Neutron scattering: a tool for materials investigations 11 - - PowerPoint PPT Presentation

neutron scattering a tool for materials investigations
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Neutron scattering: a tool for materials investigations 11 - - PowerPoint PPT Presentation

Neutron scattering: a tool for materials investigations 11 September 2017 University of Tartu Kim Lefmann Short presentation Favorite techniques: Kim Lefmann Neutron scattering Danish, 53 years Numerical simulations Low


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Neutron scattering: a tool for materials investigations

11 September 2017 University of Tartu

Kim Lefmann

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SLIDE 2

Short presentation

  • Kim Lefmann
  • Danish, 53 years
  • Ph.D. 1995 physics (NBI), U. Cph.
  • Post doc, Helsinki U. Techn. 1995-96
  • Senior Scientist at Risø 1997-2008
  • Ass. Prof., NBI, Univ. Cph. 2008-
  • Board of the Danish neutron/X-ray

instrument center, DANSCATT

  • Leader of the NNSP Neutron School
  • Favorite techniques:

Neutron scattering Numerical simulations Low temperature techniques

  • Research interests:

Quantum magnetism Frustrated magnetism Multiferroics Nanoscale magnetism Superconductivity Instrumentation

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What is a neutron?

  • A part of the atomic nucleus

–Made of 3 quarks –Mass and spin like the proton –Electrically neutral

  • Can react with nuclei
  • Can scatter off nuclei
  • A slow neutron behaves as a wave
  • Interference !
  • Used to investigate

–Chemical composition –Materials structure and properties

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Elastic and inelastic scattering

  • Elastic: Bragg law n λ = 2 d sin θ
  • Wave number

k = 2 π / λ

  • Scattering vector q = ki - kf

= 2 π / d ki kf q

  • kf

ki kf q

  • kf

q’

  • Inelastic: Conservation laws
  • Energy transfer: ħω = Ei-Ef
  • Energy conservation ħω = ħω(q’)
  • Momentum conservation q = q’
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SLIDE 5

E- and q-coverage

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Why neutrons ? (1)

The neutron has a wavelength (Å) and an energy (meV) comparable to typical atomic spacings and vibrational energies - so you can study both atomic structure and dynamics (simultaneously if required) Neutrons tell you ‘where the atoms are and what the atoms do’

(Nobel Prize citation for Brockhouse and Shull 1994)

  • M. Christensen (AU Chemistry), Nature Materials 2008
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SLIDE 7
  • L. Arleth, KU NBI

Why neutrons ? (2)

The neutron scattering cross-section varies randomly through the periodic table and is isotope dependent - distinguish light and heavy atoms

  • r atoms of similar Z

enabling the technique of isotopic substitution/contrast variation

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Why neutrons ? (3)

The neutron is a weak probe - giving a direct and quantitative link with theory and computer simulation/modelling

P.K. Willendrup, E.B. Knudsen,

  • K. Lefmann et al

McStas, DTU-KU software

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SLIDE 9

Why neutrons ? (4)

The neutron is highly penetrating - enabling studies of thick samples and samples in complex sample environment

15 T magnet, PSI, 2004 (Carlsberg and FNU)

  • H. Haack et al,

science museum 2005

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Why neutrons ? (5)

The neutron has a magnetic moment but no charge - enabling studies of magnetic structure and dynamics

Student team, KU, NBI, 2005

  • > C. Bahl et al, Physica B, 2007
  • T. B. S. Jensen et al, Risø, Phys Rev B 2008
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European neutron facilities

  • Projects are selected

from scientific value

  • ILL is ”members only”

(DK is a member)

  • Other important: BNC, MLZ, HZB, ISIS, LLB, PSI,
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Owned by: UK, D, F Members: 12 other countries 2015 (typical year):

  • 40 instruments
  • 834 experiments
  • 4184 instrument days
  • 1386 users
  • 556 publications

