The DOI matches its Crossref record; 35 of the 35 references it cites were found in a registry or an index; 8 of the 8 sources its claims cite were checked for support.
Observation of a large-gap topological-insulator class with a single Dirac cone on the surface
Open accessAbstract
Y. Xia, 2 D. Qian, 3 D. Hsieh, 2 L. Wray, A. Pal, H. Lin, A. Bansil, D. Grauer, Y. S. Hor, R. J. Cava, and M. Z. Hasan 2 Department of Physics, Princeton University, Princeton, NJ 08544, USA Princeton Center for Complex Materials, Princeton University, Princeton, NJ 08544, USA Department of Physics, Shanghai Jiao Tong University, Shanghai 200030, China Department of Physics, Northeastern University, Boston, MA 02115, USA Department of Chemistry, Princeton University, Princeton, NJ 08544, USA (Dated: Submitted for publication in December 2008)
Overview
Integrity signals
Registry
Cites
Statistics
Verification
Claims the paper makes
8 of 8 cited sources checked · 5 supported · 0 flagged · accuracy not yet measured
The cited sources support only part of this claim — read each source’s verdict below.
In the paper
“Therefore, if the chemical potential (Fermi level) lies inside the bandgap, as it should in purely insulating Bi 2 Se 3 , its surface must carry a global π mod 2π Berry phase.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
What the sources say
- Partly supportedcites [7] Fu, L. & Kane, C. L. Topological insulators with inversion symmetry. Phys. Rev. B 76, 045302 (2007). sourceExperimental — accuracy not yet measured
The “Strong topological insulator” section says that an electron circling a surface Fermi arc acquires a quantized Berry phase when the arc encloses a single Dirac point (page unavailable in our copy). It does not establish this for Bi₂Se₃ or say that placing the chemical potential in a bulk gap alone guarantees it; the result is conditional on the strong topological-insulator phase. (LLM, conf=0.88)
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passes- Partly supported
The cited sources support only part of this claim — read each source’s verdict below.
In the paper
“This provides evidence that insulating Bi 2 Se 3 belongs to the Z 2 = -1 topological class in the Fu-Kane-Mele topological classification scheme for band insulators.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
What the sources say
- Partly supportedcites [7] Fu, L. & Kane, C. L. Topological insulators with inversion symmetry. Phys. Rev. B 76, 045302 (2007). sourceExperimental — accuracy not yet measured
Section II describes a Z₂ classification of band insulators, supporting the attribution of the classification scheme to this paper. But the paper’s materials discussion identifies Bi₁₋ₓSbₓ, strained α-Sn and HgTe—not Bi₂Se₃—as strong topological insulators. It does not provide evidence for the claimed classification of insulating Bi₂Se₃. Page numbers were unavailable in our copy. (LLM, conf=0.86)
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passes- Partly supported
The cited sources support only part of this claim — read each source’s verdict below.
In the paper
“Its simplest topological surface spectrum would make it possible to observe and study many exotic quantum phenomena predicted in topological field theories, such as the Majorana fermions 14 , magnetic monopole image 9,10 or topological exciton condensates 15 , by transport probes.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
What the sources say
- Supportedcites [14] Fu, L. & Kane, C. L. Superconducting proximity effect and Majorana fermions at the surface of a topological insulator. Phys. Rev. Lett. 100, 096407 (2008). source
Citation 14 is attached to Majorana fermions, not to the separately cited magnetic-monopole image or exciton condensates. The paper predicts Majorana bound states on a proximitized topological-insulator surface (p. 1) and proposes measuring thermal conductance along a junction as a probe of its Majorana modes (p. 4). (LLM, conf=0.93)
- Partly supportedcites [9] Franz, M. High-energy physics in a new guise. Physics 1, 36 (2008). sourceExperimental — accuracy not yet measured
Split into 2 atoms — 0 confirmed, 2 partially supported, 0 disputed, 0 misattributed, 0 unverifiable. Expand the claim to see per-atom verdicts.
- Supportedcites [10] Qi, X.-L., Li, R., Zang, J. & Zhang, S.-C. Inducing a magnetic monopole with topological surface states. Science 323, 1184–1187 (2009). source
The opening passage (p. 1) says that a charge near a topological-insulator surface induces an image magnetic monopole and that its field can be measured experimentally. The experimental proposal (p. 4) describes detecting a resulting supercurrent with a superconducting ring. This supports the magnetic-monopole-image example to which this citation is attached; the other examples have separate citations. (LLM, conf=0.92)
- Supportedcites [15] Seradjeh, B., Moore, J. E. & Franz, M. Exciton condensation and charge fractionalization in a topological insulator film. Preprint at <http://arxiv.org/abs/0902.1147v1> (2009). source
Split into 2 atoms — 2 confirmed, 0 partially supported, 0 disputed, 0 misattributed, 0 unverifiable. Expand the claim to see per-atom verdicts.
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passes- Supported
Every source the paper cites for this claim was checked and supports it.
In the paper
“This topology is consistent with the Z 2 = -1 class in the Fu-Kane-Mele classification scheme 7 .”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
What the sources say
- Supportedcites [7] Fu, L. & Kane, C. L. Topological insulators with inversion symmetry. Phys. Rev. B 76, 045302 (2007). source
The paper’s discussion of Z₂ invariants (Eq. 1.1) defines the classification through a parity product, (−1)^ν, and says the invariant distinguishes nontrivial topological phases. This supports using the paper to identify the −1 class; it does not need to calculate the citing authors’ particular topology. (LLM, conf=0.88)
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passes- Supported
A result the paper reports from its own data — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“The red curve is measured right at the -point, which suggests that the Dirac point lies inside the bulk bandgap.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
Load-bearingStrength:hedged· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesA result the paper reports from its own data — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“Here we present an angle-resolved photoemission spectroscopy study that reveals the first observation of such a topological state of matter featuring a single surface Dirac cone realized in the naturally occurring Bi 2 Se 3 class of materials.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
Load-bearingStrength:plain· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passes- Rests on an assumption: Before this study, nothing was known about the surface states of Bi2Se3.
