Nature Physics  Letter
Dirac node arcs in PtSn_{4}
 Yun Wu^{1, 2}^{, }
 LinLin Wang^{1}^{, }
 Eundeok Mun^{1, 2}^{, n1}
 D. D. Johnson^{1, 2, 3}^{, }
 Daixiang Mou^{1, 2}^{, }
 Lunan Huang^{1, 2}^{, }
 Yongbin Lee^{1}^{, }
 S. L. Bud’ko^{1, 2}^{, }
 P. C. Canfield^{1, 2}^{, }
 Adam Kaminski^{1, 2}^{, }
 Journal name:
 Nature Physics
 Year published:
 DOI:
 doi:10.1038/nphys3712
In topological quantum materials^{1, 2, 3} the conduction and valence bands are connected at points or along lines in the momentum space. A number of studies have demonstrated that several materials are indeed Dirac/Weyl semimetals^{4, 5, 6, 7, 8}. However, there is still no experimental confirmation of materials with line nodes, in which the Dirac nodes form closed loops in the momentum space^{2, 3}. Here we report the discovery of a novel topological structure—Dirac node arcs—in the ultrahigh magnetoresistive material PtSn_{4} using laserbased angleresolved photoemission spectroscopy data and density functional theory calculations. Unlike the closed loops of line nodes, the Dirac node arc structure arises owing to the surface states and resembles the Dirac dispersion in graphene that is extended along a short line in the momentum space. We propose that this reported Dirac node arc structure is a novel topological state that provides an exciting platform for studying the exotic properties of Dirac fermions.
Subject terms:
At a glance
Figures
Main
The discovery of nontrivial surface states in topological insulators^{1} has attracted a lot of interest and initiated quests for diverse novel topological states in condensed matter. Topological nodal states with conduction and valence bands touching at points (Dirac/Weyl semimetals) or lines (line node semimetals) have been proposed to exist in multilayer heterostructures^{2}. A possible extension of these states to three dimensional (3D) single crystals was proposed in βcristobalite BiO_{2} (ref. 9) and A_{3}Bi (A = Na, K, Rb; ref. 10), which are thought to host bulk 3D Dirac points protected by crystal symmetry. Subsequently, Na_{3}Bi and Cd_{3}As_{2} were experimentally demonstrated to be 3D Dirac semimetals^{4, 5, 11, 12}. Subsequently, another type of massless particle—the Weyl fermion^{13}—was found in states that were predicted to exist in a family of noncentrosymmetric transition metal TaAs, TaP, NbP and NbAs (refs 14,15). These materials were confirmed as Weyl semimetals by reports of Fermi arc states connecting the Weyl points as a unique signature^{6, 7, 8}. Although experimental evidence supports the existence of Dirac semimetals and Weyl semimetals, clear signatures of semimetals with line nodes are yet to be discovered. Several groups proposed that line node structures may exist in graphene networks^{16}, rare earth monopnictides^{17}, antiperovskite Cu_{3}PdN/Cu_{3}ZnN (refs 18,19), SrIrO_{3} (ref. 20), TlTaSe_{2} (ref. 21), Ca_{3}P_{2} (ref. 22) and CaAgX (X = P, As; ref. 23), but so far no direct evidence has been reported. Several angleresolved photoemission spectroscopy (ARPES) studies in PbTaSe_{2} (ref. 24) and ZrSiS (ref. 25) presented some evidence of the existence of Diraclike features and ‘drumhead’ surface states, but further research is still needed to understand fully their significance and relation to Dirac line nodes.
