2019
DOI: 10.1073/pnas.1821533116
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Emergence of topological electronic phases in elemental lithium under pressure

Abstract: Lithium, a prototypical simple metal under ambient conditions, has a surprisingly rich phase diagram under pressure, taking up several structures with reduced symmetry, low coordination numbers, and even semiconducting character with increasing density. Using firstprinciples calculations, we demonstrate that some predicted highpressure phases of elemental Li also host topological electronic structures. Beginning at 80 GPa and coincident with a transition to the Pbca phase, we find Li to be a Dirac nodal line s… Show more

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Cited by 12 publications
(5 citation statements)
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“…The Mo atom’s 4d orbitals split into two energy levels, i.e, E (d , d ) and E (d , d ), whereas the Li atom’s 2p orbitals yield the E (p , p ) and the A (p ) orbitals as well as into the A orbital arising from the H atom’s 1s orbital. The band structure evidences a coupling between the E of Mo atom and the E orbitals of Li atom and reveals a Dirac-like cone, as also found recently 42 , 43 , at the -point in Fig. 5 a, which is originated from the coupling between the - and -bonds.…”
Section: Resultssupporting
confidence: 82%
“…The Mo atom’s 4d orbitals split into two energy levels, i.e, E (d , d ) and E (d , d ), whereas the Li atom’s 2p orbitals yield the E (p , p ) and the A (p ) orbitals as well as into the A orbital arising from the H atom’s 1s orbital. The band structure evidences a coupling between the E of Mo atom and the E orbitals of Li atom and reveals a Dirac-like cone, as also found recently 42 , 43 , at the -point in Fig. 5 a, which is originated from the coupling between the - and -bonds.…”
Section: Resultssupporting
confidence: 82%
“…If the states near the Fermi level are of the same orbital character and also close in energy, they can couple together effectively through a Rashba Hamiltonian, further reducing the band gap at relevant points in the BZ [14]. Several routes to inducing topological phase transitions (TPTs) from normal to topological insulator (TI) have been proposed in solid-state systems, including using temperature [15,16], pressure [17], and strain [18]. Topological Anderson insulators are an example where onsite disorder pushes a trivial insulator through a gapless state into a topologically nontrivial state [19,20].…”
Section: Introductionmentioning
confidence: 99%
“…Theory has suggested that compressed Group I elements and alloys may possess topological properties. For example, DFT calculations concluded that forms of dense hydrogen [18] and Na hP 4 [19] both possess metallic surface states, the band structure of Li 5 H presents Dirac-like features [20], and various phases of Li at intermediate pressures were computed to be topological semimetals with nodal loops or lines in the vicinity of the Fermi level, E F [21,22]. The interest in topological semimetals stems from their unique properties including high mobilities [23], giant magnetoresistance [24], and because their massless fermions make it possible to simulate intriguing high-energy and relativistic physics phenomena in table-top experiments [25].…”
mentioning
confidence: 99%