A result the paper reports from its own data — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“This is consistent with the fact that naturally grown Bi 2 Se 3 semiconductor used in our experiment is n-type, as independently confirmed by our transport measurements.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
Load-bearingStrength:plain· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesA result the paper reports from its own data — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“Taking the bottom of the 'U' band as the bulk conduction-band minimum, we estimate that a bandgap of about 0.3 eV is realized in the bulk of the undoped material.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
Load-bearingStrength:hedged· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesA result the paper reports from its own data — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“The calculated band topology with realistic SOC leads to a single ring-like surface FS, which is singly degenerate so long as the chemical potential is inside the bulk bandgap.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesA result the paper reports from its own data — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“A global agreement between the experimental band structure (Fig. 1a-c) and our theoretical calculation (Fig. 1f) is obtained by considering a rigid shift of the chemical potential by about 200 meV with respect to our calculated band structure (Fig. 1f) of the formula compound Bi 2 Se 3 .”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passes
- It may state two separate claims as one. 7
- Probably not a substantial claim. 2
Every source the paper cites for this claim was checked and supports it.
In the paper
“All the observed features are centred around .None of the three TRIMs located at M are enclosed by any FS, in contrast to what is observed in Bi 1-x Sb x (ref.5).”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
What the sources say
- Supportedcites [5] Hsieh, D. et al. A topological Dirac insulator in a quantum spin Hall phase. Nature 452, 970–974 (2008). source
The citation supports the contrast with Bi₁₋ₓSbₓ, not the citing authors’ description of their own Fermi surface. The source reports a narrow electron pocket around M in Bi₀.₉Sb₀.₁ (p. 6), unlike the citing authors’ observation that no M point is enclosed. (LLM, conf=0.94)
Load-bearingStrength:plain· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesIt may state two separate claims as one.
- Supported
A result the paper reports from its own data — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“The 'V' bands cross E F at 0.09 Å -1 along -M and at 0.10 Å -1 along -K, and have nearly equal band velocities, approximately 5 × 10 5 m s -1 , along the two directions.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
Load-bearingStrength:plain· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesIt may state two separate claims as one.
A result the paper reports from its own data — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“In our k z -dependent study of the bands (Fig. 2b) we also observe two bands dispersing in k z that have energies below -0.3 eV (blue dotted bands), reflecting the bulk valence bands, in addition to two other non-dispersive features associated with the two sides of the pure SS Dirac bands.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesIt may state two separate claims as one.
A result the paper reports from its own data — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“Our calculated result shows that no surface band crosses the Fermi level if SOC is not included in the calculation, and only with the inclusion of the realistic values of SOC (based on atomic Bi) does the calculated spectrum show singly degenerate gapless surface bands that are guaranteed to cross the Fermi level.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesIt may state two separate claims as one.
A result the paper reports from its own data — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“Our photonenergy study did not indicate a strong k z dispersion of the lowestlying energy bands on the 'U', although the full continuum does have some dispersion (Fig. 2).”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
Load-bearingStrength:hedged· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesIt may state two separate claims as one.
What the paper did — it cites no source for this, so there is none to check. The quote shows it is in the paper.
In the paper
“The surface band quasiparticle signal is stable throughout the entire measurement duration.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Experimental methods.
Strength:plain· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✗ Load-bearing: fails✗ Based: failsProbably not a substantial claim. The paper’s conclusions may not depend on it. The paper may give no reason why it holds.
A conclusion the paper draws from its own results — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“Because of the simplest possible topological surface spectrum realized in Bi 2 Se 3 , it can be considered as the 'hydrogen atom' of strong topological insulators.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
Tests✓ Asserted: passes✗ Checkable: fails✗ Load-bearing: fails✓ Based: passesProbably not a substantial claim. It may be too vague to check against evidence. The paper’s conclusions may not depend on it.
A conclusion the paper draws from its own results — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“We note that in purely insulating Bi 2 Se 3 the Fermi level should lie deep inside the bandgap and only pure surface bands will contribute to surface conduction.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes? Based: unclearIt may state two separate claims as one.
A conclusion the paper draws from its own results — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“The lack of strong dispersion yet close one-to-one correspondence to the calculated bulk band structure suggests that the inner electron pocket continuum features are probably a mixture of surface-projected conduction-band states, which also includes some band-bending effects near the surface and the full continuum of bulk conduction-band states sampled from a few layers beneath the surface.”
§ Observation of a large-gap topological-insulator class with a single Dirac cone on the surface > Abstract
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesIt may state two separate claims as one.
The paper relies on this without support.
Before this study, nothing was known about the surface states of Bi2Se3.
“All previous experimental studies of Bi 2 Se 3 have focused on the material's bulk properties; nothing is known about its SSs.”
Claims other papers make about this one
Each is checked against this paper’s own text: does it say what the citing paper says it does?
The source backs part of the claim, not all of it — or backs it for a different population, condition or comparison.
In the citing paper
“The inverted band structure is closely related to topological insulators, such as Bi2Te3 and Bi2Se34243.”
From Photonic simulation of topological excitations in metamaterials (2014) · cites this paper as [43]
Experimental — accuracy not yet measuredThe cited source says what the claim attributes to it.
In the citing paper
“Strong 3D topological insulators, on the other hand, have topological surface states that form unpaired Dirac points16,28–30”
From Observation of an unpaired photonic Dirac point (2020) · cites this paper as [29]
In the citing paper
“These results show that the topological order observed in Pb 1 À x Sn x Te is distinct from that previously discovered in Bi 1 À x Sb x or Bi 2 Se 3 (refs 1-5).”
From Observation of a topological crystalline insulator phase and topological phase transition in Pb1−xSnxTe (2012) · cites this paper as [4]
In the citing paper
“Because the topological order in TlBi(S 1 -δ Se δ ) 2 originates from Bi and Se atoms and to illustrate an analogy with the known topological insulator Bi 2 Se 3 ( 6, 8, 11 )”
From Topological Phase Transition and Texture Inversion in a Tunable Topological Insulator (2011) · cites this paper as [8]
In the citing paper
“In 2008, work led by a Princeton group used angle-resolved photoemission spectroscopy (ARPES) and first-principles calculations to study the surface band structure of Bi 2 Se 3 and observe the characteristic signature of a topological insulator in the form of a single-Dirac-cone (21,22).”
