inelastic neutron scattering b. fultz, j. lin, o. delaire, m. kresch caltech

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Inelastic Neutron Scattering B. Fultz, J. Lin, O. Delaire, M. Kresch Caltech Science interests Where is the field going? Tasks and goals of the DANSE subproject Looking for new scientific opportunities

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Inelastic Neutron Scattering B. Fultz, J. Lin, O. Delaire, M. Kresch Caltech. Science interests Where is the field going? Tasks and goals of the DANSE subproject Looking for new scientific opportunities. Excitations in Solids: An Optical Illusion of Space-Time Correlations. - PowerPoint PPT Presentation

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Page 1: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Inelastic Neutron Scattering B. Fultz, J. Lin, O. Delaire, M. Kresch Caltech

Science interestsWhere is the field going?Tasks and goals of the DANSE subprojectLooking for new scientific opportunities

Page 2: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Excitations in Solids:

An Optical Illusion ofSpace-Time Correlations

Page 3: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech
Page 4: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech
Page 5: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech
Page 6: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

ARCS software is going well

Page 7: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

ARCS reduction software demo…

Page 8: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

WBS 10: Science Scope for Inelastic Scattering

1) spin correlations in magnets, superconductors, and materials close to metal-insulator transitions

2) vibrational excitations in solids and their relationship to phase diagrams and equations of state of materials

3) tunneling and reorientation transitions of small molecules on surfaces

4) vibrational spectra of molecules or individual atoms such as hydrogen

5) diffusional motions and relaxation processes studied by quasielastic scattering

Page 9: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Tasks for Inelastic Scattering WBS 10

10.1.1.1 Data reduction for CNCS 08/31/06 02/15/07 10.1.1.2 Data reduction for SEQUOIA 03/01/08 08/16/0810.1.2.1 Data reduction for HYSPEC 05/06/10 07/06/1010.1.2.2 Data reduction for Backscatter 02/07/07 03/16/07

10.2.1.1 Gilat-Raubenheimer method 01/05/08 03/08/08 10.2.1.2 Pack and Monkhorst method 03/11/10 05/08/1010.2.2.1 Polycrystal 07/31/07 01/06/08 10.2.2.2 Single Crystal 11/13/08 06/14/0910.2.2.3 Dispersion Algorithms 08/12/08 11/14/0810.2.3 Separation of Nuclear and Spin Scattering 11/23/09 03/16/1010.2.4.1 CLIMAX 04/21/07 08/11/07 10.2.5 Chemical Spectroscopy Preprocessing 03/01/10 02/28/11

10.3.1.1 Coherent Inelastic Scattering Kernel 03/11/07 04/21/07 10.3.1.2 Incoherent Inelastic Scattering Kernel 04/06/07 04/21/0710.3.1.3 G(r,t) from individual neutron scatterings 03/25/08 11/09/0810.3.1.4 G(r,t) from dynamics simulation 07/03/10 09/18/1010.3.2.1 Multiple scattering correction 04/21/09 12/06/0910.3.3 Disordered Spin Dynamics 04/13/09 02/28/11

Page 10: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Science Activity for Physical Chemistry: Dynamics of Excited Materials and Molecules

• Density-functional methods have revolutionized the calculation of electronic structure• They are not justified for excited states, however.• New effort to study excited states of molecules by pump-probe Raman spectrometry

Page 11: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Science Activity for Physical Chemistry: Hydrogen Molecule Dynamics in Physisorption

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Rotational Librational

Ground

Excited

Page 12: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Entropy

W is the number of

equivalent ways of

finding a system with the

same macrostate.

Ways of “what”?

Page 13: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Classical Limit

1 2

p1…p3N–3

q1…q3N–3

S = kB lnV1

V2( )

~1/

Page 14: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Phonon DOS of V with 3d-series solutes

• increasing stiffening along 3d series

• Ti: softening,

• Cr-Ni: stiffening

• impurity masses ~ host

• trend opposite to mass increase

electronic / size effect

Page 15: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Entropy of Alloying

Page 16: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Use Case

Inelastic Scattering with Fermi Chopper Instruments

• Approach:

- Reduce NeXus file to “S(Q,E)”

- S(Q,E) to phonon DOS, g(E)

-

reduce<include>NeXUSfile

g(E)Z(T)User<include>BvK

• Goal: Obtain phonon partition function, Z(T).

Page 17: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Today – Three Problems

• /M differs between atoms (neutron weighting)

• Q information will be rich, but neglected in analysis

• Errors in Z are unknown - reliability of thermodynamic quantities?

Computation will Solve These

Page 18: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Today (Neutron De-weighting Solution)NeXusreductiongnw(E), d2/dΩdE B v K{Φ1 ’, ...}xx/M |QU (exp iQr) |2,Compare

Alter(Φ1 , ..}xx

( )g E .phononthermo py, , Z F SLaptop Linux Clustergnw( )E

Page 19: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Near Future: Fits with Q information

Page 20: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

New CapabilityZ, Pmm, displ.PHONONVASPE(Q)Linux ClusterLaptopARCS, parampyre-McStasNeXus{Φ1 , ...}xx, M params

Page 21: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Error Bars in Thermodynamic Quantitiesreduce<include>VASP

E(Q)g(E)<include>BvKZex(T)User<include>SimulNeXus<include>Zth(T)

Page 22: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Error Bars in Thermodynamic QuantitiesB v Kg(E)phononthermo.pyZ, F, SError in Freductiongnw(E), d2/dΩdE B v K{Φ1xx’, ...}/M |QU (exp iQr) |2,Compare

Alter(Φ1 , ..}xx

( )g E .phononthermo py, , Z F SLaptop Linux Clustergnw( )E, , .Z Pmm displPHONONVASP(E Q) Linux ClusterLaptop, ARCS param-pyre McStasNeXus{Φ1 , ...}xx, M params

Page 23: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Test Case – Use Known Force Constants from NiB v Kg(E)phononthermo.pyZ, F, SError in Freductiongnw(E), d2/dΩdE B v K{Φ1xx’, ...}/M |QU (exp iQr) |2,Compare

Alter(Φ1 , ..}xx

( )g E .phononthermo py, , Z F SLaptop Linux Clustergnw( )E, , .Z Pmm displPHONONVASP(E Q) Linux ClusterLaptop, ARCS param-pyre McStasNeXus{Φ1 , ...}xx, M params

Page 24: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Resolution of a Fermi Chopper Spectrometer (e.g., Windsor)

~4.2 for ARCS

Page 25: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

ARCS Has Moveable Fermi Choppers

Page 26: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Typical ARCS Resolution (Energy Dependent)

Page 27: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Multiple Energies Give Higher Resolution

Page 28: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

Summary of WBS 10: Inelastic Scattering

1) Scope for:- physical chemistry of small molecules- phonon excitations in solids- magnetic excitations in solids

2) Progress with ARCS and other inelastic instruments has been crucial for establishing the science scope

3) Experience in materials theory is essential too

Page 29: Inelastic Neutron Scattering B.  Fultz, J. Lin, O. Delaire, M. Kresch  Caltech

end of presentation