Evidence for \pms-wave pairing symmetry in LiFeAs: specific heat study

Evidence for s-wave pairing symmetry in LiFeAs: specific heat study

Dong-Jin Jang, J. B. Hong, Y. S. Kwon, and T. Park tp8701@skku.edu Department of Physics, Sungkyunkwan University, Suwon 440-746, Republic of Korea    K. Gofryk, F. Ronning, J. D. Thompson Los Alamos National Laboratory, Los Alamos, NM 87545, USA    Yunkyu Bang ykbang@chonnam.co.kr Department of Physics, Chonnam National University, Kwangju 500-757, Republic of Korea
Abstract

We report specific heat capacity measurements on a LiFeAs single crystal at temperatures down to 400 mK and magnetic fields up to 9 Tesla. A small specific heat jump at and finite residual density of states at  K in the superconducting (SC) state indicate that there are strong unitary scatterers that lead to states within the SC gap. A sub-linear magnetic field dependence of the Sommerfeld coefficient at  K is equally well fitted by both a nodal d-wave gap as well as a sign changing multiband s-wave gap. When impurity effects are taken into account, however, the linear temperature dependence of the electronic specific heat at low temperatures argues against a nodal d-wave superconducting gap. We conclude that the SC state of LiFeAs is most compatible with the multiband s-wave SC state with the gap values .

pacs:
74.70.Xa, 74.25.Bt, 74.20.Rp

I Introduction

Information on the superconducting (SC) pairing symmetry is important for the understanding of the SC pairing mechanism. For the newly discovered Fe-pnictide superconductors, determination of the SC order parameter has been controversial partly due to its sensitive dependence on measurement probes and material stoichiometry. Kamihara (); Ishida () In the ’1111’ phase of REFeAsO (RE = rare earth), a fullly gapped scenario is supported by angle-resolved photoemission spectroscopy(ARPES) and tunnelling measurements, Kondo (); Chen () but a gap symmetry with nodes on the Fermi surface is suggested by far-infrared ellipsometric measurements. Dubroka () Penetration depth measurements reported either a full gap or a nodal gap for RE = Sm,Pr Malone (); Hashimoto () and RE=La, fletcher09 () respectively. Identification of the SC gap symmetry is also controversial in the ’122’ phase of AeFeAs (Ae = alkaline earth). For electron doped BaFeAs, full gaps are reported from ARPES Terashima () and scanning tunnelling microscopy (STM) measurements, Yin () but anisotropic or nodal gaps are supported by specific heat, Jang () thermal conductivity, Tanatar (); Dong () penetration depth, Gordon (); Hashimoto () Raman scattering, Mushuler () nuclear magnetic resonance (NMR), Ning () and muon spin resonance (SR). Williams () For hole-doped Ba122, multiple gaps without nodes are reported from specific heat Mu () and thermal conductivity. Luo ()

LiFeAs, the so-called ’111’ phase, is unique in that it is superconducting without carrier doping and the residual resistivity ratio (RRR) is about 50, one of the highest among Fe-based SC compounds, song10 () holding promise for a determination of the superconducting gap symmetry without complications from material defects. stewart09 (); Gofryk () Various spectroscopic and thermodynamic measurements suggest an isotropic SC gap without nodes on the Fermi surface. Inosov (); Wei (); kim11 (); tanatar11 () Previous specific heat measurements, a direct bulk probe of the electronic density of states (DOS), suggest multiple SC gaps to explain its temperature dependence. Wei (); stockert11 () The analysis, however, is limited due to lack of specific heat data below 2 K, where a difference in the DOS becomes prominant among different types of SC pairing symmetry. In order to elucidate the nature of the order parameter of LiFeAs, we measured the specific heat of LiFeAs single crystals down to 400 mK and under magnetic field up to 9 Tesla. A large value of the Sommerfeld coefficient  mJ/molK) in the SC state at zero magnetic field and small specific heat jump ratio at indicates the presence of large elastic scattering due to impurities. Here is the specific heat at in the normal state. When the impurity effects are taken into account, observation of a linear temperature dependence of the low- specific heat and a sublinear magnetic field dependence of the Sommerfeld coefficient excludes a d-wave SC gap, but is consistent with the sign changing multiband s-wave state with the gap values .

