High bias anomaly in YBa 2 Cu 3 O 7 /LaMnO 3+δ /YBa 2 Cu 3 O 7 Superconductor/Ferromagnetic Insulator/Superconductor junctions: Evidence for a long-range superconducting proximity effect through the conduction band of a ferromagnetic insulator. We study the perpendicular transport characteristics of small superconductor/ ferromagnetic insulator/ superconductor (YBa2Cu3O7−x/ LaMnO 3+δ / YBa2Cu3O7−x) tunnel junctions. At a large bias voltage V ∼ 1 V we observe a step-like onset of excess current that occurs below the superconducting transition temperature T < Tc and is easily suppressed by a magnetic field. The phenomenon is attributed to a novel type of the superconducting proximity effect of non-equilibrium electrons injected into the conduction band of the ferromagnetic insulator via a Fowler-Nordheim tunneling process. The occurrence of a strongly non-equilibrium population is confirmed by the detection of photon emission at large bias voltage. Since the conduction band in our ferromagnetic insulator is strongly spin polarized, the long-range (20 nm) of the observed proximity effect provides evidence for an unconventional spin-triplet superconducting state.
I. INTRODUCTIONThe manganite perovskite La 2−x (Ca,Sr) x MnO 3 exhibits a rich phase diagram of unusual electronic and magnetic properties. Most prominent is the so-called colossal magneto-resistance (CMR) effect which occurs at 0.15 < x < 0.5 in the context of a transition from a paramagnetic and insulating or poorly conducting state to a ferromagnetic and half metallic state [1,2]. At somewhat lower doping at 0.1 < x < 0.15, the corresponding transition leads into a ferromagnetic insulating (FI) state which is a consequence of charge localization below the spin-polaron mobility edge and orbital ordering at low T [3][4][5][6]. This FI state can also be achieved in off stoichiometric LaMnO 3+δ in which the hole doping is due to La or Mn vacancies. While half-metallic manganites are considered as promising spin-polarizers [7], the FI manganite can be an ideal spin-filter material for use in tunnel barriers with low leakage currents. Efficient spin-filters are on demand for spintronic applications [8]. Spin polarization depends on many parameters including the density of states (DOS) of electronic bands [7,[9][10][11][12], orbital hybridization and various material issues at interfaces and on the bias voltage [13]. Metallic ferromagnets provide only modest spin polarization because both majority (↑) and minority (↓) spin bands are crossing the Fermi level E F [14]. This problem is obviated in insulating and halfmetallic ferromagnets with separated majority and minority bands at E F , which, therefore, can facilitate an almost complete spin-polarization [8,[13][14][15].The antagonism between superconductivity (S) and ferromagnetism (F) leads to a variety of novel effects in hybrid S/F heterostructures [16,17], such as the stabilization of unconventional spin-triplet superconductivity [17,18], or the realization of π-Josephson junctions [19], that are interest...