Co-reporter:Hiroyuki Inoue;András Gyenis;Zhijun Wang;Jian Li;Seong Woo Oh;Shan Jiang;Ni Ni;B. Andrei Bernevig
Science 2016 Volume 351(Issue 6278) pp:1184-1187
Publication Date(Web):11 Mar 2016
DOI:10.1126/science.aad8766
Sinking into the bulk of a Weyl semimetal
A recently discovered class of topological materials, Weyl semimetals, have surface states in the form of so-called Fermi arcs. Inoue et al. used a high-resolution scanning tunneling microscope to explore the properties of these states in the material TaAs. They mapped the scattering of electrons off impurities on the surface of the material and compared the data to the predictions of density functional theory. The data could be reconciled with the theory only if electrons associated with Ta orbitals on the Fermi arcs sank into the bulk of the material.
Science, this issue p. 1184
Co-reporter:Benjamin E. Feldman;Mallika T. Randeria;András Gyenis;Fengcheng Wu;Huiwen Ji;R. J. Cava;Allan H. MacDonald
Science 2016 Vol 354(6310) pp:316-321
Publication Date(Web):21 Oct 2016
DOI:10.1126/science.aag1715
Relating interactions and nematicity
The electronic system in a strongly correlated material can sometimes be less symmetrical than the underlying crystal lattice. This loss of symmetry, caused by interactions and dubbed electronic nematicity, has been observed in a number of exotic materials. However, establishing a direct connection between the interactions and nematicity is tricky. Feldman et al. used scanning tunneling microscopy to image the wave functions of electrons on the surface of bismuth placed in an external magnetic field. The exchange interactions in the material caused a loss of symmetry, which was reflected in the orientations of the electrons' elliptical orbits.
Science, this issue p. 316
Co-reporter:András Gyenis;Eduardo H. da Silva Neto;Ronny Sutarto;Enrico Schierle;Eugen Weschke;Joe D. Thompson;Eric D. Bauer;Zachary Fisk;Feizhou He;Mariam Kavai;Ryan E. Baumbach;Andrea Damascelli;Pegor Aynajian
Science Advances 2016 Volume 2(Issue 10) pp:e1601086
Publication Date(Web):14 Oct 2016
DOI:10.1126/sciadv.1601086
Probing the quasi-particle interference of heavy fermions by resonant x-ray scattering and scanning tunneling spectroscopy.
Co-reporter:Stevan Nadj-Perge;Jian Li;Sangjun Jeon;Hua Chen;Ilya K. Drozdov;Allan H. MacDonald;Jungpil Seo;B. Andrei Bernevig
Science 2014 Volume 346(Issue 6209) pp:
Publication Date(Web):
DOI:10.1126/science.1259327
A possible sighting of Majorana states
Nearly 80 years ago, the Italian physicist Ettore Majorana proposed the existence of an unusual type of particle that is its own antiparticle, the so-called Majorana fermion. The search for a free Majorana fermion has so far been unsuccessful, but bound Majorana-like collective excitations may exist in certain exotic superconductors. Nadj-Perge et al. created such a topological superconductor by depositing iron atoms onto the surface of superconducting lead, forming atomic chains (see the Perspective by Lee). They then used a scanning tunneling microscope to observe enhanced conductance at the ends of these chains at zero energy, where theory predicts Majorana states should appear.
Science, this issue p. 602; see also p. 547
Co-reporter:Eduardo H. da Silva Neto;Pegor Aynajian;Alex Frano;Riccardo Comin;Enrico Schierle;Eugen Weschke;András Gyenis;Jinsheng Wen;John Schneeloch;Zhijun Xu;Shimpei Ono;Genda Gu;Mathieu Le Tacon
Science 2014 Volume 343(Issue 6169) pp:393-396
Publication Date(Web):24 Jan 2014
DOI:10.1126/science.1243479
Abstract
Besides superconductivity, copper-oxide high-temperature superconductors are susceptible to other types of ordering. We used scanning tunneling microscopy and resonant elastic x-ray scattering measurements to establish the formation of charge ordering in the high-temperature superconductor Bi2Sr2CaCu2O8+x. Depending on the hole concentration, the charge ordering in this system occurs with the same period as those found in Y-based or La-based cuprates and displays the analogous competition with superconductivity. These results indicate the similarity of charge organization competing with superconductivity across different families of cuprates. We observed this charge ordering to leave a distinct electron-hole asymmetric signature (and a broad resonance centered at +20 milli–electron volts) in spectroscopic measurements, indicating that it is likely related to the organization of holes in a doped Mott insulator.
