CCP4 Workshop Chicago 2011 Data Integration with XDS

Size: px
Start display at page:

Download "CCP4 Workshop Chicago 2011 Data Integration with XDS"

Transcription

1 CCP4 Workshop Chicago 2011 Data Integration with XDS Dept. of Structural Chemistry, University of Göttingen June CCP4 Chicago 2011: XDS 1/29

2 The XDS Distribution XDS is an integration program for monochromatic X-ray data originally written by W. Kabsch now co-authored by K. Diederichs availability: XDS main program suite xds-viewer viewer for control images (.cbf-files) Wiki and auxiliary programs maintained by Kay Diederichs XDSi (GUI) pkursula/xdsi.html CCP4 Chicago 2011: XDS 2/29

3 XDS Characteristics Some of the special features of XDS: 3-dimensional spot integration Correction for Radiation Damage Optimised for new Pilatus Detector Command-line program Parallelised: Fast! Simple to read documentation CCP4 Chicago 2011: XDS 3/29

4 Learning Curve Why newbies often do not like XDS: 1. No GUI, only command line 2. error messages may initially appear cryptic 3. users must read (rather than look at graphics) Once understood, the program flow is simple and very easy to set up Understanding XDS gets you better data quality (also with other integration programs) CCP4 Chicago 2011: XDS 4/29

5 Documentation XDS and accompanying programs come with very clean (html-) documentation. Every step of the program and every keyword is described, and reading is not interrupted by many cross-links. Documentation contains both technical information for those who want to understand how XDS works in details as well as user information that help setting up the integration process. CCP4 Chicago 2011: XDS 5/29

6 Other Sources of Information Wiki Tips, tricks, tutorials,... CCP4bb Sign up at CCP4 Chicago 2011: XDS 6/29

7 Templates Templates of input scripts for all supported detector formats Only very few adjustments necessary to get started Beamlines often generate appropriate input scripts generate XDS.INP from XDSwiki for MARCCD, ADSC, and TODO CCP4 Chicago 2011: XDS 7/29

8 XDS.INP XDS is controlled by one single input file: XDS.INP. Name cannot be changed Each data set must be run in separate directory to avoid overwriting of files. Contains about 100 Keywords a of the form KEYWORD=VALUE Only about 10 Keywords must be modified for most data sets (e.g. distance, number of images, etc.) Most important one: image names, detector JOB= XYCORR INIT COLSPOT IDXREF DEFPIX XPLAN INTEGRATE CORRECT Each name stands for one of the steps XDS carries out during data integration. (XPLAN is optional and corresponds to the BEST [2] or STRATEGY [1] output to report optimal data collection range(s)) a also called cards for historical reasons CCP4 Chicago 2011: XDS 8/29

9 The Steps XYINIT writes files for positional corrections of the detector plane. Most modern detectors provide already corrected images so that these to files are normally flat. INIT determines initial detector background IDXREF indexing: unit cell dimensions and crystal orientation DEFPIX set active dectector area (exclude resolution cut-off, beam stop shadow,... ) (XPLAN, optional) generate strategy table with data completeness depending on starting angle total scan width INTEGRATE determine reflection intensities CORRECT applies corrections (polarisation, Lorentz-correction,... ), scales reflections, reports data statistics CCP4 Chicago 2011: XDS 9/29

10 Program Flow Each step must be passed at least once - the subsequent steps depend on files produced by the previous steps. Each step creates a log-file (XYINIT.LP, INIT.LP,...). IDXREF is the main hurdle - once unit cell and crystal orientation are determined, integration usually runs smoothly. CORRECT summarises the quality of the data. Mostly IDXREF.LP and CORRECT.LP should be inspected. CCP4 Chicago 2011: XDS 10/29

11 Step Dependencies Step XYCORR (Important) output files INIT COLSPOT IDXREF DEFPIX SPOT.XDS XPARM.XDS FRAME.cbf SPOT.XDS BKGPIX.cbf ABS.cbf red: Text files with parameters or data cyan: control images (use xds-viewer) black: data files for further processing INTEGRATE INTEGRATE.HKL FRAME.cbf CORRECT XDS_ASCII.HKL GXPARM.XDS CCP4 Chicago 2011: XDS 11/29

12 SPOT.XDS written by COLSPOT: Detector coordinates and Intensity of strong spots to be used for indexing: X(pixel) Y(pixel) #image counts amended by Miller-Indices IDXREF after determination of unit cell and crystal orientation X(pixel) Y(pixel) #image counts H K L < : cannot index within tolerance (MAXIMUM_ERROR_OF_SPOT_POSITION) CCP4 Chicago 2011: XDS 12/29

13 !!! ERROR!!! SOLUTION IS INACCURATE Correct indexing is crucial for data integration. If XDS cannot index more than 70 % of all reflections listed in SPOT.XDS, it stops with the above error message. Most common reasons: 1. Wrong ORGX, ORGY 2. Poor data quality XDS has a very robust indexing method and depending on the situation, one can usually continue integration by one or a combination of the following means. CCP4 Chicago 2011: XDS 13/29

14 Wrong ORGX, ORGY The detector origin ORGX, ORGY in XDS.INP is provided in pixels. Typically it is in the centre of the detector, so a good start is ORGX=NX/2, ORGY=NY/2, i.e. half the detector dimensions. Illustration of the sensitivity to ORGX, ORGY Diffraction image from Thaumatin with a medium size cell 58 Å, 58 Å, 150 Å, 90, 90, 90. Coordinates of the four magnified spots: Coordinates Difference Difference(mm) An offset of the origin of about 0.5 mm means a shift of 1 in Miller-Indices, mis-indexing. CCP4 Chicago 2011: XDS 14/29

