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1 BROOKHAVEN SCIENCE ASSOCIATES
Dynamics of materials with X-ray Photon Correlation Spectroscopy - Opportunities and detector requirements
Andrei Fluerasu [email protected]
Washington DC, August 2012
Quasi-static speckles from colloidal suspension near random compact packing volume fraction
Speckles near the (409) Bragg peak of concanavalin A
2 BROOKHAVEN SCIENCE ASSOCIATES
X-ray Photon Correlation Spectroscopy
Impact: Understanding dynamics may be the critical element in switching from a science ofobservation to a science of control.
“How do we characterize and control matter away—especially very far away—from equilibrium?” Directing Matter and Energy: Five Challenges for Science and Imagination (BESAC)
XPCS• “Mesoscale” structure determines most (if not all)
macroscopic properties of materials. • X-ray Photon Correlation Spectroscopy (XPCS)
measures collective “meso-scale” dynamics
Scientific opportunities● Structure and dynamics of complex materials:
colloids, emulsions, polymers, gels and glasses, membranes, liquid crystals, bio-materials
● “crowded” systems = structure & dynamics affected by entropy, weak forces
● Wide range of time & length scales
Examples of mesoscale structure: (a) porous silicon; (b) sponge phase in a polymer blend (S. Mochrie)(c) bicontinuous microstructure arrested by interfacial colloidal jamming (A. Moharaz et al.); (d) self-assembled amphiphilic nanotubes (Park C et al. PNAS 2006;103:1199-1203)
a) b) c)
d)
Applications: → photonics, lithography, high-tech materials, photovoltaics, paints, food, cosmetics, etc→ fundamental science: glass transition, rheology, jamming, non-equilibrium physics, complexity (“more is different” - P. Anderson)
3 BROOKHAVEN SCIENCE ASSOCIATES
XPCS: New Opportunities
However: Current detector technology is limited to 1-3 kHz maximum frame rate
New detectors enabling > MHz acquisition are required in order to capitalize on the unprecedented performance of the new, high brightness, light sources
XPCS at NSLS-II:• “Mesoscale” structure determines most (if not all)
macroscopic properties of materials. • X-ray Photon Correlation Spectroscopy (XPCS)
measures collective “meso-scale” dynamics
Focus on:● Soft matter: colloids, emulsions, polymers, gels and
glasses, membranes, liquid crystals, bio-materials● “crowded” systems = structure & dynamics
affected by entropy, weak forces● Wide range of time & length scales
Examples of mesoscale structure: (a) porous silicon; (b) sponge phase in a polymer blend (S. Mochrie)(c) bicontinuous microstructure arrested by interfacial colloidal jamming (A. Moharaz et al.); (d) self-assembled amphiphilic nanotubes (J. Douliez et al.)
a) b)
10μm
c)
d)
Applications: → photonics, lithography, high-tech materials, photovoltaics, paints, food, cosmetics, etc→ fundamental science: glass transition, rheology, jamming, non-equilibrium physics, complexity (“more is different” - P. Anderson)
XPCS at high brightness SR sources: NSLS-II, APS, ERL(?)
• SNR=brightness*τ1/2
• e.g. NSLS-II >10 x brighter than other SRs
• 100 x faster time scales (i.e. reaching 1 μs) and shorter length scales than was ever possible before.
4 BROOKHAVEN SCIENCE ASSOCIATES
XPCS 101
From R. Leheny
Dynamic structurefactor
Reference: e.g. M. Sutton, CR Physique 9, 657 (2008)
5 BROOKHAVEN SCIENCE ASSOCIATES
What is an ideal XPCS detector?
•Specifications (from P. Siddons)● 1000 Mpixels● 1 μm pixels● 1 ns frame rate; no dead time● 100% efficiency at all energies● 100 bit dynamic range● free
From O. Shpyrko
6 BROOKHAVEN SCIENCE ASSOCIATES
Maxipix (ESRF)• Based on chip developed by Medipix collaboration
• 1.4 kHz, 55 μm pix size, single ph sensitivity,100% efficiency (8keV), ~12-bit dynamic range
C. Ponchut et al., J. Instrumentation 6, 01069 (2011)
• Enabled new science (@ ID10, ESRF) e.g. :• cooperative behavior of nanoparticles suspended in a
supercooled liquid C. Caronna et al., Phys. Rev. Lett. 100, 055702 (2008)
• Dynamics and rheology under steady shear flow A. Fluerasu et al., New J. of Phys. 12, 035023 (2010)
Detectors for XPCS - Current State of the Art
Eiger (SLS)• To become available ~2013
• 24 kHz*, 75 μm pix size, single ph sensitivity,100% efficiency (8keV), ~12-bit dynamic rangeB. Schmidt, unpublished* Dectris development – 3kHz (but possible future upgrades)
7 BROOKHAVEN SCIENCE ASSOCIATES
Next best option for an XPCS detector?
