Fast core rotation in red-giant stars revealed by gravity-dominated mixed modes. Paul G. Beck1 ... 13 Orbital Sciences Corporation/NASA Ames Research Center, Moffett Field, CA 94035, USA. When the core hydrogen is .... corresponding rotational splitt
ing (TRSB), hosting an intrinsic Cooper pair magnetiza- tion [1, 2]. This can ... site to explain current experiments, but it has previously been shown .... Ginzburg-Landau free energy â We now consider super- conductivity at the level of the Ginzb
modified classical action SJ k containing the IR-cutoff and source terms. The semiclassi- cal expansion will be applied to this integral. Therefore we need to know the absolute minimum Ïmin(x; J, k) of this functional. In section V we derive a suffi
Dec 22, 2015 - Bi2Se3 is one of the best studied TIs [14, 15], and most interestingly, Cu intercalation between the .... Hor, Y. S., Williams, A. J., Checkelsky, J. G., Roushan, P., Seo, J., Xu, Q., Zandbergen,. H.W., Yazdani, A. ... Additional infor
Jun 7, 2018 - a large sample of globular clusters using proper motions from Gaia DR2. We detect signatures of rotation in the tangential component of proper ...
Nov 23, 2016 - Department of Physics & Astronomy, University of Sussex, Brighton BN1 9QH, ... For example, superfluid Helium can support linear structures.
Jan 11, 1999 - ticular (nonlinear) gauge obtained by adopting an origin, ËÏ, in the coset ... in collaboration with H. Tann  aims at accounting for the origin of.
Jun 19, 2000 - We construct models in which electroweak symmetry is spontaneously bro- ken by supersymmetric strong dynamics at the TeV scale. The order pa ...... grated out and the S-color gauge coupling will rapidly go from fixed point behavior to.
EFI-2000-11. Fermilab-Conf-00-077-T. ELECTROWEAK SYMMETRY BREAKING BY EXTRA. DIMENSIONS. Hsin-Chia Cheng. Enrico Fermi Institute, The ...
Feb 27, 2017 - We consider a system of interacting fermions described by the NambuâJona- ..... dial contribution to energy, can be determined as follows.
Jul 4, 2007 - Because of the large negative contribu- tion from top quark loop, either extra gauge bosons [1, 3, 4] or ... blet Model (IDM) because the extra (or inert) doublet does not couple to the quarks (and leptons in ... (resp. between DM and H
Dec 2, 2016 - KEK Theory Center, High Energy Accelerator Research Organization,. 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan. Graduate University for ...
The pair-field appears when the mean-field approx- imation is applied, which results in the Hartree-Fock-. 1See A. Goodman's contribution to this meeting and , ..... Here we used eâiÎ±Ï = eâiIÏ. A strong M = 1 pair- field implies that adjace
Aug 1, 2017 - symmetric pair production takes place in a vacuum with no monopole condensation. Our results strongly indicate that the chiral symmetry is ...
Abstract: We uncover that the breaking point of the -symmetry in optical wave- guide arrays has a dramatic impact on light localization induced by the ...
where GN is broken down to SU(3) Ã SU(2) Ã U(1)nâ3 by the bifundamental link fields and the ... 1Current Address: School of Natural Sciences, Institute for Advanced Study, Einstein Drive,. Princeton, NJ 08540. ... the supersymmetric. 5-dimensiona
1 SETI Institute, 189 Bernardo Ave, Mountain View, CA 94043, USA. 2Department ... Mueller Matrix; Symmetry; light scattering; zenith and off-zenith; polarization;.
which leads to an asymmetric shape of skyrmions . .... difference in the measured dI/dV signal is revealed for those parts of the spin spiral with a local in- ...
Invited talk at the 8th General Meeting, European Women in Mathematics, ... The second is more like the supporting cast, without which the theory, although it ...
Apr 28, 2005 - Gauge symmetry breaking is at the core of the current understanding of the particle interactions. Yet the Higgs particle remains as an enigma in ...
May 27, 2014 - dered bundles of the magnetic lines of force with a sig- nificant degree of long-range ..... a different destiny of a particle on the off-equatorial circular orbit when its ..... force problem which concerns the motion of the particle
A difficulty arises when one deals with theories where the symmetry breaking is ... have a simple expression in terms of Veff and the other functions entering Seff.