15 Complaints about ORGX, ORGY A good indicator of a wrongly set origin: 1. refined detector distance far from real value 2. ORGX, ORGY drift far away from initial value IDXREF.LP: ***** DIFFRACTION PARAMETERS USED AT START OF INTEGRATION ***** [...] DETECTOR ORIGIN (PIXELS) AT (XDS.INP: ) CRYSTAL TO DETECTOR DISTANCE (mm) (XDS.INP: 200) The detector distance reported during data collection (image header) should be correct within fractions of mm at a proper beamline and not drift by 11 mm. CCP4 Chicago 2011: XDS 15/29

16 1. Start with ORGX=NX/2, ORGY=NY/2 (use adxv [3] to read out header information). Often XDS refines these values reasonably well. Correcting ORGX, ORGY CCP4 Chicago 2011: XDS 16/29

17 2. Check the image for the beam centre. At θ = 0 this correpsonds well to ORGX, ORGY. Ice rings are particularly usefule, they are centred at about the beam centre (use circle fitting option in mosflm). Correcting ORGX, ORGY CCP4 Chicago 2011: XDS 17/29

18 Carry on regardless The XDS error message SOLUTION IS INACCURATE does not necessarily mean that something is seriously wrong. XDS is rather careful. The step IDXREF still refines the experimental parameters and writes them into XPARM.XDS. This is all we need to continue. Check IDXREF.LP for Number of indexed reflections ***** INDEXING OF OBSERVED SPOTS IN SPACE GROUP # 1 ***** 1909 OUT OF 2506 SPOTS INDEXED. 0 REJECTED REFLECTIONS (REASON: OVERLAP) 597 REJECTED REFLECTIONS (REASON: TOO FAR FROM IDEAL POSITION) with 30 % of indexed reflections the parameters in XPARM.XDS are probably good enough to converged to the correct values during INTEGRATE and CORRECT. refined detector distance and detector origin do not shift too much Set JOB = DEFPIX INTEGRATE CORRECT and integrate your data. If something did seriously go wrong, the file XPARM.XDS was not written. CCP4 Chicago 2011: XDS 18/29

19 DEFPIX: active detector mask DEFPIX sets the area of the detector which is taken into account during integration. It takes into account: 1. INCLUDE_RESOLUTION_RANGE default: 20 Å to detector edge. 2. VALUE_RANGE_FOR_TRUSTED_DETECTOR_PIXELS exclude shadowed regions, e.g. beamstop, cryo stream nozzle 3. UNTRUSTED_RECTANGLE exclude gaps of CCD chips e.g. Pilatus detector 4. EXCLUDE_RESOLUTION_RANGE exclude ice rings from data integration CCP4 Chicago 2011: XDS 19/29

20 VALUE RANGE FOR TRUSTED DETECTOR PIXELS ABS.cbf BKGPIX.cbf, all included VALUE RANGE FOR TRUSTED DETECTOR PIXELS= CCP4 Chicago 2011: XDS 20/29

21 VALUE RANGE FOR TRUSTED DETECTOR PIXELS ABS.cbf BKGPIX.cbf, shadows removed VALUE RANGE FOR TRUSTED DETECTOR PIXELS= CCP4 Chicago 2011: XDS 21/29

22 INTEGRATE and CORRECT: Intensity determination and fine tuning INTEGRATE determine spot intensities based on parameters (saved in XPARM.XDS) CORRECT experimental corrections (e.g. Lorentz- and Polarisation-correction), refine parameters and determine space group (saved to GXPARM.XDS) CORRECT write FRAME.cbf: predicted spot positions encircled check correctness of predictions CCP4 Chicago 2011: XDS 22/29

23 Recycling Parameters (in GXPARM.XDS) depend on measured intensities Intensities (including corrections) depend on Parameters rename GXPARM.XDS to XPARM.XDS and rerun XDS (JOB = DEFPIX INTEGRATE CORRECT) to improve results. This way one should also set the correct high- and low- resolution cut-offs CCP4 Chicago 2011: XDS 23/29

24 Resolution Cut-Off The default resolution range in XDS is 20 Å to the detector edge INCLUDE_RESOLUTION_RANGE= Medium to low resolution data: increase 20 Å to 30 Å or even 50 Å (check BKGPIX.cbf) After second round of integration: determine high-resolution cut-off. My favourite: xprep - higher number of resolution shells than e.g. listed in CORRECT.LP Why after second round? Correct space group rather than P 1 more symmetry related reflections more reliable data statistics, especially I/σ I CCP4 Chicago 2011: XDS 24/29

25 High Resolution Cut-Off Resolution #Data #Theory %Complete Redundancy Mean I Mean I/s Rmerge Rsigma Inf <----- I/sigma > <----- I/sigma < Inf CCP4 Chicago 2011: XDS 25/29

26 Low Resolution Cut-Off BKGPIX.cbf BKGPIX.cbf Default resolution range (20 Å - edge) - includes noise at edge - loose low resolution reflections Adjusted resolution range (40 Å Å) - I/σ I 2 in outer shell - low resolution reflection important for shape of molecule (MR, refinement) CCP4 Chicago 2011: XDS 26/29

27 Generating XDS.INP Download detector specific template and fill in manually. Advantage: Double-check of experimental settings do never solely rely on correctness of image headers! Many beamlines offer automatic generation of XDS.INP. Crucial: Beamline specific chip borders and list of dead pixels for Pilatus detectors. Script generate XDS.INP by Kay Diederichs XDS.INP Works with MAR-CCD, ADSC, and Pilatus 6M detectors Number of images Reads all information from image header BKGPIX.cbf from Pilatus detector: Chip borders and dead pixels excluded. CCP4 Chicago 2011: XDS 27/29

