Survey
* Your assessment is very important for improving the work of artificial intelligence, which forms the content of this project
* Your assessment is very important for improving the work of artificial intelligence, which forms the content of this project
Tuning the quantum critical point by Mn impurities and chemical pressure in LaFeAsO0.89F0.11 Samuele Sanna Physics Department University of PAVIA, Italy Sanna, SIF2015, 24th September 2015 Coworkers P. Carretta, M. Moroni University of PAVIA, Italy R. De Renzi, P.Bonfà, S. Bordignon, G. Allodi Univ. of PARMA, Italy F. Hammerath, B. Büchner, G. Prando, R. Kappenberger, S. J. Singh, S. Wurmehl IFW Dresden, Germany M. Moroni Univ. Pavia F. Hammerath R. Kappenberger IFW Dresden IFW Dresden Sanna, SIF2015, 24th September 2015 T. Shiroka, ETH, Zürich, Switzerland Y. Kobayashi, M. Sato, Nagoya University, Japan G. Lamura, M. Putti CNR-SPIN and Univ. of GENOVA, Italy P. Carretta Univ. Pavia R. De Renzi Univ. Parma Tuning magnetism and superconductivity in 1111 REFeAsO (RE1111) RE Charge doping, e.g. F O Hydrostatic pressure Chemical pressure Substitution Mn Fe Sanna, SIF2015, 24th September 2015 FO REFeAsO: e- charge doping RE = La Luetkens et al, Nature Materials (2009) RE = Sm Sanna et al, PRB 80, 052503 (2009) LaFeAsO1-xFx SmFeAsO1-xFx SDW Sanna, SIF2015, 24th September 2015 Fe/Mn substitution in optimally F-doped RE1111 SmFeAsO1-zFz Hammerat PRB 92, 020505(R) (2015) Sanna PRB (2009) Sm La0.8Y0.2 La Mn is a poison for SC in RE=La ! Less than 0.2%of Mn is enough to kill SC Process heavily affected by chemical pressure Sanna, SIF2015, 24th September 2015 Fe/Mn substitution in optimally F-doped RE1111 LaFe1-xMnxAsO0.89F0.11 x=0-0.002 ≈ isoelectronic conditions Mn Magnetic SC Sato et al., JPSJ 79, 014710 (2010) Resistivity is rapidly increased Charge localization by Mn Hammerath et al. PRB 89, 134503 (2014) Mn quickly restores static magnetism Sanna, SIF2015, 24th September 2015 Evidence for a QCP LaFe1-xMnxAsO0.89F0.11 Magnetic correlation length x=0-0.002 ≈ isoelectronic conditions Magnetic SC Hammerath et al. PRB 89, 134503 (2014) 2D AFM spin fluctuations @ QCP LaFeAsO0.89F0.11 very close to a QCP! Sanna, SIF2015, 24th September 2015 Chemical pressure and Mn impurity effects unpublished Mn drives the system through a QCP Chemical pressure moves the QCP away Magnetic correlations depressed by a smaller ion Why ? For stripe collinear order magnetism enhanced for smaller RE Q=(p/a, 0) Giovannetti Nat. Commun. 2, 398 (2011) Orthomagnetic order induced by Mn ? Gastiasoro & Andersen, PRL 113, 067002 (2014) Sanna, SIF2015, 24th September 2015 Nanoscopic coexistence Q=(p/a, p/a) Chemical pressure and Mn impurity effects unpublished Mn drives the system through a QCP Chemical pressure moves the QCP away Superconductivity suppressed by Mn Why ? 1) Mn suppresses (p/a, 0) fluctuations which sustain superconductivity 2) Mn induces charge localization 3) Mn pins the stripes Hammerat PRB 92, 020505(R) (2015) Sanna, SIF2015, 24th September 2015 Nanoscopic coexistence Main conclusions (and questions) REFe1-xMnxAsO0.89F0.11 optimally F-doped • Mn is a poison for SC in La1111 (xc=0.002 !) possible orthomagnetic order? • Chemical pressure moves away the QCP why ?? PRB 89, 134503 (2014) PRB 92, 020505(R) (2015) Sanna, SIF2015, 24th September 2015