Jun 7, 2018 - chosen to be less then 2a, therefore, the resultant condition d < 2a âª Î» is .... and invisibility regions of a symmetric trimer (design D3h) with the ... a = 0.5 Âµm, Îµ1 = 3.9 (SiO2), Îµ2 = 1.0 (air), Âµ1 = Âµ2 = 1.0, T = 300 K, Âµc
Aug 5, 2016 - (Color online) Fermi surfaces of the tetragonal and monoclinic .... (Color online) Calculated band structures for LaO0.5F0.5BiS2 of the tetragonal structure (a) with and (b) without SOC, and (f)-(g) those for the monoclinic one. ......
Rotation symmetry breaking in La2−x Srx CuO4 revealed by ARPES E. Razzoli,1, 2, ∗ C. E. Matt,1, 3 Y. Sassa,1, 3, 4 M. M˚ ansson,5, 6, 7 O. Tjernberg,7 G. Drachuck,8 M. Monomo,9 M. 10 10 11 1 Oda, T. Kurosawa, Y. Huang, N. C. Plumb, M. Radovic,1 A. Keren,8 L. Patthey,1 J. Mesot,1, 3, 12 and M. Shi1
arXiv:1706.04696v1 [cond-mat.supr-con] 14 Jun 2017
Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland 2 D´epartement de Physique and Fribourg Center for Nanomaterials, Universit´e de Fribourg, CH-1700 Fribourg, Switzerland 3 Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland 4 Department of Physics and Astronomy, Uppsala University, S-75121 Uppsala, Sweden 5 Laboratory for Quantum Magnetism (LQM),Ecole Polytechnique F´ed´erale de Lausanne (EPFL), Station 3, CH-1015 Lausanne, Switzerland 6 Laboratory for Neutron Scattering, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland 7 KTH Royal Institute of Technology, Materials Physics, Electrum 229, 164 40 Kista, Stockholm, Sweden 8 Physics Department, Technion, Israel Institute of Technology, Haifa 32000, Israel 9 Department of Applied Sciences, Muroran Institute of Technology, Muroran 050-8585, Japan 10 Department of Physics, Hokkaido University, Sapporo 060-0810, Japan 11 Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China 12 Institut de la Matiere Complexe, EPF Lausanne, CH-1015, Lausanne, Switzerland (Dated: March 12, 2018) Using angle-resolved photoemission spectroscopy it is revealed that in the vicinity of optimal doping the electronic structure of La2−x Srx CuO4 cuprate undergoes an electronic reconstruction associated with a wave vector q a = (π, 0). The reconstructed Fermi surface and folded band are distinct to the shadow bands observed in BSCCO cuprates and in underdoped La2−x Srx CuO4 with x ≤ 0.12, which shift the primary band along the zone diagonal direction. Furthermore the folded bands appear only with q a = (π, 0) vector, but not with q b = (0, π). We demonstrate that the absence of q b reconstruction is not due to the matrix-element effects in the photoemission process, which indicates the four-fold symmetry is broken in the system. PACS numbers: 74.72.Gh, 74.25.Jb, 79.60.-i
Since the discovery of high-temperature cuprate superconductors, the study of various instabilities (e.g. magnetic and charge order) emerging in close proximity to superconductivity has attracted much attention. Significant efforts have been devoted to reveal other instabilities than superconducting one, as a function of doping and temperature, and how they are intertwined with the superconductivity. Recently an incipient incommensurate charge-density-wave (CDW) in underdoped YBa2 Cu3 O6+y (YBCO) with hole concentrations in the range of 0.09 to 0.13 per planar Cu ion has been reported independently from high-energy Xray diffraction1 and resonant soft X-ray scattering2 experiments. Similar charge modulations along the Cu-O bonding directions of underdoped Bi2 Sr2−x Lax CuO6+δ (Bi2201) and Bi2 Sr2 CaCu2 O8+δ (Bi2212) have also been observed in scanning-tunneling microscopy and resonant x-ray scattering measurements, with the ordering vector approaching to a commensurate wave vector (0.25 × π/a) when the hole doping is increasing3,4 . For underdoped La-based “214” family of cuprates (La2−x−y (Sr,Ba)x (Nd,Eu)y CuO4 ) at a doping level x ≈ 1/8 an unidirectional modulated antiferromagnetism5 combined with a commensurate charge modulation of period 4 lattice constant (stripe order) has long been iden-
tified, and at the same doping level the superconducting transition temperature is dramatically reduced6,7 . The presence of stripe order in La2−x Srx CuO4 has been debated for long time and only recently scattering measurements have shown evidence for a CDW with a wave vector q displaying a doping dependence similar to the one observed in Bi2201 and La2−x Bax CuO4 8–10 . However, so far, angle-resolved photoemission spectroscopy (ARPES) measurements have not shown any evidence of band folding associated with charge ordering along the Cu-O bond direction in cuprates11–13 . In this letter, applying ARPES to nearly optimally doped LSCO (x = 0.15, 0.17) we show that in the superconducting phase the Fermi surface (FS) is reconstructed along the Cu-O bond direction associated with a wave vector q a = (π, 0). This wave vector could be related to the second harmonic of an incipient CDW in the region of optimal doping, which is the smooth continuation with doping of the incipient CDW as observed in other cuprates, or could point to a new instability in the system.
