Laue diffraction software for reciprocal space data visualisation and analysis

Size: px
Start display at page:

Download "Laue diffraction software for reciprocal space data visualisation and analysis"

Transcription

1 Laue diffraction software for reciprocal space data visualisation and analysis Dr Gail N. Iles Neutrons 2.0: International Workshop Software for Neutron Scattering Berlin, Germany Tuesday 26th March 2013

2 CONTENTS FALCON Fast Acquisition Laue Camera for Neutrons iccd scintillator plate detectors CYCLOPS Hardware Software Laue Diffraction data Physics Typical experiment Visualisation Analysis 2

3 LAUE DIFFRACTION SOFTWARE E11 AT HZB ~50% of 4π FALCON Backscattering Detector Transmission Detector Neutrons Iles and Schorr Acta Cryst. (2012). A68, s134 Gail N. Iles Neutrons 2.0, Berlin March

4 FALCON DETECTOR 6 Li + 1 n 4 He (2.05 MeV) + 3 T (2.75 MeV) 3 T 3 He 1+ + e - + ν e 400mm 4 high-performance thermoelectrically-cooled imageintensified CCD cameras view each scintillator via close-focus lenses Sample Table 2048 (h) x 2048 (w) pixels on 400mm x 400mm plate => 206 µm 2 pixel size 16 and 20-bit digitization with fast readout: 0.5s and 8s respectively 16-bit: 60,000 e- per pixel 20-bit: 960,000 e- per pixel 4

5 FALCON ACQUISITION SOFTWARE GAIL N. 5

6 ILL LAUE INSTRUMENT CYCLOPS 8 Scintillator Plates Ouladdiaf et al. J. Appl. Cryst. (2011). 44, iccds per plate 70% of 4π 170x170μm resolution 6

7 CYCLOPS SOFTWARE PSL Acquisition software Image PRO LAUEGEN ESMERALDA 7

8 PHYSICS Each spot represents one wavelength White beam Wavelength ~ 0.8 < λ < 5.0 Å (thermal neutrons) Each spot has a particular intensity 8

9 TYPICAL EXPERIMENT Sample Environment Single temperature measurements Sweeping temperature measurements Single magnetic field measurement Field-cooled measurements Single-crystal geometry ω rotation Scintillator/iCCD technology 3 images taken per measurement criteria (averaged) 100 temperatures 360deg w / 5deg = 72 sample positions 60s exposure time = 36Mb file Typical 3-day experiment => 2000 files ~ 30 Gb data 9

10 ANORTHITE CaAl 2 Si 2 O 8 P-1 => 514 C a = 8.173Å b = Å c = Å α = β = γ = Chatterji, Iles, Ouladdiaf, ILL TEST-2084: P1-to-I1 phase transition in anorthite, July

11 VISUALISATION 11

12 VISUALISATION: IMAGEJ 12

13 VISUALISATION: IMAGEJ 13

14 VISUALISATION: IMAGEJ 14

15 VISUALISATION: IMAGEJ 15

16 LAUE DIFFRACTION SOFTWARE ANALYSIS Gail N. Iles Neutrons 2.0, Berlin March

17 ANALYSIS: ESMERALDA 17

18 ANALYSIS: ESMERALDA 18

19 ANALYSIS: ESMERALDA 19

20 ANALYSIS: ESMERALDA 20

21 ANALYSIS: ESMERALDA File types: Tif/Bitmap/Img/Reo/Raw/hbin Image Tools Adjust for good brightness/contrast levels 21

22 ANALYSIS: ESMERALDA Image Tools Removes dead pixels Reorders detectors Converts CYCLOPS geometry to be comparable to image-plate detectors e.g. LADI/VIVALDI/KOALA 22

23 ANALYSIS: ESMERALDA Backscattering detector now centred on incoming neutron beam Indication that geometrical conversion occurred successfully Only spots left are reflections 23

24 ANALYSIS: ESMERALDA Automatic Peak Finding 24

25 ANALYSIS Calculation Tools Automatic Orientation Stepwise rotating around nodals 25

26 ANALYSIS 26

27 ANALYSIS 27

28 SUMMARY FALCON Commissioning 2013 Open to users 2014 CYCLOPS Provides data as 36Mb.tif files Leads the field in Laue CCD instrumentation Laue Diffraction data Acquisition software custom-written by Photonic Science Visualisation software e.g. ImageJ hkl files and intensity integration - Esmeralda Twinned structures shelxl? 28

29 THANK YOU FOR YOUR ATTENTION 29

R-AXIS RAPID. X-ray Single Crystal Structure Analysis System. Product Information

R-AXIS RAPID. X-ray Single Crystal Structure Analysis System. Product Information The Rigaku Journal Vol. 15/ number 2/ 1998 Product Information X-ray Single Crystal Structure Analysis System R-AXIS RAPID 1. Introduction X-ray single crystal structure analysis is known as the easiest

More information

membrane sample EUV characterization

membrane sample EUV characterization membrane sample EUV characterization Christian Laubis, PTB Outline PTB's synchrotron radiation lab Scatter from structures Scatter from random rough surfaces Measurement geometries SAXS Lifetime testing

More information

Outline. Motivation Experimental Set-Up Theory behind the set-up Results Acknowledgements

Outline. Motivation Experimental Set-Up Theory behind the set-up Results Acknowledgements Outline Motivation Experimental Set-Up Theory behind the set-up Results Acknowledgements Motivation Attosecond pulses could be used to study time-dependence of atomic dynamics. Greater control of pulse

More information

Instrumentation for Neutron Imaging

Instrumentation for Neutron Imaging Instrumentation for Neutron Imaging Burkhard Schillinger Heinz Maier-Leibnitz Zentrum B.Schillinger 1 Radiography principle: Cone beam vs. parallel beam: Resolution and L/D What happens at a Neutron guide?

