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0.1-meV Optics Update

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The IXS Group Current Members Xianrong Huang, 0.1 meV crystal optics Marcelo Honnicke, multilayer mirrors for analyzer system Jeff Keister, R&D beamline operation, ... – PowerPoint PPT presentation

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Title: 0.1-meV Optics Update


1
0.1-meV Optics Update
Yong Cai Inelastic X-ray Scattering
GroupExperimental Facilities Division, NSLS-II
Experimental Facilities Advisory Committee
Meeting April 23-24, 2009
2
The IXS Group
  • Current Members
  • Xianrong Huang, 0.1 meV crystal optics
  • Marcelo Honnicke, multilayer mirrors for analyzer
    system
  • Jeff Keister, RD beamline operation, upgrade and
    support
  • Zhong Zhong, NSLS DI beamline spokesperson (M)
  • Scott Coburn, engineering design (50)
  • Leo Reffi, mechanical design (on loan from design
    group)
  • Bill Struble, crystal cutting and lab support
  • Yong Cai, IXS beamline, group leader
  • Future Members (per staffing plan)
  • Postdoctoral Fellow (Crystal fabrication, optics
    testing, etc.) offer accepted, to start around
    June 1
  • Scientific Associate (Crystal fabrication lab)
    Searching
  • Beamline Scientist (IXS beamline) - Searching

3
Outline
  • Summary of progress to date, issues plan
  • Current optical scheme and technical challenges
  • Near-term milestones and longer-term plan
  • Summary

4
Summary of Progress to Date, Issues Plan
Since last EFAC Meeting (May 5-7, 2008)
  • Major progress in building up the infrastructure
    to support the RD program
  • RD beamline and optics test end station at NSLS
    (X16A)
  • Crystal fabrication labs (Bldg 703)
  • RD activities have been focused on gaining a
    better understanding of the technical
    requirements and challenges of the optics
  • 0.1meV crystal optics
  • Multilayer mirrors
  • Issues and plan
  • Crystal fabrication capabilities (equipment
    staffing)
  • Access to more advanced light source(s) for
    prototyping

5
0.1meV Crystal Optics
  • CDW and CDDW optics schemes at 9.1 keV proposed
    by Yu. Shvydko, verified by our dynamical theory
    calculations (Xianrong Huang)

CDW
CDDW
  • Large angular acceptance (gt100 µrad)
  • High efficiency (50)
  • Sharp tails (Borrmann effect), more important
    than resolution!

6
Beamline and Spectrometer Optics Layout
20 µrad Divergence
  • Major parameters determined and verified for E
    9.13 keV, ??e 5 µrad, and h 0.5 mm

?E of CDW ?E of CDDW Te ( 90 f) Length of D
2 meV 1 meV 4.5 120 mm
0.7 meV 0.3 meV 1.5 380 mm
0.2 meV 0.1 meV 0.4 1400 mm!
  • Comb crystal proposed by Yu. Shvydko a possible
    solution to the long D crystal length, but a
    major challenge to fabricate (in progress)

7
Comb Crystal Fabrication
  • Current approach employed by APS
  • Cut directly from a monolithic crystal.
  • Polishing the diffraction surface a major
    challenge.
  • Alternative approach to be explored
  • Prepare reference Si(100) surface from a
    monolithic block
  • Cut individual fins allowing fine polishing of
    diffraction surface
  • Align individual blocks using reference surface
    on symmetric backscattering Si(800) reflection
  • Mechanical positioning a challenge, but more
    solvable

As-cut surface roughness 35.4 nm by AFM
Reference Si(800) reflection
Fine polishing
T
Reference surface
100mm
5mm
8
CDDW for 1meV Channel Cut

Channel-cut (grazing 7?)
  • No need for long D crystal
  • Switchable between 0.1 and 1 meV
  • Require incident beam collimated to 20 ?rad no
    problem for monoanalyzer needs high-precision
    mirror.
  • CC causes 20 efficiency loss

Tails sharper than Lorentz
9
Other Major Technical Challenges
  • Lattice homogeneity of the crystal ?d/d ?E/E
    10-8 (0.1 meV/10 keV)
  • Temperature uniformity and stability ?T 4 mK
    (?d/d a?T and thermal coefficient of Si
    a2.56?10-6 K-1)
  • Surface qualityslope errors (straightness of
    surface) lt 10 µrad, crystal bending (due to
    mounting or gravity sag) lt 0.2 µrad, surface
    roughness (causes diffused scattering) lt 2 nm
  • Crystal angular stability lt 0.2 µrad as a
    result of energy tuning by angular rotation,
    independent of resolution 0.1 1 meV,
  • CDW/CDDW analyzer requires 501001 multilayer
    focusing mirrors for 510 mrad acceptance