ARPES experiments were carried out at the Surface and Interface Spectroscopy beamline at the Swiss
TABLE I: Tight-binding coefficient and basis functions used in fitting the experimental data. The second column lists the coefficient of each term (meV) following the convention: P (k) = ti ηi (k). i 0 1 2 3
FIG. 1: (a) LEED pattern taken at T = 12 K and Ee = 185 eV. (b) FS mapping for LSCO x = 0.17. Dashed-pointed black line is a TB fit as explained in the text.
Light Source of Paul Sherrer intitute on single crystals La2−x Srx CuO4 (LSCO). The doping values used for the measurements are x = 0.15 and 0.17 with superconducting transition temperature (Tc ) of 38 K and 35 K, respectively. The crystals were grown in traveling solvent floating zone furnaces. All samples were characterized by x-ray diffraction, and their superconducting transitions were determined by magnetization measurements. Circularly polarized light with hν = 55 eV was used in order to maximize the signal. The spectra were recorded with Scienta R4000 analyzers. The energy and angle resolutions were ∼ 15 meV and 0.1 - 0.15◦ , respectively. The Fermi level was determined by recording photoemission spectra from polycrystalline copper on the sample holder. The samples were cleaved in situ by using a specially designed cleaver14 . Low-energy electron diffraction analysis of the cleaved samples shows a clear (1 × 1) pattern with no sign of surface reconstruction [see Fig. 1(a)]. During the measurements, the base pressure always remained less than 5 × 10−11 mbar.
Figure 1(b) shows the spectral weight mapping in kspace at Fermi level (EF ). The superimposed dashed black line is the FS obtained from a tight binding (TB) fit to the kF extracted from the peak positions of momentum distribution curves (MDC) at EF and to the MDC peak positions, as a function of binding energy, along the zone diagonal (nodal dispersion). The basis functions and the obtained fitting coefficients with the constraint t3 /t2 = −1/215 are listed in Table I. Luttinger sum rule16 gives a hole concentration of x ∼ 0.19, slightly bigger than the nominal doping x = 0.17, in agreement with the observation in early studies17 . To enhance the weak features, in Fig. 2(a) we display the intensity map at EF in logarithmic color scale. Besides the primary FS in Map I, in the middle of the intensity plot [see also Fig. 1 (b)], two weak but clearly visible pieces of FS appear on the left and right sides of the primary FS. In Fig. 2(b) we plot the kF extracted
ti 134 181 -23 12
ηi (k) 1 -2[cos(kx a) + cos(ky a)] -4[cos(kx a) cos(ky a)] -2[cos(2kx a) + cos(2ky a)]
from the peak positions in Map I of MDC at EF for both the primary FS (red triangles) and the weak pieces of FS (blue circles). It can be seen that the two weak pieces of FS mirror the primary FS about the vertical lines at kx = ±π/2, which is equivalent to shifting the primary FS by a commensurate wave vector q a = (π, 0) (dashed violet line). The appearance of the weak pieces of FS indicates that a Fermi surface reconstruction related to a wave vector q a occurs in the system. The reconstructed FS is different to the shadow FS previously observed in LSCO18,19 and in BSCCO cuprates20 because in those cases the shadow FS is connected to the primary FS by a wave vector along the zone diagonal, i.e. in