More information

High Energy Digital Radiography & 3D-CT for Industrial Systems

High Energy Digital Radiography & 3D-CT for Industrial Systems DIR 2007 - International Symposium on Digital industrial Radiology and Computed Tomography, June 25-27, 2007, Lyon, France High Energy Digital Radiography & 3D-CT for Industrial Systems Non-Destructive

More information

Week 9: Chap.13 Other Semiconductor Material

Week 9: Chap.13 Other Semiconductor Material Week 9: Chap.13 Other Semiconductor Material Exam Other Semiconductors and Geometries -- Why --- CZT properties -- Silicon Structures --- CCD s Gamma ray Backgrounds The MIT Semiconductor Subway (of links

More information

Properties of a Detector

Properties of a Detector Properties of a Detector Quantum Efficiency fraction of photons detected wavelength and spatially dependent Dynamic Range difference between lowest and highest measurable flux Linearity detection rate

More information

Optical design of shining light through wall experiments

Optical design of shining light through wall experiments Optical design of shining light through wall experiments Benno Willke Leibniz Universität Hannover (member of the ALPS collaboration) Vistas in Axion Physics: A Roadmap for Theoretical and Experimental

More information

Single Photon Interference Katelynn Sharma and Garrett West University of Rochester, Institute of Optics, 275 Hutchison Rd. Rochester, NY 14627

Single Photon Interference Katelynn Sharma and Garrett West University of Rochester, Institute of Optics, 275 Hutchison Rd. Rochester, NY 14627 Single Photon Interference Katelynn Sharma and Garrett West University of Rochester, Institute of Optics, 275 Hutchison Rd. Rochester, NY 14627 Abstract: In studying the Mach-Zender interferometer and

More information

Charged-Coupled Devices

Charged-Coupled Devices Charged-Coupled Devices Charged-Coupled Devices Useful texts: Handbook of CCD Astronomy Steve Howell- Chapters 2, 3, 4.4 Measuring the Universe George Rieke - 3.1-3.3, 3.6 CCDs CCDs were invented in 1969

More information

Status of the Electron Beam Transverse Diagnostics with Optical Diffraction Radiation at FLASH

Status of the Electron Beam Transverse Diagnostics with Optical Diffraction Radiation at FLASH Status of the Electron Beam Transverse Diagnostics with Optical Diffraction Radiation at FLASH M. Castellano, E. Chiadroni, A. Cianchi, K. Honkavaara, G. Kube DESY FLASH Seminar Hamburg, 05/09/2006 Work

More information

Nature Methods: doi: /nmeth Supplementary Figure 1. Resolution of lysozyme microcrystals collected by continuous rotation.

Nature Methods: doi: /nmeth Supplementary Figure 1. Resolution of lysozyme microcrystals collected by continuous rotation. Supplementary Figure 1 Resolution of lysozyme microcrystals collected by continuous rotation. Lysozyme microcrystals were visualized by cryo-em prior to data collection and a representative crystal is

More information

Notes on the Configuration, Installation, and Use of the 4Spots ImageJ plug-in

Notes on the Configuration, Installation, and Use of the 4Spots ImageJ plug-in Configuring 4spots The 4spots plugin will quickly measure the length of two g-vectors, as well as the angle between them. It will further use these values to compute associated d-spacings. This is accomplished

More information

How Does One Obtain Spectral/Imaging Information! "

How Does One Obtain Spectral/Imaging Information! How Does One Obtain Spectral/Imaging Information! How do we measure the position, energy, and arrival time of! an X-ray photon?! " What we observe depends on the instruments that one observes with!" In

More information

Data collection. Refinement. R[F 2 >2(F 2 )] = wr(f 2 ) = S = reflections 1118 parameters

Data collection. Refinement. R[F 2 >2(F 2 )] = wr(f 2 ) = S = reflections 1118 parameters organic compounds Acta Crystallographica Section E Structure Reports Online ISSN 1600-5368 Non-merohedrally twinned hexamethylenetetramine 4-nitrophenol water (1/2/1), triclinic modification Seik Weng

More information

Charge-Coupled Device (CCD) Detectors pixel silicon chip electronics cryogenics

Charge-Coupled Device (CCD) Detectors pixel silicon chip electronics cryogenics Charge-Coupled Device (CCD) Detectors As revolutionary in astronomy as the invention of the telescope and photography semiconductor detectors a collection of miniature photodiodes, each called a picture

More information

Gas scintillation Glass GEM detector for high-resolution X-ray imaging and CT

Gas scintillation Glass GEM detector for high-resolution X-ray imaging and CT Gas scintillation Glass GEM detector for high-resolution X-ray imaging and CT Takeshi Fujiwara 1, Yuki Mitsuya 2, Hiroyuki Takahashi 2, and Hiroyuki Toyokawa 2 1 National Institute of Advanced Industrial

More information

Photon Diagnostics. FLASH User Workshop 08.

