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Probing	
  materials	
  at	
  ILL:	
  an	
  overview	
  of	
  structure	
  
inves7ga7on	
  with	
  neutrons	
  
Viviana	
  CRISTIGLIO	
  
Instrument	
  Scien6st	
  at	
  the	
  Ins6tut	
  Laue	
  Langevin	
  
	
  
	
  
-­‐	
  Neutrons	
  science	
  at	
  high	
  T	
  
-­‐ 	
  Carbon	
  nanotubes	
  
-­‐ 	
  Li	
  ba=eries	
  
	
  
Industrial	
  materials,	
  Energy	
  
The	
  liquid	
  state	
  is	
  fundament	
  state	
  of	
  the	
  ma=er	
  and	
  is	
  an	
  
essen6al	
  stage	
  for	
  various	
  technological	
  applica1ons	
  
Metallurgy	
   Op6c	
  fibers	
   Aerospace	
  propulsion	
  
Why	
  do	
  we	
  need	
  HT?	
  
Glass	
  making	
  :	
  from	
  liquid	
  to	
  glass	
  by	
  quenching	
  
	
  
Design	
  of	
  new	
  glasses	
  :	
  Storing	
  nuclear	
  waste	
  
	
  
Food	
  and	
  drink	
  
Chemistry,	
  
Pharmaceu6cs,	
  
Cosme6cs	
  
Structure	
  of	
  Liquids	
  by	
  diffrac6on	
  
Unlike	
  crystals,	
  the	
  structural	
  informa6on	
  for	
  liquids	
  and	
  glasses	
  is	
  described	
  in	
  terms	
  of:	
  
1.  Probabilis6c	
  atomic	
  distribu6on	
  func6ons.	
  
2.  Mean	
  atomic	
  distribu6on	
  around	
  each	
  chemical	
  
species	
   given	
   by	
   the	
   Pair	
   Distribu6on	
   Func6on	
  	
  	
  
g(r).	
  
g(r)	
   is	
   the	
   probability	
   to	
   find	
   an	
   atom	
   at	
   a	
  
distance	
  r	
  from	
  another	
  taken	
  at	
  the	
  origin	
  
Interatomic	
  distances	
  
Coordina6on	
  number	
  
Spa6al	
  distribu6on	
  
of	
  atoms	
  or	
  
molecules	
  in	
  the	
  
system	
  
Crystalline	
  solids	
  
Equilibrium	
  posi6ons	
  
Well	
  defined	
  Bragg	
  peaks	
  
Amorphous	
  
Distribu6on	
  of	
  equilibrium	
  	
  
posi6ons	
  
	
  	
  	
  	
  No	
  Bragg	
  peaks	
  
Structure of Crystalline and Amorphous Solids
Diffusive	
  
Mo6ons	
  
Internal	
  	
  
Dynamics	
  
Structural	
  informa7on	
  
Collec6ve	
  dynamics	
  
Coherent	
  
σcoh	
  
4π	
  
Incoherent	
  
σinc	
  
4π	
  
Sca=ering	
  cross	
  sec6on	
   σ	
  =	
  σcoh	
  +	
  σinc	
  
Coherent	
  and	
  Incoherent	
  ScaAering	
  
More	
  sensi6ve	
  to	
  light	
  elements	
  (H,	
  Li,	
  Bo)	
  	
  
But	
  
	
  Isotopic	
  subs6tu6on	
  ()	
  
	
  H/D	
  exchange	
  	
  
Complexity	
  	
  in	
  the	
  data	
  interpreta6on	
  
à Mul6-­‐techniques	
  approach	
  	
  
	
  	
  	
  	
  	
   	
  
Why	
  neutrons	
  are	
  useful	
  for	
  liquids?	
  