ILL – the neutron Mekka

DK and S are members

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Production of neutrons

Traditional, nuclear reactor Modern, proton accelerator

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Intensity vs time

1940 1950 1960 1970 1980 1990 2000 2010 10

10

10

12

10

14

10

16

10

18

CP-1 CP-2 X-10 NRX MTR NRU HFIR HFBRILL ANS

ZIN-P WNR ZING-P' KENS IPNS LANSCE ISIS SNS JNS ESS

Reactors Spallation Sources

Peak flux n/cm

2 s

Year of first operation

ILL ISIS ANS (canceled) SNS J-PARC ESS

  • Neutron scattering suffers from lack of intensity
  • What does the future bring?
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SLIDE 15

SNS, Oak Ridge, Tennessee

  • Short-pulses
  • 1.4 MW
  • 20 instruments
  • First neutrons

April 2006

  • Users from 2008
  • World leading
  • ... together with

Japanese project J-PARC

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The ESS project

Accelerator:

  • Length: 600 m
  • Protons: 2.0 GeV
  • Power: 5 MW

Neutrons:

  • Long pulses (2.86 ms)
  • 15 (22+) instruments

2 DK-N instruments

  • 10  SNS

Construction:

  • 2014-2020 (2025)
  • 1.843 G€

Site contenders:

  • Bilbao (E)
  • Debrechen (H)
  • Lund (S)

28/5-2009 Bruxelles: Lund chosen as ESS site 4/7-2014: Final building decision !

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SLIDE 17
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SLIDE 18

Recent ESS photos

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Neutrons for many fields of science

  • Condensed matter physics

(magnetism, superconductivity, glasses, liquids)

  • Materials research

(stress/strain, hydrogen in materials)

  • Soft condensed matter

(polymers, composites)

  • Structural chemistry

(catalysis, reactions, parametric studies, molecular spectroscopy)

  • Geology

(minerals at high P,T, hydrogen in rocks)

  • Life sciences

(membranes, protein structure, -dynamics, and -complexes)

  • Nanoscience (most of that above)
  • Particle physics

(basic properties of the neutron, basic quantum mechanics)

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Protein Crystallography by small angle neutron scattering

Determination of Protein confor- mations in solution H-D substitution:

  • Partial labeling of

functional groups

  • Improved contrast

situation The 50S subunit in the map of the 70S E.coli ribosome. Left: Neutron data; solution scattering Right: X-ray crystallography

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Native Membranes and Biosensors

structural investigations in active state

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Neutron reflection

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Biological Membranes

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Studies of catalysis

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Artists view of a Palladium catalyst, passivated by methyl groups. Studied by molecular spectroscopy at ISIS Penetration: In-situ studies

  • f catalytic processes

Flux: Real sized reactors can be studied Instruments: Spectroscopy

  • f reaction intermediates,

with or without H

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Process Monitoring and Optimization

Nanosized magnetic storage devices. Investigation of spin-reversal and spin-dynamics in magnetic nanostructures by inelastic neutron scattering

Magnetoelectronics

The picture can't be displayed.
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Magnetic fluctuations in superconductors

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  • Simple cuprate HTSC (La2-xSrx)CuO4
  • Superconducting below 38 K - why?
  • has incommensurate magnetism

(antiferromagnet with long repetition)

  • These data: x = 0.16 (optimal doping)
  • Short range fluctuations; nm range
  • A gap in the fluctuation spectrum opens up in

the SC phase

  • Magnetism connected

with HTSC!

  • B. Lake et al, Nature (1999)

; Science (2001); Nature (2002)

  • B. Lake et al, Nature Materials (2005)

N.B. Christensen et al, Phys. Rev. Lett. (2004)

  • J. Chang et al, Phys. Rev. Lett (2009)
  • A. Tranum-Rømer et al, Phys. Rev. B (2013)
  • L. Udby et al, Phys. Rev. Lett. (2013)

... many theory papers by B.M. Andersen and P. Hedegård