Nematic-driven anisotropic electronic properties of underdoped detwinned Ba(Fe1-xCox)2As2 revealed by optical spectroscopy

Enlarged view: Figure 2.15
Figure 2.15: (a) Reflectivity (R(ω)) of BaFe2As2 measured at 10 K and p = 0.8 bar, displaying the optical anisotropy in the MIR spectral range. The inset shows R(ω) up to the visible and ultraviolet range with a logarithmic frequency scale. Above 3000 cm-1 the spectra for both polarization directions merge together. (b-c) p dependence of Rratio(ω) = Ra/Rb at 10 K for increasing (b) and decreasing p (c). The temperature of 10 K was achieved within a zero-pressure cooling (ZPC) procedure. Values of Rratio(ω) are determined at 1500 cm-1 (vertical dashed line). Applied stress is given in bar and corresponds to p of He gas inside the volume of the pressure device.

We demonstrate the capability of optics to get insights into the nematic-driven tetragonal-to-orthorhombic structural transition in the underdoped regime of the title compounds. We have designed a novel pressure device, allowing us to perform optical reflectivity (R(ω)) measurements as a function of temperature under a variable in-plane uniaxial stress (Fig. 2.15), thus with adjustable population of the two twin orientations. The device consists of a sealed spring bellows, which can be expanded or retracted by varying the pressure of He-gas held inside, so that uniaxial stress on the lateral edge of the specimen can be tuned in-situ. The main findings evinced from our work are (i) the capability to release in-situ p, as symmetry breaking field, and thus to observe the anisotropy of the electrodynamic response at T << Ts for unstressed but fully detwinned crystals and (ii) the hysteretic nature (Fig. 2.16) of the optical anisotropy upon varying the stress due to the motion of the nematic domain walls. Moreover, the optical anisotropy gets progressively depleted with increasing Co-content in the underdoped regime, consistent with the doping dependence of the orthorhombicity but contrary to the non-monotonic behavior observed for the dc anisotropy. Our data give clear cut evidences for the impact of the ferro-elastic transition at energy scales deep into the electronic structure and for its fluctuations over a remarkable temperature interval above Ts. The discovered optical fingerprint of the nematic fluctuations originates from an intrinsic pressure-induced electronic anisotropy and bears testimony for the electronic nature of the structural phase transition. We have not observed any changes in the optical anisotropy at T < Tc in the underdoped regime, which would suggest that superconductivity emerges within an electronic polarized state.

Enlarged view: Figure 2.16
Figure 2.16: (a-e) Pressure dependence of ΔRratio=Rratio(p,ω)-1 at selected temperatures above and below Ts achieved in the ZPC 'pressure-loop' experiment for x = 0 and 4.5% Co-doping (full and open symbols denote increasing and decreasing pressure, respectively). The dashed and dotted lines are guide to the eyes. The upper right panel (f) displays the real part σ1(ω) of the optical conductivity for x = 0% and 4.5% Co-doping at Ts, emphasizing the mid-infrared peak overlapped to the low frequency tail of the stronger near-infrared absorption at about 4000 cm-1. The vertical dotted lines mark the position of the mid-infrared peak at ω = 1500 and 900 cm-1 for x = 0% and 4.5% Co-doping, respectively, where Rratio is read.
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