Ii Experiments

Single crystalline LiFeAs, which is formed in a nmm tetragonal CuSb-type structure with and , was synthesized in a sealed tungsten crucible by the Bridgeman method. song10 () X-ray diffraction pattern analysis showed that crystals from this batch are homogeneous and well oriented. This growth technique seems to avoid inclusion of impurities that can lead to an anomalous Schottky-like upturn in the low-temperature specific heat of Fe-based superconductors, making it a useful synthesis technique for a specific heat study of SC gap symmetry. Jang () The crystals used in the current study are from the same batch that has been used for previous transport, thermodynamic, and spectroscopic studies. song10 (); tanatar11 (); kim11 () A Quantum Design PPMS (Physical Properties Measurement System) with a He option was used to measure specific heat down to 400 mK and up to 9 T for magnetic fields applied parallel and perpendicular to the crystalline c-axis.

Figure 1: (color online) (a) Specific heat of LiFeAs at zero magnetic field is plotted down to 400 mK. The red solid line is an estimated normal state specific heat from a polynomial form described in the text. (b) Calculated electronic entropy in the superconducting state () and in the normal state .

Iii Results

Figure 1(a) shows the temperature-dependent specific heat capacity of a LiFeAs single crystal at zero field. A superconducting transition occurs at 15 K (=), which is determined from the mid-point of the the specific heat anomaly. The measured specific heat () consists of electronic () and phononic () contributions, i.e., . Non-Debye behavior has been often reported in Fe-based superconductors and ascribed to a large Einstein contribution or a low Debye temperature . Because an Einstein phonon contribution is negligible below 25 K in LiFeAs, a second term of the harmonic-lattice approximation is added to the phonon specific heat: stockert11 () The specific heat is best described by the least-squares fit with  mJ/moleK,  mJ/moleK and  mJ/moleK. The electronic Sommerfeld coefficient ( mJ/moleK) at zero magnetic field in the normal state is comparable with previously reported values of 23, 20, and 10 mJ/moleK from Refs. [28], [24], and [27], respectively. The Debye temperature estimated from the fit is 294 K, which is similar to 310 K from Ref. [27]. Figure 1b shows the electronic entropy in the normal (squares) and superconducting (circles) states after subtracting the non-electronic contribution. The two entropies become equal at , which satisfies the entropy constraint, . From the electronic entropy in Fig. 1(b), we estimate the superconducting condensation energy 363 mJ/mole and thermodynamic critical field 0.23 T. When we use the Ginzburg-Landau parameter 297 of LiFeAs from a SANS experiment, Inosov () the upper critical field is 9.4 T. For comparison, from penetration measurements is 17 T. Cho ()

Figure 2: (color online) Normalized electronic specific heat coefficient (black open circles) and the best fits of the two SC gap models: d-wave (blue circles) and s-wave (red triangles) models. For the d-wave model, and are obtained for the best results. Here, is the maximum gap of the d-wave gap . For the s-wave model, , , and are obtained from the least squares fit. We note that the inversely related ratios between and are an intrinsic property of the s-wave pairing model with a dominant interband paring interaction. bang09 () Inset: Low- temperature specific heat in the main panel is magnified to show a notable difference between the two gap models.

Figure 2 shows the electronic specific heat coefficient of LiFeAs at zero magnetic field after subtracting the phononic contribution: =. The specific heat jump at is 7.65 mJ/molK at zero field. The jump relative to the normal state specific heat is (=), which is much smaller than the BCS value 1.43, indicating that the quasiparticles participating in the SC condensation experience strong elastic scattering because inelastic scattering usually enhances the jump ratio. bang04 () Also the substantial value of the Sommerfeld coefficient in the SC state, which accounts for about 45 % of the normal state value , also supports the presence of strong (unitary) scatterers because weak (Born limit) scatterers are not capable of inducing states inside the SC gap of unconventional superconductors. bang09 () These results suggest that any model to explain the nature of the SC gap symmetry of LiFeAs should take into account the effects of impurity scattering.

To extract information on the gap symmetry from the specific heat of LiFeAs, we consider two typical unconventional SC gap models that represent two extreme limits, i.e., a d-wave SC gap with nodes and a s-wave gap without nodes, and fit the experimental data in Fig.2. Here we used the d-wave model to represent the generic behavior of a nodal SC gap state. The impurity effect is calculated using the self-consistent -matrix approximation (SCTA). bang09 () In each gap model, we determine the fitting parameters such as , the impurity concentration parameter by finding the best overall fit to the data, where is the zero-energy density of states. The results are shown in Fig. 2 overlayed with the experimental data. Both models provided reasonably good fittings for the overall shape, the specific heat jump , and the value. However, we find that the two models show qualitative differences for at low temperatures and this low temperature behavior of is what reflects the intrinsic properties of the gap symmetry, with which we can unambiguously identify the most compatible gap symmetry.

