220 likes | 244 Views
NanoCTM final network meeting and workshop Poznań, 23-27 September 2013. Spin thermopower in the overscreened Kondo model. Tomaž Rejec, Rok Žitko, Jernej Mravlje and Anton Ramšak Department of Physics, University of Ljubljana Jožef Stefan Institute, Ljubljana. Outline.
E N D
NanoCTM final network meeting and workshop Poznań, 23-27 September 2013 Spin thermopower in the overscreened Kondo model Tomaž Rejec, Rok Žitko, Jernej Mravlje and Anton Ramšak Department of Physics, University of Ljubljana Jožef Stefan Institute, Ljubljana
Outline • Spin-Seebeck coefficient • Kondo models (fully screened, underscreened, overscreened) • NRG results
Spin-Seebeck coefficient TL=TR L V=0 R
Spin-Seebeck coefficient TL=TR L V≠0 R
Spin-Seebeck coefficient TL=TR L V≠0 R
Spin-Seebeck coefficient TL>TR L V=0 R
Spin-Seebeck coefficient TL>TR L V=0 R
Spin-Seebeck coefficient TL>TR L ed≠0 V=0 R
Spin-Seebeck coefficient TL>TR L ed≠0 V≠0 R Seebeck coefficient
Spin-Seebeck coefficient TL>TR L B≠0 V=0 R
Spin-Seebeck coefficient TL>TR L B≠0 V=0 R Spin current!
Spin-Seebeck coefficient TL>TR L B≠0 Vs≠0 R Spin-Seebeck coefficient Spin voltage:
Spin-Seebeck coefficient For small DT, Vs: Non-interacting QD: B>G B=G B<G
Kondo models NFL: J1=J2 : overscreened Kondo effect
Kondo models S=1/2; i=1 : fully screened Kondo model S=1/2; i=1,2 : overscreened Kondo model S=1; i=1 : underscreened Kondo model
Results – fully screened Kondo model B=TK B>G B=G B<G
Summary • Measuring the spin thermopower at low magentic fields would provide a sensitive test for distinguishing between fully screened, underscreened and overscreened Kondo behaviour • Possible applications: generation of spin current for spintronics applications, sensitive measurement of low magnetic fields