Photon Diagnostics. FLASH User Workshop 08. Photon Diagnostics FLASH User Workshop 08 Kai.Tiedtke@desy.de Outline What kind of diagnostic tools do user need to make efficient use of FLASH? intensity (New GMD) beam position intensity profile on the

More information

Single Photon Interference Laboratory

Single Photon Interference Laboratory Single Photon Interference Laboratory Renald Dore Institute of Optics University of Rochester, Rochester, NY 14627, U.S.A Abstract The purpose of our laboratories was to observe the wave-particle duality

More information

Nature Protocols: doi: /nprot Supplementary Figure 1. Schematic diagram of Kőhler illumination.

Nature Protocols: doi: /nprot Supplementary Figure 1. Schematic diagram of Kőhler illumination. Supplementary Figure 1 Schematic diagram of Kőhler illumination. The green beam path represents the excitation path and the red represents the emission path. Supplementary Figure 2 Microscope base components

More information

Pixel Array Detectors: Counting and Integrating

Pixel Array Detectors: Counting and Integrating Pixel Array Detectors: Counting and Integrating Roger Durst, Bruker AXS October 13, 2016 1 The quest for a perfect detector There is, of course, no perfect detector All available detector technologies

More information

Very short introduction to light microscopy and digital imaging

Very short introduction to light microscopy and digital imaging Very short introduction to light microscopy and digital imaging Hernan G. Garcia August 1, 2005 1 Light Microscopy Basics In this section we will briefly describe the basic principles of operation and

More information

Triclinic polymorphs of triphenylphosphine and triphenylphosphine sulfide

Triclinic polymorphs of triphenylphosphine and triphenylphosphine sulfide electronic papers Acta Crystallographica Section C Crystal Structure Communications ISSN 0108-2701 Triclinic polymorphs of triphenylphosphine and triphenylphosphine sulfide Burkhard Ziemer, Annegrit Rabis

More information

Overview of performance and improvements to fixed exit double crystal monochromators at Diamond. Andrew Dent, Physical Science Coordinator, DLS

Overview of performance and improvements to fixed exit double crystal monochromators at Diamond. Andrew Dent, Physical Science Coordinator, DLS Overview of performance and improvements to fixed exit double crystal monochromators at Diamond Andrew Dent, Physical Science Coordinator, DLS Overview Diffraction limit Geometric magnification Source

More information

metal-organic papers Hydridotetrakis(triphenylphosphito)cobalt(I) Comment Experimental

metal-organic papers Hydridotetrakis(triphenylphosphito)cobalt(I) Comment Experimental metal-organic papers Acta Crystallographica Section E Structure Reports Online ISSN 1600-5368 Hydridotetrakis(triphenylphosphito)cobalt(I) Jonathan D. Crane* and Nigel Young Department of Chemistry, University

More information

Image Formation and Capture. Acknowledgment: some figures by B. Curless, E. Hecht, W.J. Smith, B.K.P. Horn, and A. Theuwissen

Image Formation and Capture. Acknowledgment: some figures by B. Curless, E. Hecht, W.J. Smith, B.K.P. Horn, and A. Theuwissen Image Formation and Capture Acknowledgment: some figures by B. Curless, E. Hecht, W.J. Smith, B.K.P. Horn, and A. Theuwissen Image Formation and Capture Real world Optics Sensor Devices Sources of Error

More information

Imaging in the EUV region. Eberhard Spiller

Imaging in the EUV region. Eberhard Spiller Imaging in the EUV region Eberhard Spiller Introduction to Imaging Applications Astronomy Microscopy EUV Lithography Direct Reconstruction E. Spiller, June 11, 2008 2 Imaging with light Waves move by λ

More information

GSPC detectors development for neutron reflectometry and SANS Instruments WP22 / Task 22.2

GSPC detectors development for neutron reflectometry and SANS Instruments WP22 / Task 22.2 GSPC detectors development for neutron reflectometry and SANS Instruments WP22 / Task 22.2 Objective : The proposed JRA aims at the development of new detector technologies based on Gaseous Scintillation

More information

WP640 Imaging Colorimeter. Backlit Graphics Panel Analysis

WP640 Imaging Colorimeter. Backlit Graphics Panel Analysis Westboro Photonics 1505 Carling Ave, Suite 301 Ottawa, ON K1V 3L7 Wphotonics.com WP640 Imaging Colorimeter Backlit Graphics Panel Analysis Issued: May 5, 2014 Table of Contents 1.0 WP600 SERIES IMAGING

More information

organic papers 2-[4-(Dimethylamino)phenyl]-4,5-diphenyl- 1H-imidazole isopropanol solvate Comment

organic papers 2-[4-(Dimethylamino)phenyl]-4,5-diphenyl- 1H-imidazole isopropanol solvate Comment organic papers Acta Crystallographica Section E Structure Reports Online ISSN 1600-5368 2-[4-(Dimethylamino)phenyl]-4,5-diphenyl- 1H-imidazole isopropanol solvate Hassan Martinez, a Horst Puschmann, b

More information

Data collection. Refinement. R[F 2 >2(F 2 )] = wr(f 2 ) = S = reflections 595 parameters

Data collection. Refinement. R[F 2 >2(F 2 )] = wr(f 2 ) = S = reflections 595 parameters organic compounds Acta Crystallographica Section E Structure Reports Online ISSN 1600-5368 Hydronium perchlorate dibenzo-18- crown-6 (1/1): monoclinic polymorph Michaela Pojarová, a * Karla Fejfarová a