neutrons	
  
X-­‐rays	
  
Bragg law
Radioactive waste disposal
Aqueous Solutions in Confined Systems
Underground	
  Research	
  Laboratory	
  
at	
  Meuse	
  Haute-­‐Marne,	
  ANDRA,	
  
French	
  Na6onal	
  Agency	
  for	
  the	
  
Management	
  of	
  Radioac6ve	
  Waste	
  
Clays have wide environmental applications,
but particularly in waste disposal
Radioactive waste disposal
SiO2	
  
(Network	
  former)	
  
Si-­‐O	
  	
  
Strong	
  bond	
  
Al2O3	
  
(Intermediate	
  element)	
  
Ca/Mg/Na-­‐O	
  
(Network	
  modifier)	
  
Al-­‐O	
  
Less	
  strong	
  
bond	
  
+	
   +	
  
4	
  Bridging	
  oxygens	
  
3	
  Bridging	
  oxygens	
  Strong	
  liquid	
   Fragile	
  liquid	
  
Alumino-­‐silicates	
  	
  	
  	
  	
  	
  	
  Ca/Mg/Na	
  -­‐	
  Al2O3	
  -­‐	
  SiO2	
  
Alumino-­‐silicates	
  
Ca/Mg/Na	
  -­‐	
  Al2O3	
  -­‐	
  SiO2	
  
©	
  Britannica	
  
©	
  D.	
  Neuville	
  
Etna,	
  Sicily	
  
Crust	
  and	
  mantle	
  forma6on,	
  magma6c	
  ocean	
  
Candidate	
  for	
  waste	
  storage	
  
New	
  class	
  of	
  cements	
  
ü Maintain	
  the	
  purity	
  of	
  the	
  sample	
  
ü Access	
  very	
  high	
  temperatures	
  (>	
  3000°C)	
  
ü Absence	
  of	
  heterogeneous	
  nuclea6on	
  
ü Easy	
  access	
  to	
  metastable	
  states	
  
ü Undercooling	
  (Several	
  hundreds	
  degrees	
  below	
  	
  
	
  	
  	
  	
  the	
  mel6ng	
  point)	
  
Aerodynamic	
  levita7on	
  
r (Å)
g(r)
Glass	
  
Ca-­‐O	
  correla6on	
  less	
  pronounced	
  
	
  
Difficult	
  to	
  solve	
  the	
  Ca-­‐O	
  because	
  its	
  mostly	
  
composed	
  by	
  O-­‐O	
  (50%of	
  the	
  total	
  g(r))	
  
	
  
Molecular	
  dynamics	
  model	
  for	
  experimental	
  
data	
  interpreta6on	
  
Ca-­‐O	
  
Liquid	
  
r (Å)
Pair	
  Distribu6on	
  Func6on:	
  
From	
  Molecular	
  
Dynamics	
  calcula6ons	
  	
  
Liquid	
  CA	
  (SiO2	
  =	
  0)	
  
Diffusion	
  coefficient:	
  
D	
  [10-­‐10	
  m2s-­‐1]
1000/T	
  [K]	
  
Arrhenius	
  plot	
  
1-­‐	
  Si	
  atoms	
  have	
  a	
  lower	
  self	
  diffusion	
  
2-­‐	
  Si	
  
SiO4	
  tetrahedra	
  
O,	
  Ca	
  
Dcoherent	
   When	
  SiO2	
  
Introduc6on	
   Instrumenta6on	
   Structure	
   Dynamic	
   Conclusion	
  
•  QENS	
  setup	
  
•  Mul6-­‐nozzle	
  Aero.	
  Lev.	
  
•  Benefits	
  
•  Objec6ves	
  
• Glassy	
  state	
  
• Liquid	
  state	
  
• QENS	
  
• IXS	
  
What	
  is	
  the	
  common	
  point	
  between:	
  
Volcanic	
  lava,	
  Magma,	
  Silicate	
  melt,	
  Glass	
  ?	
  
