The NCNR Spin-Polarized Triple-Axis Spectrometer (SPINS) The SPINS instrument is located at the heart of the cold neutron guide hall of the NIST Center.

Slides:



Advertisements
Similar presentations
Focusing monochromators/analyzers Asymmetric diffraction geometry of the monochromator Dispersive double crystal monochromator Two wavelength sandwich.
Advertisements

W. M. Snow Physics Department Indiana University/IUCF EDM collab meeting Monitoring the Cold Neutron Beam (During Experiment) What to measure (fluence.
Jin Huang & Vincent Sulkosky Massachusetts Institute of Technology Boson 2010 Workshop Sept 20, JLab.
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=
Photoelectron Spectroscopy Lecture 7 – instrumental details –Photon sources –Experimental resolution and sensitivity –Electron kinetic energy and resolution.
4-1 Chap. 7 (Optical Instruments), Chap. 8 (Optical Atomic Spectroscopy) General design of optical instruments Sources of radiation Selection of wavelength.
Managed by UT-Battelle for the Department of Energy Current and Future Instrument Development Projects at Oak Ridge Lee Robertson Instrument DevelopmentGroup.
NMR Broad Band Spectrometer
III. Analytical Aspects Summary Cheetham & Day, Chapters 2, 3 Chemical Characterization of Solid-State Materials Chemical Composition: Bulk, Surface, …
Slide # 1 SPM Probe tips CNT attached to a Si probe tip.
Polarized Beams Using He-3 at the NCNR Triple-Axis Spectrometers Ross Erwin Tom Gentile Wangchun Chen Sarah McKenney.
Progress on the New High Intensity Cold Neutron Spectrometer, MACS C. Broholm 1,2, T. D. Pike 1,2, P. K. Hundertmark 1,2, P. C. Brand 2, J. W. Lynn 2,
Conceptual Design: MACS is designed to maximize the efficiency for energy resolved surveys of Q-space in the sub-thermal energy range. Two innovations.
HLab meeting 10/14/08 K. Shirotori. Contents SksMinus status –SKS magnet trouble –Magnetic field study.
Neutron Conversion Factors E (meV) =  -2 (Å -2 ) E (meV) = k 2 (Å -2 ) E (meV) =  10 6  -2 (m 2 /  sec 2 ) T (K) = E (meV)
ハイパー核ガンマ線分光用 磁気スペクトロメータ -SksMinus- 東北大学 大学院理学研究科 白鳥昂太郎 ATAMI.
Recoil Polarimetry in Meson Photoproduction at MAMI Mark Sikora, Derek Glazier, Dan Watts School of Physics, University of Edinburgh, UK Introduction The.
Designer and Manufacturer of Scientific Instruments Since 1985.
Dynamics Neutron Scattering and Dan Neumann
HYSPEC HYSPEC INSTRUMENT DESIGN – OUTLINE  The two “models” considered for HYSPEC – inside & outside (Mark)  A breakdown of the components of the two.
HYSPEC Recent progress and polarization analysis capabilities ORNL: B. Winn, V. Ovidiu Garlea, M. Graves- Brook, Peter Jiang, X. (Tony) Tong BNL: L. Passell,
Proposal for a High Intensity Chopper Spectrometer at LANSCE Science requiring high sensitivity neutron spectroscopy Limitations of current instrumentation.
NCNR, NIST Gaithersburg, MD Internet: Neutron Spin Echo Spectroscopy (NSE) Dobrin P. Bossev, Steven.
MACS –a New High Intensity Cold Neutron Spectrometer at NIST February 17, 2003Timothy D. Pike1 Developing MACS A Third Generation Cold Neutron Spectrometer.
Setup for hypernuclear gamma-ray spectroscopy at J-PARC K.Shirotori Tohoku Univ. Japan for the Hyperball-J collaboration J-PARC E13 hypernuclear  -ray.
5th workshop on scientific collaboration/JINR/Dubna HJL Basis HFR IBR-2 user policy collaboration Project REMUR: Investigation of the structure.
Choosing the Right Neutron Spectrometer Dan Neumann NIST Center for Neutron Research
Why Diffraction, Why Neutrons? J. A. Dura Neutron Small Angle Scattering and Reflectometry NCNR Summer School on June 26, 2006.
Building MACS  Goals of the MACS project  Funding and time line  Technical overview  Possible IDG contributions  Process for IDG involvement in MACS.
Managed by UT-Battelle for the Department of Energy Polarized 3 He Filling Stations Xin Tong (Tony) Instrument Development Group Neutron Facilities Development.
HYSPEC IDT HYSPEC - Hybrid Spectrometer for the Single Crystal and Polarized Neutron Studies at the SNS Steve Shapiro and Igor Zaliznyak Center for Neutron.
Virtual experiments in University teaching Kim Lefmann MCNSI public, ISIS, 27/9-05.
Polarized Neutrons in ANSTO – From LONGPOL to Pelican, Taipan, Sika, Platypus and Quake Dehong Yu and Shane Kennedy Bragg Institute, ANSTO, Australia.
MACS Concept and Project Status Making best use of CW source MACS-imizing incident flux MACS-imizing detection efficiency From concept to reality Collin.