28 XDSSTAT The program XDSSTAT (Kay Diederichs, also from the XDS Wiki) creates more detailed statistics from XDS integration. The output can be viewed with a file browser - similar tables like scala output. General rule of thumb: developers like encouragment if you miss a feature point it out to the program author to increase the chance of the feature being incorporated (One of the most efficient examples : Paul Emsley & Bernd Lohkamp (Coot), Pavel Afonine (phenix)). CCP4 Chicago 2011: XDS 28/29

29 References 1. Leslie, A.G.W., Recent changes to the MOSFLM package for processing film and image plate data, Joint CCP4 + ESF-EAMCB Newsletter on Protein Crystallography (1992), No A.N. Popov and Bourenkov, Choice of data-collection parameters based on statistic modeling Acta Crystallogr. (2003). D59, Andrew Arvai, arvai/adxv.html CCP4 Chicago 2011: XDS 29/29

Nature Protocols: doi: /nprot

Nature Protocols: doi: /nprot Supplementary Tutorial A total of nine examples illustrating different aspects of data processing referred to in the text are given here. Images for these examples can be downloaded from www.mrc- lmb.cam.ac.uk/harry/imosflm/examples.

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

Processing data collected with Pilatus/Eiger detectors. James Parkhurst IUCR Computing School, Bangalore, August 2017

Processing data collected with Pilatus/Eiger detectors. James Parkhurst IUCR Computing School, Bangalore, August 2017 Processing data collected with Pilatus/Eiger detectors James Parkhurst IUCR Computing School, Bangalore, August 2017 Introduction Overview of Pilatus/Eiger detectors Overview of the DIALS integration program

More information

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

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

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

Focus on an optical blind spot A closer look at lenses and the basics of CCTV optical performances,

Focus on an optical blind spot A closer look at lenses and the basics of CCTV optical performances, Focus on an optical blind spot A closer look at lenses and the basics of CCTV optical performances, by David Elberbaum M any security/cctv installers and dealers wish to know more about lens basics, lens

More information

DATA COLLECTION WITH R-AXIS II, AN X-RAY DETECTING SYSTEM USING IMAGING PLATE

DATA COLLECTION WITH R-AXIS II, AN X-RAY DETECTING SYSTEM USING IMAGING PLATE THE RIGAKU JOURNAL VOL. 7 / NO. 2 / 1990 Technical Note DIFFRACTION DATA COLLECTION WITH R-AXIS II, AN X-RAY DETECTING SYSTEM USING IMAGING PLATE ATSUSHI SHIBATA R&D Division, Rigaku Corporation 1. Introduction

More information

research papers Protein crystallography with a novel large-area pixel detector 550 doi: /s J. Appl. Cryst. (2006).

research papers Protein crystallography with a novel large-area pixel detector 550 doi: /s J. Appl. Cryst. (2006). Journal of Applied Crystallography ISSN 0021-8898 Received 4 October 2005 Accepted 5 May 2006 Protein crystallography with a novel large-area pixel detector Gregor Hülsen,* 2 Christian Broennimann, Eric

More information

Instructions XRD. 1 Choose your setup , Sami Suihkonen. General issues

Instructions XRD. 1 Choose your setup , Sami Suihkonen. General issues Instructions XRD 28.10.2016, Sami Suihkonen General issues Be very gentle when closing the doors Always use Cu attenuator when count rate exceeds 500 000 c/s Do not over tighten optical modules or attach

More information

Agilent SuperNova and PX Scanner Systems COMPACT, HIGH-PERFORMANCE SOLUTIONS FOR STRUCTURAL BIOLOGY

Agilent SuperNova and PX Scanner Systems COMPACT, HIGH-PERFORMANCE SOLUTIONS FOR STRUCTURAL BIOLOGY Agilent SuperNova and PX Scanner Systems COMPACT, HIGH-PERFORMANCE SOLUTIONS FOR STRUCTURAL BIOLOGY AGILENT SUPERNOVA AND PX SCANNER SYSTEMS COMPACT, HIGH-PERFORMANCE SOLUTIONS FOR STRUCTURAL BIOLOGY Fully-integrated

More information

LYNXEYE XE-T. < 380 ev. Innovation with Integrity. Energy. Resolution. High-Resolution Position Sensitive Detector with Superb Energy Resolution XRD

LYNXEYE XE-T. < 380 ev. Innovation with Integrity. Energy. Resolution. High-Resolution Position Sensitive Detector with Superb Energy Resolution XRD Energy < 380 ev Resolution High-Resolution Position Sensitive Detector with Superb Energy Resolution The is the next generation "Compound Silicon Strip" detector with superb energy resolution for ultrafast

More information

PANalytical X pert Pro Gazing Incidence X-ray Reflectivity User Manual (Version: )

PANalytical X pert Pro Gazing Incidence X-ray Reflectivity User Manual (Version: ) University of Minnesota College of Science and Engineering Characterization Facility PANalytical X pert Pro Gazing Incidence X-ray Reflectivity User Manual (Version: 2012.10.17) The following instructions

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 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

metal-organic compounds

metal-organic compounds metal-organic compounds Acta Crystallographica Section E Structure Reports Online ISSN 1600-5368 Monoclinic, C2=c a = 14.519 (3) Å b = 14.303 (3) Å c = 12.461 (3) Å = 101.94 (3) V = 2531.6 (9) Å 3 Z =4