Co-reporter:Ali Yazdani;Brian Zhou;Shawn Mack;Pedram Roushan;David D. Awschalom;David A. Huse;Anthony Richardella
Science 2010 Volume 327(Issue 5966) pp:665-669
Publication Date(Web):05 Feb 2010
DOI:10.1126/science.1183640
Co-reporter:John Mydosh;Yingkai Huang;Pegor Aynajian;Abhay Pasupathy;Colin V. Parker;Eduardo H. da Silva Neto
PNAS 2010 Volume 107 (Issue 23 ) pp:10383-10388
Publication Date(Web):2010-06-08
DOI:10.1073/pnas.1005892107
Heavy electronic states originating from the f atomic orbitals underlie a rich variety of quantum phases of matter. We use atomic scale imaging and spectroscopy with the
scanning tunneling microscope to examine the novel electronic states that emerge from the uranium f states in URu2Si2. We find that, as the temperature is lowered, partial screening of the f electrons’ spins gives rise to a spatially modulated Kondo–Fano resonance that is maximal between the surface U atoms. At
T = 17.5 K, URu2Si2 is known to undergo a second-order phase transition from the Kondo lattice state into a phase with a hidden order parameter.
From tunneling spectroscopy, we identify a spatially modulated, bias-asymmetric energy gap with a mean-field temperature dependence
that develops in the hidden order state. Spectroscopic imaging further reveals a spatial correlation between the hidden order
gap and the Kondo resonance, suggesting that the two phenomena involve the same electronic states.
Co-reporter:Aakash Pushp;Colin V. Parker;Abhay N. Pasupathy;Kenjiro K. Gomes;Shimpei Ono;Zhijun Xu;Jinsheng Wen;Genda Gu
Science 2009 Volume 324(Issue 5935) pp:1689-1693
Publication Date(Web):26 Jun 2009
DOI:10.1126/science.1174338
Cuprate Analysis
Despite more than 20 years of intensive effort, the mechanism providing superconductivity in the cuprates remains elusive and contentious, partly because the cuprates are inhomogeneous. Scanning tunneling spectroscopy (STS) and high-resolution, angle-resolved photoemission spectroscopy provide energy and momentum information about the excitations in the high-temperature cuprate superconductors. Pushp et al. (p. 1689, published online 4 June) provide a STS study of the cuprate Bi2Sr2CaCu2O8+δ over a range of doping levels and temperatures. This methodology for analyzing the spectra takes into account the inhomogeneity and may provide insight into how a superconducting pairing mechanism evolves from the parent insulating state.
Co-reporter:Pedram Roushan,
Jungpil Seo,
Colin V. Parker,
Y. S. Hor,
D. Hsieh,
Dong Qian,
Anthony Richardella,
M. Z. Hasan,
R. J. Cava
&
Ali Yazdani
Nature 2009 460(7259) pp:1106
Publication Date(Web):2009-08-09
DOI:10.1038/nature08308
Topological insulators are materials in which a relativistic effect known as spin–orbit coupling gives rise to surface states that resemble chiral edge modes in quantum Hall systems, but with unconventional spin textures. It has been suggested that a feature of such spin-textured boundary states is their insensitivity to spin-independent scattering, which is thought to protect them from backscattering. Here, scanning tunnelling spectroscopy and angle-resolved photoemission spectroscopy are used to confirm this prediction.
