First Principles Investigations of Plutonium Americium and their

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First Principles Investigations of Plutonium Americium and their Mixtures using Dynamical Mean Field Theory

First Principles Investigations of Plutonium Americium and their Mixtures using Dynamical Mean Field Theory Gabriel. Kotliar Physics Department and Center for Materials Theory Rutgers University. Funded by : DOE BES and NNSA. Washington February 5 -8 (2007).

Outline and Conclusion • First Principles Computations of Actinides. • DMFT Results for Plutonium

Outline and Conclusion • First Principles Computations of Actinides. • DMFT Results for Plutonium and Americium • Preliminary Results for compounds Pu. O 2, Pu. 5 Am. 5. • Mott transition in the actinide series: important science problem. • New theoretical methodologies developed at Universities. DMFT concepts, allow close interaction with experimentalists, key validation and progress.

Computational Approach to a First Principles Description of the Actinides must include • Relativistic

Computational Approach to a First Principles Description of the Actinides must include • Relativistic Effects, Spin Orbit Coupling • Realistic band structure, complex structures • Atomic Multiplet effects (F 0 F 2 F 4 F 6) • Treat localization –delocalization on the same footing. • LDA+DMFT. Compute total energies from a functional of the photoemission spectra.

DMFT Phonons in fcc d-Pu C 11 (GPa) C 44 (GPa) C 12 (GPa)

DMFT Phonons in fcc d-Pu C 11 (GPa) C 44 (GPa) C 12 (GPa) C'(GPa) Theory 34. 56 33. 03 26. 81 3. 88 Experiment 36. 28 33. 59 26. 73 4. 78 ( Dai, Savrasov, Kotliar, Ledbetter, Migliori, Abrahams, Science, 9 May 2003) (experiments from Wong et. al, Science, 22 August 2003)

Volume and Spectra alpa->delta volume collapse transition F 0=4, F 2=6. 1 F 0=4.

Volume and Spectra alpa->delta volume collapse transition F 0=4, F 2=6. 1 F 0=4. 5, F 2=7. 15 Gouder Havela Lander

Americium f 6 -> L=3, S=3, J=0 Mott Transition? "soft" phase f localized "hard"

Americium f 6 -> L=3, S=3, J=0 Mott Transition? "soft" phase f localized "hard" phase f bonding A. Lindbaum, S. Heathman, K. Litfin, and Y. Méresse, Phys. Rev. B 63, 214101 (2001) J. -C. Griveau, J. Rebizant, G. H. Lander, and G. Kotliar Phys. Rev. Lett. 94, 097002 (2005)

Am within LDA+DMFT Large multiple effects: F(0)=4. 5 e. V S. Y. Savrasov, K.

Am within LDA+DMFT Large multiple effects: F(0)=4. 5 e. V S. Y. Savrasov, K. Haule, and G. Kotliar Phys. Rev. Lett. 96, 036404 (2006) F(2)=8. 0 e. V F(4)=5. 4 e. V F(6)=4. 0 e. V

Probe for Valence and Multiplet structure: EELS&XAS 5 f 7/2 A plot of the

Probe for Valence and Multiplet structure: EELS&XAS 5 f 7/2 A plot of the X-ray absorption as a function of energy 5 f 5/2 4 d 5/2 ->5 f 7/2 hv 4 d 3/2 4 d 5/2 Core splitting~50 e. V Excitations from 4 d core to 5 f valence core valence Electron energy loss spectroscopy (EELS) or X-ray absorption spectroscopy (XAS) B=B 0 - 4/15<l. s>/(14 -nf) 4 d 3/2 ->5 f 5/2 Core splitting~50 e. V Energy loss [e. V] Branching ratio B=A 5/2/(A 5/2+A 3/2)

From J. Shim K. Haule and G. Kotliar to appear in Nature. B=B 0

From J. Shim K. Haule and G. Kotliar to appear in Nature. B=B 0 - 4/15<l. s>/(14 -nf) B 0 = (3/5) (for d->f transitions)

B=B 0 - 4/15<l. s>/(14 -nf) LDA+DMFT One measured quantity B, two unknowns Close

B=B 0 - 4/15<l. s>/(14 -nf) LDA+DMFT One measured quantity B, two unknowns Close to atom (IC regime) Itinerancy tends to decrease <l. s> [a] G. Van der Laan et al. , PRL 93, 97401 (2004). [b] G. Kalkowski et al. , PRB 35, 2667 (1987) [c] K. T. Moore et al. , PRB 73, 33109 (2006).

First results on Compounds, Pu. O 2, Pu-Am mixture, 50%Pu, 50%Am Lattice expands ->

First results on Compounds, Pu. O 2, Pu-Am mixture, 50%Pu, 50%Am Lattice expands -> Kondo collapse is expected charge transfer Pu d phase stabilized by shift to mixed valence nf~5. 2 ->nf~5. 4 Hybridization decreases, but nf increases, Tk does not change significantly!

Outline and Conclusion • First Principles Computations of Actinides. • DMFT Results for Plutonium

Outline and Conclusion • First Principles Computations of Actinides. • DMFT Results for Plutonium and Americium • Preliminary Results for compounds Pu. O 2, Pu. 5 Am. 5. • Mott transition in the actinide series: important science problem. • New theoretical methodologies developed at Universities. DMFT concepts, allow close interaction with experimentalists, key validation and progress.

Acknowlegment References-Collaborators • Electronic correlations in metallic Plutonium within dynamical meanfield picture: S. Savrasov,

Acknowlegment References-Collaborators • Electronic correlations in metallic Plutonium within dynamical meanfield picture: S. Savrasov, G. Kotliar, and E. Abrahams, Nature 410, 793 (2001). • Calculated Phonon Spectra of Plutonium at High Temperatures: X. Dai, S. Y. Savrasov, G. Kotliar, A. Migliori, H. Ledbetter, and E. Abrahams, Science 300, 953 -955 (2003). • Many-Body Electronic Structure of Americium metal: Sergej Y. Savrasov, Kristjan Haule, Gabriel Kotliar, Phys. Rev. Lett. 96, 036404 (2006). • J. Shim K. Haule and G. Kotliar , Fluctuating valence in a correlated solid and the anomalous properties of delta-plutonium: to appear in Nature next month. Experimentalists: LANL: A. Migliori, (resonant ultrasound) J. Singleton (magnetotrasnport ) J. Thompson, (EELS X-Ray J. Joyce (Photoemission), J. Lashley (specific heat) Livermore: J. Wong (X Ray scattering) K. Moore J. Tobin (EELS and XAS ) M. Fluss (transport) ITU: . L. Havela J. C. Griveaux and G. Lander (transport under pressure )