More information

X-RAY OPTICS FOR TWO-DIMENSIONAL DIFFRACTION

X-RAY OPTICS FOR TWO-DIMENSIONAL DIFFRACTION Copyright (c)jcpds-international Centre for Diffraction Data 2002, Advances in X-ray Analysis, Volume 45. 332 ABSTRACT X-RAY OPTICS FOR TWO-DIMENSIONAL DIFFRACTION Bob B. He and Uwe Preckwinkel Bruker

More information

Stitching MetroPro Application

Stitching MetroPro Application OMP-0375F Stitching MetroPro Application Stitch.app This booklet is a quick reference; it assumes that you are familiar with MetroPro and the instrument. Information on MetroPro is provided in Getting

More information

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS. GUI Simulation Diffraction: Focused Beams and Resolution for a lens system

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS. GUI Simulation Diffraction: Focused Beams and Resolution for a lens system DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS GUI Simulation Diffraction: Focused Beams and Resolution for a lens system Ian Cooper School of Physics University of Sydney ian.cooper@sydney.edu.au DOWNLOAD

More information

Data Quality Monitoring of the CMS Pixel Detector

Data Quality Monitoring of the CMS Pixel Detector Data Quality Monitoring of the CMS Pixel Detector 1 * Purdue University Department of Physics, 525 Northwestern Ave, West Lafayette, IN 47906 USA E-mail: petra.merkel@cern.ch We present the CMS Pixel Data

More information

PixInsight Workflow. Revision 1.2 March 2017

PixInsight Workflow. Revision 1.2 March 2017 Revision 1.2 March 2017 Contents 1... 1 1.1 Calibration Workflow... 2 1.2 Create Master Calibration Frames... 3 1.2.1 Create Master Dark & Bias... 3 1.2.2 Create Master Flat... 5 1.3 Calibration... 8

More information

Preparing your artwork for clear Zipper Pulls using Illustrator

Preparing your artwork for clear Zipper Pulls using Illustrator Preparing your artwork for clear Zipper Pulls using Illustrator This tutorial contains everything you need to know about creating your own, printed clear acrylic zipper pulls. Including how to format your

More information

Experiment 1: Fraunhofer Diffraction of Light by a Single Slit

Experiment 1: Fraunhofer Diffraction of Light by a Single Slit Experiment 1: Fraunhofer Diffraction of Light by a Single Slit Purpose 1. To understand the theory of Fraunhofer diffraction of light at a single slit and at a circular aperture; 2. To learn how to measure

More information

Studies on MCM D interconnections

Studies on MCM D interconnections Studies on MCM D interconnections Speaker: Peter Gerlach Department of Physics Bergische Universität Wuppertal D-42097 Wuppertal, GERMANY Authors: K.H.Becks, T.Flick, P.Gerlach, C.Grah, P.Mättig Department

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

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

Creo Parametric 4.0 Basic Design

Creo Parametric 4.0 Basic Design Creo Parametric 4.0 Basic Design Contents Table of Contents Introduction...1 Objective of This Textbook...1 Textbook Outline...2 Textbook Conventions...3 Exercise Files...3 System Configuration...4 Notes

More information

PANalytical X pert Pro High Resolution Specular and Rocking Curve Scans User Manual (Version: )

PANalytical X pert Pro High Resolution Specular and Rocking Curve Scans User Manual (Version: ) University of Minnesota College of Science and Engineering Characterization Facility PANalytical X pert Pro High Resolution Specular and Rocking Curve Scans User Manual (Version: 2012.10.17) The following

More information

Small Angle Scattering Platform for Structural Biology

Small Angle Scattering Platform for Structural Biology Small Angle Scattering Platform for Structural Biology Petra Pernot, ESRF OUTLINE: SAXS/SANS in Grenoble: new SAS platform of CISB Conversion of ID14-EH3 from MX to bio-saxs MAXINF2 Integration Workshop

More information

Supplementary Information

Supplementary Information Supplementary Information Supplementary Figure 1. Modal simulation and frequency response of a high- frequency (75- khz) MEMS. a, Modal frequency of the device was simulated using Coventorware and shows

More information

Agilent Xcalibur and Gemini X-ray Diffractometers ENHANCED CHEMICAL CRYSTALLOGRAPHY SOLUTIONS

Agilent Xcalibur and Gemini X-ray Diffractometers ENHANCED CHEMICAL CRYSTALLOGRAPHY SOLUTIONS Agilent Xcalibur and Gemini X-ray Diffractometers ENHANCED CHEMICAL CRYSTALLOGRAPHY SOLUTIONS AGILENT XCALIBUR AND GEMINI X-RAY DIFFRACTOMETERS ENHANCED CHEMICAL CRYSTALLOGRAPHY SOLUTIONS Agilent s Xcalibur

More information

PSI with the Swiss Light Source SLS. Christian Broennimann. Paul Scherrer Institut 5232 Villigen PSI

PSI with the Swiss Light Source SLS. Christian Broennimann. Paul Scherrer Institut 5232 Villigen PSI Solid State Detector Development at the Swiss Light Source Christian Brönnimann Group Leader SLS Detector Group Paul Scherrer Institut CH-5232 Villigen-PSI, Switzerland PSI with the Swiss Light Source

More information

Experiment #12 X-Ray Diffraction Laboratory

Experiment #12 X-Ray Diffraction Laboratory Physics 360/460 Experiment #12 X-Ray Diffraction Laboratory Introduction: To determine crystal lattice spacings, as well as identify unknown substances, a x-ray diffractometer is used to replace the traditional

More information

Monoclinic, P2 1 =c a = (3) Å b = (3) Å c = (15) Å = (3) V = (5) Å 3. Data collection.