From Three-Dimensional Topological Insulators (2011) · cites this paper as [21]
In the citing paper
“This can be understood because the origin of the topological insulator state in Bi 2 Se 3 is a symmetry inversion that occurs at the point 7,18 , and the electronic states close to the Brillouin-zone boundary are similar to those of topologically trivial materials.”
From A topological insulator surface under strong Coulomb, magnetic and disorder perturbations (2011) · cites this paper as [7]
In the citing paper
“Topological insulators embody a state of bulk matter characterized by spin-momentum-locked surface states that span the bulk bandgap 1-7 .”
From A topological insulator surface under strong Coulomb, magnetic and disorder perturbations (2011) · cites this paper as [7]
In the citing paper
“Momentum along the ẑ axis is determined using an inner potential of 9.5 eV, consistent with previous photoemission investigations of undoped Bi 2 Se 3 (refs 7,22).”
From A topological insulator surface under strong Coulomb, magnetic and disorder perturbations (2011) · cites this paper as [7]
In the citing paper
“Bi2 Se3 is one of a handful of known topological insulators.”
From Superconductivity in Cu x Bi 2 Se 3 and its Implications for Pairing in the Undoped Topological Insulator (2010) · cites this paper as [9]
In the citing paper
“These robust low-dimensional conducting states are topologically protected against all time-reversal-invariant perturbations, such as scattering by non-magnetic impurities, crystalline defects, and distortion of the surface itself.”
From Aharonov–Bohm interference in topological insulator nanoribbons (2010) · cites this paper as [4]
In the citing paper
“In contrast to graphene, which has four Dirac cones (2 doubly degenerate cones at the K and K 0 points in momentum space) [9], the remarkable property of topological edge states is that their dispersion is characterized by an odd number of nondegenerate Dirac cones.”
From Observation of Time-Reversal-Protected Single-Dirac-Cone Topological-Insulator States in Bi2Te3 and Sb2Te3 (2009) · cites this paper as [7]
In the citing paper
“They were recently proposed [2-4] and shortly afterwards discovered in the Bi1 x Sb x [5,6] and Bi2 Se 3 [7,8] materials.”
From Observation of Time-Reversal-Protected Single-Dirac-Cone Topological-Insulator States in Bi2Te3 and Sb2Te3 (2009) · cites this paper as [7]
In the citing paper
“More recently, angle-resolved photoemission spectroscopy (ARPES) and theoretical [7,19] evidence suggest that Bi2 Se 3 is a large band gap ( 300 meV ) single-Dirac-cone topological insulator.”
From Observation of Time-Reversal-Protected Single-Dirac-Cone Topological-Insulator States in Bi2Te3 and Sb2Te3 (2009) · cites this paper as [7]
In the citing paper
“there is an additional contribution to the density of states around momentum ¯ Γ from the spin-degenerate bulk conduction band in Bi 2 Se 3 [15].”
From A tunable topological insulator in the spin helical Dirac transport regime (2009) · cites this paper as [15]
In the citing paper
“Later, Bi x Sb 1 -x was suggested to be a three-dimensional (3D) TI[8] with topologically non-trivial surface states, which were observed by angle-resolved photoemission spectroscopy (ARPES)[9].”
From Model Hamiltonian for topological insulators (2010) · cites this paper as [9]
Citations
Cites
Generalized Gradient Approximation Made Simple
Perdew, J. P., Burke, K., & Ernzerhof, M. (1996) · Physical Review Letters · doi:10.1103/physrevlett.77.3865 · Cited by 215,824
Geim, A. K., & Novoselov, K. S. (2007) · Nature Materials · doi:10.1038/nmat1849 · Cited by 39,979 · cited 1×
“Two such phases are the quantum spin Hall insulator [4] and the strong topological insulator [5, 6, 7] both realized in the vicinity of a Dirac point but yet quite distinct from graphene [16].”
BackgroundHandbook of X-Ray Photoelectron Spectroscopy
Moulder, J. F. (1995) · Medical Entomology and Zoology · Cited by 23,662
Quantum Spin Hall Insulator State in HgTe Quantum Wells
König, M., Wiedmann, S., Brüne, C., Roth, A., Buhmann, H., Molenkamp, L. W., Qi, X.-L., & Zhang, S.-C. (2007) · Science · doi:10.1126/science.1148047 · Cited by 6,151 · cited 4×
“Recent theories and experiments have suggested that strong spin–orbit coupling effects in certain band insulators can give rise to a new phase of quantum matter, the so-called topological insulator, which can show macroscopic entanglement effects [1, 2, 3, 4, 5, 6, 7].”
BackgroundInfluentialSuperconducting Proximity Effect and Majorana Fermions at the Surface of a Topological Insulator
Fu, L., & Kane, C. L. (2008) · Physical Review Letters · doi:10.1103/physrevlett.100.096407 · Cited by 4,868 · cited 5×
“Such systems feature two-dimensional surface states whose electrodynamic properties are described not by the conventional Maxwell equations but rather by an attached axion field, originally proposed to describe strongly interacting particles [8, 9, 10, 11, 12, 13, 14, 15].”
BackgroundInfluentialTopological Insulators in Three Dimensions
Fu, L., Kane, C. L., & Mele, E. J. (2007) · Physical Review Letters · doi:10.1103/physrevlett.98.106803 · Cited by 4,651 · cited 1×
“Recent theories and experiments have suggested that strong spin–orbit coupling effects in certain band insulators can give rise to a new phase of quantum matter, the so-called topological insulator, which can show macroscopic entanglement effects [1, 2, 3, 4, 5, 6, 7].”
BackgroundTopological insulators with inversion symmetry
Fu, L., & Kane, C. L. (2007) · Physical Review B · doi:10.1103/physrevb.76.045302 · Cited by 4,252 · cited 9×
“Topological quantum properties are directly probed from the nature of the electronic states on the surface by studying the way surface bands connect the material’s bulk valence and conduction bands in momentum space [5, 6, 7].”
BackgroundResultInfluentialA topological Dirac insulator in a quantum spin Hall phase
Hsieh, D., Qian, D., Wray, L., Xia, Y., Hor, Y. S., Cava, R. J., & Hasan, M. Z. (2008) · Nature · doi:10.1038/nature06843 · Cited by 3,523 · cited 14×
“Topological quantum properties are directly probed from the nature of the electronic states on the surface by studying the way surface bands connect the material’s bulk valence and conduction bands in momentum space [5, 6, 7].”
