Design of the cryo sample stage for nano scanning

Slides:



Advertisements
Similar presentations
NSLS-II Soft X-ray Undulator Beamlines
Advertisements

Investigation of Proton Irradiation-Induced Creep of Ultrafine Grain Graphite Anne A. Campbell & Gary S. Was University of Michigan Research Supported.
December 10, 2008 TJRParticle Refrigerator1 The Particle Refrigerator Tom Roberts Muons, Inc. A promising approach to using frictional cooling for reducing.
D ESIGN C ONSIDERATIONS FOR THE ESRF U PGRADE P ROGRAM E XPERIMENTAL H ALL EX2 S LAB David Martin David Martin ESRF Alignment and GEodesy1.
The Use of Small Coolers for Hydrogen and Helium Liquefaction
05/20/ High-Current Polarized Source Developments Evgeni Tsentalovich MIT.
Diffraction Enhanced Imaging at the UK Synchrotron Radiation Source M.Ibison, K.C.Cheung, K.Siu, C.J.Hall, R.A.Lewis, A. Hufton, S.J.Wilkinson, K.D.Rogers,
Purity measurement at SOLEIL Nicolas HUBERT # on behalf of the diagnostics group: N. Hubert, L. Cassinari, F. Dohou, M. El Ajjouri, M. Labat, D. Pédeau,
A Serializer ASIC for High Speed Data Transmission in Cryogenic and HiRel Environment Tiankuan Liu On behalf of the ATLAS Liquid Argon Calorimeter Group.
18/7/2002Ivan Hruska EP/ATE1 LV brick for TILECAL  How to power the electronics of TILECAL ? Power supply as close as possible to electronics ?  Positives.
Effective lens aperture Deff
DDDs, Screening micrographs and CTF (Practical work) Vahid Abrishami.
Understanding typical users for this instrument Graduate studentGraduate student –not an X-ray expert but wants to make a spatially resolved measurement;
SCU Segmented Cryostat Concept M. Leitner, S. Prestemon, D. Arbelaez, S. Myers September 2 nd, 2014.
Nanonics CryoView 2000™ CryoView 2000™ Product Presentation.
Peter J. LaPuma1 © 1998 BRUKER AXS, Inc. All Rights Reserved This is powder diffraction!
SAXS/WAXS Conversion for Beamline Engineering Review.
“hands-off” Screening with TOPAZ Chips For the purposes of testing both crystallization behavior and capability of the “tray goniometer”, chips were built.
SEM Scanning Electron Microscope
S. Claudet - 31st May 2007Power refrigeration for LHC Power refrigeration at 4.5K & 1.8K for the LHC S. Claudet, CERN AT-ACR.
Alba, 13 December 2012Detectors at BL22 – CLÆSS 1 of 8 Detectors at BL 22 - CLÆSS.
High Intensity Polarized Electron Gun Studies at MIT-Bates 10/01/2008 PESP Evgeni Tsentalovich MIT.
1 BROOKHAVEN SCIENCE ASSOCIATES A Wiggler Beamline for XAS at NSLS-II Paul Northrup NSLS-II Project and Environmental Sciences Department Brookhaven National.
MONALISA Update David Urner ATF2 Meeting Dec
Cryogenic Summary - K. C. Wu Testing D2L102 in MAGCOOLJune, 02 Difference between D2L102 and D2L101 Operating Summary Cooldown to 100 K and 6 K Test Condition.
Date 2007/Sept./12-14 EDR kick-off-meeting Global Design Effort 1 Cryomodule Interface definition N. Ohuchi.
SPL cryomodule specification meeting, CERN 19th October 2010 SPL cryomodule specification: Goals of the meeting SPL cryomodule specification: Goals of.
Studies on 2.45 GHz microwave ion sources Abhishek Nag IISER, KOLKATA Presented By: G.O. Rodrigues IUAC, New Delhi Supervised By:
Present status of production target and Room design Takashi Hashimoto, IBS/RISP 2015, February.
CW Cryomodules for Project X Yuriy Orlov, Tom Nicol, and Tom Peterson Cryomodules for Project X, 14 June 2013Page 1.
1/20 LHCb upgrade, Jeroen van Tilburg Nikhef Jamboree, 14 Dec 2015 Preparing for the LHCb upgrade.
ESS | Non-Invasive Beam Profile Measurements| | C. Böhme Non-Invasive Beam Profile Measurement Overview of evaluated methods.
METHODOLOGY Nanotechnology Prof. Dr. Abdul Majid Department of Physics
Yb:YAG Regenerative Amplifier for A1 Ground Laser Hut Rui Zhang ACCL Division V, RF-Gun Group Nov 20, 2015 SuperKEKB Injector Laser RF Gun Review.
LCLS-II Technical Requirements
Polarization Dependence in X-ray Spectroscopy and Scattering
David Urner Oxford University/JAI
Improving & combining the spatiale & temporal resolution
Microprobe activities in Lund
Using a digital micromirror device for high-precision laser-based manufacturing on the microscale Please use the dd month yyyy format for the date for.
Re-entrant BPM R&D for ILC Main Linac
Instrumentation for Accelerators Technologies for the HL-LHC
Mentored by Brian Schuster and Jonathan Ligda
MeV Ion Microbeams and Radiation Biology at the University of Surrey
Electron Microscope Dr. Laxmi Kant Pandey.
RECONSTRUCTED CELL STRUCTURE Jakob Andreasson
Lesson Overview 7.1 Life is Cellular.
Lesson Overview 7.1 Life is Cellular.
Operation experience of cryogenic system and cryomodules for the superconducting linear accelerator at IUAC, New Delhi. T S Datta ( On behalf of Cryogenics.
Lesson Overview 7.1 Life is Cellular.
Design of an integrated liquid flow cell for correlative microscopy
Scanning Probe Microscope
Automation from a user perspective
Lesson Overview 7.1 Life is Cellular.
Do it with electrons !.
Lesson Overview 7.1 Life is Cellular.
Volume 110, Issue 4, Pages (February 2016)
Lesson Overview 7.1 Life is Cellular.
Lesson Overview 7.1 Life is Cellular Objectives:
Cryomodules Challenges for PERLE
Types of Microscopy Type Probe Technique Best Resolution Penetration
Volume 110, Issue 4, Pages (February 2016)
Atomic Force Microscope
Lesson Overview 7.1 Life is Cellular.
Present Status of Orbit Stabilization at SPring-8
Coherent X-ray Imaging Instrument WBS 1.3
Lesson Overview 7.1 Life is Cellular.
Lesson Overview 7.1 Life is Cellular.
T. Mitsuhashi, John Flanagan G. Mitsuka
Presentation transcript:

Design of the cryo sample stage for nano scanning overview Introduction Design of the cryo sample stage for nano scanning Cooldown test results Beamline test results Future development: sample changer Conclusion Bonus development: 3D printed pinhole support Martin Rosenthal, ID13 l USM 2019 Tutorial1: sample preservation l 04/02/2019 l PSCM - Peter van der Linden

Nano scanning capabilities: most often a complete endstation Introduction We want to investigate material properties at the nano scale: architecture, distribution of atomic species, crystal structure Nano scanning capabilities: most often a complete endstation Bionanoprobe @APS, Kotobuki-1@Spring-8, ID16A @ESRF Biological samples: Data acquisition is limited by radiation damage Cryoprotection is necessary With higher beam intensity  fast detection to outrun the radiation damage + added advantage to scan faster than the temperature drift l USM 2019 Tutorial1: sample preservation l 04/02/2019 l PSCM - Peter van der Linden

Partnership University of Göttingen / PSCM Example Partnership University of Göttingen / PSCM Jan‐David Nicolas - Scanning x‐ray diffraction and coherent imaging of soft biological samples Oral presentation Wednesday microsymposium UDM2 X‐ray microscopy in biology: recent applications, challenges and opportunities Scanning SAXS at cryogenic temperatures. Left: optical micrograph of the fluorescently-labeled actin network (Phalloidin-Alexa488) of an induced pluripotent stem cell-derived cardiomyocyte. The corresponding darkfield-contrast SAXS map is shown on the right. Although the sample chamber configuration was not optimized for SAXS recordings, the cell nuclei could still be imaged. l USM 2019 Tutorial1: sample preservation l 04/02/2019 l PSCM - Peter van der Linden

Nano scanning chamber design XY Scanner: Piezo PI-733, range 100 um, resolution 5nm Sample cooling by LN2 + braids Sample support for SiN membranes Modular construction: input window/piezo support, Cryo unit, output window, connector box 200x200x100mm 14kg  Huber 17cm l USM 2019 Tutorial1: sample preservation l 04/02/2019 l PSCM - Peter van der Linden

Cooldown testing Cooldown time ~1 hour Temperature drops  pressure drops a decade Shields and piezo drop a few degrees in temperature l USM 2019 Tutorial1: sample preservation l 04/02/2019 l PSCM - Peter van der Linden

Cooldown testing Position drift 10’s of microns during cooldown BUT drift stops when cold l USM 2019 Tutorial1: sample preservation l 04/02/2019 l PSCM - Peter van der Linden

PARAMETERS AND DATA FROM 1ST XRAY TEST Operating Temperature reached < 90 K Operating Pressure reached < 10-6 mbar pumping continuously Maximum piezo scan range for optical alignment: 100 x 100 mm Typical scan size for x-ray experiments: 10x10 and 2x2 mm X-ray beam size used: 100 x 300 nm (V x H) Sample movements look at least as precise as with other devices Sample change 8-12 hours including vacuum pumping WAXS pattern from Al2O3 grains Total intensity map of Kevlar fiber l USM 2019 Tutorial1: sample preservation l 04/02/2019 l PSCM - Peter van der Linden

Radiation damage Successive scans of a hair l USM 2019 Tutorial1: sample preservation l 04/02/2019 l PSCM - Peter van der Linden

Sample changer BUDGET DEMAND 2019 Cryogenic sample transfer: Sample holder copy of ID32 Changer has two sample positions for the old and new sample Magnetic manipulator On board LN2 for autonomy 50cm / 4kg 25mm / 10g Load new sample in docking station Close and pump vacuum Place sample in parking position Connect to chamber Pump intermediate space Remove old sample + park Pick new sample from parking Place new sample Remove sample changer l USM 2019 Tutorial1: sample preservation l 04/02/2019 l PSCM - Peter van der Linden

Chamber for ID16 Piezo scan chamber for ID16: Design is done, chamber not built Needs another sample support, braids and window cap Beam in and out through front window Sample support reversed Front window for fluorescence Rear window for transmission Changeover in < 1 day Sample changer to fit the two l USM 2019 Tutorial1: sample preservation l 04/02/2019 l PSCM - Peter van der Linden

conclusions The concept works: nano scale movements, cryoprotection Small improvements: piezo cabling, input window, … It needs the sample changer for efficient operation Suitable for other beamlines Acknowledgements: ID13: Lionel Lardière, Martin Rosenthal, Manfred Burghammer Göttingen: Jan-David Nicolas, Tim Salditt PSCM: Manon Chesneau, Pierre Lloria, Diego Pontoni l USM 2019 Tutorial1: sample preservation l 04/02/2019 l PSCM - Peter van der Linden