Monoclinic, P2 1 =c a = (3) Å b = (3) Å c = (15) Å = (3) V = (5) Å 3. Data collection. organic compounds Acta Crystallographica Section E Structure Reports Online ISSN 1600-5368 Tectorigenin monohydrate: an isoflavone from Belamcanda chinensis Benguo Liu, a * Yuxiang Ma, b Han Gao a and

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

Bruker D8 HRXRD. Collecting Reciprocal Space Maps using the LynxEye Position Sensitive Detector

Bruker D8 HRXRD. Collecting Reciprocal Space Maps using the LynxEye Position Sensitive Detector Bruker D8 HRXRD Collecting Reciprocal Space Maps using the LynxEye Position Sensitive Detector Scott A Speakman, Ph.D. MIT Center for Materials Science and Engineering For help in the X-ray Lab, contact

More information

Autodesk Inventor 2016

Autodesk Inventor 2016 Parametric Modeling with Autodesk Inventor 2016 Randy H. Shih SDC PUBLICATIONS Better Textbooks. Lower Prices. www.sdcpublications.com Powered by TCPDF (www.tcpdf.org) Visit the following websites to learn

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

Contents Foreword 1 Feedback 2 Legal information 3 Getting started 4 Installing the correct Capture One version 4 Changing the version type 5 Getting

Contents Foreword 1 Feedback 2 Legal information 3 Getting started 4 Installing the correct Capture One version 4 Changing the version type 5 Getting Contents Foreword 1 Feedback 2 Legal information 3 Getting started 4 Installing the correct Capture One version 4 Changing the version type 5 Getting to know Capture One Pro 6 The Grand Overview 6 The

More information

Phase plates for cryo-em

Phase plates for cryo-em Max Planck Institute of Biochemistry Martinsried, Germany MAX PLANCK SOCIETY Phase plates for cryo-em Rado Danev Max Planck Institute of Biochemistry, Martinsried, Germany. EMBO course 2017, London, UK

More information

FEI Falcon Direct Electron Detector. Best Practice Document

FEI Falcon Direct Electron Detector. Best Practice Document FEI Falcon Direct Electron Detector Best Practice Document 2 1. Introduction FEI Falcon Direct Electron Detector Best Practice Application Guide The FEI Falcon Detector is based on direct electron detection

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

LYNXEYE XE. Innovation with Integrity. High-Resolution Energy-Dispersive Detector for 0D, 1D, and 2D Diffraction XRD

LYNXEYE XE. Innovation with Integrity. High-Resolution Energy-Dispersive Detector for 0D, 1D, and 2D Diffraction XRD High-Resolution Energy-Dispersive Detector for 0D, 1D, and 2D Diffraction The is the first energy dispersive 0D, 1D, and 2D detector operating at room temperature for ultra fast X-ray diffraction measurements.

More information

Structural Biology. Single crystal X-ray diffraction and SAXS. Systems designed for structural biology

Structural Biology. Single crystal X-ray diffraction and SAXS. Systems designed for structural biology Structural Biology Single crystal X-ray diffraction and SAXS Systems designed for structural biology Rigaku Oxford Diffraction THE POWER OF SYNERGY Combining the single crystal groups from Rigaku and Oxford

More information

Philip Sperling. Sales Science and New Materials, YXLON International GmbH, Essener Bogen 15, Hamburg, Germany.

Philip Sperling. Sales Science and New Materials, YXLON International GmbH, Essener Bogen 15, Hamburg, Germany. A new generation of x-ray computed tomography devices for quality inspection and metrology inspection in the field of additive manufacturing and other sciences Philip Sperling Sales Science and New Materials,

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

Processing of Bruker & Nonius CCD data

Processing of Bruker & Nonius CCD data Processing of Bruker & Nonius CCD data Louis J. Farrugia, Department of Chemistry University of Glasgow GLASGOW G12 8QQ Scotland Processing of Bruker & Nonius CCD data There are two main stages of CCD

More information

Pixel Detector for the Protein Crystallography Beamline at the SLS

Pixel Detector for the Protein Crystallography Beamline at the SLS Pixel Detector for the Protein Crystallography Beamline at the SLS PSI Ch. Brönnimann 1, E. Eikenberry 1, S. Kohout 1, B. Schmitt 1, C. Schulze 1, R. Baur 2 and R.Horisberger 2 1 Swiss Light Source, Paul

More information

Study on Imaging Quality of Water Ball Lens

Study on Imaging Quality of Water Ball Lens 2017 2nd International Conference on Mechatronics and Information Technology (ICMIT 2017) Study on Imaging Quality of Water Ball Lens Haiyan Yang1,a,*, Xiaopan Li 1,b, 1,c Hao Kong, 1,d Guangyang Xu and1,eyan

More information

HRMA Ghost Image Properties

HRMA Ghost Image Properties 20.1. Ghost Images Geometry 07 Jul 1999 in progress Chapter 20 HRMA Ghost Image Properties Terrance J. Gaetz 20.1 Ghost Images Geometry Ghost images occur when photons reach the focal plane after missing

More information

Computer Generated Holograms for Optical Testing

Computer Generated Holograms for Optical Testing Computer Generated Holograms for Optical Testing Dr. Jim Burge Associate Professor Optical Sciences and Astronomy University of Arizona jburge@optics.arizona.edu 520-621-8182 Computer Generated Holograms

More information

Chapter 28 Physical Optics: Interference and Diffraction

Chapter 28 Physical Optics: Interference and Diffraction Chapter 28 Physical Optics: Interference and Diffraction 1 Overview of Chapter 28 Superposition and Interference Young s Two-Slit Experiment Interference in Reflected Waves Diffraction Resolution Diffraction