More information

X-ray investigation of crystal structures / Laue method with digital X-ray detector (XRIS) (Item No.: P )

X-ray investigation of crystal structures / Laue method with digital X-ray detector (XRIS) (Item No.: P ) X-ray investigation of crystal structures / Laue method with digital X-ray detector (XRIS) (Item No.: P2541602) Curricular Relevance Area of Expertise: Physik Education Level: Hochschule Topic: Moderne

More information

Low Voltage Electron Microscope

Low Voltage Electron Microscope LVEM5 Low Voltage Electron Microscope Nanoscale from your benchtop LVEM5 Delong America DELONG INSTRUMENTS COMPACT BUT POWERFUL The LVEM5 is designed to excel across a broad range of applications in material

More information

X-Ray Spectroscopy with a CCD Detector. Application Note

X-Ray Spectroscopy with a CCD Detector. Application Note X-Ray Spectroscopy with a CCD Detector In addition to providing X-ray imaging solutions, including CCD-based cameras that image X-rays using either direct detection (0.5-20 kev) or indirectly using a scintillation

More information

190 nm (6.5 ev) Laser-ARPES. Laser ARPES using a Tunable ps UV Source

190 nm (6.5 ev) Laser-ARPES. Laser ARPES using a Tunable ps UV Source 190 nm (6. ev) Laser-ARPES Laser ARPES using a Tunable ps UV Source 1 190 nm (6. ev) UV Source Laser ARPES/ARUPS with a High-Power UV Source Tunable deep-uv pulses from 190... 21 nm (6.....77 ev) are available

More information

1 Introduction Installation... 4

1 Introduction Installation... 4 Table of contents 1 Introduction... 3 2 Installation... 4 3 Measurement set up... 5 3.1 Transmissive spatial light modulator...5 3.2 Reflective spatial light modulator...6 4 Software Functions/buttons...

More information

Examination, TEN1, in courses SK2500/SK2501, Physics of Biomedical Microscopy,

Examination, TEN1, in courses SK2500/SK2501, Physics of Biomedical Microscopy, KTH Applied Physics Examination, TEN1, in courses SK2500/SK2501, Physics of Biomedical Microscopy, 2009-06-05, 8-13, FB51 Allowed aids: Compendium Imaging Physics (handed out) Compendium Light Microscopy

More information

Ground-based optical auroral measurements

Ground-based optical auroral measurements Ground-based optical auroral measurements FYS 3610 Background Ground-based optical measurements provides a unique way to monitor spatial and temporal variation of auroral activity at high resolution up

More information

Camera Test Protocol. Introduction TABLE OF CONTENTS. Camera Test Protocol Technical Note Technical Note

Camera Test Protocol. Introduction TABLE OF CONTENTS. Camera Test Protocol Technical Note Technical Note Technical Note CMOS, EMCCD AND CCD CAMERAS FOR LIFE SCIENCES Camera Test Protocol Introduction The detector is one of the most important components of any microscope system. Accurate detector readings

More information

Mini Workshop Interferometry. ESO Vitacura, 28 January Presentation by Sébastien Morel (MIDI Instrument Scientist, Paranal Observatory)

Mini Workshop Interferometry. ESO Vitacura, 28 January Presentation by Sébastien Morel (MIDI Instrument Scientist, Paranal Observatory) Mini Workshop Interferometry ESO Vitacura, 28 January 2004 - Presentation by Sébastien Morel (MIDI Instrument Scientist, Paranal Observatory) MIDI (MID-infrared Interferometric instrument) 1st generation

More information

Supplementary Figure 1

Supplementary Figure 1 Supplementary Figure 1 Technical overview drawing of the Roadrunner goniometer. The goniometer consists of three main components: an inline sample-viewing microscope, a high-precision scanning unit for

More information

Infrared Single Shot Diagnostics for the Longitudinal. Profile of the Electron Bunches at FLASH. Disputation

Infrared Single Shot Diagnostics for the Longitudinal. Profile of the Electron Bunches at FLASH. Disputation Infrared Single Shot Diagnostics for the Longitudinal Profile of the Electron Bunches at FLASH Disputation Hossein Delsim-Hashemi Tuesday 22 July 2008 7/23/2008 2/ 35 Introduction m eb c 2 3 2 γ ω = +

More information

FIRST INDIRECT X-RAY IMAGING TESTS WITH AN 88-mm DIAMETER SINGLE CRYSTAL

FIRST INDIRECT X-RAY IMAGING TESTS WITH AN 88-mm DIAMETER SINGLE CRYSTAL FERMILAB-CONF-16-641-AD-E ACCEPTED FIRST INDIRECT X-RAY IMAGING TESTS WITH AN 88-mm DIAMETER SINGLE CRYSTAL A.H. Lumpkin 1 and A.T. Macrander 2 1 Fermi National Accelerator Laboratory, Batavia, IL 60510

More information

Photoacoustic imaging with coherent light

Photoacoustic imaging with coherent light Photoacoustic imaging with coherent light Emmanuel Bossy Institut Langevin, ESPCI ParisTech CNRS UMR 7587, INSERM U979 Workshop Inverse Problems and Imaging Institut Henri Poincaré, 12 February 2014 Background:

More information

Page 1. Ground-based optical auroral measurements. Background. CCD All-sky Camera with filterwheel. Image intensifier

Page 1. Ground-based optical auroral measurements. Background. CCD All-sky Camera with filterwheel. Image intensifier Ground-based optical auroral measurements FYS 3610 Background Ground-based optical measurements provides a unique way to monitor spatial and temporal variation of auroral activity at high resolution up

More information

Supplementary Material

Supplementary Material Supplementary Material Reactivity of 2-substituted hydrazinecarbothioamides towards tetracyanoethylene and convenient synthesis of (5-amino-2-diazenylthiazolylmethylene)malononitrile derivatives Alaa A.