the (π, π) direction. It is important to mention that we have observed a reconstructed FS related to the wave vector q a = (π, 0), which is nearly parallel to the cut direction, but found no sign for a reconstruction corresponding to wave vector q b = (0, π). The lack of the q b -folded band might be due to two different effects; the q b folded band is present but not observed due to ARPES selection rules (the socalled ”matrix element effects”)21 or the this folded band is not present and the C4 rotational symmetry of the system is broken in favor of C2 symmetry. To confirm that the lack of q b reconstruction is not due to the matrix element effects in the photoemission process, we rotated the sample about the surface normal (c-axis) by 90◦ and acquired ARPES data with otherwise unchanged experimental conditions. In case of a matrix element effects we would expect to see the band folded again in direction parallel to the (new) cut direction, i.e. along the (0, π) = q b . As shown in Map II of Fig. 2(a) and in the corresponding kF in Fig. 2(b) (light-blue pentagons and green rhombus), the reconstructed FS is not displaced along q b but still follow the original folding direction q a . This observation demonstrates that the reconstruction of FS is not due to matrix elements effects and it ascertains that the four-fold symmetry is broken in the system. The q a reconstruction is further illustrated in Fig. 3 which shows the band dispersions along cut 1-4 as indicated in Fig. 2(b). All the folded-bands associated with the reconstruction can be reproduced after shifting the primary band by wave vector q a . On the other hand, no folded-band related to q b reconstruction was observed. We have investigated the folded bands in LSCO in a wide doping range. For x ≤ 0.12 a folded band related
FIG. 2: ARPES Intensity plots of La2−x Srx CuO4 (x = 0.17). The data were taken at 12 K. (a) FS intensity maps in the kx − ky plane at hν = 55 eV and T = 12 K . Map II is the same as Map I but after a 90◦ rotation of the sample. The FS maps in I-II are obtained by integrating ARPES spectral weight in an energy window of EF ± 20 meV. (b) Red triangles (green rombus) and blue circles (light-blue pentagons) are the kF for the primary band (PB) and the folded band (FB) extracted from the MDCs peaks for the sample oriented like in Map I (Map II), respectively. Dashed-pointed black line is a TB fit to the PB data, dashed violet line is the TB FS shifted by q a = (π, 0), and dotted orange line is the TB FS shifted by q b = (0, π) .
to a shifting of the primary band by q = (π, π) was observed19 . For x ≥ 0.22, except the primary FS and band, there is no indication for any observable reconstructed FS and folded band in our ARPES data acquired in the same experimental conditions. The q a = (π, 0) FS reconstruction and the associated band folding appear only in the vicinity of optimally doped samples (x = 0.15, 0.17). Figure 4 shows the ARPES spectra taken from a slightly underdoped LSCO sample with x = 0.15. Although the intensity is weaker than the case for x = 0.17, the folded bands are still clearly visible, as indicated by the arrows in Figs. 4(a)-(e). The kF extracted from the peak positions of MDC at EF show that the folded bands and their FS result from a q a = (π, 0) reconstruction [Fig. 4(f)].