• Amorphous	
  material	
  
• Disordered	
  at	
  the	
  atomic	
  length	
  scale	
  
• Very	
  high	
  temperature	
  
• SiO2	
  -­‐	
  Al2O3	
  -­‐	
  CaO	
  	
  
How	
  the	
  viscosity	
  of	
  a	
  volcanic	
  lava	
  changes	
  with	
  
temperature?	
  	
  With	
  its	
  chemical	
  composi6on?	
  
©	
  Britannica	
  
©	
  Britannica	
  
©	
  D.	
  Neuville	
  
Etna,	
  Sicily	
  
The liquid state is also an essential stage for
various technological applications:
Metallurgy	
   Op6c	
  fibers	
  
• Design	
  of	
  new	
  glasses	
  (storing	
  nuclear	
  waste,…)	
  
Applica6ons	
  
Aerospace	
  propulsion	
  
3	
  
Crust	
  and	
  mantle	
  forma6on,	
  magma6c	
  ocean	
  
Calcium	
  AluminoSilicate	
  (CAS)	
  
SiO2	
  
(Network	
  former)	
  
Tetrahedral	
  
Si-­‐O	
  
Strong	
  bond	
  
Al2O3	
  
(Intermediate	
  element)	
  
CaO	
  
(Network	
  modifier)	
  
Tetrahedral	
  
Al-­‐O	
  
Less	
  strong	
  bond	
  >>	
  
+	
   +	
  
4	
  Bridging	
  oxygens	
  
3	
  Bridging	
  oxygens	
  
Strong	
  liquid	
   Fragile	
  liquid	
  
4	
  
Introduc6on	
   Instrumenta6on	
   Structure	
   Dynamic	
   Conclusion	
  
•  QENS	
  setup	
  
•  Mul6-­‐nozzle	
  Aero.	
  Lev.	
  
•  Benefits	
  
•  Objec6ves	
  
• Glassy	
  state	
  
• Liquid	
  state	
  
• QENS	
  
• IXS	
  
Objec6ves	
  of	
  this	
  thesis	
  (1)	
  
Two	
  furnaces,	
  same	
  principle!	
  
• High	
  temperatures	
  
• Silicate	
  Melts	
  
Important	
  to	
  be	
  able	
  to	
  study	
  the	
  proper6es	
  of	
  	
  high	
  temperature	
  liquids:	
  
First	
  objec1ve	
  of	
  this	
  thesis:	
  
Develop	
  and	
  Combine	
  
different	
  techniques	
  on	
  large	
  scale	
  
instruments	
  in	
  order	
  to	
  study	
  the	
  
structure	
  and	
  dynamics	
  	
  
of	
  high	
  temperature	
  liquids.	
  
ESRF	
  
ILL	
  
5	
  
Introduc6on	
   Instrumenta6on	
   Structure	
   Dynamic	
   Conclusion	
  
•  QENS	
  setup	
  
•  Mul6-­‐nozzle	
  Aero.	
  Lev.	
  
•  Benefits	
  
•  Objec6ves	
  
• Glassy	
  state	
  
• Liquid	
  state	
  
• QENS	
  
• IXS	
  
Objec6ves	
  of	
  this	
  thesis	
  (2)	
  
Monitor	
  the	
  evolu1on	
  of	
  viscosity	
  η	
  
Study	
  the	
  dynamics	
  
Neutron	
  and	
  X-­‐ray	
  Inelas6c	
  Sca=ering	
  
Angell	
  Plot	
  
Study	
  the	
  structure	
  
(Neutron	
  and	
  X-­‐ray	
  Diffrac6on)	
  
The microscopic mechanisms approaching
the glass transition are still not well
understood:	
   Rapid	
  change	
  in	
  the	
  
dynamical	
  proper6es	
  like	
  the	
  	
  
viscosité	
  (	
  η	
  )	
  
Correlate	
  
Structure	
  	
  and	
  
Dynamics?	
  
Add	
  strong	
  glass	
  former	
  “SiO2”	
  
+	
  
6	
  
Introduc6on	
   Instrumenta6on	
   Structure	
   Dynamic	
   Conclusion	
  
•  QENS	
  setup	
  
•  Mul6-­‐nozzle	
  Aero.	
  Lev.	
  
