Software fayre: raw data hkl file



Similar documents
Quick Guide for Data Collection on the NIU Bruker Smart CCD

Introduction to X-Ray Powder Diffraction Data Analysis

Diffraction of a Circular Aperture

X-Ray Diffraction HOW IT WORKS WHAT IT CAN AND WHAT IT CANNOT TELL US. Hanno zur Loye

Powder diffraction and synchrotron radiation

Processing Data with rsmap3d Software Services Group Advanced Photon Source Argonne National Laboratory

X-ray Powder Diffraction Pattern Indexing for Pharmaceutical Applications

This is an author-deposited version published in: Handle ID:.

Phasing & Substructure Solution

CT for the production floor: Recent developments in Hard- and Software for industrial CT Systems

Diffraction Course Series 2015

X-ray thin-film measurement techniques

FTIR Instrumentation

Introduction to Powder X-Ray Diffraction History Basic Principles

Absolute Structure Absolute Configuration

LIST OF CONTENTS CHAPTER CONTENT PAGE DECLARATION DEDICATION ACKNOWLEDGEMENTS ABSTRACT ABSTRAK

Laue lens for Nuclear Medicine

BIG data big problems big opportunities Rudolf Dimper Head of Technical Infrastructure Division ESRF

Microscopy and Nanoindentation. Combining Orientation Imaging. to investigate localized. deformation behaviour. Felix Reinauer

Trimble Realworks Software

CALIBRATION AND ANALYSIS OF HELIOSTATS

Hunting Ghosts. For the development of imaging optical STRAY LIGHT ANALYSIS IN IMAGING OPTICS

Lecture Notes, CEng 477

Analysis Programs DPDAK and DAWN

ON-LINE MONITORING OF AN HADRON BEAM FOR RADIOTHERAPEUTIC TREATMENTS

Scan Time Reduction and X-ray Scatter Rejection in Dual Modality Breast Tomosynthesis. Tushita Patel 4/2/13

Fundamentals of Cone-Beam CT Imaging

Chapter 3 SYSTEM SCANNING HARDWARE OVERVIEW

Quality Estimation for Scalable Video Codec. Presented by Ann Ukhanova (DTU Fotonik, Denmark) Kashaf Mazhar (KTH, Sweden)

Phase determination methods in macromolecular X- ray Crystallography

Polarization Dependence in X-ray Spectroscopy and Scattering. S P Collins et al Diamond Light Source UK

High Resolution Planetary Imaging Workflow

From Pixel to Info-Cloud News at Leica Geosystems JACIE Denver, 31 March 2011 Ruedi Wagner Hexagon Geosystems, Geospatial Solutions Division.

Chapter 8. Low energy ion scattering study of Fe 4 N on Cu(100)

Application Note #503 Comparing 3D Optical Microscopy Techniques for Metrology Applications

Spectroscopy Using the Tracker Video Analysis Program

Rb 82 Cardiac PET Scanning Protocols and Dosimetry. Deborah Tout Nuclear Medicine Department Central Manchester University Hospitals

High Resolution Spatial Electroluminescence Imaging of Photovoltaic Modules

AURA - Analysis Utility for Room Acoustics Merging EASE for sound reinforcement systems and CAESAR for room acoustics

Crystalline perfection of an aluminium single crystal determined by neutron diffraction

Color holographic 3D display unit with aperture field division

ZEISS Axiocam 506 color Your Microscope Camera for Imaging of Large Sample Areas Fast, in True Color, and High Resolution

Purchasing a cardiac CT scanner: What the radiologist needs to know

1 One Dimensional Horizontal Motion Position vs. time Velocity vs. time

Quick Start Users Guide for Bruker SMART APEX II Diffractometer

Micro-CT for SEM Non-destructive Measurement and Volume Visualization of Specimens Internal Microstructure in SEM Micro-CT Innovation with Integrity

" {h k l } lop x odl. ORxOS. (2) Determine the interplanar angle between these two planes:

X-ray Diffraction and EBSD

Electron density is complex!

Fig.1. The DAWN spacecraft

Structure Factors

LASER ENGRAVING REFLECTIVE METALS TO CREATE SCANNER READABLE BARCODES Paper P516

technical notes trimble realworks software

Synthetic Sensing: Proximity / Distance Sensors

Study of the Human Eye Working Principle: An impressive high angular resolution system with simple array detectors

IN-LINE PARTICLE SIZE MEASUREMENTS FOR CEMENT AND OTHER ABRASIVE PROCESS ENVIRONMENTS

Measuring large areas by white light interferometry at the nanopositioning and nanomeasuring machine (NPMM)