More information

Simulation team in Vienna. Joao Alves, Werner Zeilinger, Rainer Köhler, Michael Mach

Simulation team in Vienna. Joao Alves, Werner Zeilinger, Rainer Köhler, Michael Mach The Simulation team in Vienna Kieran Leschinski and Oliver Czoske Joao Alves, Werner Zeilinger, Rainer Köhler, Michael Mach What is SimCADO? SimCADO is a python package which allows one to simulate mock

More information

Lecture Notes 10 Image Sensor Optics. Imaging optics. Pixel optics. Microlens

Lecture Notes 10 Image Sensor Optics. Imaging optics. Pixel optics. Microlens Lecture Notes 10 Image Sensor Optics Imaging optics Space-invariant model Space-varying model Pixel optics Transmission Vignetting Microlens EE 392B: Image Sensor Optics 10-1 Image Sensor Optics Microlens

More information

Superconducting Transition-Edge Sensors and Superconducting Tunnel Junctions for Optical/UV Time-Energy Resolved Single-Photon Counters

Superconducting Transition-Edge Sensors and Superconducting Tunnel Junctions for Optical/UV Time-Energy Resolved Single-Photon Counters Superconducting Transition-Edge Sensors and Superconducting Tunnel Junctions for Optical/UV Time-Energy Resolved Single-Photon Counters NHST Meeting STScI - Baltimore 10 April 2003 TES & STJ Detector Summary

More information

Sensitive measurement of partial coherence using a pinhole array

Sensitive measurement of partial coherence using a pinhole array 1.3 Sensitive measurement of partial coherence using a pinhole array Paul Petruck 1, Rainer Riesenberg 1, Richard Kowarschik 2 1 Institute of Photonic Technology, Albert-Einstein-Strasse 9, 07747 Jena,

More information

CrysAlis Pro : New Features in Agilent's User-Inspired X-ray Crystallography Software Platform

CrysAlis Pro : New Features in Agilent's User-Inspired X-ray Crystallography Software Platform CrysAlis Pro : New Features in Agilent's User-Inspired X-ray Crystallography Software Platform Mathias Meyer Agilent Technologies Poland Oliver Presly Agilent Technologies UK Crystallographic Software:

More information

Indiana University JEM-3200FS

Indiana University JEM-3200FS Indiana University JEM-3200FS Installation Specification Model: JEM 3200FS Serial Number: EM 15000013 Objective Lens Configuration: High Resolution Pole Piece (HRP) JEOL Engineer: Michael P. Van Etten

More information

ejs002_cm2_co ejs002_stak1_co ejs002_ofit_co ejs002_stak2_co

ejs002_cm2_co ejs002_stak1_co ejs002_ofit_co ejs002_stak2_co ejs002_cm2_co ejs002_cm3_co ejs002_cm1_co ejs002_stak1_co ejs002_ofit_co ejs002_stak2_co ejs002_t1a_co ejs002_t1b_co ejs002_t2a_co ejs002_t2b_co ejs002_v12 1 9 Feb 2004 Acta Cryst. (2003). C59,

More information

BEAM HALO OBSERVATION BY CORONAGRAPH

BEAM HALO OBSERVATION BY CORONAGRAPH BEAM HALO OBSERVATION BY CORONAGRAPH T. Mitsuhashi, KEK, TSUKUBA, Japan Abstract We have developed a coronagraph for the observation of the beam halo surrounding a beam. An opaque disk is set in the beam

More information

GBS765 Hybrid methods

GBS765 Hybrid methods GBS765 Hybrid methods Lecture 3 Contrast and image formation 10/20/14 4:37 PM The lens ray diagram Magnification M = A/a = v/u and 1/u + 1/v = 1/f where f is the focal length The lens ray diagram So we

More information

A Novel Design of a High-Resolution Hodoscope for the Hall D Tagger Based on Scintillating Fibers

A Novel Design of a High-Resolution Hodoscope for the Hall D Tagger Based on Scintillating Fibers A Novel Design of a High-Resolution Hodoscope for the Hall D Tagger Based on Scintillating Fibers APS Division of Nuclear Physics Meeting October 25, 2008 GlueX Photon Spectrum Bremsstrahlung in diamond

More information

COMPOSITE MATERIALS AND STRUCTURES TESTING BY ELECTRONIC HOLOGRAPHY

COMPOSITE MATERIALS AND STRUCTURES TESTING BY ELECTRONIC HOLOGRAPHY COMPOSITE MATERIALS AND STRUCTURES TESTING BY ELECTRONIC HOLOGRAPHY Dan N. Borza 1 1 Laboratoire de Mécanique de Rouen, Institut National des Sciences Appliquées de Rouen Place Blondel, BP 08, Mont-Saint-Aignan,

More information

Introduction to Transmission Electron Microscopy (Physical Sciences)