The q a = (π, 0) electronic reconstruction in the vicinity of optimal doping of LSCO (x = 0.15, 0.17) is different to the previously observed shadow bands and FS duplication along the zone diagonal in cuprates18–20 . This rules out the possibility that the q a = (π, 0) reconstruction is due to structurally orthorhombic distortions (LTO) of the crystal structure from tetragonality, because in that case one would expect that a copy of the primary FS is shifted along the (π, π) direction22 . A low temperature tetragonal reconstruction (LTT), as the one observed in
La2−x Bax CuO4 23 , localized at the surface of LSCO could explain the (π−0) reconstruction. Indeed LSCO has been reported to be on the verge of a LTO to LTT transition at low temperature24 , which could get stabilized at the surface during the cleaving procedure. However while our measurements report that the (π − 0) reconstruction is stabilized only in a narrow range of optimal dopings (x = 0.15 − 0.17), inelastic neutron-scattering measurements show that at the LTO-LTT structure instability is stronger at low dopings (x ≤ 0.12)25 . The opposite dependence of the LTO-LTT instability and of the reported (π−0) folding suggests that two effect may not be related. The absence in the LEED patterns [see e.g. Fig. 1(a)] of any signature of 1 × 2 or 2 × 1 surface reconstruction indicates that the folding could result from a dynamic charge modulation or from a nontrivial structural distortion, similar but different to the case of Bi2212 shadows bands22 , where a orthorombic distortion was observed in LEED only at very low energies (below 20 eV)26 . The strong doping dependence of the folded bands suggests that the folding, independently from its origin, is somehow tied to the electronic properties of the sample. The q a folded bands were observed at T = 12 K which is well below the superconducting temperature 38 K and 35 K for LSCO with x = 0.15 and x = 0.17, respectively. This suggests that if the q a electronic reconstruction is associated with an instability in the system such as a density wave, the ordering coexists with superconducting instability. We note that the q a wave vector asso-
k|| [π/a] (g)
0 kx [π/a]
-0.05 -0.10 -0.15
FIG. 3: Dispersion of the primary and folded band along selected cuts for La2−x Srx CuO4 (x = 0.17). The data were taken at 12 K. (a)-(b) MDC at the EF −0.01 meV and ARPES intensity map for the cut 1 in 2(c), respectively. (c)-(d) MDC at the EF − 0.01 meV and ARPES intensity map for the cut 2 in 2(d), respectively. (e)-(f) MDC at the EF − 0.01 meV and ARPES intensity map for the cut 3 in 2(c), respectively. (g)(h) MDC at the EF − 0.01 meV and ARPES intensity map for the cut 4 in 2(d), respectively. The dispersion of the band folded by q a = (π, 0) (dashed violet line) and q b = (0, π) (dotted orange line) are superimposed to the intensity maps in (b),(h) and (d),(f), respectively.
ciated with the electronic reconstruction is unexpected from the smooth continuation of the incipient incommensurate charge-density-wave along the Cu-O bonding direction, observed in LSCO8–10 and other underdoped cuprates1–4 . There, with increasing doping, the incipient incommensurate wave vector is approaching a commensurate one (π/2, 0), instead of q a = (π, 0). However, one possibility could be that the observed q a corresponds to band-folding associated with two times of (π/2, 0), and the electronic states related to the (π/2, 0) reconstruction is too weak to be observed due to the matrix element effects in the photoemission process. Another possibility is that the q a reconstructed FS is related the change of FS topology near x = 0.1719 . In LSCO, at the doping level slightly above x = 0.17, the primary FS changes from a hole-like pocket centered at the (π, π) point to an electron-like pocket centered at the Γ point, the center of the BZ. Accompanying with the topological change of the FS a Van Hove singularity at (π, 0) saddle-point approaches the Fermi level. The large and discontinuous density of states near EF could result in a dynamic charge modulation which leads to a spontaneous breakdown of the point group symmetry27,28 . The charge modulations
0.5 1.0 1.5
0.5 1.0 1.5
0.5 1.0 1.5
FIG. 4: (a)-(e) ARPES Intensity plots of La2−x Srx CuO4 (x = 0.15) along the cuts (from top to bottom) shown in (f). The data were taken at 12 K. White arrows indicate the folded band. (f) Black curves are FS of the primary band. The violet curve is a copy of the primary FS, but shifted by q a = (π, 0). Black lines indicate the momentum cuts. Red triangles and blue empty circles are kF of the primary and the folded bands, which are determined from MDCs at zero binding energy.
could involve the whole crystal or the bulk system could be on the verge of a (π, 0) electronic reconstruction which get stabilized only at the surface by the disorder and/or the breaking of translational symmetry, similarly to what was shown for the stripe order in LSCO with x = 1/829 . Regardless of the exact origin, our observation indicates that at low temperatures an instability associated with the breaking of C4 symmetry coexists with superconductivity near the optimal doping of LSCO. However, it is unclear whether the observed q a = (π, 0) electronic reconstruction is general for hole-doped superconducting cuprates, or is particularly related to LSCO.
In summary, using ARPES we revealed the presence of a weaker folded band which resembles the primary band shifted by q a = (π, 0) in the superconducting state of nearly optimally doped LSCO (x = 0.15, 0.17). We show that the absence of a q b = (0, π) folded band is intrinsic but not due to the matrix element effects of the photoemission process, which indicates that the C4 symmetry is broken in the system. The unusual doping dependence of such folded band deserves further study to identify its origin.