Many topological nodal semimetals, such as Cd_{3}As_{2} (ref. 26), NbP (ref. 27) and WTe_{2} (ref. 28), exhibit extremely large magnetoresistance. Before these discoveries, a similar effect was observed in PtSn_{4}, with a magnetoresistance of ≃5 × 10^{5}% and no obvious saturation at 1.8 K and 140 kOe (ref. 29). However, the band structure of this material has not been studied experimentally in detail owing to the very complex Fermi surface (FS) revealed by calculations^{29}. Here we demonstrate that, despite its complex FS in the centre region of the Brillouin zone, there are also very interesting features close to the boundary of the zone, that is, the Z and X points, which are the signatures of a topological quantum material. Whereas most of the topological quantum materials were predicted by theory first and verified by experiment later, we present an opposite approach: we focused on ultrahigh nonsaturating magnetoresistance, and on this basis we searched for topological states in PtSn_{4} by means of ultrahigh resolution ARPES, followed with band structure calculations.
The crystal structure, Fermi surface and band dispersion along key directions in the Brillouin zone (BZ) for PtSn_{4} are shown in Fig. 1. Figure 1b shows the ARPES intensity integrated within 10 meV of the chemical potential. Highintensity areas mark the contours of the FS sheets. The FS consists of at least one large electron pocket at the centre of BZ, surrounded by several other electron and hole FS sheets, consistent with the quantum oscillation result^{29}. Figure 1c shows the calculated bulk FS, which matches the data well close to the centre of the zone and Z point in Fig. 1b, and is also consistent with the calculated FS using the full potential linearized augmented plane wave (FLAPW) method within the local density approximation (LDA; ref. 29). However, it does not predict the FS crossings close to the X point, missing a set of nearly parallel FS sheets that are present in Fig. 1b. On the other hand, these experimental features are reproduced well by a calculation of the surface states using the slab method; results of which are shown in Fig. 1d. Band dispersions along several cuts in proximity to the Z and X points are shown in Fig. 1e–l. Close to the Z point (Fig. 1e, g), the dispersion resembles a Diraclike feature, but the intensity within the band contour indicates a bulk origin and is consistent with corresponding band calculations shown in Fig. 1f, h. Close to the X point (Fig. 1i, k), the band dispersion is also Diraclike, but very sharp, and thus more likely to be due to surface states; moreover, it is consistent with the slab calculation shown in Fig. 1j, l. The data in Fig. 1 demonstrate that the experimentally observed band structure has both bulk and surface components. The former dominate the Fermi surface close to the Z point, and the latter is prominent close to the X point. The linear dispersion and gapless band crossings strongly suggest that both bulk and surface features at the edge of the Brillouin zone may have topological character, possibly linked to the ultrahigh magnetoresistance, similar to Cd_{3}As_{2} (ref. 5), NbP (ref. 8) and WTe_{2} (ref. 30).
In Fig. 2 we focus on the interesting features near the Z point in more detail. An enlarged image from the red box in Fig. 2a is shown in panel b, where two triangularshaped FS sheets are observed. The detailed evolution of band dispersions along cuts no. 1 to no. 8 is shown in Fig. 2c. A sharp linear dispersion starts to cross at a binding energy of ~200 meV in cut no. 1, and the Dirac point moves up in energy in cuts no. 2–no. 5, finally reaching the Fermi level in cut no. 6, as indicated by red arrows. Then, the Dirac point moves up above the Fermi level and becomes a sharp, shallow hole pocket in cuts no. 7 and no. 8. This movement of the Dirac nodes forms a line in the energy–momentum space in the proximity of Z.
Whereas the behaviour described above has previously been predicted by theory, the structure in the proximity of the X point is far more interesting. We now examine the Fermi surface and band dispersion in a small area in the part of the Brillouin zone that is marked by the red box in Fig. 3a. The Fermi surface in this region consists of a short arc along the symmetry line and two longer, nearly parallel segments on either side of this arc. Detailed band dispersion along cuts no. 1 to no. 12 are shown in Fig. 3c. The data along cut no. 1 show Diraclike dispersion, with the top and bottom bands merging at a single gapless point. The band is very sharp, consistent with its surface origin. As we move closer to the X point, two things happen: a gap develops between top and bottom bands and both top and bottom bands split into two parts symmetric about the k_{z} = 0 line (cuts no. 2–no. 4). Before reaching the X point, the gap vanishes and there are two gapless Diraclike features in close proximity to the X point. The inner bands of the two Dirac features merge along the symmetry line and form an arc at the chemical potential visible in Fig. 3b. The two gapless, Diraclike features extend along one direction in the proximity of the X point between k_{x} ≈ 0.95π/a and 1.05π/a (cuts no. 5 and no. 10 marked by the red frame in Fig. 3c). Outside this momentum range a gap develops, separating the upper and lower portion of the band that is, cuts no. 4.5 and no. 10.5 are already gapped. This gives rise to two arcs of Dirac nodes located at a binding energy of ~60 meV, one on each side of the Γ–X symmetry line, which we named Dirac node arcs.
