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Transport near a quantum critical point in BaFe2(As1−xPx)2

Abstract

The physics of quantum critical phase transitions connects to some of the most difficult problems in condensed matter physics, including metal–insulator transitions, frustrated magnetism and high-temperature superconductivity. Near a quantum critical point, a new kind of metal emerges, the thermodynamic and transport properties of which do not fit into the unified phenomenology for conventional metals—the Landau Fermi-liquid theory—characterized by a low-temperature limiting T-linear specific heat and a T2 resistivity1. Studying the evolution of the temperature dependence of these observables as a function of a control parameter leads to the identification of both the presence and the nature of the quantum phase transition in candidate systems. In this study we measure the transport properties of BaFe2(As1−xPx)2 below the critical temperature Tc by suppressing superconductivity with high magnetic fields. At sufficiently low temperatures, the resistivity of all compositions () crosses over from a linear to a quadratic temperature dependence, consistent with a low-temperature Fermi-liquid ground state. As compositions with optimal Tc are approached from the overdoped side, this crossover becomes steeper, consistent with models of quantum criticality where the effective Fermi temperature TF goes to zero.

Main

The iron-based superconductors are part of a family of unconventional superconductors that exhibit several competing orders. The parent material BaFe2As2 is a tetragonal paramagnet at high temperature and becomes an orthorhombic metallic antiferromagnet at 140 K (ref. 2). As the material is electron doped, hole doped or isovalently substituted this transition is rapidly suppressed, giving rise to superconductivity. In this work, we attempt to understand the nature of the low- T metallic state of the Fe-based superconductor BaFe2(As1−xPx)2 by suppressing the superconductivity in a high magnetic field. Even though BaFe2(As1−xPx)2 is isovalently substituted, we will describe the chemical composition–temperature (xT) phase diagram using language commonly applied to electron/hole-doped compounds, namely ‘underdoped’ refers to materials that exhibit a structural/magnetic instability, and ‘overdoped’ for paramagnetic compounds that do not. For this material, the maximum Tc (optimal doping) occurs at x = 0.30.

BaFe2(As1−xPx)2 is a multi-band compound with both electron- and hole-like carriers and the magnetoresistance is therefore a sum of contributions from all Fermi surfaces. In Fig. 1 we illustrate the magnetoresistance as a function of temperature and field for a range of compositions from x = 0.31 to x = 0.73 and Tc spanning 29.5 K to 0 K. For all temperatures measured, a quadratic magnetoresistance fit captures most of the data and the intercept ρ0,T is extrapolated (shown by black lines in Fig. 1). At low fields, this fit deviates from the quadratic dependence in the near-optimally doped samples, even at temperatures T>Tc, although the deviation ostensibly disappears at sufficiently high T (see Supplementary Section A). This may be due to a complex balance of mobilities between electron and hole pockets or due to superconducting fluctuations persisting at T>Tc, as seen in cuprate materials3,4. Thus, ρ0,T is slightly overestimated, causing an offset in the zero-field resistance estimate δR≡(ρexptlρfit)|0,T. Within the present data set, this offset is of the order 10−2ρ/ρ300. We proceed assuming that δR has a negligible effect on the evolution of ρ0,T with T, and discuss the consequences of this assumption in Supplementary Section B. In the simplest case of an ordinary metal, the magnetoresistance of a multi-band system is expected to be B2 at low magnetic fields, but for an unequal number of electrons and holes the resistivity will eventually saturate5. If a material is perfectly compensated, however, the magnetoresistance will remain B2 up to very high fields6. The compound BaFe2(As1−xPx)2 is isovalently substituted, forcing the system to remain compensated6,7 as a function of x. The magnetoresistance thus exhibits a B2 dependence over a wide field range, consistent with our observations. It should be noted that recent photoemission work 6 has observed a slight hole doping with P substitution at the surface near optimal P compositions (but returning to perfectly compensated in the overdoped region). However, the ratio nh/ne remains close, implying that B2 resistivity is appropriate for values of the magnetoresistance up to ρ(B)10×ρ0,T for optimally doped samples (where the affect is greatest). In Fig. 1 the largest magnetoresistance we observe at optimal compositions occurs at 4 K and ρ(B)<1.2×ρ0,T, if ρ0,T is taken as the B = 0 intercept, putting the present data far from the saturation regime. We therefore analyse this data with the quadratic functional form with some confidence of its validity. As a further caveat, it is important to point out that an established understanding of magnetoresistance near a quantum critical metal does not at present exist, and this fact may compromise our model of magnetoresistance (although several treatments exist8). Nevertheless, our data suggest that a B2 law is valid, at least empirically, for compounds in the overdoped part of the pnictide phase diagram.

Figure 1: Magnetic field dependence of the magnetoresistance for overdoped BaFe2(As1−xPx)2.
figure 1

Each of the seven samples has a distinct Tc. Each different coloured curve has been offset for clarity and corresponds to a different temperature in the range indicated; raw data curves are in Supplementary Section A. The black lines are fits to a standard magnetoresistance model ρ(B) = ρ0,T+ABB2.