BackgroundInfluentialSelf-citationTopological field theory of time-reversal invariant insulators
Qi, X.-L., Hughes, T. L., & Zhang, S.-C. (2008) · Physical Review B · doi:10.1103/physrevb.78.195424 · Cited by 3,329 · cited 2×
“The strong-topological-insulator phase contains surface states (SSs) with novel electromagnetic properties [7, 8, 9, 10, 11, 12, 13, 14, 15].”
BackgroundThermoelectric Cooling and Power Generation
DiSalvo, F. J. (1999) · Science · doi:10.1126/science.285.5428.703 · Cited by 3,240
Flagged first, then by citations
Research works printed but not linked: 1
- Wyckoff, R. W. G. Crystal Structures (Krieger, 1986).
Cited by
Sorted by citations
Items 1,101–1,200 of 3,793
Aguilera, I., Friedrich, C., & Blügel, S. (2019) · Physical review. B./Physical review. B · doi:10.1103/physrevb.100.155147 · Cited by 37
1/4 is the new 1/2 when topology is intertwined with Mottness
Mai, P., Zhao, J., Feldman, B. E., et al. (2023) · Nature Communications · doi:10.1038/s41467-023-41465-6 · Cited by 37
Gooth, J., Hamdou, B., Dorn, A., Zierold, R., & Nielsch, K. (2014) · Applied Physics Letters · doi:10.1063/1.4883887 · Cited by 34
Photoemission-induced gating of topological insulators
Kordyuk, A. A., Kim, T. K., Zabolotnyy, V. B., Evtushinsky, D. V., Bauch, M., Heß, C., Büchner, B., Berger, H., & Борисенко, С. В. (2011) · Physical Review B · doi:10.1103/physrevb.83.081303 · Cited by 36
High‐Temperature Thermoelectric Properties of Sn‐Doped β‐As 2 Te 3
Vaney, J., Carreaud, J., Delaizir, G., Pradel, A., Alejandra, P. A., Morin, C., Alleno, E., Monnier, J., Gonçalves, A. P., Candolfi, C., et al. (2015) · Advanced Electronic Materials · doi:10.1002/aelm.201400008 · Cited by 37
Shokr, E. K., Ibrahim, E. M. M., Hakeem, A. M. A., et al. (2013) · Journal of Experimental and Theoretical Physics · doi:10.1134/s1063776113020064 · Cited by 37
Majorana-Hubbard model on the square lattice
Affleck, I. K., Rahmani, A., & Pikulin, D. I. (2017) · Physical review. B./Physical review. B · doi:10.1103/physrevb.96.125121 · Cited by 35
Levy, I., Garcia, T. A., Shafique, S., & Tamargo, M. C. (2018) · Journal of Vacuum Science & Technology B Nanotechnology and Microelectronics Materials Processing Measurement and Phenomena · doi:10.1116/1.5017977 · Cited by 35
Dependence of superconductivity in CuxBi2Se3 on quenching conditions
Schneeloch, J. A., Zhong, R., Xu, Z., Gu, G. D., & Tranquada, J. M. (2015) · Physical Review B · doi:10.1103/physrevb.91.144506 · Cited by 36
Neupane, M., Xu, S., Sankar, R., Gibson, Q., Wang, Y. J., Belopolski, I., Alidoust, N., Bian, G., Shibayev, P., Sanchez, D. S., et al. (2015) · Physical Review B · doi:10.1103/physrevb.92.075131 · Cited by 43
Self-citationTopology and Symmetry in Quantum Materials
Singh, B., Lin, H., & Bansil, A. (2022) · Advanced Materials · doi:10.1002/adma.202201058 · Cited by 40
Self-citationIntrinsic spin Hall effect in topological insulators: A first-principles study
Farzaneh, S. M., & Rakheja, S. (2020) · Physical Review Materials · doi:10.1103/physrevmaterials.4.114202 · Cited by 39
Engineering Topological Surface States: HgS, HgSe, and HgTe
Virot, F., Hayn, R., Richter, M., & van den Brink, J. (2013) · Physical Review Letters · doi:10.1103/physrevlett.111.146803 · Cited by 37
Minimum Thermal Conductivity in Weak Topological Insulators with Bismuth‐Based Stack Structure
Wei, P., Yang, J., Yang, J., et al. (2016) · Advanced Functional Materials · doi:10.1002/adfm.201600718 · Cited by 37
Chen, Y. (2011) · Frontiers of Physics · doi:10.1007/s11467-011-0197-9 · Cited by 37
Lateral and Vertical Two-Dimensional Layered Topological Insulator Heterostructures
Li, Y., Zhang, J., Zheng, G. W., Sun, Y., Hong, S. S., Xiong, F., Wang, S., Lee, H. R., & Cui, Y. (2015) · ACS Nano · doi:10.1021/acsnano.5b04068 · Cited by 36
Ta4SiTe4 : A possible one-dimensional topological insulator
Liu, S., Yin, H., Singh, D. J., & Liu, P. (2022) · Physical review. B./Physical review. B · doi:10.1103/physrevb.105.195419 · Cited by 37
Direct observation of the spin–orbit coupling effect in magnetic Weyl semimetal Co3Sn2S2
Liu, D., Liu, E., Xu, Q., Shen, J., Li, Y. W., Pei, D., Liang, A., Dudin, P., Kim, T. K., Cacho, C., et al. (2022) · npj Quantum Materials · doi:10.1038/s41535-021-00392-9 · Cited by 42
Spin current in topologically trivial and nontrivial noncentrosymmetric superconductors
Lu, C.-K., & Yip, S. (2010) · Physical Review B · doi:10.1103/physrevb.82.104501 · Cited by 36
Plank, H., Pernul, J., Gebert, S., Danilov, S. N., König‐Otto, J. C., Winnerl, S. F., Lanius, M., Kampmeier, J., Mußler, G., Aguilera, I., et al. (2018) · University of Regensburg Publication Server (University of Regensburg) · Cited by 36
Creating topological interfaces and detecting chiral edge modes in a two-dimensional optical lattice
Goldman, N., Jotzu, G., Messer, M., Görg, F., Desbuquois, R., & Esslinger, T. (2016) · Physical Review A · doi:10.1103/physreva.94.043611 · Cited by 37