10
Angular Stability
  • Energy Tuning by D crystal rotation ? Tuning
    rate 0.07 meV/µrad
  • This implies also
  • Angular vibrations of C,W, D all change ?, must
    be stable lt 0.2 ?rad (independent of targeted
    energy resolution ?E)
  • Lattice bending due to gravity sag or mounting
    changes ?, so must be lt 0.2 ?rad, for all C, W,
    D.

11
Laterally Graded Multi-layer Mirror
0.2 0.3 mm
CDW or CDDW
  • Design Objectives
  • Angular acceptance 5 mrad x 5 mrad
  • To retain a q resolution of 0.01 nm-1
  • Corresponding to 0.1 mrad in horizontal
    acceptance at 9.1 keV or 20 µm transverse width
    at 200 mm from source. Possible solution use
    area detector!
  • Laterally projected source size due to sample
    thickness may be a limiting factor, but not a
    severe problem due to lessen q resolution
    required at higher q. (0.1 mrad 20 µm projected
    source size at 200mm)

Strip Detector
0.1 mrad
5 mrad
Horizontal Scattering Plane
12
Ideal Mirror Figure
  • Parabolic ellipsoid (focusing collimator)
  • Horizontal collimation to 0.1 mrad or better is
    required in order to retain the q resolution!
  • Vertical focusing (up to 0.1 mrad) to minimize D
    crystal length for analyzer, but may limit the
    horizontal q resolution at low q.
  • Vertical collimation to less than 20 µrad may
    allow the use of 2nd channel cut for resolution
    switching between 0.1 and 1 meV for the analyzer,
    and/or possible energy dispersive and q resolved
    detection in the vertical direction with an area
    detector
  • A real challenge to make!

Sample first focus (f1)
Sample
CDW/CDDW
13
Alternative Mirror Configurations
  • A single toroidal mirror to approximate the ideal
    surface
  • Montel optics parabolic (collimator) in a double
    bounce geometry (involving beam inversion of L-R
    and U-D)
  • KB configuration
  • A single mirror only for vertical
    focusing/collimating
  • Horizontal angular acceptance of C crystal
    3mrad!Horizontal energy dispersion of D crystal
    E(f) E0(1-f2/2)

14
Other Works Accomplished
  • Multilayer parameters determined and optimized
    both for parabolic and elliptical figures.
  • Mirror specifications for a non-graded flat
    surfaceSi or B4C layer 1.5 nm, W layer 1.0 nm,
    100 bi-layers on Si substrateTheoretical peak
    reflectivity 85
  • Figure specifications
  • In-house ray-tracing codes developed to examine
    performance of the multilayer mirrors including
    effects of slope error, roughness, and interlayer
    thickness fluctuation (dd/d).
  • Actively in contact with possible vendors for
    test mirrors
  • Test plan using RD beamline at NSLS developed.

Figure P (mm) Tm (rad) dx (mm) dy (mm) d1 (nm) d2 (nm)
Parabolic 0.30796 0.02775 36.17 1.002 2.3495 2.5710
Elliptical 0.30193 0.02775 35.94 0.953 2.3513 2.5683
15
First CDW-CDW Test at NSLS
  • Proof of Principles
  • Collimation effect of C crystal
  • Enhanced Bormann transmission of W crystal
  • Most importantly, the dispersion effect of the D
    crystal
  • ?E 10 meV achieved, possible causes being
    analyzed

16
New CDW-CDW Test
  • Aim for a more controlled study of the optics to
    understand conditions to achieve the targeted
    energy resolution.
  • Verify sharp tail in resolution function with new
    optical path
  • New C/W crystal to minimize strain

Bill Strubles first crystal With help from Shu
Cheung
17
Optics Test End Station
D crystal in oven
C/Wcrystal
  • Current components designed to test CDW-CDW
    scheme with temperature control ovens
  • Include a double-crystal diffraction / imaging
    stage for characterizing crystal quality
  • Flexible and adaptable for other schemes (e.g.,
    CDDW, comb crystals, )
  • Most components fabricated and assembled, and
    being installed on RD beamline

18
Temperature Control Oven
Room T
D crystal
Outer Oven, ?T 0.5 mK
Inner Oven, ?T 0.25 mK
15 hr
  • First oven tests passive controlling on both
    inner (45 C) and outer (35 C) ovens.
  • Excellent stability uniformity to be tested.