In Fig. 2 we show the zero-field normalized resistivity cooling curves of these materials in blue and the values of ρ0,T extrapolated from the data in Fig. 2 in green—the latter connects smoothly to the former such that analysis of the power law is possible at T<Tc. There are broadly two schools of thought as to how this power law should be analysed in correlated electron systems. Recent studies on the cuprates9, and on pnictide and organic superconductors10 have suggested a transport law that combines linear and quadratic components

However, in heavy-fermion materials such as CePd2Si2 (refs 11, 12) it is found that a single power law n captures the transport behaviour, accounting for a crossover from Fermi-liquid to quantum critical regimes as some critical parameter is varied, such as doping or magnetic field. In its most general form the transport will look like

Taking the derivative provides a simple way to distinguish equation (1) from equation (2), giving a finite (negligible) intercept in the former (latter). In Fig. 3a,b we illustrate this derivative for all of the samples considered using the normal-state data shown in Fig. 2. In all cases, we observe (within experimental error) a zero intercept, suggesting that equation (2) is best able to describe the data for BaFe2(As1−xPx)2. Furthermore, the dρ/dT curves are linear at low temperature, suggesting that all samples recover a n = 2 power law expected of a Fermi liquid. As optimal doping is approached, the range in T over which this applies steadily decreases. In addition, the slope of these curves ( = 2A) sharply peaks, or even diverges, as optimal doping is approached, as shown in Fig. 3c. In certain cuprate and heavy-fermion superconductors, this behaviour has been interpreted as an indication of the proximity to a quantum critical point9,13,14 (QCP). In this context, the cusp seen in dρ/dT perhaps marks the crossing of a border in the xT phase diagram, above which quantum critical fluctuations dominate.

Figure 2: The zero-field temperature dependence of the resistivity at the indicated composition.
figure 2

Each curve has been normalized to the room-temperature value ρT/ρ300 in blue, together with the zero-field intercept extracted from the corresponding high-field magnetoresistance shown in Fig. 1 in green.

Figure 3: Derivative of the resistivity interpolated over the full temperature range.
figure 3

a, The derivative of the resistivity for all samples in Fig. 2, including data from zero-field and high-field experiments, interpolated to form differentiable curves. b, An enlargement of the data shown in a with linear fits to the low- T behaviour (grey lines). c, The pronounced increase in the value 2A (open circles) at compositions between x = 0.73 and 0.37, suggests the proximity of a QCP below the superconducting dome. The data are consistent with the KWR (ref. 20) A/m*2 = constant, as can be seen by comparison with previous determinations (red circles) of the effective mass m* (refs 15, 16, 17). The line is a fit to a phenomenological divergence of the effective mass near a QCP (ref. 19) [C0C1ln(xxc)]2, with xc = 0.32. Error bars have been determined using the standard deviation of the data from the least-squares fit.

The presence of a QCP in the P-substituted phase diagram has been suggested by certain thermodynamic measurements7,15,16,17. In the traditional approach to quantum criticality18, the effective dimensionality deff is defined as the sum of the spatial dimension d and the dynamical exponent z, which characterizes the temporal fluctuations. In quasi-two-dimensional systems near an antiferromagnetic (AFM) critical point, d = 2, z = 2 and deff ( = 4) is at the upper critical dimension where one would expect the specific heat divided by temperature to vary as [C0C1ln(xxc)] (ref. 19). Comparing our study to previous determinations17 of m*2, we observe that our data are consistent with this model if the electron–electron scattering is assumed to be proportional to the mass enhancement, namely that the Kadowaki–Woods ratio (KWR) holds20. It has been shown that the average mass enhancement (of one of the Fermi surfaces) quantitatively agrees with the mass enhancement estimated by comparing the Sommerfeld coefficient γ to the density-functional calculated value γ0 = 6.94 mJ mol−1 K−2, where γ was determined from the superconducting heat capacity jump ΔC/Tc (ref. 17). Using this renormalization of the band mass m*/mb, we estimate that the KWR A/γ2 ranges from ≈7 μΩ cm mol2 K2 J−2 at x = 0.34, to ≈15 μΩ cm mol2 K2 J−2 for our most overdoped sample x = 0.73. The factor of two change could arise from the discrepancy in estimating m* from the heat capacity jump versus the de Haas–van Alphen mass in ref. 17. These values agree with other correlated electron materials, specifically heavy-fermion compounds that have A/γ210 μΩ cm mol2 K2 J−2 (refs 20, 21, 22). We subsequently fit our data to a phenomenological critical power law19A[C0C1ln(xxc)]2 over x≥0.34. If we fix xc = 0.32 and C0 = 1, the fit yields C1 = 0.98. This curve is shown as a dashed line in Fig. 3c. The fit is sensitive to the choice of xc, and choosing xc = 0.3 yields the same values as ref. 17. The difference between the present determination of xc and earlier works15,16,17 may be due to the effect of finite magnetic field13. On the other hand, it may be due to the complicated nature of interpreting transport at compositions near the AFM transition (See Supplementary Section C), or deviations of the magnetoresistance from conventional behaviour near a QCP (ref. 8). In addition, even though BaFe2(As1−xPx)2 is the cleanest of the superconducting materials with the BaFe2As2 structure23, it is possible that disorder also affects the exact determination of xc.

