2006 F. Zocca, A. Pullia, S.Riboldi, C. Cattadori.
LC Power Distribution & Pulsing Workshop, May 2011 Super-ALTRO Demonstrator Test Results LC Power Distribution & Pulsing Workshop, May nd November.
Outline Transmitters (Chapters 3 and 4, Source Coding and Modulation) (week 1 and 2) Receivers (Chapter 5) (week 3 and 4) Received Signal Synchronization.
Noise and Data Errors Nominal Observation for “1” Nominal Observation for “0” Probability density for “0” with Noise Probability density for “1” with Noise.
Timing in Thick Silicon Detectors Andrej Studen, University of Michigan, CIMA collaboration.
The Spectrum n Jean Baptiste Fourier ( ) discovered a fundamental tenet of wave theory.
MuTr Chamber properties K.Shoji Kyoto Univ.. Measurement of MuTr raw signal Use oscilloscope & LabView Read 1 strip HV 1850V Gas mixture Ar:CO 2 :CF 4.
PM signals quantification. …Toward a good methodology instrumentation examples1 A PM tube is a vacuum device Photocathode  Converts incident Photons into.
CERN PH MIC group P. Jarron 07 November 06 GIGATRACKER Meeting Gigatracker Front end based on ultra fast NINO circuit P. Jarron, G. Anelli, F. Anghinolfi,
Oscar Alonso – Future Linear Colliders Spanish Network 2015 – XII Meeting - Barcelona, January 2015 O. Alonso, J. Canals, M. López, A. Vilà, A. Herms.
The Proposed Holographic Noise Experiment Rainer Weiss, MIT On behalf of the proposing group Fermi Lab Proposal Review November 3, 2009.
Analog Circuits Hiroyuki Murakami. CONTENTS Structure of analog circuits Development of wide linear range CSA system Problem of analog circuits How to.
Front End. Charge pre-amp and detector Voltage regulator. TOP side. Detector linear voltage regulator BOTTOM side. Charge pre-amp.
A General Purpose Charge Readout Chip for TPC Applications
Section 6.4 Graphs of Polar Equations
HPD with external readout
A Fast Binary Front - End using a Novel Current-Mode Technique
Sinusoids: continuous time
Lesson 7: Anti-Aliasing Filtering
Amplifiers: A Bio amplifier is an electrophysiological device, a variation of the instrumentation amplifier, used to gather and increase the signal integrity.
Accidental Coincidence Rates
Development of hybrid photomultiplier for Hyper-Kamiokande
Pre-installation Tests of the LHCb Muon Chambers
8.7 Gated Integration instrument description
1.5.4 The High-Voltage Power Supply : The high-voltage power supply (HVPS) provides a positive or negative voltage necessary for.
Peng Chen, Kevin D. Gillis  Biophysical Journal 
Presentation transcript:

Charges Sensing Preamplifier & noise instrumentation examples1 A little example of noise measurement in time domain and frequency domain I acquired noise after a CSP (sampling 10ns) :  = 0.170mV RMS

Charges Sensing Preamplifier & noise instrumentation examples2 We know that Cf=2pF (It’s written on the preamp!) We know a charge pulse gives a “step” response whose amplitude is We measured Vrms = 0.160mV  the Equivalent Noise Charge (ENC) is 0.34fC = 2100 charges = 7.6keV in Silicon detectors We will do far better later…

Charges Sensing Preamplifier & noise instrumentation examples3 For the moment let’s look at the specifications of our system: Detector : CSP : Polarization : Feedback :

Charges Sensing Preamplifier & noise instrumentation examples4 The noise spectral density is : v.noise <- ts(v.csp, start=0, frequency=1/(0.01e-6)) S <- spectrum(v.noise, spans=c(5,5)) plot (c(100,1e8), c(1e-9,1e-5), type="n", log="xy", xlab="frequency (Hz)", ylab="spectral density (V/Hz^1/2)") grid() lines(S$freq, sqrt(2*S$spec))

Charges Sensing Preamplifier & noise instrumentation examples5 The noise spectral density is :

Charges Sensing Preamplifier & noise instrumentation examples6 Let’s compare it to CSP theory :

Charges Sensing Preamplifier & noise instrumentation examples7 And, obviously : That’s all folks! Noise can be measured in time domain But the full description is easier in frequency domain We are able to select components in order to make less Noise than the detector itself. (except the noise voltage of the preamp.)