We now proceed to demonstrate that the Diraclike dispersion shown in Fig. 3 is gapless by plotting the momentum dispersion curves (MDCs) and energy dispersion curves (EDCs). Figure 4c shows the EDC extracted along the red dashed line in 4b. The red arrow marks the peak located at roughly 90 meV below the Fermi level (Fig. 4a), and demonstrates the absence of an energy gap in this single Diraclike feature. In Fig. 4d, we show the double Diraclike features along cut no. 8 (Fig. 3c). The EDCs shown in 4f are extracted along the red dashed lines marked as 1, 2, 3 in Fig. 4e. The red arrows in Fig. 4e, f mark the locations of the peaks at a binding energy of ~60 meV, and show the gapless nature of these dispersions. The same cut measured at two other photon energies (6.36 eV and 6.05 eV) is shown in Fig. 4g and h, respectively. It is clear that the band dispersion does not vary with the incident photon energy (within 16% of the Brillouin zone), demonstrating its surface origin. As such, those states do not have dispersion along a direction perpendicular to the sample surface (that is, k_{y}). The surfacestate calculation using a 42layer slab shows that the conduction and valence bands are separated by roughly 23 meV in the single Dirac feature. However, a further increase in the layer number reduces the gap size significantly, as shown in Fig. 4j. To better illustrate the Dirac node arc structure, we plot the location of the Dirac nodes in momentum space in Fig. 4k by extracting the peak positions of the MDCs at each node (that is, at a binding energy of 90 meV in the single Dirac dispersion and 60 meV at the proximity of the X point in the double Dirac dispersion, as marked by the red dashed lines in Fig. 4a, d). In Fig. 4l, the schematic of the double Dirac node arc structure is shown, with two Dirac dispersions extending along one dimension in momentum space.
Our results show that, near the X point, the single Dirac dispersion evolves into two gapped dispersions and, before reaching the X point, the gaps close and two gapless Diraclike feature emerge extending along one dimension in momentum space, forming a Dirac node arc. These novel features differ from previously predicted Dirac line nodes that form closed loops in momentum space. We proposed that this novel topological nodal structure could be an ideal platform for studying the exotic properties of Dirac fermions. Finally, we note that most of the recently discovered ultrahigh magnetoresistive materials^{26, 27, 28} seem to also possess Dirac or Weyl features in the band dispersions^{5, 8, 30}. As we have demonstrated, this opens an avenue for discovering and identifying novel topological states and relativistic behaviour based on rudimentary transport measurements.
Methods
Sample growth.
Single crystals of PtSn_{4} were grown out of a Snrich binary melt^{31}. The constituent elements, with an initial stoichiometry of Pt_{0.04}Sn_{0.96}, were placed in an alumina crucible and sealed in a quartz tube under a partial Ar pressure. After the quartz ampoule was heated up to 600 °C, the ampoule was cooled down to 350 °C over 60 h (ref. 29). To decant the Sn readily at this temperature, a fritdisc crucible was used^{32}.
Sample preparation and measurements.