More information

research papers The ner things in X-ray diffraction data collection 1718 P ugrath X-ray diffraction data collection Acta Cryst. (1999).

research papers The ner things in X-ray diffraction data collection 1718 P ugrath X-ray diffraction data collection Acta Cryst. (1999). Acta Crystallographica Section D Biological Crystallography ISSN 0907-4449 The ner things in X-ray diffraction data collection J. W. P ugrath Molecular Structure Corporation, 9009 New Trails Drive, The

More information

STEM Spectrum Imaging Tutorial

STEM Spectrum Imaging Tutorial STEM Spectrum Imaging Tutorial Gatan, Inc. 5933 Coronado Lane, Pleasanton, CA 94588 Tel: (925) 463-0200 Fax: (925) 463-0204 April 2001 Contents 1 Introduction 1.1 What is Spectrum Imaging? 2 Hardware 3

More information

Light. Path of Light. Looking at things. Depth and Distance. Getting light to imager. CS559 Lecture 2 Lights, Cameras, Eyes

Light. Path of Light. Looking at things. Depth and Distance. Getting light to imager. CS559 Lecture 2 Lights, Cameras, Eyes CS559 Lecture 2 Lights, Cameras, Eyes These are course notes (not used as slides) Written by Mike Gleicher, Sept. 2005 Adjusted after class stuff we didn t get to removed / mistakes fixed Light Electromagnetic

More information

Optical design of a high resolution vision lens

Optical design of a high resolution vision lens Optical design of a high resolution vision lens Paul Claassen, optical designer, paul.claassen@sioux.eu Marnix Tas, optical specialist, marnix.tas@sioux.eu Prof L.Beckmann, l.beckmann@hccnet.nl Summary:

More information

Production of HPDs for the LHCb RICH Detectors

Production of HPDs for the LHCb RICH Detectors Production of HPDs for the LHCb RICH Detectors LHCb RICH Detectors Hybrid Photon Detector Production Photo Detector Test Facilities Test Results Conclusions IEEE Nuclear Science Symposium Wyndham, 24 th

More information

FLAT FIELDS FOR FILTER WHEEL OFFSET POSITIONS

FLAT FIELDS FOR FILTER WHEEL OFFSET POSITIONS FLAT FIELDS FOR FILTER WHEEL OFFSET POSITIONS R. C. Bohlin, T. Wheeler, and J. Mack October 29, 2003 ABSTRACT The ACS filter wheel movements are accurate to one motor step, which leads to errors that exceed

More information

Experience of synchrotron sources and optics modelling at Diamond Light Source

Experience of synchrotron sources and optics modelling at Diamond Light Source Experience of synchrotron sources and optics modelling at Diamond Light Source Lucia Alianelli Outline Microfocus MX beamline optics design (Principal Beamline Scientist G. Evans) Surface and interface

More information

Multiwire Real-Time Back-Reflection Laue Diffractometer

Multiwire Real-Time Back-Reflection Laue Diffractometer Standard Operating Procedure for the Multiwire Real-Time Back-Reflection Laue Diffractometer Scott A Speakman, Ph.D Center for Materials Science and Engineering at MIT Speakman@mit.edu 617-253-6887 http://prism.mit.edu/xray

More information

5.0 NEXT-GENERATION INSTRUMENT CONCEPTS

5.0 NEXT-GENERATION INSTRUMENT CONCEPTS 5.0 NEXT-GENERATION INSTRUMENT CONCEPTS Studies of the potential next-generation earth radiation budget instrument, PERSEPHONE, as described in Chapter 2.0, require the use of a radiative model of the

More information

Use of Back Scattered Ionizing Radiation for Measurement of Thickness of the Catalytic Agent Active Material

Use of Back Scattered Ionizing Radiation for Measurement of Thickness of the Catalytic Agent Active Material 18th World Conference on Nondestructive Testing, 16- April 1, Durban, South Africa Use of Back Scattered Ionizing Radiation for Measurement of Thickness of the Catalytic Agent Active Material Boris V.

More information

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS RAYLEIGH-SOMMERFELD DIFFRACTION INTEGRAL OF THE FIRST KIND CIRCULAR APERTURES

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS RAYLEIGH-SOMMERFELD DIFFRACTION INTEGRAL OF THE FIRST KIND CIRCULAR APERTURES DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS RAYLEIGH-SOMMERFELD DIFFRACTION INTEGRAL OF THE FIRST KIND CIRCULAR APERTURES Ian Cooper School of Physics, University of Sydney ian.cooper@sydney.edu.au

More information

Physics 1C. Lecture 24A. Finish Chapter 27: X-ray diffraction Start Chapter 24: EM waves. Average Quiz score = 6.8 out of 10.

Physics 1C. Lecture 24A. Finish Chapter 27: X-ray diffraction Start Chapter 24: EM waves. Average Quiz score = 6.8 out of 10. Physics 1C Lecture 24A Finish Chapter 27: X-ray diffraction Start Chapter 24: EM waves Average Quiz score = 6.8 out of 10 This is a B- Diffraction of X-rays by Crystals! X-rays are electromagnetic radiation

More information

KODAK DIGITAL ROC Professional Plug-In 2.1

KODAK DIGITAL ROC Professional Plug-In 2.1 KODAK DIGITAL ROC Professional Plug-In 2.1 Installing Kodak's DIGITAL ROC Professional Plug-In If you have not downloaded and installed DIGITAL ROC Professional, go to: http://www.asf.com/download/ Download

More information

NSERC Summer Project 1 Helping Improve Digital Camera Sensors With Prof. Glenn Chapman (ENSC)