•  Benefits	
  
•  Objec6ves	
  
• Glassy	
  state	
  
• Liquid	
  state	
  
• QENS	
  
• IXS	
  
The	
  common	
  principle	
  is	
  to	
  apply	
  a	
  force	
  to	
  counteract	
  the	
  
gravity	
  
G	
  
F	
  
Various	
  levita7on	
  techniques	
  have	
  been	
  developed	
  
Levita7on	
  techniques	
  
Electromagne6c	
  field	
  
Electrosta6c	
  field	
  
Acous6c	
  wave	
  
Gas	
  flow	
   Gas	
  film	
  levita6on	
  
	
  
Aerodynamic	
  levita1on	
  	
  
Possible	
  to	
  reach	
  very	
  high	
  liquid	
  temperatures	
  (>3000°C)	
  
No	
  container	
  effect	
  
These	
  methods	
  maintain	
  the	
  sample	
  purity	
  
Easy	
  access	
  to	
  the	
  supercooled	
  state	
  	
  	
  
Advantages	
  :	
  
(few	
  hundred	
  degrees	
  below	
  the	
  mel6ng	
  point)	
  	
  
Limita6ons	
  for	
  QENS	
  
X-­‐rays:	
  
Diffrac6on	
  
Inelas6c	
  Sca=ering	
  
o 	
  Flux	
  of	
  X-­‐ray	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  >>	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  Flux	
  of	
  Neutrons	
  
o 	
  Current	
  configura6on:	
  Half	
  of	
  the	
  sample	
  is	
  s6ll	
  masked	
  by	
  the	
  nozzle.	
  
Neutrons:	
  
Diffrac6on	
  
Inelas6c	
  Sca=ering	
  
1.	
  Bigger	
  diameter	
  
2.	
  Levitated	
  completely	
  outside	
  the	
  nozzle	
  
Sample:	
  
Diameter	
  ∼	
  2.7	
  mm	
  
9	
  
Introduc6on	
   Instrumenta6on	
   Structure	
   Dynamic	
   Conclusion	
  
•  QENS	
  setup	
  
•  Mul6-­‐nozzle	
  Aero.	
  Lev.	
  
•  Benefits	
  
•  Objec6ves	
  
• Glassy	
  state	
  
• Liquid	
  state	
  
• QENS	
  
• IXS	
  

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Viviana Cristiglio (May 27th 2014)