Co-reporter:Kenjiro K. Gomes, Abhay N. Pasupathy, Aakash Pushp, Colin Parker, Shimpei Ono, Yoichi Ando, Genda Gu, Ali Yazdani
Journal of Physics and Chemistry of Solids 2008 Volume 69(Issue 12) pp:3034-3038
Publication Date(Web):December 2008
DOI:10.1016/j.jpcs.2008.06.136
High-resolution scanning tunneling microscopy has been used to study the formation of Cooper pairs in the cuprate superconductor Bi2Sr2CaCu2O8+δBi2Sr2CaCu2O8+δ. We measured the evolution of the tunneling gap as function of temperature (from 20 to 180 K) and doping (x=0.12–0.22)(x=0.12–0.22). Real space mapping of the density of states establish that the tunneling gap observed below the transition temperature (Tc)(Tc) vanish inhomogenously in space, leading to the formation of a unique intermediate state, where nanoscale regions of pairing are present. Despite the inhomogeneity, we find that locally the gap spectrum evolves smoothly across TcTc and, over a wide range of doping (x⩾0.16)(x⩾0.16), the energy gap ΔΔ vanishes at a temperature TpTp, following a local criterion 2Δ/kBTp=7.9±0.52Δ/kBTp=7.9±0.5. Our observations suggest that at least in optimally doped and overdoped samples, all our measurements can be described with one single energy scale and that the gap measured above and below TcTc must have the same origin. In the underdoped regime, this simple description fails to capture the temperature evolution of the local electronic states, indicating the presence of an additional phenomenon.
Co-reporter:Abhay N. Pasupathy;Aakash Pushp;Kenjiro K. Gomes;Colin V. Parker;Jinsheng Wen;Zhijun Xu;Genda Gu;Shimpei Ono;Yoichi Ando
Science 2008 Volume 320(Issue 5873) pp:196-201
Publication Date(Web):11 Apr 2008
DOI:10.1126/science.1154700
Abstract
Identifying the mechanism of superconductivity in the high-temperature cuprate superconductors is one of the major outstanding problems in physics. We report local measurements of the onset of superconducting pairing in the high–transition temperature (Tc) superconductor Bi2Sr2CaCu2O8+δ using a lattice-tracking spectroscopy technique with a scanning tunneling microscope. We can determine the temperature dependence of the pairing energy gaps, the electronic excitations in the absence of pairing, and the effect of the local coupling of electrons to bosonic excitations. Our measurements reveal that the strength of pairing is determined by the unusual electronic excitations of the normal state, suggesting that strong electron-electron interactions rather than low-energy (<0.1 volts) electron-boson interactions are responsible for superconductivity in the cuprates.
Co-reporter:Kenjiro K. Gomes,
Abhay N. Pasupathy,
Aakash Pushp,
Shimpei Ono,
Yoichi Ando
&
Ali Yazdani
Nature 2007 447(7144) pp:569
Publication Date(Web):2007-05-31
DOI:10.1038/nature05881
Pairing of electrons in conventional superconductors occurs at the superconducting transition temperature Tc, creating an energy gap Δ in the electronic density of states (DOS)1. In the high-Tc superconductors, a partial gap in the DOS exists for a range of temperatures above Tc (ref. 2). A key question is whether the gap in the DOS above Tc is associated with pairing, and what determines the temperature at which incoherent pairs form. Here we report the first spatially resolved measurements of gap formation in a high-Tc superconductor, measured on Bi2Sr2CaCu2O8+δ samples with different Tc values (hole concentration of 0.12 to 0.22) using scanning tunnelling microscopy. Over a wide range of doping from 0.16 to 0.22 we find that pairing gaps nucleate in nanoscale regions above Tc. These regions proliferate as the temperature is lowered, resulting in a spatial distribution of gap sizes in the superconducting state3, 4, 5. Despite the inhomogeneity, we find that every pairing gap develops locally at a temperature Tp, following the relation 2Δ/kBTp = 7.9 ± 0.5. At very low doping (≤0.14), systematic changes in the DOS indicate the presence of another phenomenon6, 7, 8, 9, which is unrelated and perhaps competes with electron pairing. Our observation of nanometre-sized pairing regions provides the missing microscopic basis for understanding recent reports10, 11, 12, 13 of fluctuating superconducting response above Tc in hole-doped high-Tc copper oxide superconductors.
Co-reporter:Dale Kitchen,
Anthony Richardella,
Jian-Ming Tang,
Michael E. Flatté
and
Ali Yazdani
Nature 2006 442(7101) pp:436
Publication Date(Web):
DOI:10.1038/nature04971