Repeatability Test of Attocube Piezo Stages

Slides:



Advertisements
Similar presentations
Measuring Instruments
Advertisements

RHESSI/GOES Xray Analysis using Multitemeprature plus Power law Spectra. J.McTiernan (SSL/UCB)
RHESSI/GOES Xray Analysis using Multitemeprature plus Power law Spectra. J.McTiernan (SSL/UCB) ABSTRACT: We present spectral fits for RHESSI and GOES solar.
Prepared using support of U.S. Department of Energy under Contract No. DE-AC02-76SF00515 by the Stanford Linear Accelerator Center, Stanford, California.
Conceptual Cost Estimating
Journal Question: In the science classes you have taken throughout your life, do you accept what you are taught to be true/fact? Why or why not? Explain.
Light Gates –To Collect Data Not Connected To Computer 1.Press enter to select timing 2.Press or to select Set Timing Mode 3.Press Enter 4.Press or to.
P. Skopintsev1,2,3, A. Singer1, J. Bach4, L. Müller1, B. Beyersdorff2, S. Schleitzer1, O. Gorobtsov1, A. Shabalin1, R.P. Kurta1, D. Dzhigaev1,5, O.M. Yefanov1,
Alignment Tools Used To Locate A Wire And A Laser Beam In The VISA Undulator Project Wire Finder CALIBRATION A special fixture was constructed to calibrate.
Science Fair Information.
MESH Crystal Injectors
The Electromagnetic Spectrum High Harmonic Generation
Mathematical Derivation of Probability
Jonathan Donkers1, Lin Zhang1+
Measuring the Thickness of Cryosheet Jets
Madhu Karra1, Jason Koglin1,2
Sentiment Analysis and Data visualization Techniques of Experiments
Image Processing For Soft X-Ray Self-Seeding
Structure and Function: Ubiquitination of NEMO and Optineurin
Characterizing Optics with White-Light Interferometry
Matter in Extreme Conditions at LCLS:
Kevin Shimbo1, Matt Hayes+
X-Ray Shielding Introduction Application Research Conclusions
Crystallography images
Hutch 4 (XCS) Laser System
Anomaly Detection LCLS data: Introduction Research Conclusion
MAKING WAY FOR LCLS II HERRIOTT CELL IGNIS THE NEED FOR LCLS-II
A remote EPICS monitoring tool
EASE: Alert Management
Designing and Prototyping Optics Table and Shelves
Managing Diffraction Beam
Integration of Blu-Ice into
Effects of Wrapping Vacuum
Scintillation Material Encapsulation Fixture
LCLS CXI Sample Chambers and Engineering Solutions
Values to Normalize Data
Designing a molecular probe for detection
LAMP Vacuum System Documentation
G6PD Complex Structural Study Crystallization Setup
Your Name, Elias Catalano, Robert Sublett, Robin Curtis
Determining a Detector’s Saturation Threshold
HXRSD Helium Enclosure
Crystallography Labeling Using Machine Learning
IT Inventory and Optimization
Structural study of soluble ammonia monooxygenase
Creation and development of a PRP database
IT Inventory and Optimization
Electro Optic Sampling of Ultrashort Mid-IR/THz Pulses
Margaret Koulikova1, William Colocho+
Analytical Solutions for Heat Distribution in KB Mirror Systems
Analytical Solutions for Temperature
Barron Montgomery1,2, Christopher O’Grady2, Chuck Yoon2, Mark Hunter2+
Elizabeth Van Campen, Barrack Obama2, Stephen Curry1,2, Steve Kerr2+
Advanced Methods of Klystron Phasing
Ryan Dudschus, Alex Wallace, Zachary Lentz
Jennifer Hoover1, William Colocho2
X-Ray Spectrometry Using Cauchois Geometry For Temperature Diagnostics
Robert Pushor, Catherine LeCocq, Brian Fuss, Georg Gassner
Redesigning of The SED Calendars
Automatic compression control for the LCLS injector laser
Russell Edmonds1, Matt Hayes2+ 1LCLS Summer Research Intern
Prototype and Design of High-Speed X-Ray Chopper
Title of Your Poster Introduction Research Conclusions Acknowledgments
Reconstruction algorithms Challenges & Future work
Welcome to the Stanford Synchrotron Radiation Laboratory (SSRL) at the Stanford Linear Accelerator Center (SLAC) * 2575 Sand Hill Road, Menlo Park, CA.
Emergency Information
Electrical components and systems
DYNAMIC APERTURE OF JLEIC ELECTRON COLLIDER
GridLAB-D Workshop: Tariff Design Study
Presentation transcript:

Repeatability Test of Attocube Piezo Stages Onaopemipo Alagbe1, Hongliang Shi1, Drew Barada1+ 1Linac Coherent Light Source, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA. +Contact: abarada@slac.stanford.edu Introduction The stability of the Autocollimator itself was also examined to account for any noise in the readings for repeatability. This was done by recording the values gotten from the autocollimator while a fixed mirror was placed in front of it. The testing procedure used is shown below: The stage controller was turned on. In preparation for the installation and assembly of the X-Ray Split and Delay system it was necessary to carry out some tests on components of the system. The Attocube piezo stages are one such component. These stages provide high resolution positioning using an optoelectronic encoder. There are three types of these stages to be used in the system: Goniometers, Linear Stages and Vertical Positioning Stages. The purpose of the tests are to determine the repeatability of the stages, and to ensure they adhere to specifications. The stage controller was turned off. The stage was homed. The stage was moved to 200μ° The stage was moved to the zero position. 5X Fig 5: Setup used for fixed stability test. The repeatability for the stages was tested while trying to simulate a continuous working environment, i.e. when the controller is kept turned on for some time. Repeatability for a situation where the controller is used at different times was also simulated, i.e. when the controller is turned off and on again. Each test was conducted while values were collected within a period of 10 minutes. Research The stage that was tested was the goniometer. The repeatability of the home, zero, and an arbitrary position on the encoder were tested. The arbitrary position selected was 200μ°. The instrument used to measure the position of the goniometer was an ELCOMAT Autocollimator. Fig 6: Graph showing the stability of Autocollimator over 5 hours. It can be seen that the stability of the Autocollimator is about 1.5μrad. This difference caused by subtle vibrations in the room will be taken into account when analysing the data. Conclusions The repeatability stated in the specifications for the stage states that the repeatability of the stage is 50μ°, which is approximately 1μrad. Based on the stability of the autocollimator, the expected repeatability was estimated to be around 2μrad. The values obtained when the controller is left on, meet specifications. When the controller is turned off and on, the repeatability meets expectations. The tests performed were closed loop tests, future tests with open loop settings should be carried out in the future to see how the stage reacts without feedback control. Fig 3: Graph showing the average values for the home and arbitrary position. Fig 1: The stage propped up, with a mirror mounted on it. Acknowledgments Use of the Linac Coherent Light Source (LCLS), SLAC National Accelerator Laboratory, is supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences under Contract No. DE-AC02-76SF00515. Acknowledgment also goes to Hongliang Shi and Andrew Barada for mentorship and guidance through the program. Fig 4: Graph showing the average values for the zero, home and arbitrary values while the controller was turned on and off. Controller left on: Repeatability of Zero position = 0.43μrad Repeatability of 200μ° = 0.407μrad Controller Turned off and on: Repeatability of Home position = 1.72μrad Repeatability of Zero position = 1.611μrad Repeatability of 200μ° = 1.772μrad Fig 2: An aerial view of the Autocollimator/Stage setup used to take measurements. Date: 08/07/2017