Page: 1 of 6 Page: 1 of 6

GE Medical Systems Training in Partnership. Module 8: IQ: Acquisition Time

We bring quality to light. MAS 40 Mini-Array Spectrometer. light measurement

Introduction to the EXAFS data analysis

Realization of a UV fisheye hyperspectral camera

Extraction Heights for STIS Echelle Spectra

Intrusion Log Sharing University of Wisconsin-Madison

Extreme-AO for GMT. Center for Astronomical Adaptive Optics, University of Arizona Subaru Telescope, National Astronomical Observatory of Japan

Resolution Enhancement of Photogrammetric Digital Images

DICOM Correction Item

Multi-Channel Radiochromic Film Dosimetry. Adapted from A.Micke Spain, April 2014

EXPERIMENT 11 UV/VIS Spectroscopy and Spectrophotometry: Spectrophotometric Analysis of Potassium Permanganate Solutions.

WAVELENGTH OF LIGHT - DIFFRACTION GRATING

Basics of X-ray diffraction: From symmetry to structure determination

X-ray diffraction techniques for thin films

R/F. Efforts to Reduce Exposure Dose in Chest Tomosynthesis Targeting Lung Cancer Screening. 3. Utility of Chest Tomosynthesis. 1.

Data-analysis scheme and infrastructure at the X-ray free electron laser facility, SACLA

Comparative crystal structure determination of griseofulvin: Powder X-ray diffraction versus single-crystal X-ray diffraction

Architectural Photogrammetry Lab., College of Architecture, University of Valladolid - jgarciaf@mtu.edu b

To determine vertical angular frequency, we need to express vertical viewing angle in terms of and. 2tan. (degree). (1 pt)

Light Control and Efficacy using Light Guides and Diffusers

Planetary Imaging Workshop Larry Owens

Classical direct methods


Introduction to CCDs and CCD Data Calibration

Rapid structure determination of disordered materials: study of GeSe 2 glass

Simplifying Opto- Mechanical Product Development: How a new product reduces cost, stress, and time to market

Functional neuroimaging. Imaging brain function in real time (not just the structure of the brain).

Handbook on the Ultrasonic Examination. Austenitic Welds

Designing a Schematic and Layout in PCB Artist

PDF Created with deskpdf PDF Writer - Trial ::

Physics testing of image detectors

Information about the T9 beam line and experimental facilities

The Waves Dorrough Meter Collection. User Guide

Robot Perception Continued

Introduction to Fourier Transform Infrared Spectrometry

Transcription:

Software fayre: raw data hkl file malvaro@vt.edu Matteo Alvaro www.crystal.vt.edu This work was supported by: NSF grant - Earth Sciences Division EAR-0738692 Department of Geosciences, Virginia Tech. College of Science, Virginia Tech. Topics Software fayre: going from raw data to hkl file Experimental and data processing challenges PD Vs. CCD Choice of the right software Quick overview of the software available Practical session Area detectors (CCD) Point detectors (PD) Oxford diffraction (Diego Gatta) Bruker (Tonci Balic-Zunic ) STOE (Andrzej Grzechnik, Karen Friese) XDS (Andrzej Grzechnik, Karen Friese) WinIntegrstp (Ross Angel)

Practical sessions SOFTWARE FOR AREA DETECTOR Oxford diffraction (Diego & Fabrizio) Bruker (Tonci) STOE (Karen & Andrzej) XDS (Karen & Andrzej) SOFTWARE FOR POINT DETECTOR WinIntegrstp (Ross) Intensity data collection Crystallographic basis Data Collection Data Collection Data integration Crystallographic basis Data integration CCD is shoot first and ask questions later R.J. Angel

Intensities at high pressure: Challenges Very precise data to measure very small changes in structures at high pressures. Absorption by DAC s components Conventional DAC with Beryllium seats, Rings steel gasket Diffracted intensities reduced Scattering by DAC s components Highly structured background Double diffraction Limited access 1/3 or less than the entire dataset Limited equivalent reflections Rejection of aberrant intensities Low signal Marburg-type DAC with Highly rhenium structure gasketbackground 350um Intensities at high pressure: Solutions Point detector Experimental Accurate peak positions (offset) Multiple scans Higher collimation Slits settings Detector distance Data processing Optimized scan speed Optimized integration algorithms (Step scans) Profile fitting Recovery of weak data Area detector Experimental Poor peak positions (no offset) Beryllium cone (post integr. corr) Exposure time/generator power Detector distance Data processing Masking solutions (global, local) Multiple indexing (diamonds, Qz) Overlap checking Every reflection profile in a data set must be visually examined by the 350um experimentalist (open to human misjudgement and errors!!)