Mao, S., Yamakage, A., & Kuramoto, Y. (2011) · Physical Review B · doi:10.1103/physrevb.84.115413 · Cited by 35
Klintenberg, M. K., Haraldsen, J. T., & Balatsky, A. V. (2014) · Applied Physics Research · doi:10.5539/apr.v6n4p31 · Cited by 36
Gas Doping on the Topological Insulator Bi2Se3 Surface
Koleini, M. M., Frauenheim, T., & Yan, B. (2013) · Physical Review Letters · doi:10.1103/physrevlett.110.016403 · Cited by 36
Sun, H., Tan, S., Feng, M., Zhao, J., & Petek, H. (2018) · The Journal of Physical Chemistry C · doi:10.1021/acs.jpcc.8b03353 · Cited by 35
Neupane, M., Liu, C., Xu, S.-Y., et al. (2012) · Physical Review B · doi:10.1103/physrevb.85.094510 · Cited by 36
Self-citationNearly Massless Electrons in the Silicon Interface with a Metal Film
Kim, K. S., Jung, S. C., Kang, M.-H., et al. (2010) · Physical Review Letters · doi:10.1103/physrevlett.104.246803 · Cited by 36
Axionic band topology in inversion-symmetric Weyl-charge-density waves
Wieder, B. J., Lin, K.-S., & Bradlyn, B. (2020) · Physical Review Research · doi:10.1103/physrevresearch.2.042010 · Cited by 39
Progress and prospects in the quantum anomalous Hall effect
Chi, H., & Moodera, J. S. (2022) · APL Materials · doi:10.1063/5.0100989 · Cited by 40
Ambipolar transport in bulk crystals of a topological insulator by gating with ionic liquid
Segawa, K., Ren, Z., Sasaki, S., Tsuda, T., Kuwabata, S., & Ando, Y. (2012) · Physical Review B · doi:10.1103/physrevb.86.075306 · Cited by 37
Energy spectrum and broken spin-surface locking in topological insulator quantum dots
Kundu, A., Zazunov, A., Yeyati, A. L., Martin, T., & Egger, R. (2011) · Physical Review B · doi:10.1103/physrevb.83.125429 · Cited by 36
Rasche, B., Isaeva, A. A., Gerisch, A., Kaiser, M., den Broek, W. V., Koch, C. T., Kaiser, U. A., & Ruck, M. (2013) · Chemistry of Materials · doi:10.1021/cm4010823 · Cited by 37
Probing lattice dynamics and electron-phonon coupling in the topological nodal-line semimetal ZrSiS
Singha, R., Samanta, S., Chatterjee, S., Pariari, A., Majumdar, D., Satpati, B., Wang, L., Singha, A., & Mandal, P. (2018) · Physical review. B./Physical review. B · doi:10.1103/physrevb.97.094112 · Cited by 36
Fragile topology in line-graph lattices with two, three, or four gapped flat bands
Chiu, C., Ma, D., Song, Z., Bernevig, B. A., & Houck, A. (2020) · Physical Review Research · doi:10.1103/physrevresearch.2.043414 · Cited by 37
Evolution of electronic structure upon Cu doping in the topological insulator Bi 2 Se 3
Tanaka, Y., Nakayama, K., Souma, S., Sato, T., Xu, N., Zhang, P., Richard, P. J. H., Ding, H. Q., Suzuki, Y., Das, P., et al. (2012) · Physical Review B · doi:10.1103/physrevb.85.125111 · Cited by 36
Models of three-dimensional fractional topological insulators
Maciejko, J., Qi, X.-L., Karch, A., & Zhang, S. (2012) · Physical Review B · doi:10.1103/physrevb.86.235128 · Cited by 39
Growth of high-quality Bi2Se3 topological insulators using (Bi1-xInx)2Se3 buffer layers
Wang, Y., Ginley, T. P., & Law, S. (2018) · Journal of Vacuum Science & Technology B Nanotechnology and Microelectronics Materials Processing Measurement and Phenomena · doi:10.1116/1.5015968 · Cited by 35
Cornfeld, E., & Carmeli, S. (2021) · Physical Review Research · doi:10.1103/physrevresearch.3.013052 · Cited by 38
Cao, G., Ouyang, R., Ghiringhelli, L. M., Scheffler, M., Liu, H., Carbogno, C., & Zhi-dong, Z. (2020) · MPG.PuRe (Max Planck Society) · Cited by 36
Spin-orbit coupling enhanced superconductivity in Bi-rich compounds ABi3 (A = Sr and Ba)
Shao, D., Luo, X., Lu, W. J., et al. (2016) · Scientific Reports · doi:10.1038/srep21484 · Cited by 36
Growth of multilayers of Bi2Se3/ZnSe: Heteroepitaxial interface formation and strain
Li, H. D., Wang, Z., Guo, X., Wong, T. L., Wang, N., & Xie, M. (2011) · Applied Physics Letters · doi:10.1063/1.3548865 · Cited by 35
Strong out-of-plane magnetic anisotropy of Fe adatoms on Bi2Te3
Eelbo, T., Waśniowska, M., Sikora, M., Dobrzański, M., Kozłowski, A., Pulkin, A., Autès, G., Miotkowski, I., Yazyev, O. V., & Wiesendanger, R. (2014) · Physical Review B · doi:10.1103/physrevb.89.104424 · Cited by 36
Sun, Y., Chen, X., Franchini, C., Li, D., Yunoki, S., Li, Y., & Fang, Z. (2011) · Physical Review B · doi:10.1103/physrevb.84.165127 · Cited by 33
Group 14 element-based non-centrosymmetric quantum spin Hall insulators with large bulk gap
Ma, Y., Kou, L., Du, A., & Heine, T. (2015) · Nano Research · doi:10.1007/s12274-015-0842-7 · Cited by 36
Chen, Y., & Kee, H. (2014) · Physical Review B · doi:10.1103/physrevb.90.195145 · Cited by 36
Nanoindentation of Bi2Se3 Thin Films
Lai, H.-D., Jian, S., Tuyen, L. T. C., Le, P. H., Luo, C., & Juang, J. (2018) · Micromachines · doi:10.3390/mi9100518 · Cited by 35
“Recently, topological insulators (TIs) have attracted enormous research attention owing to their intriguing fundamental physical properties, such as their conduction mechanisms [1,2], as well as their potential applications in the emergent fields of spintronics [3], optoelectronics [4] and quantum computation [5].”