We illustrate the evolution of the power law n as a function of temperature and doping in Fig. 4. We fit dρ/dT with a sliding temperature window to the equation dρ/dT = n A Tn−1, with a window width ΔT = 7 K. From this we extract the average power law n(T), where the mid-point of the window is taken as the temperature, shown in Fig. 4. For all compositions considered, n→2 at low T, consistent with the linear slope observed in dρ/dT, Fig. 3b. The crossover to n = 2 may be interpreted as the re-entrance to Fermi-liquid behaviour (marked (TFL) in Fig. 4). Compositions in the range 0.31<x<0.34, where Fig. 3c suggests 2A diverges, are indicated by a grey line.

Figure 4: Colour plot of the power-law dependence n as a function of temperature and doping.
figure 4

The data have been interpolated over the discrete dopings measured. The black dashed line is a guide to the eye, indicating the region of the phase diagram that can be interpreted as the re-entrance of Fermi-liquid-like behaviour (TFL). Compositions where 2A is thought to diverge (Fig. 3c) are indicated by the grey line. The black data points connected by a solid line are the superconducting Tc at that composition.

In marked contrast to the situation found for hole-doped cuprates, where the T-linear resistivity remains robust over an extended range of doping9, BaFe2(As1−xPx)2 is found to exhibit behaviour associated with a more conventional picture of quantum criticality in which ρ(T) always crosses over from a T-linear to a T2 dependence below a temperature scale that diminishes on approach to the QCP. In accordance with this picture, the coefficient of the T2 resistivity is also found to diverge as the QCP is approached. Although there is at present no accepted theory explaining the origin of T-linear resistivity in quantum critical metals, a common point of view is that it is associated with Fermi-surface ‘hotspots’—regions of the Fermi surface with strongly enhanced scattering. Such regions are thought to dominate the transport of many strongly correlated metals24, particularly as disorder increases12, accounting for the strong dependence of the scattering on T. Away from optimal doping, the iron-based superconductors order anti-ferromagentically, and hotspots on electron and hole Fermi surfaces25 are therefore expected. Our data can be broadly understood in this context—as an AFM QCP is approached from the overdoped side, the Fermi-surface hotspots become increasingly ‘hotter’, sharply changing the nature of the transport as a function of temperature. However, why it is that the resistivity is strictly T-linear and why this dependence is common to so many metals near a QCP remains an open question.

Methods

Single crystals of BaFe2(As1−xPx)2 were grown by a self-flux method described elsewhere23. High magnetic fields were made available at the NHMFL, Tallahassee (45 T, static) and at Los Alamos National Labs (65 T pulsed). In the presence of a magnetic field, the stationary states are quantized into Landau levels, which are separated by the cyclotron energy ωcyc. When a material is superconducting, this energy scale competes with the nucleation of Cooper pairs defining an upper critical field Hc2, which depends on 1/ξ2, where ξ is the superconducting coherence length. Beyond Hc2 the system is considered to be in the ‘normal metal’ state, exhibiting metallic magnetoresistance. Samples with a Tc≤24 K were measured in the hybrid magnet in Tallahassee; samples with Tc≥27.5 K were measured in pulsed fields in Los Alamos.

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Acknowledgements

H-H.K., J.G.A. and I.R.F. acknowledge support of the US DOE, Office of Basic Energy Sciences under contract DE-AC02-76SF00515. J.G.A. would like to thank the NHMFL Visiting Scientist Program for valuable support while this data was taken. N.E.H. acknowledges a Royal Society Wolfson Research Merit Award and funding from the EPSRC (UK) grant EP/K016709/1. The National High Magnetic Field Laboratory is supported through NSF/DMR 1157490. R.D.M. acknowledges US DOE BES-‘Science of 100 tesla’.

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J.G.A. and I.R.F. conceived of this experiment. J.G.A., R.D.M., H.H.K., P.M.C.R. and M.W. performed the experiments. J.G.A., R.D.M., N.E.H. and I.R.F. performed the analysis. All authors contributed in writing the paper.

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Correspondence to James G. Analytis.

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Analytis, J., Kuo, HH., McDonald, R. et al. Transport near a quantum critical point in BaFe2(As1−xPx)2. Nature Phys 10, 194–197 (2014). https://doi.org/10.1038/nphys2869

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