Investigating the superconducting state of 2\(H\)-NbS\(_2\) as seen by the vortex lattice

• Published in: arXiv.org 2024-04
• Main Authors: Alshemi, A, Campillo, E, gan, E M, Cubitt, R, Abdel-Hafiez, M, Blackburn, E
• Format: Article
• Language: English
• Subjects: Anisotropy; Charge density waves; Magnetic fields; Neutron scattering; Niobium; Penetration depth; Superconductivity
• ISSN: 2331-8422
• DOI: 10.48550/arxiv.2404.19049

2\(H\)-NbS\(_2\) is a classic example of an anisotropic multi-band superconductor, with significant recent work focussing on the interesting responses seen when high magnetic fields are applied precisely parallel to the hexagonal niobium planes. It is often contrasted with its sister compound 2\(H\)-NbSe\(_2\) because they have similar onset temperatures for superconductivity, but 2\(H\)-NbS\(_2\) has no charge density wave whereas in 2\(H\)-NbSe\(_2\) the charge density wave order couples strongly to the superconductivity. Using small-angle neutron scattering, a bulk-sensitive probe, we have studied the vortex lattice and how it responds to the underlying superconducting anisotropy. This is done by controlling the orientation of the field with respect to the Nb planes. The superconducting anisotropy, \(\Gamma_{ac} = 7.07 \pm 0.2\), is found to be field independent over the range measured (0.15 to 1.25 T), and the magnetic field distribution as a function of the applied magnetic field is found to be in excellent quantitative agreement with anisotropic London theory modified with a core-size cut-off correction, providing the first complete validation of this model. We find values of \(\lambda_{ab} = 141.9 \pm 1.5 \) nm for the in-plane London penetration depth, and \(\lambda_{c} \sim\) 1 \textmu m for the out-of-plane response. The field-independence indicates that we are primarily sampling the larger of the two gaps generating the superconductivity in this material.