Introduction to Transmission Electron Microscopy (Physical Sciences) Introduction to Transmission Electron Microscopy (Physical Sciences) Centre for Advanced Microscopy Program 9:30 10:45 Lecture 1 Basics of TEM 10:45 11:00 Morning tea 11:00 12:15 Lecture 2 Diffraction

More information

2013 LMIC Imaging Workshop. Sidney L. Shaw Technical Director. - Light and the Image - Detectors - Signal and Noise

2013 LMIC Imaging Workshop. Sidney L. Shaw Technical Director. - Light and the Image - Detectors - Signal and Noise 2013 LMIC Imaging Workshop Sidney L. Shaw Technical Director - Light and the Image - Detectors - Signal and Noise The Anatomy of a Digital Image Representative Intensities Specimen: (molecular distribution)

More information

1 Diffraction of Microwaves

1 Diffraction of Microwaves 1 Diffraction of Microwaves 1.1 Purpose In this lab you will investigate the coherent scattering of electromagnetic waves from a periodic structure. The experiment is a direct analog of the Bragg diffraction

More information

Upgrade of the ultra-small-angle scattering (USAXS) beamline BW4

Upgrade of the ultra-small-angle scattering (USAXS) beamline BW4 Upgrade of the ultra-small-angle scattering (USAXS) beamline BW4 S.V. Roth, R. Döhrmann, M. Dommach, I. Kröger, T. Schubert, R. Gehrke Definition of the upgrade The wiggler beamline BW4 is dedicated to

More information

CCDS. Lesson I. Wednesday, August 29, 12

CCDS. Lesson I. Wednesday, August 29, 12 CCDS Lesson I CCD OPERATION The predecessor of the CCD was a device called the BUCKET BRIGADE DEVICE developed at the Phillips Research Labs The BBD was an analog delay line, made up of capacitors such

More information

Sensitivity Enhancement of Bimaterial MOEMS Thermal Imaging Sensor Array using 2-λ readout

Sensitivity Enhancement of Bimaterial MOEMS Thermal Imaging Sensor Array using 2-λ readout Sensitivity Enhancement of Bimaterial MOEMS Thermal Imaging Sensor Array using -λ readout O. Ferhanoğlu, H. Urey Koç University, Electrical Engineering, Istanbul-TURKEY ABSTRACT Diffraction gratings integrated

More information

Where detectors are used in science & technology

Where detectors are used in science & technology Lecture 9 Outline Role of detectors Photomultiplier tubes (photoemission) Modulation transfer function Photoconductive detector physics Detector architecture Where detectors are used in science & technology

More information

ikon-m 934 DO Series

ikon-m 934 DO Series X-Ray diffraction pattern of the Synchrotron Soleil,France. Courtesy of Vincent Jacques Low Light Imaging X-Ray Cameras Features and Benefits Open front end 1 CF152 flange and knife-edge sealing provided

More information

The new CMOS Tracking Camera used at the Zimmerwald Observatory

The new CMOS Tracking Camera used at the Zimmerwald Observatory 13-0421 The new CMOS Tracking Camera used at the Zimmerwald Observatory M. Ploner, P. Lauber, M. Prohaska, P. Schlatter, J. Utzinger, T. Schildknecht, A. Jaeggi Astronomical Institute, University of Bern,

More information

Laser stabilization and frequency modulation for trapped-ion experiments

Laser stabilization and frequency modulation for trapped-ion experiments Laser stabilization and frequency modulation for trapped-ion experiments Michael Matter Supervisor: Florian Leupold Semester project at Trapped Ion Quantum Information group July 16, 2014 Abstract A laser

More information

General principles of image processing in cryo-em

General principles of image processing in cryo-em Lecture 13 E. Orlova Birkbeck College, London General principles of image processing in cryo-em Cryo EM & 3D Image Processing 8 July 2016 Thiruvananthapuram, India William Lawrence Bragg Crystallography

More information

Attilio Andreazza INFN and Università di Milano for the ATLAS Collaboration The ATLAS Pixel Detector Efficiency Resolution Detector properties

Attilio Andreazza INFN and Università di Milano for the ATLAS Collaboration The ATLAS Pixel Detector Efficiency Resolution Detector properties 10 th International Conference on Large Scale Applications and Radiation Hardness of Semiconductor Detectors Offline calibration and performance of the ATLAS Pixel Detector Attilio Andreazza INFN and Università

More information

Development of a fast EUV movie camera for Caltech spheromak jet experiments

Development of a fast EUV movie camera for Caltech spheromak jet experiments P1.029 Development of a fast EUV movie camera for Caltech spheromak jet experiments K. B. Chai and P. M. Bellan ` California Institute of Technology kbchai@caltech.edu Caltech Spheromak gun 2 Target: study

More information

Degradation sources in the SolACES instrument and how to correct them

Degradation sources in the SolACES instrument and how to correct them Degradation sources in the SolACES instrument and how to correct them Christian Erhardt, Dr. Marcel Pfeifer, Dr. Raimund Brunner, Dr. Gerhard Schmidtke Fraunhofer IPM, Freiburg, Germany Dr. Bernd Nikutowski

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Optically reconfigurable metasurfaces and photonic devices based on phase change materials S1: Schematic diagram of the experimental setup. A Ti-Sapphire femtosecond laser (Coherent Chameleon Vision S)