  • 1. Probing  materials  at  ILL:  an  overview  of  structure   inves7ga7on  with  neutrons   Viviana  CRISTIGLIO   Instrument  Scien6st  at  the  Ins6tut  Laue  Langevin       -­‐  Neutrons  science  at  high  T   -­‐   Carbon  nanotubes   -­‐   Li  ba=eries     Industrial  materials,  Energy  
  • 2. The  liquid  state  is  fundament  state  of  the  ma=er  and  is  an   essen6al  stage  for  various  technological  applica1ons   Metallurgy   Op6c  fibers   Aerospace  propulsion   Why  do  we  need  HT?   Glass  making  :  from  liquid  to  glass  by  quenching     Design  of  new  glasses  :  Storing  nuclear  waste     Food  and  drink   Chemistry,   Pharmaceu6cs,   Cosme6cs  
  • 3. Structure  of  Liquids  by  diffrac6on   Unlike  crystals,  the  structural  informa6on  for  liquids  and  glasses  is  described  in  terms  of:   1.  Probabilis6c  atomic  distribu6on  func6ons.   2.  Mean  atomic  distribu6on  around  each  chemical   species   given   by   the   Pair   Distribu6on   Func6on       g(r).   g(r)   is   the   probability   to   find   an   atom   at   a   distance  r  from  another  taken  at  the  origin   Interatomic  distances   Coordina6on  number  
  • 4. Spa6al  distribu6on   of  atoms  or   molecules  in  the   system   Crystalline  solids   Equilibrium  posi6ons   Well  defined  Bragg  peaks   Amorphous   Distribu6on  of  equilibrium     posi6ons          No  Bragg  peaks   Structure of Crystalline and Amorphous Solids
  • 5. Diffusive   Mo6ons   Internal     Dynamics   Structural  informa7on   Collec6ve  dynamics   Coherent   σcoh   4π   Incoherent   σinc   4π   Sca=ering  cross  sec6on   σ  =  σcoh  +  σinc   Coherent  and  Incoherent  ScaAering  
  • 6. More  sensi6ve  to  light  elements  (H,  Li,  Bo)     But    Isotopic  subs6tu6on  ()    H/D  exchange     Complexity    in  the  data  interpreta6on   à Mul6-­‐techniques  approach                 Why  neutrons  are  useful  for  liquids?   neutrons   X-­‐rays   Bragg law
  • 8. Aqueous Solutions in Confined Systems Underground  Research  Laboratory   at  Meuse  Haute-­‐Marne,  ANDRA,   French  Na6onal  Agency  for  the   Management  of  Radioac6ve  Waste   Clays have wide environmental applications, but particularly in waste disposal Radioactive waste disposal
  • 9. SiO2   (Network  former)   Si-­‐O     Strong  bond   Al2O3   (Intermediate  element)   Ca/Mg/Na-­‐O   (Network  modifier)   Al-­‐O   Less  strong   bond   +   +   4  Bridging  oxygens   3  Bridging  oxygens  Strong  liquid   Fragile  liquid   Alumino-­‐silicates              Ca/Mg/Na  -­‐  Al2O3  -­‐  SiO2  
  • 10. Alumino-­‐silicates   Ca/Mg/Na  -­‐  Al2O3  -­‐  SiO2   ©  Britannica   ©  D.  Neuville   Etna,  Sicily   Crust  and  mantle  forma6on,  magma6c  ocean   Candidate  for  waste  storage   New  class  of  cements  
  • 11. ü Maintain  the  purity  of  the  sample   ü Access  very  high  temperatures  (>  3000°C)   ü Absence  of  heterogeneous  nuclea6on   ü Easy  access  to  metastable  states   ü Undercooling  (Several  hundreds  degrees  below            the  mel6ng  point)   Aerodynamic  levita7on  
  • 12. r (Å) g(r) Glass   Ca-­‐O  correla6on  less  pronounced     Difficult  to  solve  the  Ca-­‐O  because  its  mostly   composed  by  O-­‐O  (50%of  the  total  g(r))     Molecular  dynamics  model  for  experimental   data  interpreta6on   Ca-­‐O   Liquid   r (Å) Pair  Distribu6on  Func6on:   From  Molecular   Dynamics  calcula6ons     Liquid  CA  (SiO2  =  0)  
  • 13. Diffusion  coefficient:   D  [10-­‐10  m2s-­‐1] 1000/T  [K]   Arrhenius  plot   1-­‐  Si  atoms  have  a  lower  self  diffusion   2-­‐  Si   SiO4  tetrahedra   O,  Ca   Dcoherent   When  SiO2  