BackgroundInfluentialAb initiostudies of adatom- and vacancy-induced band bending in Bi2Se3
Förster, T., Krüger, P., & Rohlfing, M. (2015) · Physical Review B · doi:10.1103/physrevb.91.035313 · Cited by 35
Induced spin texture in semiconductor/topological insulator heterostructures
Hutasoit, J. A., & Stanescu, T. D. (2011) · Physical Review B · doi:10.1103/physrevb.84.085103 · Cited by 33
Crystal Chemistry and Bonding Patterns of Bismuth-Based Topological Insulators
Isaeva, A. A., & Ruck, M. (2020) · Inorganic Chemistry · doi:10.1021/acs.inorgchem.9b03461 · Cited by 35
Structural and electrical study of the topological insulator SnBi2Te4 at high pressure
Vilaplana, R., Sans, J. A., Manjon, F. J., Andrada‐Chacón, A., Sánchez-Benítez, J., Popescu, C., Gomis, O., Pereira, A. L. J., García-Domene, B., Rodríguez-Hernández, P., et al. (2016) · Journal of Alloys and Compounds · doi:10.1016/j.jallcom.2016.06.170 · Cited by 35
Finite-Size and Composition-Driven Topological Phase Transition in (Bi1–xInx)2Se3 Thin Films
Salehi, M., Shapourian, H., Koirala, N., Brahlek, M., Moon, J., & Oh, S. (2016) · Nano Letters · doi:10.1021/acs.nanolett.6b02044 · Cited by 35
Direct observation of a gap opening in topological interface states of MnSe/Bi2Se3 heterostructure
Matetskiy, A. V., Kibirev, I. A., Hirahara, T., Hasegawa, S., Zotov, A. V., & Saranin, A. A. (2015) · Applied Physics Letters · doi:10.1063/1.4930151 · Cited by 35
Strong spin-orbit coupling and Zeeman spin splitting in angle dependent magnetoresistance of Bi2Te3
Dey, R., Pramanik, T., Roy, A., et al. (2014) · Applied Physics Letters · doi:10.1063/1.4881721 · Cited by 35
Chen, Z., Garcia, T. A., Jesus, J. D., Zhao, L., Deng, H., Secor, J., Begliarbekov, M., Krusin-Elbaum, L., & Tamargo, M. C. (2013) · Journal of Electronic Materials · doi:10.1007/s11664-013-2890-7 · Cited by 36
Spin-orbital ground states of superconducting doped topological insulators: A Majorana platform
Wray, L. A., Xu, S., Xia, Y., Qian, D., Fedorov, A. V., Lin, H., Bansil, A., Fu, L., Hor, Y. S., Cava, R. J., et al. (2011) · Physical Review B · doi:10.1103/physrevb.83.224516 · Cited by 35
Self-citationFragility of Fermi arcs in Dirac semimetals
Wu, Y., Jo, N. H., Wang, L., Schmidt, C. A., Neilson, K. M., Schrunk, B., Swatek, P., Eaton, A., Bud’ko, S. L., Canfield, P. C., et al. (2019) · Physical review. B./Physical review. B · doi:10.1103/physrevb.99.161113 · Cited by 36
Polyakov, A., Meyerheim, H. L., Crozier, E. D., Gordon, R. A., Mohseni, K., Roy, S., Ernst, A., Vergniory, M. G., Zubizarreta, X., Otrokov, M. M., et al. (2015) · Physical Review B · doi:10.1103/physrevb.92.045423 · Cited by 35
Atomic relaxations at the (0001) surface of Bi 2 Se 3 single crystals and ultrathin films
Roy, S., Meyerheim, H. L., Mohseni, K., Ernst, A., Otrokov, M. M., Vergniory, M. G., Mußler, G., Kampmeier, J., Grützmacher, D., Tusche, C., et al. (2014) · Physical Review B · doi:10.1103/physrevb.90.155456 · Cited by 35
Kumar, D., & Lakhani, A. (2015) · physica status solidi (RRL) - Rapid Research Letters · doi:10.1002/pssr.201510260 · Cited by 38
PbTe/PbSnTe heterostructures as analogs of topological insulators
Buczko, R., & Cywiński, Ł. (2012) · Physical Review B · doi:10.1103/physrevb.85.205319 · Cited by 34
Polymorphism in Thermoelectric As2Te3
Morin, C., Corallini, S., Carreaud, J., Vaney, J., Delaizir, G., Crivello, J., Lopes, E. B., Alejandra, P. A., Monnier, J., Candolfi, C., et al. (2015) · Inorganic Chemistry · doi:10.1021/acs.inorgchem.5b01676 · Cited by 35
Helicity-dependent terahertz emission spectroscopy of topological insulator Sb2Te3 thin films
Tu, C.-M., Chen, Y.-C., Huang, P. W., Chuang, P., Lin, M.-Y., Cheng, C., Lin, J.-Y., Juang, J., Wu, K.-H., Huang, J. C. A., et al. (2017) · Physical review. B./Physical review. B · doi:10.1103/physrevb.96.195407 · Cited by 36
Gaussian beam methods for the Dirac equation in the semi-classical regime
Huang, Z., Jin, S., Wu, H., & Yin, D. (2012) · Communications in Mathematical Sciences · doi:10.4310/cms.2012.v10.n4.a14 · Cited by 33
Zhang, H. B., Yu, H. L., & Yang, G. (2011) · Europhysics Letters (EPL) · doi:10.1209/0295-5075/95/56002 · Cited by 36
High-temperature quantum oscillations of the Hall resistance in bulk Bi2Se3
Busch, M., Chiatti, O., Pezzini, S., Wiedmann, S., Sánchez‐Barriga, J., Rader, O., Yashina, L. V., & Fischer, S. F. (2018) · Scientific Reports · doi:10.1038/s41598-017-18960-0 · Cited by 34
Probe knots and Hopf insulators with ultracold atoms 1 DONG
Deng, L., Wang, S.-T., Sun, K., & Duan, L. (2015) · Chinese Physics Letters · doi:10.1088/0256-307x/35/1/013701 · Cited by 15
Gautam, S., Verma, A. K., Balapure, A., Singh, B., Ganesan, R., Kumar, M. S., Singh, V. N., Gahtori, B., & Kushvaha, S. S. (2022) · Journal of Electronic Materials · doi:10.1007/s11664-022-09498-7 · Cited by 35