More information

MICRO XRF OF LIGHT ELEMENTS USING A POLYCAPILLARY LENS AND AN ULTRA THIN WINDOW SILICON DRIFT DETECTOR INSIDE A VACUUM CHAMBER

MICRO XRF OF LIGHT ELEMENTS USING A POLYCAPILLARY LENS AND AN ULTRA THIN WINDOW SILICON DRIFT DETECTOR INSIDE A VACUUM CHAMBER Copyright JCPDS - International Centre for Diffraction Data 2005, Advances in X-ray Analysis, Volume 48. 229 MICRO XRF OF LIGHT ELEMENTS USING A POLYCAPILLARY LENS AND AN ULTRA THIN WINDOW SILICON DRIFT

More information

Standard Operating Procedure Bruker Quest Diffractometer with copper wavelength X-ray microsource

Standard Operating Procedure Bruker Quest Diffractometer with copper wavelength X-ray microsource Standard Operating Procedure Bruker Quest Diffractometer with copper wavelength X-ray microsource X-ray Crystallography Laboratory Purdue Department of Chemistry The following is a guide for collecting

More information

X-Ray diffraction pattern of the Synchrotron Soleil,France. Courtesy of Vincent Jacques. Direct Detection X-Ray Imaging. Specifications Summary

X-Ray diffraction pattern of the Synchrotron Soleil,France. Courtesy of Vincent Jacques. Direct Detection X-Ray Imaging. Specifications Summary X-Ray diffraction pattern of the Synchrotron Soleil,France. Courtesy of Vincent Jacques Low Light Imaging X-Ray Cameras Features and Benefits Open front end 1 CF152 flange and knife-edge sealing provided

More information

SONG Stellar Observations Network Group. The prototype

SONG Stellar Observations Network Group. The prototype SONG Stellar Observations Network Group The prototype F. Grundahl1, J. Christensen Dalsgaard1, U. G. Jørgensen2, H. Kjeldsen1,S. Frandsen1 and P. Kjærgaard2 1) Danish AsteroSeismology Centre, University

More information

Introduction to Electron Microscopy

Introduction to Electron Microscopy Introduction to Electron Microscopy Prof. David Muller, dm24@cornell.edu Rm 274 Clark Hall, 255-4065 Ernst Ruska and Max Knoll built the first electron microscope in 1931 (Nobel Prize to Ruska in 1986)

More information

The Hong Kong University of Science and Technology Final Year Project presentation 2007

The Hong Kong University of Science and Technology Final Year Project presentation 2007 The Hong Kong University of Science and Technology Final Year Project presentation 2007 Project supervisor: Dr. Andrew Poon Department of Electronic and Computer Engineering Wong Ka Ki Chris, ee_wkkaf,

More information

Recent Development and Study of Silicon Solid State Photomultiplier (MRS Avalanche Photodetector)

Recent Development and Study of Silicon Solid State Photomultiplier (MRS Avalanche Photodetector) Recent Development and Study of Silicon Solid State Photomultiplier (MRS Avalanche Photodetector) Valeri Saveliev University of Obninsk, Russia Vienna Conference on Instrumentation Vienna, 20 February

More information

PoS(LHCP2018)031. ATLAS Forward Proton Detector

PoS(LHCP2018)031. ATLAS Forward Proton Detector . Institut de Física d Altes Energies (IFAE) Barcelona Edifici CN UAB Campus, 08193 Bellaterra (Barcelona), Spain E-mail: cgrieco@ifae.es The purpose of the ATLAS Forward Proton (AFP) detector is to measure

More information

Application of CMOS sensors in radiation detection

Application of CMOS sensors in radiation detection Application of CMOS sensors in radiation detection S. Ashrafi Physics Faculty University of Tabriz 1 CMOS is a technology for making low power integrated circuits. CMOS Complementary Metal Oxide Semiconductor

More information

Monochromatic X-ray sources based on Table-top electron accelerators and X-ray tubes. A.P. Potylitsyn TPU, Tomsk, Russia

Monochromatic X-ray sources based on Table-top electron accelerators and X-ray tubes. A.P. Potylitsyn TPU, Tomsk, Russia Monochromatic X-ray sources based on Table-top electron accelerators and X-ray tubes A.P. Potylitsyn TPU, Tomsk, Russia The main radiation mechanisms in amorphous targets: Bremsstrahlung Transition radiation

More information

The Henryk Niewodniczański INSTITUTE OF NUCLEAR PHYSICS Polish Academy of Sciences ul. Radzikowskiego 152, Kraków, Poland.

The Henryk Niewodniczański INSTITUTE OF NUCLEAR PHYSICS Polish Academy of Sciences ul. Radzikowskiego 152, Kraków, Poland. The Henryk Niewodniczański INSTITUTE OF NUCLEAR PHYSICS Polish Academy of Sciences ul. Radzikowskiego 152, 31-342 Kraków, Poland. www.ifj.edu.pl/reports/2003.html Kraków, grudzień 2003 Report No 1931/PH

More information

Applications of Optics

Applications of Optics Nicholas J. Giordano www.cengage.com/physics/giordano Chapter 26 Applications of Optics Marilyn Akins, PhD Broome Community College Applications of Optics Many devices are based on the principles of optics

More information

Vertical Tests of ILC Cavities and Detection of X-Rays from Field Emission

Vertical Tests of ILC Cavities and Detection of X-Rays from Field Emission Vertical Tests of ILC Cavities and Detection of X-Rays from Field Emission Pardis Niknejadi California State Polytechnic University, Pomona, CA 91768 Elizabeth Olhsson University of Oregon, Eugene, OR

