NEUTRON SCIENCE - NIST€¦ · March 25, 2014 . Rob Dimeo, Director . NIST Center for Neutron...

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Rob Dimeo, Director March 25, 2014 NIST Center for Neutron Research NEUTRON SCIENCE at the

Transcript of NEUTRON SCIENCE - NIST€¦ · March 25, 2014 . Rob Dimeo, Director . NIST Center for Neutron...

Page 1: NEUTRON SCIENCE - NIST€¦ · March 25, 2014 . Rob Dimeo, Director . NIST Center for Neutron Research . NEUTRON SCIENCE . a t the

Rob Dimeo, Director March 25, 2014

NIST Center for Neutron Research

NEUTRON SCIENCE

at t

he

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NIST LABORATORIES

MEASUREMENT LABORATORIES

TECHNOLOGY LABORATORIES

USER FACILITIES

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…assure the availability of neutron measurement capabilities to meet the needs of US researchers from industry, university, and government agencies.

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June 2013

Photo credit: Brian Renegar

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20 MW D2O moderated 30 fuel elements

/sn/cm105.1 214×=Φat mid-plane (un-fueled region)

7 cycles/year 38 day cycles 250 days/year

NEUTRON PRODUCTION

NEUTRON SCATTERING FUNDAMENTALS

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NIST cold source

NEUTRON SCATTERING FUNDAMENTALS NEUTRON PRODUCTION

Cold neutrons (long λ, small E) are well-suited for probing structure and dynamics of soft matter such as polymers and biomolecules.

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28 250 2 instruments operating days proposal calls/year

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Unique instruments to address the needs of the scientific community

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2013 NCNR RESEARCH PARTICIPANTS

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NEUTRON SCATTERING FACILITIES

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E ~ atomic motion

WHY NEUTRON SCATTERING?

Pen

etra

ting

Scattering power varies randomly across the periodic table and from isotope to isotope

λ ~ interatomic spacing

Mag

neti

c

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θ2cos2222fifi kkkkk −+=

fi kkk

−=

NEUTRON SCATTERING FUNDAMENTALS

ii Ek ,

ff Ek ,

sample (scatterer)

2θ fi EEE −=

kp

=

KINEMATICS

( )n

ii m

kE2

2

=

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NEUTRON SCATTERING FUNDAMENTALS DYNAMICS

),(4

2

ωπ

σσ QSNkk

dEdd

i

f

f

=

Ω

( ) ( )∫ −−= te

NQS QQ

ticoh

ρρ

πω ω 0dt

21),( related to pair correlation function

),( ωQSinc

related to self correlation function

scattering function - depends on sample properties only

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DIFFRACTION where are the atoms?

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SPECTROSCOPY how are they moving?

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NEUTRON SCATTERING FUNDAMENTALS NEUTRON SPECTROSCOPY in a nutshell

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NEUTRON SCATTERING FUNDAMENTALS

phonons in crystals

glasses

water

complex fluids

quantum fluids

Reorientational dynamics

rotational tunneling

C60

NEUTRON SPECTROSCOPY in a nutshell

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NEUTRON SCATTERING FUNDAMENTALS

polycarbonate

α-lactalbumin

crystal field splitings

spin waves

Local spin resonances

NEUTRON SPECTROSCOPY in a nutshell

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Neutron Imaging Viewing Operational Fuel Cells in Real-Time

Problem:Water management in fuel cell; metal cell components; scattering from hydrogen

Solution: Neutron imaging

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REORIENTATIONAL DYNAMICS IN NANOCONFINED LiBH4

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Verdal et. al., J. Phys. Chem. C 117 (35) 17983 (2013)

Bulk LiBH4 dynamics

two-fold jumps

three-fold jumps

𝐴𝐴0 𝑄𝑄 =12

1 + 𝑗𝑗0 𝑄𝑄𝑄𝑄𝐻𝐻−𝐻𝐻

𝐴𝐴0 𝑄𝑄 = 𝑗𝑗02 𝑄𝑄𝑄𝑄𝐻𝐻−𝐻𝐻

𝑆𝑆 𝑄𝑄,𝜔𝜔 = 𝐴𝐴0 𝑄𝑄 𝛿𝛿 𝜔𝜔 + 𝐴𝐴𝑖𝑖(𝑄𝑄)𝐿𝐿𝑖𝑖(𝜔𝜔)𝑖𝑖

C2|C3

REORIENTATIONAL DYNAMICS IN NANOCONFINED LiBH4

330 K

350 K

400 K

C2|C3

trigonal disorder

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Verdal et. al., J. Phys. Chem. C 117 (35) 17983 (2013)

LiBH4 in NPC-4 nm

REORIENTATIONAL DYNAMICS IN NANOCONFINED LiBH4

2.5 3.0 3.5 4.0 4.5 5.01E-3

0.01

0.1

1

10

HWHM

(meV

)1000/T (K-1)