A pure d-wave superconductor is expected to produce a -linear specific heat coefficient such as because of the V-shaped density of state (DOS) . However, the large value of () indicates a substantial amount of unitary impurities. When the unitary impurities create a zero energy impurity band inside the d-wave gap, the DOS around zero energy becomes a constant, , which in turn produces a constant, temperature independent, specific heat coefficient for a finite range of low temperatures, as can be seen in the inset of Fig.2 (blue circles). Our experimental data, however, show , implying that the low energy DOS should have the form . This type of constant V-shape DOS was indeed predicted for a s-wave gap with unitary impurities. bang09 () As can be seen in Fig.2 and its inset, the s-wave gap model with unitary impurities provide an excellent fit at low temperatures as well as for the overall shape of , but the d-wave model fails to explain the low temperature behavior.

Figure 3: (color online) Low temperature specific heat capacity for magnetic fields applied parallel to the crystalline -axis and -plane in panels (a) and (b), respectively. In Fig. 3(a) the magnetic field intensity is 0, 1, 2, 3, 5, 7, and 9 T from bottom to top curves, and it is 0, 1, 3, 5, 7, and 9 T in Fig. 3(b). Straight lines are the results from the least-squares fit of and used to obtain the zero temperature value of /. (c) Anisotropy of the Sommerfeld coefficient which is obtained from the extrapolation of the data in Fig. 3(a) and (b) for the two field orientations. Here for magnetic field along the c-axis.

The dependence on magetic field of the low-temperature specific heat of LiFeAs is shown in Fig. 3(a) and 3(b) for different field orientations of and , respectively. The lack of a Schottky-like anomaly up to the highest applied magnetic field enables us to unambiguously determine the Sommerfeld coefficient from the least-squares fits of to the low specific heat. As shown in Fig. 3(c), the anisotropy in the quasiparticle density of states is almost constant (2.4) over the experimental field range and an anisotropy ratio of the upper critical fields between the two field directions is estimated to be 1.7 through the relationship: Jang (); Ichioka () =. The anisotropy from this thermodynamic measurement is in good agreement with that obtained from transport properties where was directly measured under high magnetic field. Cho (); khim11 ()

A sub-linear magnetic field dependence of is displayed in Fig. 4, which is often taken as evidence for a nodal gap structure such as a d-wave state that is known to have a generic dependence due to Doppler effects of the nodal quasiparticles by the supercurrent circulating around the vortices. Recent theoretical work, however, showed that the s-wave state with different gap sizes () can also show a strong field dependence of bang10 () In Fig. 4, we show theoretical calculations for both s-wave (dotted line) and d-wave (dashed line) models to fit the data with , where we use the same fitting parameters obtained from the analysis of the specific heat as a function of temperature (see Fig. 2). It is clear that the s-wave model equally well reproduces the field dependence of which has been taken as a signature for a nodal gap structure. Thus, in combination with our analysis of the zero field temperature dependence, our data favors the sign changing multiband superconductivity of s-wave state. This multiple SC gap scenario is consistent with recent ARPES, stockert11 () penetration depth, kim11 () and heat transport measurements, tanatar11 () where two distinct full SC gaps were reported.

Figure 4: (color online) Field dependent Sommerfeld coefficient extrapolated from Fig. 3a for field applied along the crystalline c-axis. The black dotted line is the theoretical fit with the s-wave model and grey dashed line is the fit with the d-wave model, respectively. Here we used the upper critical field of 17 Tesla from Ref. [29].

To summarize, we have reported the specific heat capacity of a LiFeAs single crystal under magnetic field. The small specific heat jump ratio at and substantial residual density of states at  K in the SC state indicate that impurity effects due to strong unitary scatterers should be included to explain the specific heat results. The zero-field specific heat data at high temperatures above 2 K and sub-linear magnetic field dependence of the Sommerfeld coefficient are equally well described by nodal and nodeless multiband SC gaps with impurity effects. However, the low-temperature electronic specific heat below 2 K excludes the nodal d-wave state, but is consistent with the sign changing multiband superconductivity of s-wave state.

This work was supported by the NRF grant funded by Korea government (MEST) (No. 2010-0029136 & 2011-0021645). Work at Los Alamos was performed under the auspices of the U. S. Department of Energy/Office of Science and supported in part by the Los Alamos LDRD program. YB was supported by the grant NRF-2010-0009523 funded by the National Research Foundation of Korea. DJ acknowledges support from the Postdoctoral Research Program of Sungkyunkwan University (2011).

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