More information

Laser Scanning for Surface Analysis of Transparent Samples - An Experimental Feasibility Study

Laser Scanning for Surface Analysis of Transparent Samples - An Experimental Feasibility Study STR/03/044/PM Laser Scanning for Surface Analysis of Transparent Samples - An Experimental Feasibility Study E. Lea Abstract An experimental investigation of a surface analysis method has been carried

More information

Paper Synopsis. Xiaoyin Zhu Nov 5, 2012 OPTI 521

Paper Synopsis. Xiaoyin Zhu Nov 5, 2012 OPTI 521 Paper Synopsis Xiaoyin Zhu Nov 5, 2012 OPTI 521 Paper: Active Optics and Wavefront Sensing at the Upgraded 6.5-meter MMT by T. E. Pickering, S. C. West, and D. G. Fabricant Abstract: This synopsis summarized

More information

9. Microwaves. 9.1 Introduction. Safety consideration

9. Microwaves. 9.1 Introduction. Safety consideration MW 9. Microwaves 9.1 Introduction Electromagnetic waves with wavelengths of the order of 1 mm to 1 m, or equivalently, with frequencies from 0.3 GHz to 0.3 THz, are commonly known as microwaves, sometimes

More information

Spatial resolution. Spatial resolution

Spatial resolution. Spatial resolution 11/05/00 Refraction Compound refractive lenses (concave) Snigirev et al, NATURE 199 patents: Tomie 1995 x-rays: n = 1 - δ - i β < 1 www.accel.de Chromatic lenses Prod.: Lengeler @RWTH Aachen, D need of

More information

Properties of Neutron Pixel Detector based on Medipix-2 Device

Properties of Neutron Pixel Detector based on Medipix-2 Device Properties of Neutron Pixel Detector based on Medipix-2 Device Jan Jakubek, Tomas Holy, Eberhard Lehmann, Stanislav Pospisil, Josef Uher, Jiri Vacik, Daniel Vavrik Abstract - Neutron transmission radiography

More information

CALICE AHCAL overview

CALICE AHCAL overview International Workshop on the High Energy Circular Electron-Positron Collider in 2018 CALICE AHCAL overview Yong Liu (IHEP), on behalf of the CALICE collaboration Nov. 13, 2018 CALICE-AHCAL Progress, CEPC

More information

Exercise questions for Machine vision

Exercise questions for Machine vision Exercise questions for Machine vision This is a collection of exercise questions. These questions are all examination alike which means that similar questions may appear at the written exam. I ve divided

More information

Scintillation Counters

Scintillation Counters PHY311/312 Detectors for Nuclear and Particle Physics Dr. C.N. Booth Scintillation Counters Unlike many other particle detectors, which exploit the ionisation produced by the passage of a charged particle,

More information

ITk silicon strips detector test beam at DESY

ITk silicon strips detector test beam at DESY ITk silicon strips detector test beam at DESY Lucrezia Stella Bruni Nikhef Nikhef ATLAS outing 29/05/2015 L. S. Bruni - Nikhef 1 / 11 Qualification task I Participation at the ITk silicon strip test beams

More information

Track and Vertex Reconstruction on GPUs for the Mu3e Experiment

Track and Vertex Reconstruction on GPUs for the Mu3e Experiment Track and Vertex Reconstruction on GPUs for the Mu3e Experiment Dorothea vom Bruch for the Mu3e Collaboration GPU Computing in High Energy Physics, Pisa September 11th, 2014 Physikalisches Institut Heidelberg

More information

Properties of optical instruments. Projection optical systems

Properties of optical instruments. Projection optical systems Properties of optical instruments Projection optical systems Instruments : optical systems designed for a specific function Projection systems: : real image (object real or at infinity) Examples: videoprojector,,

More information

Deep- Space Optical Communication Link Requirements

Deep- Space Optical Communication Link Requirements Deep- Space Optical Communication Link Requirements Professor Chester S. Gardner Department of Electrical and Computer Engineering University of Illinois cgardner@illinois.edu Link Equation: For a free-

More information

Diamond X-ray Rocking Curve and Topograph Measurements at CHESS

Diamond X-ray Rocking Curve and Topograph Measurements at CHESS Diamond X-ray Rocking Curve and Topograph Measurements at CHESS G. Yang 1, R.T. Jones 2, F. Klein 3 1 Department of Physics and Astronomy, University of Glasgow, Glasgow, UK G12 8QQ. 2 University of Connecticut

More information

ZEISS Axiocam 503 color Your 3 Megapixel Microscope Camera for Fast Image Acquisition Fast, in True Color and Regular Field of View

ZEISS Axiocam 503 color Your 3 Megapixel Microscope Camera for Fast Image Acquisition Fast, in True Color and Regular Field of View Product Information Version 1.0 ZEISS Axiocam 503 color Your 3 Megapixel Microscope Camera for Fast Image Acquisition Fast, in True Color and Regular Field of View ZEISS Axiocam 503 color Sensor Model

More information

Photometry for Traffic Engineers...

Photometry for Traffic Engineers... Photometry for Traffic Engineers... Workshop presented at the annual meeting of the Transportation Research Board in January 2000 by Frank Schieber Heimstra Human Factors Laboratories University of South

More information