250400Temperature (K)

333 286 222 200

1010

1011

1012

1013

ω (s-1)

388 K (bulk)

in 4 nm NPC

bulk Ea= 11.3 ± 0.8 kJ/mol

Ea= 15 ± 1 kJ/mol

C2/C3

Isotropic rotational diffusion

330 K

400 K

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Verdal et. al., J. Phys. Chem. C 117 (35) 17983 (2013)

REORIENTATIONAL DYNAMICS IN NANOCONFINED LiBH4

4 nm

two types of BH4- anions in 4 nm

cylindrical pores

-10 -5 0 5

Neut

ron

Coun

ts

Neutron Energy Transfer (meV)

400 K Q=3 Å-1

interface core

core anions interface anions

core BH4- anions with slower,

bulk-like, jump reorientations interface BH4

- anions with faster, more disordered reorientations

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THICKNESS FLUCTUATIONS IN CELL MEMBRANES

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Do thickness fluctuations in biological membranes exist and do they form pores thus allowing proteins to work their way inside?

Woodka et. al., PRL 109 058102 (2012)

THICKNESS FLUCTUATIONS IN CELL MEMBRANES

Requires measurements of longer time scales ⇒ NSE

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Woodka et. al., PRL 109 058102 (2012)

THICKNESS FLUCTUATIONS IN CELL MEMBRANES

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Fluctuations measured in a biological membrane for the first time directly using NSE. The means by which they form pores remains unsolved.

Woodka et. al., PRL 109 058102 (2012)

THICKNESS FLUCTUATIONS IN CELL MEMBRANES

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SEALING BIOMEMBRANES VIA BIO-MIMETIC POLYMERS A structural and dynamics study

SANS REFLECTOMETRY

NEUTRON SPIN-ECHO

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J.-Y. Wang et. al., submitted

SEALING BIOMEMBRANES VIA BIO-MIMETIC POLYMERS A structural and dynamics study

Trauma can disrupt barrier function of cell membrane’s barrier function Cell repair process can be too slow resulting in dysfunction and/or damage

Biocompatible polymer material is a candidate for sealing the cell and enhancing cell survival

Must gain a thorough understanding of the fundamental mechanism responsible for the sealing action

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J.-Y. Wang et. al., submitted

SEALING BIOMEMBRANES VIA BIO-MIMETIC POLYMERS

Neutron Reflectometry

A structural and dynamics study

d75-DPPC is a surrogate for cell membrane

Sealant is a biocompatible polymer (HP_27K) with phosphorylcholine (PC) pendant groups that mimic phospholipids

1,2-dipalmytoyl (d62)-sn-glycerol-3-phosphocholine-1,1,2,2,-d4-N,N,N-trimethyl-d9

Head group thickness = 0.62 nm Tail group thickness = 1.59 nm Little difference in SLD But at T=25 oC the high packing density might limit ability of PC polymer to interact with the lipids (which would not change the NR profile much).

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J.-Y. Wang et. al., submitted

SEALING BIOMEMBRANES VIA BIO-MIMETIC POLYMERS

Small Angle Neutron Scattering

A structural and dynamics study

DMPC used as a surrogate for cell membrane SANS measurements spanning Tm show little difference in scattering profile Sealant has little influence on structure of lipid membranes

1,2-dimyristoyl-sn-glycerol-3-phosphocholine

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J.-Y. Wang et. al., submitted

SEALING BIOMEMBRANES VIA BIO-MIMETIC POLYMERS

Neutron Spin Echo

A structural and dynamics study

DMPC used as a surrogate for cell membrane Measured membrane fluctuations Bending modulus larger (stiffer) for system with sealant Sealant interacts through PC-PC head groups ⇒ Sealant suppresses membrane fluctuations

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ZnCu3(OD)6Cl2

Geometric frustration →QSL

QUANTUM SPIN LIQUID

Herbertsmithite Kagome lattice antiferromagnet

T.-H. Han et. al., Nature 492 11659 (2012)

S=1/2

Zn2+

Cu2+

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Rodriguez et. al., unpublished

QUANTUM SPIN LIQUID…NOT

T = 2.2 K

E = 2.75 meV E = 2.25 meV

E = 1.75 meV E = 0.75 meV

In contrast to a quantum spin liquid, this system magnetically orders at low temperature and sharp excitations appear

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T.-H. Han et. al., Nature 492 11659 (2012)

QUANTUM SPIN LIQUID

Diffuse: no sharp features that would indicate the presence of long-range magnetic order

T = 1.6 K

E = 6 meV

E = 2 meV

E = 0.75 meV

Model calculations

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T.-H. Han et. al., Nature 492 11659 (2012)

QUANTUM SPIN LIQUID

Continuum of spin excitations in 2-D magnet Direct evidence for fractionalized excitations

S=1 excitation breaks up into two S=1/2 spinons

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Thank You

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