NSERC Summer Project 1 Helping Improve Digital Camera Sensors With Prof. Glenn Chapman (ENSC) NSERC Summer 2016 Digital Camera Sensors & Micro-optic Fabrication ASB 8831, phone 778-782-319 or 778-782-3814, Fax 778-782-4951, email glennc@cs.sfu.ca http://www.ensc.sfu.ca/people/faculty/chapman/ Interested

More information

Physics 1C Lecture 27B

Physics 1C Lecture 27B Physics 1C Lecture 27B Single Slit Interference! Example! Light of wavelength 750nm passes through a slit 1.00μm wide. How wide is the central maximum in centimeters, in a Fraunhofer diffraction pattern

More information

Imaging Optics Fundamentals

Imaging Optics Fundamentals Imaging Optics Fundamentals Gregory Hollows Director, Machine Vision Solutions Edmund Optics Why Are We Here? Topics for Discussion Fundamental Parameters of your system Field of View Working Distance

More information

Using the R-Axis Spider to run thin films

Using the R-Axis Spider to run thin films Using the R-Axis Spider to run thin films In addition to loose powder samples, it is possible to run thin film samples on the R-Axis Spider. Use the zero background plate holder for your thin film sample.

More information

The HOIS recommended practice for in-service computed radiography of pipes. Dr Stephen F Burch, WCNDT 2012, Durban, SA. April 2012

The HOIS recommended practice for in-service computed radiography of pipes. Dr Stephen F Burch, WCNDT 2012, Durban, SA. April 2012 The HOIS recommended practice for in-service computed radiography of pipes WCNDT 2012, Durban, SA. April 2012 Dr Stephen F Burch, ESR Technology, Oxfordshire,UK steve.burch@esrtechnology.com ESR Technology

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

Creo Parametric 2.0: Introduction to Solid Modeling. Creo Parametric 2.0: Introduction to Solid Modeling

Creo Parametric 2.0: Introduction to Solid Modeling. Creo Parametric 2.0: Introduction to Solid Modeling Creo Parametric 2.0: Introduction to Solid Modeling 1 2 Part 1 Class Files... xiii Chapter 1 Introduction to Creo Parametric... 1-1 1.1 Solid Modeling... 1-4 1.2 Creo Parametric Fundamentals... 1-6 Feature-Based...

More information

Low-energy Electron Diffractive Imaging for Three dimensional Light-element Materials

Low-energy Electron Diffractive Imaging for Three dimensional Light-element Materials Low-energy Electron Diffractive Imaging for Three dimensional Light-element Materials Hitachi Review Vol. 61 (2012), No. 6 269 Osamu Kamimura, Ph. D. Takashi Dobashi OVERVIEW: Hitachi has been developing

More information

5-Chloro-2-(thiophen-2-yl)-1-(thiophen-2-ylmethyl)-1H- benzimidazole 6-Chloro-2-(thiophen-2-yl)-1-(thiophen-2- ylmethyl)-1h-benzimidazole (0.94/0.

5-Chloro-2-(thiophen-2-yl)-1-(thiophen-2-ylmethyl)-1H- benzimidazole 6-Chloro-2-(thiophen-2-yl)-1-(thiophen-2- ylmethyl)-1h-benzimidazole (0.94/0. Acta Crystallographica Section E Structure Reports Online ISSN 1600-5368 5-Chloro-2-(thiophen-2-yl)-1-(thiophen-2-ylmethyl)-1H- benzimidazole 6-Chloro-2-(thiophen-2-yl)-1-(thiophen-2- ylmethyl)-1h-benzimidazole

More information

Optical Components for Laser Applications. Günter Toesko - Laserseminar BLZ im Dezember

Optical Components for Laser Applications. Günter Toesko - Laserseminar BLZ im Dezember Günter Toesko - Laserseminar BLZ im Dezember 2009 1 Aberrations An optical aberration is a distortion in the image formed by an optical system compared to the original. It can arise for a number of reasons

More information

Instruction Manual for HyperScan Spectrometer

Instruction Manual for HyperScan Spectrometer August 2006 Version 1.1 Table of Contents Section Page 1 Hardware... 1 2 Mounting Procedure... 2 3 CCD Alignment... 6 4 Software... 7 5 Wiring Diagram... 19 1 HARDWARE While it is not necessary to have

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

Dynamic beam shaping with programmable diffractive optics

Dynamic beam shaping with programmable diffractive optics Dynamic beam shaping with programmable diffractive optics Bosanta R. Boruah Dept. of Physics, GU Page 1 Outline of the talk Introduction Holography Programmable diffractive optics Laser scanning confocal

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

More Info at Open Access Database by S. Dutta and T. Schmidt

More Info at Open Access Database  by S. Dutta and T. Schmidt More Info at Open Access Database www.ndt.net/?id=17657 New concept for higher Robot position accuracy during thermography measurement to be implemented with the existing prototype automated thermography

More information

Tolerancing in Zemax. Lecture 4

Tolerancing in Zemax. Lecture 4 Tolerancing in Zemax Lecture 4 Objectives: Lecture 4 At the end of this lecture you should: 1. Understand the reason for tolerancing and its relation to typical manufacturing errors 2. Be able to perform

More information

CCP4 Study Weekend What s new in CCP4? Ville Uski, CCP4 Research Complex at Harwell

CCP4 Study Weekend What s new in CCP4? Ville Uski, CCP4 Research Complex at Harwell CCP4 Study Weekend 2017 What s new in CCP4? Ville Uski, CCP4 Research Complex at Harwell What s new in CCP4 Ville Uski (CCP4, Research Complex at Harwell) MoRDa pipeline for molecular replacement Andrey

More information

Brightness and Contrast Control Reference Guide

Brightness and Contrast Control Reference Guide innovation Series Scanners Brightness and Contrast Control Reference Guide A-61506 Part No. 9E3722 CAT No. 137 0337 Using the Brightness and Contrast Control This Reference Guide provides information and

More information

Introduction: Why electrons?