Integration: Area detectors Area detector Data processing Masking solutions Global, local Static, dynamic Multiple indexing Diamonds, Qz Overlap checking 3D indexing algorithm 350um Integration: Point detector Diamond Reflection overlap Double-diffraction Weak data M=measured at the minimum speed R=Rejected R= Fails at the test of the intensity ratio 1=first attempt Point detector Data processing Diamond reflections Double-diffraction Optimized scan speed Optimized integration algorithms (Step scans) Profile fitting Recovery of weak data 2D indexing algorithm 350um

What to know: CCD and point detectors Point detector Pros Better/lower background Better handling of the refls Recovery weak data Avoid bad reflections Reflections Offsets Optimised scan speed Optimized integration algorithms (Step scans Higher collimation (small cells) Cons Long data collections UB matrix determination Long Not allowed by all the software Possible misindexing Area detector Pros Quick Peak hunting Fast intensity data collection Large number of reflections High Redundancy High background Diffuse scattering Approx equal intensities Equal scan speed Static images No handling of the refls No refls offsets Black box CCD and point detectors: Practical example Structure refinements data Bond distance values Good agreement between DAC- PD and CCD in air Almost in agreement DAC-PD DAC-CCD Bond distance esd s Always higher value on CCD Agreement betweend CCD in air and PD in DAC Data obtained on the same instrument with two different detectors

Commercial software available XDS http://xds.mpimf-heidelberg.mpg.de/html_doc/downloading.html http://www.stoe.com/pages/products/software_single.html http://www.oxford-diffraction.com/products/software-crysalis-pro/ http://www.bruker-axs.de/dataintegration.html CCD XDS software Exchange capabilities Support many detector format Pilatus, Marr555, Marr345, marccd, R-AXIS II, R-AXIS IV, R- AXIS IV++, RAXIS-V, SATURN 92, CRYSALIS, STOE, SIMENS HKL conversion to different format Indexing optimization Learned reflection profile Spatial correction at each pixel of a detector Centering the diffraction peaks Refine orientation matrix (UB) Defines the obscured regions of the detector Post integration feature Wolfgang Kabsch, author of the 100 000th publication on Crystallography Journals Online.

CCD XDS software Pro Free of charge High compatible with several instruments (home labs and large scale facilities) High level useful high pressure features No reciprocal space reconstruction No incommensurate phases Not so much interactive (black box) CCD STOE software Exchange capabilities Support many detector format Stoe IPDS II, Stoe IPDS 2T, IPDS 2T dual beam, Pilatus, HKL conversion to different format Indexing optimization Overlap Check Masking (beam stop, Be ring and diamond peaks) Multi orientation matrix feature, up to 6 matrices (twins, diamond overlap etc..) Refine orientation matrix (UB) Defines the obscured regions of the detector (each frames has it own mask) Incommensurate structures Reciprocal space reconstruction Post integration feature

CCD STOE software Pro Free of charge High level useful high pressure features Reciprocal space reconstruction Quite much interactive (allowed a lot of user intervention) Not Highly compatible with several instruments Hand made masking of the shadowed areas of the detector Use of the mask to optimize the integration profile CCD Oxford Diffraction software Exchange capabilities Support many detector format Marr555, Marr345, marccd, HKL conversion to different format Indexing optimization Centering the diffraction peaks Refine orientation matrix (UB) Defines the obscured regions of the detector Masking (beam stop and Be ring) Multiple cells handling (twins, diamonds etc ) Post integration feature

CCD Oxford Diffraction software Pro Free of charge Compatible with different instruments (home labs and large scale facilities) High level useful high pressure features No feature for the masking of a single reflection (e.g. Diamond peaks) Not extremely interactive CCD Bruker software (SaintPlus) Exchange capabilities Support many detector format Marr555, Marr345, marccd, Pilatus coming soon (other detector formats via conversion software) HKL conversion to different format Indexing optimization Hand picking of the reflections Centering the diffraction peaks Refine orientation matrix (UB) Multiple cells handling Masking areas of the detector Post integration feature

CCD Bruker software (SaintPlus) Pro Comes with the instrument ($$$) Compatible with many instrument (Thanks to the conversion software) Hand picking of the reflections Tricky handling of the unit cell parameters and multiple cells Difficult handling of the overlapping (diamond peaks) Not so much interactive (black box) Very recommended OLD versions of the software!!! PD WinIntegrSTP software Exchange capabilities Support many point detector format Xcalibur, Xscans, STOE, Philips Febo, CAD4, old version Single HKL (shelx or Rfine formats) Indexing optimization Step scans integration Visual examination of the refls Centering the diffraction peaks Refine orientation matrix (UB) Different background refinements choice Post integration feature No post integration features Need other softwares Angel R.J. (2003) J. Appl. Cryst. 36, 295 300

PD WinIntegrSTP software Pro Free of charge High compatible with several instruments (home labs and large scale facilities) Mainly designed for High pressure data integration Continuously developed Flexible!! Please ask to Ross.