Lifshitz transition and Van Hove singularity in a three-dimensional topological Dirac semimetal
Xu, S., Liu, C., Belopolski, I., Kushwaha, S. K., Sankar, R., Krizan, J. W., Chang, T., Polley, C., Adell, J., Balasubramanian, T., et al. (2015) · Physical Review B · doi:10.1103/physrevb.92.075115 · Cited by 35
Self-citationMagnetic quantum oscillations for the surface states of topological insulator Bi2Se3
Wang, Z., Fu, Z., Wang, S., et al. (2010) · Physical Review B · doi:10.1103/physrevb.82.085429 · Cited by 35
Electronic Transport Evidence for Topological Nodal-Line Semimetals of ZrGeSe Single Crystals
Guo, L., Chen, T.-W., Chen, C., Chen, L., Zhang, Y., Gao, G.-Y., Yang, J., Li, X.-G., Zhao, W.-Y., Dong, S., et al. (2019) · ACS Applied Electronic Materials · doi:10.1021/acsaelm.9b00061 · Cited by 35
Spin helix of magnetic impurities in two-dimensional helical metal
Ye, F., Ding, G.-H., Zhai, H., & Su, Z. B. (2010) · Europhysics Letters (EPL) · doi:10.1209/0295-5075/90/47001 · Cited by 37
Lee, J. J., Schmitt, F., Moore, R. G., Vishik, I., Ma, Y., & Shen, Z. (2012) · Applied Physics Letters · doi:10.1063/1.4733317 · Cited by 39
Ishida, Y., 菅藤, 裕., Kikkawa, A., Taguchi, Y., Ito, Y., Ota, Y., Okazaki, K., Malaeb, W., Mulazzi, M., Okawa, M., et al. (2011) · Physical Review Letters · doi:10.1103/physrevlett.107.077601 · Cited by 35
Spin orbit torque driven magnetization switching with sputtered Bi 2 Se 3 spin current source
Ramaswamy, R., Dutta, T., Liang, S., et al. (2019) · Journal of Physics D Applied Physics · doi:10.1088/1361-6463/ab0b96 · Cited by 35
Monopole current and unconventional Hall response on a topological insulator
Zang, J., & Nagaosa, N. (2010) · Physical Review B · doi:10.1103/physrevb.81.245125 · Cited by 35
Ultrafast Surface State Spin-Carrier Dynamics in the Topological Insulator Bi2Te2Se
Iyer, V., Chen, Y. P., & Xu, X. (2018) · Physical Review Letters · doi:10.1103/physrevlett.121.026807 · Cited by 34
Synthesis and Characterization of Nanomaterials of the Topological Crystalline Insulator SnTe
Saghir, M., Lees, M. R., York, S. J., & Balakrishnan, G. (2014) · Crystal Growth & Design · doi:10.1021/cg500122b · Cited by 34
Singha, R., Salters, T. H., Teicher, S. M. L., Lei, S., Khoury, J. F., Ong, N. P., & Schoop, L. M. (2021) · Advanced Materials · doi:10.1002/adma.202103476 · Cited by 34
Quantum phase transitions in Dirac fermion systems
Boyack, R., Yerzhakov, H., & Maciejko, J. (2021) · The European Physical Journal Special Topics · doi:10.1140/epjs/s11734-021-00069-1 · Cited by 37
Interface orbital engineering of large-gap topological states: Decorating gold on a Si(111) surface
Huang, B. Q., Jin, K., Zhuang, H. L., et al. (2016) · Physical review. B./Physical review. B · doi:10.1103/physrevb.93.115117 · Cited by 34
Breaking time reversal symmetry in topological insulators
Chang, C., Wei, P., & Moodera, J. S. (2014) · MRS Bulletin · doi:10.1557/mrs.2014.195 · Cited by 36
Shon, W., Rhyee, J., Jin, Y., et al. (2019) · Physical review. B./Physical review. B · doi:10.1103/physrevb.100.024433 · Cited by 34
Quantum spin Hall effect induced by nonmagnetic and magnetic staggered potentials
Guo, H., Feng, S., & Shen, S.-Q. (2011) · Physical Review B · doi:10.1103/physrevb.83.045114 · Cited by 33
Electron transmission through atomic steps of Bi 2 Se 3 and Bi 2 Te 3 surfaces
Kobayashi, K. (2011) · Physical Review B · doi:10.1103/physrevb.84.205424 · Cited by 33
Topological Phase Transition in the Interaction of Surface Dirac Fermions in Heterostructures
Kim, J., Kim, J., Kim, K., et al. (2012) · Physical Review Letters · doi:10.1103/physrevlett.109.146601 · Cited by 34
Atom size electron vortex beams with selectable orbital angular momentum
Pohl, D., Schneider, S., Zeiger, P., et al. (2017) · Scientific Reports · doi:10.1038/s41598-017-01077-9 · Cited by 34
Tu, C.-M., Yeh, T.-T., Tzeng, W., Chen, Y., Chen, H.-J., Ku, S. A., Luo, C., Lin, J. ‐., Wu, K., Juang, J., et al. (2015) · Scientific Reports · doi:10.1038/srep14128 · Cited by 35
Nuclear magnetic resonance as a probe of electronic states of Bi 2 Se 3
Nisson, D. M., Dioguardi, A. P., Klavins, P., Lin, C. H., Shirer, K., Shockley, A. C., Crocker, J., & Curro, N. J. (2013) · Physical Review B · doi:10.1103/physrevb.87.195202 · Cited by 33
Fornari, C. I., Rappl, P. H. O., Morelhão, S. L., Peixoto, T. R. F., Bentmann, H., Reinert, F., & Abramof, E. (2016) · APL Materials · doi:10.1063/1.4964610 · Cited by 34
Frantzeskakis, E., & Grioni, M. (2011) · Physical Review B · doi:10.1103/physrevb.84.155453 · Cited by 35
Topological invariant in three-dimensional band insulators with disorder
Guo, H. (2010) · Physical Review B · doi:10.1103/physrevb.82.115122 · Cited by 34
Baruselli, P. S., & Matthias Vojta, C. (2014) · Physical Review B · doi:10.1103/physrevb.90.201106 · Cited by 34
Diffusion at the surface of topological insulators