HYSPEC HYSPEC: A High Performance Polarized Beam Hybrid Spectrometer at the SNS Beamline 14B I.Zaliznyak 1, S. Shapiro 1, L. Passell 1, V. Ghosh 1, W.
David Winogradoff Haverford College NCNR, NIST Ivan Schroder
HYSPEC IDT Polarized Beam Operation of the Hybrid Spectrometer at the pulsed Spallation Neutron Source. Outline HYSPEC: project timeline and place in the.
Lecture 9: Inelastic Scattering and Excited States 2/10/2003 Inelastic scattering refers to the process in which energy is transferred to the target,
The Magnetic phase transition in the frustrated antiferromagnet ZnCr 2 O 4 using SPINS Group B Ilir Zoto Tao Hong Yanmei Lan Nikolaos Daniilidis Sonoko.
Shielding Helium Cold neutron source Shutter Cooled filters Radial Collimators Variable Aperture Focusing monochromator on translation stage Focusing monochromator.
Spin Polarized Inelastic Neutron Scattering NIST Summer School on Neutron Spectroscopy Seung-Hun Lee Peter Gehring Sungil Park Alina Visinoiu Gokhan Caliskan.
NCNR and NIST Neutron research and probing matter with cold neutrons OR Neutrons ignored no longer!
Quantum Rotational Dynamics of CH 3 I Group D Y Liu, S Jonas, V Atakan, H Wu, S Omar-Diallo, I-K. Jeong D. Phelan.
MACS –a New High Intensity Cold Neutron Spectrometer at NIST September 24, 2002Collin L. Broholm Timothy D. Pike 1 Scientific Program and Requirements.
Parameters of the new diffractometer “ARES” Aleksey E. Sokolov PNPI NRC “KI”
Conceptual design and performance of high throughput cold spectrometer : MACS Why MACS Layout and key elements Performance Data collection Scientific program.
Cold Neutron Spectroscopy on MACS  Virtues and limitations of INS  Enhancing INS at the NCNR  Description of MACS  Science on MACS  Integration of.
Past and Future Insights from Neutron Scattering Collin Broholm * Johns Hopkins University and NIST Center for Neutron Research  Virtues and Limitations.
Neutron Scattering Group February, 2001 A High Performance Instrument for the Single Crystal Spectroscopy at the Pulsed SNS. n What is the spectrometer.
MCNSI meeting, February 2006 Contents: People –V. Ryukhtin left for part time only Multichannel focusing benders – continuation –resolution functions.
NMI3 meeting, ISIS, September 26-29, 2005 Contents: Overview of new capabilities of the RESTRAX software Numerical optimizations of TAS parameters Virtual.
A New High Intensity Cold Neutron Spectrometer at NIST J. A. Rodriguez 1,3, P. Brand 3, C. Broholm 2,3, J.C. Cook 3, Z. Huang 3, P. Hundertmark 3, J. Lynn.
Parameters of the new diffractometer TEX Responsible: Yu.Kibalin, I.Golosovsky.
CAPABILITIES Desire to measure lattice and spin dynamics in small single crystals:  Need high flux at sample position.  Low background Science Needs:
Virtual experiments for teaching and training Kim Lefmann MCNSI, ILL, 26/5-05.
An electron/positron energy monitor based on synchrotron radiation. I.Meshkov, T. Mamedov, E. Syresin, An electron/positron energy monitor based on synchrotron.
HYSPEC IDT Polarized Beam Mode for the Hybrid Spectrometer (HYSPEC) at the Spallation Neutron Source. Outline BNL’s HYSPEC project and its place in the.
HYSPEC IDT Introduction to HYSPEC: Overview of the Conceptual Design and Top Level Specifications. Outline Overview of the HYSPEC layout and principal.
Neutron Scattering Group March, 2001 A High Performance Hybrid Spectrometer for the Single Crystal Spectroscopy at the Pulsed SNS  Scientific case and.
HYSPEC IDT Options for polarization analysis with 3 He for the Hybrid Spectrometer (HYSPEC) L. Passell, V.J. Ghosh, I. Zaliznyak, S. Shapiro, W. Leonhardt,
By Abdullah Framalawi Aly Abouhaswa Polarized Neutron Spectrometry : Studying nanostructure magnetism with the use of polarized neutron reflectometry.
Moving the NPDGamma Experiment to the SNS FnPB Christopher Crawford University of Kentucky overview of NPDGamma transition to the SNS expected.
HYSPEC IDT Polarized Beam Mode for the Hybrid Spectrometer (HYSPEC) at the Spallation Neutron Source. Outline Polarization analysis and the HYSPEC place.
Introduction to spectroscopy Applications of X-ray and neutron scattering in biology, chemistry and physics 23/ Niels Bech Christensen Department.
October, 2001 Hybrid Spectrometer for Single Crystal Studies at the Pulsed SNS: an update. n Principal features of the proposed hybrid spectrometer. n.
THE NEUTRON SPECTROMETER
Hall “12 GeV” May 27, 2003 NAPP 2003: J.J. LeRose.
MIRACLES budget: Summary of the 3 configurations
Scope Setting Meeting MIRACLES
Presentation transcript:

