the 6th school on simulation and modeling physics "ab-initio methods and their...

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Tue.27 Nov. Wed.28 Nov. Thu.29 Nov. 8h30 - 9h45 Topical lecture Planets / High Pressure Topical lecture Atmospheric physics Methods: Ab-initio Molecular Dynamics 9h45 - 10h15 Coffee break 10h15 -11h30 Methods Plane waves, cut-off, k- points, pseudopotentials, DFT, etc Seminars Computer Lab 3 11h30 – 13h30 Lunch time 13h30 – 16h00 Computer Lab 1 Computer Lab 2 Computer Lab 4 he 6th School on Simulation and Modeling Physics Ab-initio methods and their applications" anoi, 27 - 29 November 2007

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The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications" Hanoi, 27 - 29 November 2007. Exploring planetary interiors by ab-initio molecular dynamics. 6 th SMP, Hanoi, Nov 27-29, 2007 Sandro Scandolo (the Abdus Salam ICTP, Trieste, Italy). - PowerPoint PPT Presentation

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Page 1: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

  Tue.27 Nov. Wed.28 Nov. Thu.29 Nov.

8h30 - 9h45Topical lecture

Planets / High PressureTopical lecture

Atmospheric physics

Methods: Ab-initio Molecular

Dynamics

9h45 - 10h15 Coffee break

10h15 -11h30Methods

Plane waves, cut-off, k-points, pseudopotentials, DFT, etc

Seminars Computer Lab 3

11h30 – 13h30 Lunch time

13h30 – 16h00 Computer Lab 1 Computer Lab 2 Computer Lab 4

The 6th School on Simulation and Modeling Physics"Ab-initio methods and their applications" Hanoi, 27 - 29 November 2007

Page 2: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

Exploring planetary interiors by ab-initio molecular dynamics

6th SMP, Hanoi, Nov 27-29, 2007

Sandro Scandolo(the Abdus Salam ICTP, Trieste, Italy)

Page 3: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

The Abdus Salam International Centre for Theoretical Physics(under UNESCO / IAEA), Trieste, Italy

ICTP’s mission:

To foster the growth of advanced studies and research in physics and mathematics, especially among researchers from developing countries

Opportunities

- Conferences / Schools throughout the year

- Associates (our faculty “in the field”)

- Visitors (junior, STEP, TRIL, etc)

- Diploma Course

www.ictp.it

Page 4: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

Materials SciencePlanetary Science

High pressure in

1951: the first man-made diamonds

1991: Earth’s core conditionsreproduced in the laboratory

Page 5: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

Shock waves Diamond anvil cell

Page 6: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

Approximations

- Born-Oppenheimer - Classical nuclei- Density functional theory

from “first principles”

Variable-cell molecular dynamics

[Parrinello & Rahman, 1981]

Page 7: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

Outline

High Pressure in Materials Science:

+ “Carbonia”: a silica-like CO2 amorph+ Novel transition metal nitrides

High pressure in Planetary Science:

+ Carbon in planetary interiors+ Melting of iron

Page 8: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

Silica-like CO2 : the crystal phases

+ Molecular CO2 predicted to tranform into a silica-like crystal at high pressure

+ Silica-like phases of CO2 predicted to be ultrahard

Molecular CO2 Candidate theoretical structures for silica-like CO2

Serra, Cavazzoni, Chiarotti, Scandolo, Tosatti, Science 284, 788 (1999)

Crystal structure of silica-like CO2

not yet determined

Is there a glass analog?

Experimental confirmation of silica-like CO2

Yoo et al, Science 283, 1510 (1999)

Page 9: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

“Carbonia”: the silica-like CO2 glass

Experimental evidence for amorphous CO2

Santoro, Gorelli, Bini, Ruocco, Scandolo, Crichton,Nature, in press (2006)

Compression by ab-initio molecular dynamics gives:

At 1000 K and 100 GPa: a crystalline phase

At 2000 K and 80 GPa: an amorphous phase

Octahedral CO6Tetrahedral CO4

Page 10: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

Platinum nitride: PtN or PtN2?

Raman shift (cm-1)

Gregoryanz et al, Nature Mat. (2004)Crowhurst et al, Science (2006)

Ab-initio calculations on structures with 1:1 stoichiometry fail to reproduce the experimentalRaman spectra

Single-bonded polymeric nitrogen

Eremets et al, Nature Mat. (2004)

Molecular N2

Polymeric N

Page 11: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

Platinum nitride: PtN2 pyriteYoung, Montoya, Lazzeri, Sanloup, Gregoryanz, Scandolo, PRB 2006

Raman spectra

X-ray diffraction

Page 12: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

MN2 with interstitial N2 units: a new class of transition metal nitrides?

Young, Sanloup, Gregoryanz, Scandolo, Hemley, Mao, PRL 96, 155501 (2006)

IrN2

Single bonded N-N

PtN2 pyrite

New “heavy” metal nitrides are superhard

Bulk modulus: 428 GPa (IrN2), 358 GPa (OsN2)

Page 13: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

H2O+CH4+NH3

Marvin Ross, “Diamonds in the sky”Nature (1981)

Methane was found to dissociate under a shock wave

Scandolo & Jeanloz, American Scientist (2003)

Page 14: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

Methane dissociation: what do simulations say

F. Ancilotto et al., Science 275, 1288 (1997)

Compressed methane Compressed methaneheated up to 4000 K

Page 15: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

Before compression After compression

Methane dissociation: the experimental confirmationL.R. Benedetti et al., Science 283, 100 (1999)

Page 16: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

Melting of Carbon

diamond liquid

BC8, SC ??

Neptune and Uranus isentrope

X. Wang, S. Scandolo, R. Car, Phys. Rev. Lett 2005

3.8

4.3

4.7

5.2

5.3-5.8

Coordination number

Page 17: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

Accuracy of DFT?: Melting of silicon

Solid

Liquid

Tm(LDA) = 1380 KTm(GGA) = 1520 KTm(meta-GGA) = 1700 K

Tm(experiment) = 1687 K

X. Wang, S. Scandolo, R. Car

Page 18: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

How hot is the centre of the Earth?

liqui

dso

lid

Inner core (solid Fe) Outer core

(liquid Fe)

Mantle

The temperature at the inner core boundary coincides with the melting temperature of Fe at 330 GPa

Page 19: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

The “optimized” potential method

“Optimized” potential at P,T

A. Laio et al, Science 287, 1027 (2000)

Page 20: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

Melting of Iron at Earth’s core pressures

Inner-Outer core boundary

A. Laio et al, Science 287, 1027 (2000)

Our results

Shock waveexperiments

Static experiments

DFT-basedcalculation byAlfe’ et al

Page 21: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

D. Stevenson, Nature 423, 239 (2003)

Page 22: The 6th School on Simulation and Modeling Physics "Ab-initio methods and their applications"

The crew:J. MontoyaA. YoungR. RousseauC. CavazzoniY. LiangX. WangA. LaioR. Car….www.quantum-espresso.org