19
Dedicated RD Beamline at NSLS
  • An existing PRT beamline, revived after major
    clean-up and repair effort of shielding, vacuum,
    safety and user interlock, beamline and
    endstation control, to allow initial testing of
    0.1 meV resolution optics
  • Existing beamline optics (a 11 focusing mirror
    and a DCM) found to be functional but required
    optimization, to be upgraded within 6-12 months.
  • Beamline granted operation status since April 10,
    2009 after beamline review and readiness
    walkthrough. (took just 1 year from inception to
    operation, but still a lot of work!)

Endstation
Mirror(11)
Source
Mono
RD beamline assembly
20
Crystal Fabrication Labs
EQUIPMENT
  • Two labs being fit out, to be completed in April
  • Cutting / Lapping Lab major equipments
  • Crystal Diffractometer (NSLS equipment)
  • Mark Blade Saw (NSLS equipment)
  • Diamond wire saw (delivered)
  • Lapping machine (delivered)
  • Strasbaugh Spindle Polisher (rough polishing)
  • Polishing / Etching Lab major equipments
  • ADT dicing saw (delivered)
  • Strasbaugh CMP polisher (superfine 0.1 nm)
  • Strasbaugh Spindle Polisher (fine polishing)
  • Chemical etching hood and wet bench
  • Partial operation in April
  • Need to consolidate fabrication equipment and
    streamline fabrication process
  • Too few staff with expertise in polishing and
    etching

X-ray Diffractometer / Blade Saw / Diamond Wire
Saw
Lapping Machine / Spindle Polisher / CMP
Polisher
High-precision dicing saw for Comb crystal
fabrication
Etching Hood
21
Overall Strategy and Near-Term Milestones
Overall strategy and timeline
2009
2010
2011
CDW/CDDW prototypes 1meV?0.5meV?0.1meV Comb
crystals fabrication and test Design and Develop
collimating multilayer mirrors
0.1 meV prototype spectrometer
Date Item Status
June 2009 Actual measurement of the resolution function for CDW scheme. Looking for a sharper tail may be more important than the actual resolution. Still on schedule, waiting on completion of end station. Key areas to watch new control system, ovens test, X16A mirror and mono.
Sept 2009 Fabrication and testing of first comb crystal cut for 1meV. Energy resolution and efficiency measured. Still on schedule, need to push for bldg 703 labs. Hire of scientific associate to fill knowhow gap (etching and polishing). Short-term outsourcing
Sept 2009 Fabrication and testing of multilayer mirror. Demonstrate required specs can be met. In progress, potential road block the on-time delivery of mirror
Nov 2009 Demonstration of the CDDW/CDDW scheme (beam pass thru all optics) Area to watch, continue investigation of alternative schemes
22
Longer-Term Plan Milestones
  • 2010
  • Develop a prototype with 1meV resolutionStrategy
    being considered a Partner User Proposal with
    APS for Sector 30
  • Demonstration experiments on Plexiglas with 1meV
    resolution (real test of energy resolution and
    tail by scattering rather than diffraction)
  • Full work on CDDW prototype to test 0.5 meV
    resolution (with comb crystals), including
    detailed exploration of crystal quality (defects,
    impurities, inhomogeneities), fabrication issues.
  • Test and improve collimating/focusing multilayer
    mirrors
  • Seek alternative approaches if encounter
    unexpected showstoppers
  • 2011
  • Test and improve analyzer optics with multilayer
    mirrors
  • Full work on CDDW prototype to test 0.1 meV
    resolution (with comb crystals)
  • Finalize design

23
Summary
  • Excellent progress has been made in establishing
    the essential infrastructure to support the RD
    program.
  • Initial test results of the asymmetric dispersion
    optics prove the working principles of the
    optics.
  • Key technical challenges to achieve the 0.1meV
    resolution for both the monochromator and
    analyzer are now well understood and being
    addressed.
  • Need to streamline crystal fabrication capability
    within the NSLS-II project, and for prototyping a
    1meV resolution instrument.
  • A modified approach with intermediate staged
    goals may be necessary for the development of the
    IXS beamline.
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