  • 14. Introduc6on   Instrumenta6on   Structure   Dynamic   Conclusion   •  QENS  setup   •  Mul6-­‐nozzle  Aero.  Lev.   •  Benefits   •  Objec6ves   • Glassy  state   • Liquid  state   • QENS   • IXS   What  is  the  common  point  between:   Volcanic  lava,  Magma,  Silicate  melt,  Glass  ?   • Amorphous  material   • Disordered  at  the  atomic  length  scale   • Very  high  temperature   • SiO2  -­‐  Al2O3  -­‐  CaO     How  the  viscosity  of  a  volcanic  lava  changes  with   temperature?    With  its  chemical  composi6on?   ©  Britannica   ©  Britannica   ©  D.  Neuville   Etna,  Sicily   The liquid state is also an essential stage for various technological applications: Metallurgy   Op6c  fibers   • Design  of  new  glasses  (storing  nuclear  waste,…)   Applica6ons   Aerospace  propulsion   3   Crust  and  mantle  forma6on,  magma6c  ocean  
  • 15. Calcium  AluminoSilicate  (CAS)   SiO2   (Network  former)   Tetrahedral   Si-­‐O   Strong  bond   Al2O3   (Intermediate  element)   CaO   (Network  modifier)   Tetrahedral   Al-­‐O   Less  strong  bond  >>   +   +   4  Bridging  oxygens   3  Bridging  oxygens   Strong  liquid   Fragile  liquid   4   Introduc6on   Instrumenta6on   Structure   Dynamic   Conclusion   •  QENS  setup   •  Mul6-­‐nozzle  Aero.  Lev.   •  Benefits   •  Objec6ves   • Glassy  state   • Liquid  state   • QENS   • IXS  
  • 16. Objec6ves  of  this  thesis  (1)   Two  furnaces,  same  principle!   • High  temperatures   • Silicate  Melts   Important  to  be  able  to  study  the  proper6es  of    high  temperature  liquids:   First  objec1ve  of  this  thesis:   Develop  and  Combine   different  techniques  on  large  scale   instruments  in  order  to  study  the   structure  and  dynamics     of  high  temperature  liquids.   ESRF   ILL   5   Introduc6on   Instrumenta6on   Structure   Dynamic   Conclusion   •  QENS  setup   •  Mul6-­‐nozzle  Aero.  Lev.   •  Benefits   •  Objec6ves   • Glassy  state   • Liquid  state   • QENS   • IXS  
  • 17. Objec6ves  of  this  thesis  (2)   Monitor  the  evolu1on  of  viscosity  η   Study  the  dynamics   Neutron  and  X-­‐ray  Inelas6c  Sca=ering   Angell  Plot   Study  the  structure   (Neutron  and  X-­‐ray  Diffrac6on)   The microscopic mechanisms approaching the glass transition are still not well understood:   Rapid  change  in  the   dynamical  proper6es  like  the     viscosité  (  η  )   Correlate   Structure    and   Dynamics?   Add  strong  glass  former  “SiO2”   +   6   Introduc6on   Instrumenta6on   Structure   Dynamic   Conclusion   •  QENS  setup   •  Mul6-­‐nozzle  Aero.  Lev.   •  Benefits   •  Objec6ves   • Glassy  state   • Liquid  state   • QENS   • IXS  
  • 18. The  common  principle  is  to  apply  a  force  to  counteract  the   gravity   G   F   Various  levita7on  techniques  have  been  developed   Levita7on  techniques   Electromagne6c  field   Electrosta6c  field   Acous6c  wave   Gas  flow   Gas  film  levita6on     Aerodynamic  levita1on     Possible  to  reach  very  high  liquid  temperatures  (>3000°C)   No  container  effect   These  methods  maintain  the  sample  purity   Easy  access  to  the  supercooled  state       Advantages  :   (few  hundred  degrees  below  the  mel6ng  point)    
  • 19. Limita6ons  for  QENS   X-­‐rays:   Diffrac6on   Inelas6c  Sca=ering   o   Flux  of  X-­‐ray                              >>                              Flux  of  Neutrons   o   Current  configura6on:  Half  of  the  sample  is  s6ll  masked  by  the  nozzle.   Neutrons:   Diffrac6on   Inelas6c  Sca=ering   1.  Bigger  diameter   2.  Levitated  completely  outside  the  nozzle   Sample:   Diameter  ∼  2.7  mm   9   Introduc6on   Instrumenta6on   Structure   Dynamic   Conclusion   •  QENS  setup   •  Mul6-­‐nozzle  Aero.  Lev.   •  Benefits   •  Objec6ves   • Glassy  state   • Liquid  state   • QENS   • IXS