Joel Barker
University of Warwick
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Publication
Featured researches published by Joel Barker.
Physical Review Letters | 2015
Joel Barker; D. Singh; A. Thamizhavel; A. D. Hillier; Martin R. Lees; Geetha Balakrishnan; D. McK. Paul; R. P. Singh
The superconductivity of the noncentrosymmetric compound La(7)Ir(3) is investigated using muon spin rotation and relaxation. Zero-field measurements reveal the presence of spontaneous static or quasistatic magnetic fields below the superconducting transition temperature T(c)=2.25 K-a clear indication that the superconducting state breaks time-reversal symmetry. Furthermore, transverse-field rotation measurements suggest that the superconducting gap is isotropic and that the pairing symmetry of the superconducting electrons is predominantly s wave with an enhanced binding strength. The results indicate that the superconductivity in La(7)Ir(3) may be unconventional and paves the way for further studies of this family of materials.
Physical Review B | 2014
Mohammad Saghir; Joel Barker; Geetha Balakrishnan; A. D. Hillier; Martin R. Lees
The superconducting properties of Sn1−xInxTe (x=0.38–0.45) have been studied using magnetization and muon-spin rotation or relaxation (μSR) measurements. These measurements show that the superconducting critical temperature Tc of Sn1−xInxTe increases with increasing x, reaching a maximum at around 4.8 K for x=0.45. Zero-field μSR results indicate that time-reversal symmetry is preserved in this material. Transverse-field muon-spin rotation has been used to study the temperature dependence of the magnetic penetration depth λ(T) in the mixed state. For all the compositions studied, λ(T) can be well described using a single-gap s-wave BCS model. The magnetic penetration depth at zero temperature λ(0) ranges from 500 to 580 nm. Both the superconducting gap Δ(0) at 0 K and the gap ratio Δ(0)/kBTc indicate that Sn1−xInxTe (x=0.38–0.45) should be considered as a superconductor with intermediate to strong coupling.
Physical Review B | 2014
R. P. Singh; A. D. Hillier; D. Chowdhury; Joel Barker; D. McK. Paul; Martin R. Lees; Geetha Balakrishnan
The superconducting properties of CaTSi3 (where T = Pt and Ir) have been investigated using muon spectroscopy. Our muon-spin-relaxation results suggest that in both these superconductors time-reversal symmetry is preserved, while muon-spin-rotation data show that the temperature dependence of the superfluid density is consistent with an isotropic s-wave gap. The magnetic penetration depths determined from our transverse-field muon-spin-rotation spectra are found to be 448(6) and 150(7) nm for CaPtSi3 and CaIrSi3, respectively.
Physical Review B | 2017
Joel Barker; B. D. Breen; Robert M. Hanson; A. D. Hillier; Martin R. Lees; Geetha Balakrishnan; D. McK. Paul; R. P. Singh
We systematically investigate the normal and superconducting properties of noncentrosymmetric
Physical Review B | 2017
D. Singh; Joel Barker; A. Thamizhavel; D. M. Paul; A. D. Hillier; R. P. Singh
{\mathrm{Re}}_{6}\mathrm{Zr}
Journal of Physics: Condensed Matter | 2017
D. Singh; Joel Barker; A. Thamizhavel; A. D. Hillier; Don McK. Paul; R. P. Singh
using magnetization, heat capacity, and electrical resistivity measurements. Resistivity measurements indicate
arXiv: Materials Science | 2018
Kévin J. A. Franke; Benjamin M. Huddart; Thomas J. Hicken; Fan Xiao; Stephen J. Blundell; Francis L. Pratt; Marta Crisanti; Joel Barker; Stewart J. Clark; Aleš Štefančič; Monica Ciomaga Hatnean; Geetha Balakrishnan; Tom Lancaster
{\mathrm{Re}}_{6}\mathrm{Zr}
Physical Review B | 2018
Kévin J. A. Franke; Benjamin M. Huddart; Thomas J. Hicken; Fan Xiao; Stephen J. Blundell; Francis L. Pratt; Marta Crisanti; Joel Barker; Stewart J. Clark; Aleš Štefančič; Monica Ciomaga Hatnean; Geetha Balakrishnan; Tom Lancaster
has poor metallic behavior and is dominated by disorder.
Physical Review B | 2018
Joel Barker; Ravi P. Singh; A. D. Hillier; D. M. Paul
{\mathrm{Re}}_{6}\mathrm{Zr}
Physical Review B | 2018
D. Singh; K. P. Sajilesh; Joel Barker; D. McK. Paul; A. D. Hillier; R. P. Singh
undergoes a superconducting transition at