Adroguer, P., Carpentier, D., Cayssol, J., & Orignac, E. (2012) · New Journal of Physics · doi:10.1088/1367-2630/14/10/103027 · Cited by 34
Matsugatani, A., Ono, S., Nomura, Y., & Watanabe, H. (2021) · Computer Physics Communications · doi:10.1016/j.cpc.2021.107948 · Cited by 34
Surface and interfacial sciences for future technologies
Zhou, X., Shen, Q., Wang, Y., et al. (2024) · National Science Review · doi:10.1093/nsr/nwae272 · Cited by 34
Aharonov-Casher Effect in Bi2Se3 Square-Ring Interferometers
Qu, F., Yang, F., Chen, J., Shen, J., Ding, Y., Lu, J., Song, Y., Yang, H., Liu, G., Fan, J., et al. (2011) · Physical Review Letters · doi:10.1103/physrevlett.107.016802 · Cited by 32
Crystal growth of Bi2Te3 and noble cleaved (0001) surface properties
Atuchin∥⊥, V. V., Golyashov, V. A., Кох, К. А., Korolkov, I. V., Kozhukhov, A. S., Кручинин, В. Н., Loshkarev, I. D., Pokrovsky, L. D., Prosvirin, I. P., Romanyuk, K. N., et al. (2015) · Journal of Solid State Chemistry · doi:10.1016/j.jssc.2015.07.031 · Cited by 33
Pal, H. K., Yudson, V. I., & Maslov, D. L. (2012) · Physical Review B · doi:10.1103/physrevb.85.085439 · Cited by 33
Half-metallic surface states and topological superconductivity in NaCoO 2 from first principles
Weng, H., Xu, G., Zhang, H., Zhang, S., Dai, X., & Fang, Z. (2011) · Physical Review B · doi:10.1103/physrevb.84.060408 · Cited by 33
Bansal, N., Cho, M. R., Brahlek, M., Koirala, N., Horibe, Y., Chen, J., Wu, W., Park, Y. D., & Oh, S. (2014) · Nano Letters · doi:10.1021/nl404363b · Cited by 35
Metadata
- Authors
- Xia, Y., Qian, D., Hsieh, D., Wray, L., Pal, A., Lin, H., Bansil, A., Grauer, D., Hor, Y. S., Cava, R. J., & Hasan, M. Z.
- Affiliations
- Princeton University (US)
- Shanghai Jiao Tong University (CN)
- Northeastern University (US)
- Corresponding author
- Hasan, M. Z.
- Venue
- Nature Physics
- Published
- 2009-05-10
- Volume
- 5
- Issue
- 6
- Pages
- 398-402
- ISSN
- 1745-2473 (ISSN-L)
- 1745-2481
- OpenAlex
- W1552055731
- Semantic Scholar
- d3bcc8a78db93feda0054d8d2f8a9f7811dfd502
- Cited by
- 3,765
- References
- 28
- Citations by year
- 2026: 105 · 2025: 141 · 2024: 142 · 2023: 155 · 2022: 199 · 2021: 208 · 2020: 225 · 2019: 198 · 2018: 272 · 2017: 252 · 2016: 274 · 2015: 291 · 2014: 267 · 2013: 297 · 2012: 308
- FWCI
- 136.90
- Type
- journal article
- Language
- en
- Open access
- bronze
- doi.org
- Licence
- Locations
- Nature Physics (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- UCL Discovery (University College London) (submittedVersion)
- CaltechAUTHORS (California Institute of Technology) (submittedVersion)
- arXiv (Cornell University)
- Funders
- National Science Foundation (0819860)
- U.S. Department of Energy (DE‐FG02‐, DEFG0205ER46200, FG02-05ER46200)
- Princeton University
- Princeton Center for Complex Materials (DMR-0819860)
- National Energy Research Scientific Computing Center
- National Natural Science Foundation of China (10874116)
- Office of Science
- Materials Research Science and Engineering Center, Harvard University (NSF-DMR-0819860, DMR-0819860)
- Division of Materials Research (DMR-0819860)
- Basic Energy Sciences (DE-FG-02-07ER46352, DE-FG02)
- Topics
- Physical Sciences › Physics and Astronomy › Condensed Matter Physics › Topological Materials and Phenomena
- Physical Sciences › Physics and Astronomy › Condensed Matter Physics › Advanced Condensed Matter Physics
- Physical Sciences › Materials Science › Materials Chemistry › 2D Materials and Applications
- Keywords
- topological insulators, Bi2Se3, surface states, spin-orbit coupling, axion field, topological superconductors, fault-tolerant quantum computing, angle-resolved photoemission
About these checks
Registry, retraction, Cites and statistics results are computed, not judged, with one exception: a printed reference that no index lists is read once by a model before it counts as a citation error. Claims are extracted by a model and kept only when their quote appears verbatim in the text; each cited source is then checked, with a model’s help, for whether it says what the claim relies on. Those verdicts can be wrong — read the claim’s quote and the cited source before relying on one.
A language model drew the claims from the paper on 2026-10-11, under version 3 of the claim definition (model deepseek-v4.1-flash, prompt extract-v3).
A second model labelled each claim on 2026-10-11 (model jev-1.13-20260917, definition revision gold-guideline-v0.2).
Cited sources are checked with a language model’s help (gpt-6-sol).
Statistics and arithmetic are recomputed, not judged.
Confidence bands are shown only for fields calibrated on our annotated test set. None is calibrated yet, so no band is shown.
What counts as a claim ›How we measure confidence ›How we check this ›
Are you an author, or do you see a problem with this page? Request a review
