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Filippone, Michele, Moca, Cătălin Paşcu, von Delft, Jan, Mora, Christophe (2017) At which magnetic field, exactly, does the Kondo resonance begin to split? A Fermi liquid description of the low-energy properties of the Anderson model. Physical Review B, 95 (16) doi:10.1103/physrevb.95.165404

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Reference TypeJournal (article/letter/editorial)
TitleAt which magnetic field, exactly, does the Kondo resonance begin to split? A Fermi liquid description of the low-energy properties of the Anderson model
JournalPhysical Review B
AuthorsFilippone, MicheleAuthor
Moca, Cătălin PaşcuAuthor
von Delft, JanAuthor
Mora, ChristopheAuthor
Year2017 (April 5)Volume95
Issue16
PublisherAmerican Physical Society (APS)
DOIdoi:10.1103/physrevb.95.165404Search in ResearchGate
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Mindat Ref. ID14245800Long-form Identifiermindat:1:5:14245800:8
GUID0
Full ReferenceFilippone, Michele, Moca, Cătălin Paşcu, von Delft, Jan, Mora, Christophe (2017) At which magnetic field, exactly, does the Kondo resonance begin to split? A Fermi liquid description of the low-energy properties of the Anderson model. Physical Review B, 95 (16) doi:10.1103/physrevb.95.165404
Plain TextFilippone, Michele, Moca, Cătălin Paşcu, von Delft, Jan, Mora, Christophe (2017) At which magnetic field, exactly, does the Kondo resonance begin to split? A Fermi liquid description of the low-energy properties of the Anderson model. Physical Review B, 95 (16) doi:10.1103/physrevb.95.165404
In(2017, April) Physical Review B Vol. 95 (16) American Physical Society (APS)

See Also

These are possibly similar items as determined by title/reference text matching only.

Filippone, Michele, Moca, Cătălin Paşcu, Weichselbaum, Andreas, von Delft, Jan, Mora, Christophe (2018) At which magnetic field, exactly, does the Kondo resonance begin to split? A Fermi liquid description of the low-energy properties of the Anderson model. Physical Review B, 98 (7) doi:10.1103/physrevb.98.075404
Filippone, Michele, Moca, Cătălin Paşcu, von Delft, Jan, Mora, Christophe (2018) Retraction: At which magnetic field, exactly, does the Kondo resonance begin to split? A Fermi liquid description of the low-energy properties of the Anderson model [Phys. Rev. B 95 , 165404 (2017)]. Physical Review B, 98 (7) doi:10.1103/physrevb.98.079902
Mora, Christophe, Moca, Cătălin Paşcu, von Delft, Jan, Zaránd, Gergely (2015) Fermi-liquid theory for the single-impurity Anderson model. Physical Review B, 92 (7) doi:10.1103/physrevb.92.075120
Filippone, Michele, Moca, Cătălin Paşcu, Zaránd, Gergely, Mora, Christophe (2014) Kondo temperature of SU(4) symmetric quantum dots. Physical Review B, 90 (12) doi:10.1103/physrevb.90.121406
Moca, Cătălin Paşcu, Alex, Arne, von Delft, Jan, Zaránd, Gergely (2012) SU(3) Anderson impurity model: A numerical renormalization group approach exploiting non-Abelian symmetries. Physical Review B, 86 (19) doi:10.1103/physrevb.86.195128
Moca, Cătălin Paşcu, Mora, Christophe, Weymann, Ireneusz, Zaránd, Gergely (2018) Noise of a Chargeless Fermi Liquid. Physical Review Letters, 120 (1). doi:10.1103/physrevlett.120.016803
Filippone, Michele, Mora, Christophe (2012) Fermi liquid approach to the quantumRCcircuit: Renormalization group analysis of the Anderson and Coulomb blockade models. Physical Review B, 86 (12) doi:10.1103/physrevb.86.125311
Karki, D. B., Mora, Christophe, von Delft, Jan, Kiselev, Mikhail N. (2018) Two-color Fermi-liquid theory for transport through a multilevel Kondo impurity. Physical Review B, 97 (19) doi:10.1103/physrevb.97.195403
Moca, Cătălin Paşcu, Chirla, Razvan, Dóra, Balázs, Zaránd, Gergely (2019) Quantum Criticality and Formation of a Singular Fermi Liquid in the Attractive SU(N>2) Anderson Model. Physical Review Letters, 123 (13). doi:10.1103/physrevlett.123.136803
Moca, Cătălin Paşcu (2002) Calculation of the penetration depth inMgB2. Physical Review B, 65 (13) doi:10.1103/physrevb.65.132509
Chirla, Razvan, Dinu, I. V., Moldoveanu, V., Moca, Cătălin Paşcu (2014) Transport in a hybrid normal metal/topological superconductor Kondo model. Physical Review B, 90 (19) doi:10.1103/physrevb.90.195108
 
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