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Correction: Electron-electron scattering and thermal conductivity of epsilon-iron at Earths core conditions (vol 19, 073022, 2017)

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CORRIGENDUM • OPEN ACCESS

Corrigendum: Electron–electron scattering and thermal conductivity of

-iron at Earth's core conditions (2017 New J. Phys.

19 073022

)

To cite this article: L V Pourovskii et al 2018 New J. Phys. 20 109501

View the article online for updates and enhancements.

(2)

New J. Phys. 20 (2018) 109501 https://doi.org/10.1088/1367-2630/aae6e1

CORRIGENDUM

Corrigendum: Electron

–electron scattering and thermal conductivity

of

ò-iron at Earthʼs core conditions (2017 New J. Phys.

19

073022)

L V Pourovskii1,2,3, J Mravlje4, A Georges1,2,5, S I Simak6and I A Abrikosov3,6 1 CPHT, Ecole Polytechnique, CNRS, Université Paris-Saclay, Route de Saclay, F-91128 Palaiseau, France 2 Collège de France, 11 place Marcelin Berthelot, F-75005 Paris, France

3 Materials Modeling and Development Laboratory, National University of Science and Technology‘MISIS’, Moscow, Russia 4 Jozef Stefan Institute, SI-1000, Ljubljana, Slovenija

5 Department of Quantum Matter Physics, University of Geneva, 24 Quai Ernest-Ansermet, 1211 Geneva 4, Switzerland 6 Department of Physics, Chemistry and Biology(IFM), Linköping University, SE-58183 Linköping, Sweden

On page 5, the caption offigure 3 should read:

Figure 3.Calculated electron–electron-scattering contribution to the electrical and thermal resistivity of hcp iron at Earth’s core density. (a) Electrical resistivity. Blue filled circles and hashed squares are our DFT +DMFT results forrxxandrzz, respectively. Green empty and hashed diamonds are the corresponding

resistivities calculated by the Boltzmann-transport code BoltzTrap(Madsen G K and Singh D J 2006 Comput. Phys. Commun.175 67) assuming a Fermi-liquid withG Z=0.09 eV.(b) Thermal conductivity. Blue filled circles and hashed squares are DFT+DMFT results fork andxx k , respectively. Green lineszz /symbols are the

corresponding conductivities obtained from our calculated electrical conductivity using the Wiedemann–Franz law with the standard Lorenz number of 2.44× 10−8WΩK−2.

The legend of thisfigure is correct. OPEN ACCESS

RECEIVED

24 September 2018

ACCEPTED FOR PUBLICATION

9 October 2018

PUBLISHED

19 October 2018

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Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.

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