We are grateful to J. Chang for useful discussions. This work was performed at SLS of the Paul Scherrer Insitut, Villigen PSI, Switzerland and it was supported by the Swiss National Science Foundation through
Present address: Quantum Matter Institute, Department of Physics and Astronomy, University of British Columbia, Vancouver, British Columbia V6T 1Z1, Canada J. Chang, E. Blackburn, A. T. Holmes, N. B. Christensen, J. Larsen, J. Mesot, Ruixing Liang, D. A. Bonn, W. N. Hardy, A. Watenphul, M. v. Zimmermann, E. M. Forgan, and S. M. Hayden Nature Physics 8, 871-876 (2012). G. Ghiringhelli, M. Le Tacon, M. Minola, S. BlancoCanosa, C. Mazzoli, N. B. Brookes, G. M. De Luca, A. Frano2, D. G. Hawthorn, F. He, T. Loew, M. Moretti Sala, D. C. Peets, M. Salluzzo, E. Schierle, R. Sutarto, G. A. Sawatzky, E. Weschke, B. Keimer, and L. Braicovich Science 337, 821-825 (2012). R. Comin, A. Frano, M. M. Yee, Y. Yoshida, H. Eisaki, E. Schierle, E. Weschke, R. Sutarto, F. He, A. Soumyanarayanan, Yang He, M. Le Tacon, I. S. Elfimov, Jennifer E. Hoffman, G. A. Sawatzky, B. Keimer, A. Damascelli Science 343, 390-392 (2014). E. H. da Silva Neto, P. Aynajian, A. Frano, R. Comin, E. Schierle, Eugen Weschke, A. Gyenis, J. Wen, J. Schneeloch, Z. Xu, S. Ono, G. Gu, M. Le Tacon, and A. Yazdani Science 343, 393-396 (2014). M. Plat´e, J. D. F. Mottershead, I. S. Elfimov, D. C. Peets, Ruixing Liang, D. A. Bonn, W. N. Hardy, S. Chiuzbaian, M. Falub, M. Shi, L. Patthey, and A. Damascelli Phys. Rev. Lett 95, 077001 (2005). J. M. Tranquada, B. J. Sternlieb, J. D. Axe, Y. Nakamura and S. Uchida, Nature 375, 561 - 563 (1995). J. M. Tranquada, J. D. Axe, N. Ichikawa, Y. Nakamura, S. Uchida, and B. Nachumi Phys. Rev. B 54, 7489 (1996). T. P. Croft , C. Lester, M. S. Senn, A. Bombardi, and S. M. Hayden, Phys. Rev. B 89, 224513 (2014). N. B. Christensen J. Chang, J. Larsen, M. Fujita, M. Oda, M. Ido, N. Momono, E. M. Forgan, A. T. Holmes, J. Mesot, M. Huecker, and M. v. Zimmermann, arXiv 1404.3192 (2014). V. Thampy, M. P. M. Dean, N. B. Christensen, Z. Islam, M. Oda, M. Ido, N. Momono, S. B. Wilkins, and J. P. Hill, arXiv 1404.3193 (2014). Y. Kohsaka, C. Taylor, P. Wahl, A. Schmidt, Jhinhwan Lee, K. Fujita, J. W. Alldredge, K. McElroy, Jinho Lee, H. Eisaki, S. Uchida, D.-H. Lee, and J. C. Davis Nature 454, 07243 (2008). J. Meng, G. Liu, W. Zhang, L. Zhao, H. Liu, X. Jia, D. Mu, S. Liu, X. Dong, J. Zhang, W. Lu, G. Wang, Y. Zhou, Y. Zhu, X. Wang, Z. Xu, C. Chen, and X. J. Zhou Nature 462, 335 (2009). A. Kanigel, M. R. Norman, M. Randeria, U. Chatterjee, S. Souma, A. Kaminski, H. M. Fretwell, S. Rosenkranz, M. Shi, T. Sato, T. Takahashi, Z. Z. Li, H. Raffy, K. Kadowaki, D. Hinks, L. Ozyuzer, and J. C. Campuzano Nature
NCCR MaNEP and the Grant No. 200021-137783. E.R. acknowledges support from the Swiss National Science Foundation (SNSF) grant no. P300P2 164649. M.M. and Y.S. acknowledge project funding from the Swedish Research Council (Dnr. 2016-06955). We thank the beam line staff of SIS for their excellent support.
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