•Photon counting provides best S/N•Specifications
● 1-9 Mpixels● 1 μs frame rate, ~10-20 ns time resolution (time stamping)● 70-80 μm pixels● negligible dead time● 100% efficiency at 8keV● 4 bit dynamic range● “electronic shutter”
•VIPIC project (FNAL/BNL) is close to matching these ideal/realistic specs:
● 10 μs frame rate, ~20 ns time resolution (time stamping)● 80 μm pixels, scalable to >1M pixels
16 Serial Output Lines (LVDS)
Preamp X6
Disc.
ts=250 ns
Program latches
Serial Output Line
Sparsification
Two 5 bit counters
Serializer and LVDS Output
Inject/option Feedback Th
2 3 7 4X64
8 BROOKHAVEN SCIENCE ASSOCIATES
Applications
•Example of science that is impossible to do without fast 2D detectors● Dynamics in out-of-equilibrium “glass” complex
materials● Non-stationary and non-equilibrium dynamics
(two-time correlations)● Speckle Visibility Spectroscopy (with applications
in mitigating beam damage, low scatterers, etc)
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Challenges:• Wide-range of time/length scales, with
samples that are often beam sensitive and/or low scatterers
• Current experiments → photon-limited
• Samples are often non-ergodig
• or non-stationary (e.g. aging) → see next slide
Correlation functions from hard-sphere suspensions near the colloidal glass transition (P. Kwasniewski et al., unpublished)
Dynamics of out-of-equilibrium system: complex fluids, “glassy” and “jammed” materials
Opportunities:• Understanding phenomena such as the
colloidal glass transition
• Understanding the interplay between dynamics and rheology; designing complex fluids with specific viscoelastic properties
Self-assembled monodisperse “supra-molecular” assemblies from polydisperse nanoparticles
T.D.Nguyen, S. Glotzer, et al.
Nature Nanotech 2011
10 BROOKHAVEN SCIENCE ASSOCIATES
Challenges:• Most complex system exhibit complex time-dependent behavior (i.e. aging)
• Dynamics is often heterogeneous
Two-time correlation functions showing non-equilibrium effects (“aging”) and heterogeneous dynamics (let) in colloidal gels or dynamical “rare events” in a colloidal glass (right) (AF et al.)
Dynamics of out-of-equilibrium system: non-stationary and aging samples
Opportunities:• Measuring time-dependent dynamics using two-time analysis
M. Sutton et al. Optics Express 11, 2268, 2003
• Characterize dynamical heterogeneities or “rare events”A. Duri and L. Cipelletti, Eur. Phys. Lett. 76, 972, 2006 C. Sanborn et al. Phy. Rev. Lett 107, 015702, 2011
• Using two-time analysis and higher order correlations to understand and control phenomena such as self-assembling in complex systems
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Beam damage, low scattering Solution: speckles are detected from single images by analyzing the probability of
measuring 1,2,3,4,... scattered photons near Bragg spots of PXs
Intensity distribution (speckles)Left: Reference sample (colloid)Right: scattering near the (409)Bragg spot of concanavalinAincoherent scattering should follow Poisson statistics while speckles from coherent illumination follow neg binomial statistics (J.W. Goodman, 2007)
Speckles from protein crystals: the low scattering limit
Challenges:
Opportunities: Measuring dynamics of proteins using speckle visibility spectroscopy
P.K. Dixon and D. J. Durian, Phys. Rev. Lett. 90, 184302 (2003)
12 BROOKHAVEN SCIENCE ASSOCIATES
Conclusions
•Exciting (& challenging) opportunities for studying microscale dynamics of materials (examples show here focus on soft- and bio- matterials)
•Unprecedented coherent flux (e.g. NSLS-II) and experimental capabilities become available
•Fast 2D detectors for coherent scattering (speckles) are the single most important required development.
•Availability of such detectors would allow experiments that would capitalize on the unprecedented brightness of the new SRs and which are otherwise impossible