2019
DOI: 10.1063/1.5087925
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Domain wall induced modulation of low field H-T phase diagram in patterned superconductor-ferromagnet stripes

Abstract: We present a systematic study of the magnetic domain wall induced modulation of superconducting transition temperature (T c ) in Nb/Ni bilayer stripes. By varying the thickness of the Ni layer from 20 nm to 100 nm we have been able to measure the low field T c -H phase diagram spanning the Néel domain wall and Bloch domain wall range of thicknesses. Micromagnetic simulations confirmed a stronger out-of-plane stray field in the Bloch domain walls compared to the Néel walls. A suppression in

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Cited by 6 publications
(5 citation statements)
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“…However, in thin films, while decreasing magnetic field from saturation value, the domain formation starts well before the magnetic field reaches zero and as a result the magnetization decreases from the saturation value. In our Ni thin films the domain formation starts around +0.1 T while decreasing magnetic field from positive saturation as reported earlier [29]. Figure 3(d) shows the same feature while ramping the field from negative saturation toward positive saturation.…”
Section: Magneto-transport Below Superconducting Transition Temperatu...supporting
confidence: 85%
See 1 more Smart Citation
“…However, in thin films, while decreasing magnetic field from saturation value, the domain formation starts well before the magnetic field reaches zero and as a result the magnetization decreases from the saturation value. In our Ni thin films the domain formation starts around +0.1 T while decreasing magnetic field from positive saturation as reported earlier [29]. Figure 3(d) shows the same feature while ramping the field from negative saturation toward positive saturation.…”
Section: Magneto-transport Below Superconducting Transition Temperatu...supporting
confidence: 85%
“…Since this measurement was done very close to the superconducting transition, the Nb layer is expected to respond to DW stray fields very sensitively. Therefore, the origin of MR peaks observed at this temperature is the usual suppression of superconductivity due to the out of plane component of DWs present in nickel as observed in earlier reports [28,29]. Since the overall DW stray field maximizes near the coercive field, the MR peaks, in this case appear near the coercive field.…”
Section: Magneto-transport Below Superconducting Transition Temperatu...supporting
confidence: 75%
“…Such pwave superconductivity offers spin and orbital degrees of freedom. We note that spintriplet Cooper pairs with odd-parity s-wave symmetry can be generated at an interface between an s-wave superconductor (SC) and a ferromagnet (F) [3,4]-for example, spinmixing due to the ferromagnetic exchange field generates m = 0 spin-triplet Cooper pairs, and broken spin-rotational symmetry converts m = 0 triplets into equal spin m = ±1 triplet pairs [5][6][7][8][9][10][11][12][13][14]. Moreover, broken inversion symmetry at an SC/F interface generates spin-orbit coupling (SOC), which creates interfacial spin-triplet superconductivity [15][16][17].…”
Section: Introductionmentioning
confidence: 99%
“…Figure 6(b) shows that dM/dH increases sharply below 20 Oe as the applied magnetic field is reduced from positive saturation, indicating the nucleation of domain walls in Py. Domain walls are known to reduce the transition temperature in S/F structures by an amount proportional to the domain density [36]. Around a field of +15 Oe the dM/dH starts to decrease sharply indicating the beginning of the rotation of the Py layer and the consequent drop in total moment.…”
Section: Resultsmentioning
confidence: 99%