The NCNR Spin-Polarized Triple-Axis Spectrometer (SPINS) The SPINS instrument is located at the heart of the cold neutron guide hall of the NIST Center for Neutron Research. SPINS

The NCNR Spin-Polarized Triple-Axis Spectrometer (SPINS) The SPINS instrument with a super-conducting magnet. zIncident Energy y14 ~ 2 meV ( 2.4 ~ 6.1 Å ) zEnergy Resolution y0.02 ~ 1 meV zSpecial Equipments ySupermirror Transmission Polarizer  A stack of single crystal Si plates with Fe/Si supermirror coatings yMulti-crystal Analyzer x11 Horizontally Focusing PG Blades yPosition Sensitive Detector  3 He, 20 × 25 cm 2 yFilters xPG or Be filters before sample xBe or BeO filters after sample

The SPINS Operation Modes I: Conventional Triple-Axis Spectroscopy (TAS) TAS is ideally suited for probing small regions of phase space Shortcoming: Low data collection rate A single point at a time Multicrystal analyzer and position-sensitive detector Improvement Monochromator Sample Analyzer Single Detector Neutron Source

The SPINS Operation Modes II: Horizontally Focusing (HF) Analyzer Mode Monochromator Multicrystal Analyzer Sample Single Detector  L = distance from sample to HF analyzer w a = total width of HF analyzer  2  = w a sin  a /L ~ 9 degree for E f =5 meV at SPINS Relaxed Q-resolution Useful for studying systems with short-range correlations

The SPINS Operation Modes III: Multiplexing Detection System for TAS Sample Flat Analyzer Position-Sensitive Detector 2i2i aa aiai  a i =  a +  2  i =  a - atan(x sin  a /(L+xcos  a )) k f i =  a /2sin  a i Q i = k i - k f i Survey (h  -Q) space by changing the incident energy and scattering angle Probes scattering events at different energy and momentum transfers simultaneously hh Q ~1meV

The SPINS Operation Modes IV: Position-Sensitive Detector in Two-Axis Mode The PSD measures E i -E cutoff EiEi S(Q,  ) d  Large angular acceptance = w / L ~ 11 o for SPINS Sample Low-pass Filter PSD L w Be or BeO The filter passes only those neutrons with 0 < E f < E cutoff