Introduction: Why electrons? Introduction: Why electrons? 1 Radiations Visible light X-rays Electrons Neutrons Advantages Not very damaging Easily focused Eye wonderful detector Small wavelength (Angstroms) Good penetration Small

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

Image analysis. CS/CME/BioE/Biophys/BMI 279 Oct. 31 and Nov. 2, 2017 Ron Dror

Image analysis. CS/CME/BioE/Biophys/BMI 279 Oct. 31 and Nov. 2, 2017 Ron Dror Image analysis CS/CME/BioE/Biophys/BMI 279 Oct. 31 and Nov. 2, 2017 Ron Dror 1 Outline Images in molecular and cellular biology Reducing image noise Mean and Gaussian filters Frequency domain interpretation

More information

Serial crystallography on in vivo grown microcrystals using synchrotron radiation

Serial crystallography on in vivo grown microcrystals using synchrotron radiation Supporting information IUCrJ Volume 1 (2014) Supporting information for article: Serial crystallography on in vivo grown microcrystals using synchrotron radiation Cornelius Gati, Gleb Bourenkov, Marco

More information

metal-organic compounds

metal-organic compounds metal-organic compounds Acta Crystallographica Section E Structure Reports Online ISSN 1600-5368 Monoclinic, P2 1 =n a = 11.6887 (5) Å b = 16.8061 (9) Å c = 11.7888 (5) Å = 103.757 (4) V = 2249.38 (18)

More information

Scodix1200 OPA System OPA - Optical Print Alignment. Daniel Schott Application Specialist

Scodix1200 OPA System OPA - Optical Print Alignment. Daniel Schott Application Specialist Scodix1200 OPA System OPA - Optical Print Alignment Daniel Schott Application Specialist September2011 What is OPA? The Optical Print Alignment (OPA) feature enables the Scodix1200 press to optically align

More information

Commissioning Results of The Protein Microcrystallography Beamline TPS 05A

Commissioning Results of The Protein Microcrystallography Beamline TPS 05A Science Advisory Committee Meeting Commissioning Results of The Protein Microcrystallography Beamline TPS 05A Construction Team Leader: Yuch-Cheng Jean 2016.09.21 0 Outline I. Beamline Introduction II.

More information

Procedures for Performing Cryoelectron Microscopy on the FEI Sphera Microscope

Procedures for Performing Cryoelectron Microscopy on the FEI Sphera Microscope Procedures for Performing Cryoelectron Microscopy on the FEI Sphera Microscope The procedures given below were written specifically for the FEI Tecnai G 2 Sphera microscope. Modifications will need to

More information

LowDose for JEOL. --Software LowDose and Advanced Data Acquisition. Version 1.1

LowDose for JEOL. --Software LowDose and Advanced Data Acquisition. Version 1.1 LowDose for JEOL --Software LowDose and Advanced Data Acquisition Version 1.1 1. Introduction This is the LowDose software for the user of JEOL electron microscopes. The LowDose software is a Plug-In for

More information

Processing EM Data using the SIMPLE GUI

Processing EM Data using the SIMPLE GUI Processing EM Data using the SIMPLE GUI Things you will need to know before launching the GUI: [where a name is given in bold_italics this denotes a simple keyword that could be used to set the parameter

More information

Detectors for single-crystal area detector diffractometers

Detectors for single-crystal area detector diffractometers Detectors for single-crystal area detector diffractometers Mathias Meyer X-ray Group Software Manager RIGAKU OXFORD DIFFRACTION Rigaku, founded in 1951, are well respected for the high performance and

More information

Guidance on Using Scanning Software: Part 5. Epson Scan

Guidance on Using Scanning Software: Part 5. Epson Scan Guidance on Using Scanning Software: Part 5. Epson Scan Version of 4/29/2012 Epson Scan comes with Epson scanners and has simple manual adjustments, but requires vigilance to control the default settings

More information

CrystalPro is a computer-controlled microscope with top quality optics.

CrystalPro is a computer-controlled microscope with top quality optics. CrystalPro is a computer-controlled microscope with top quality optics. CrystalPro has been optimised for visualising protein crystallography experiments. Its proprietary illumination system utilises both

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

research papers First results from a macromolecular crystallography system with a polycapillary collimating optic and a microfocus X-ray generator

research papers First results from a macromolecular crystallography system with a polycapillary collimating optic and a microfocus X-ray generator Journal of Applied Crystallography ISSN 0021-8898 First results from a macromolecular crystallography system with a polycapillary collimating optic and a microfocus X-ray generator Received 7 September

More information

metal-organic compounds

metal-organic compounds metal-organic compounds Acta Crystallographica Section E Structure Reports Online ISSN 1600-5368 Bis[l-1,2-bis(1H-imidazol-1-ylmethyl)- benzene-j 2 N 3 :N 30 ]disilver(i) bis(4- amino-2,5-dichlorobenzenesulfonate)

More information

Case Study: Custom CCD for X-ray Free Electron Laser Experiment

Case Study: Custom CCD for X-ray Free Electron Laser Experiment Introduction The first XFEL (X-ray Free Electron Laser) experiments are being constructed around the world. These facilities produce femto-second long bursts of the most intense coherent X-rays ever to

More information