ARPES measurements were carried out using a laboratorybased system consisting of a Scienta R8000 electron analyser and a tunable vacuum ultraviolet laser light source^{33}. The data were acquired using a tunable vacuum ultraviolet laser ARPES system, consisting of a Scienta R8000 electron analyser, picosecond Ti:sapphire oscillator and fourth harmonic generator. All data were collected with a constant photon energy of 6.7 eV, except for Fig. 4g (6.36 eV) and 4h (6.05 eV). The angular resolution was set at ~0.05° and 0.5° (0.005 Å^{−1} and 0.05 Å^{−1}) along and perpendicular to the direction of the analyser slit (and thus the cut in the momentum space), respectively; energy resolution was set at 1 meV. The size of the photon beam on the sample was ~30 μm. Samples were cleaved in situ at a base pressure lower than 1 × 10^{−10} torr. Samples were cooled using a closedcycle He refrigerator and the sample temperature was measured using a silicondiode sensor mounted on the sample holder. The energy corresponding to the chemical potential was determined from the Fermi edge of a polycrystalline Au reference in electrical contact with the sample. Samples were cleaved at 40 K and were kept at the cleaving temperature throughout the measurement.
Calculation method.
Density functional theory^{34, 35} (DFT) calculations were done in the Vienna Ab initio Simulation Package (VASP; refs 36,37) using the Perdew–Burke–Ernzerhof (PBE; ref. 38) exchange–correlation functional, a planewave basis set with projected augmented waves^{39} and the spin–orbital coupling (SOC) effect included. For the bulkband structure of PtSn_{4}, we use the conventional orthorhombic cell of 20 atoms with a Monkhorst–Pack^{40} (8 × 6 × 8) kpoint mesh. For surfaceband structure, we use slabs up to 96 atomic layers or 320 atoms with a (8 × 1 × 8) kpoint mesh and at least a 12 Å vacuum. The kinetic energy cutoff is 230 eV. The convergence with respect to the kpoint mesh was carefully checked, with total energy converged, for example, well below 1 meV/atom. We use experimental lattice parameters^{41} of a = 6.418 Å, b = 11.366 Å and c = 6.384 Å with atoms fixed in their bulk positions.
Data availability.
Raw data for this manuscript is available at http://lib.dr.iastate.edu/ameslab_datasets/2.
Change history
 Corrected online 07 April 2016
 In the version of this Letter originally published a note about colour figures was mistakenly included in all of the figure captions. These notes have now been removed in all versions of the Letter.
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Acknowledgements
This work was supported by the US Department of Energy, Office of Science, Basic Energy Sciences, Materials Science and Engineering Division. Ames Laboratory is operated for the US Department of Energy by Iowa State University under contract No. DEAC0207CH11358.
Author information
Author footnotes
Present address: Department of Physics, Simon Fraser University, Burnaby, British Columbia V5A 1S6, Canada.
 Eundeok Mun
Affiliations

Division of Materials Science and Engineering, Ames Laboratory, Ames, Iowa 50011, USA
 Yun Wu,
 LinLin Wang,
 Eundeok Mun,
 D. D. Johnson,
 Daixiang Mou,
 Lunan Huang,
 Yongbin Lee,
 S. L. Bud’ko,
 P. C. Canfield &
 Adam Kaminski

Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA
 Yun Wu,
 Eundeok Mun,
 D. D. Johnson,
 Daixiang Mou,
 Lunan Huang,
 S. L. Bud’ko,
 P. C. Canfield &
 Adam Kaminski

Department of Materials Science and Engineering, Iowa State University, Ames, Iowa 50011, USA
 D. D. Johnson
Contributions
P.C.C. initiated the work by insisting that Y.W. and A.K. design and carry out the experiment. Y.W., D.M. and L.H. acquired and analysed ARPES data. L.L.W., D.D.J. and Y.L. carried out the DFT calculations. E.M. grew the samples under the supervision of S.L.B. and P.C.C. The manuscript was drafted by Y.W. and A.K. All authors discussed and commented on the manuscript.
Competing financial interests
The authors declare no competing financial interests.
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Yun Wu
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LinLin Wang
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Eundeok Mun
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