Abstract

High-temperature superconductivity remains arguably the greatest enigma of condensed matter physics. The discovery of iron-based high-temperature superconductors [, ] has renewed the importance of understanding superconductivity in materials susceptible to magnetic order and fluctuations. Intriguingly, they show magnetic fluctuations reminiscent of superconducting (SC) cuprates [], including a ‘resonance’ and an ‘hourglass’-shaped dispersion [], which provides an opportunity to gain new insights into the coupling between spin fluctuations and superconductivity. In this paper, we report inelastic neutron scattering data on Fe1+yTe0.7Se0.3 using excess iron concentration to tune between an SC (y = 0.02) and a non-SC (y = 0.05) ground state. We find incommensurate spectra in both the samples but discover that in the one that becomes SC, a constriction toward a commensurate hourglass-shape develops well above Tc. Conversely, a spin gap and a concomitant spectral weight shift happen below Tc. Our results imply that the hourglass-shaped dispersion is most likely a prerequisite for superconductivity, whereas the spin gap and shift of spectral weight are the consequences of superconductivity. We explain this observation by pointing out that an inward dispersion toward the commensurate wave vector is needed for the opening of a spin gap to lower the magnetic exchange energy and hence provide the necessary condensation energy for the SC state to emerge.

Highlights

  • New Journal of Physics 14 (2012) 073025 1367-2630/12/073025+09$33.00 shift happen below Tc

  • In iron–arsenic-based compounds as well as in the iron chalcogenides, the emergence of superconductivity is accompanied by the opening of a spin gap and appearance of a commensurate ‘spin resonance’ and ‘hourglass’-shaped magnetic dispersion, which have been observed in several inelastic neutron scattering experiments [6,7,8]

  • We have discovered that tuning superconductivity in iron chalcogenide by small amounts of excess iron provides fresh insight into the mechanism of SC

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Summary

Introduction

New Journal of Physics 14 (2012) 073025 1367-2630/12/073025+09$33.00 shift happen below Tc. Lowering the temperature to T = 2 K reveals dramatic differences: (i) Q-scans at E = 5 meV and E = 5.5 meV narrow down into a single commensurate peak defining Ehg = 5.3(5) meV; (ii) spectral weight is removed below Ehg and shifted to above Ehg. This dramatic restructuring of the magnetic excitation spectrum is direct experimental evidence for an intricate coupling between magnetism and superconductivity, and is very reminiscent of the behavior in cuprate superconductors, with one noticeable difference: in Fe1.02Te0.7Se0.3 the spectrum is completely incommensurate at high temperature and becomes commensurate upon lowering the temperature.

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