| People | Locations | Statistics |
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| Naji, M. |
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| Motta, Antonella |
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| Aletan, Dirar |
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| Mohamed, Tarek |
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| Ertürk, Emre |
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| Taccardi, Nicola |
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| Kononenko, Denys |
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| Petrov, R. H. | Madrid |
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| Alshaaer, Mazen | Brussels |
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| Bih, L. |
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| Casati, R. |
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| Muller, Hermance |
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| Kočí, Jan | Prague |
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| Šuljagić, Marija |
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| Kalteremidou, Kalliopi-Artemi | Brussels |
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| Azam, Siraj |
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| Ospanova, Alyiya |
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| Blanpain, Bart |
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| Ali, M. A. |
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| Popa, V. |
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| Rančić, M. |
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| Ollier, Nadège |
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| Azevedo, Nuno Monteiro |
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| Landes, Michael |
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| Rignanese, Gian-Marco |
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Johrendt, Dirk
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (6/6 displayed)
- 2022The kagomé metals RbTi3Bi5 and CsTi3Bi5citations
- 2019Solid Solutions of Grimm–Sommerfeld Analogous Nitride Semiconductors II‐IV‐N2 (II=Mg, Mn, Zn; IV=Si, Ge): Ammonothermal Synthesis and DFT Calculationscitations
- 2019Solid Solutions of Grimm–Sommerfeld Analogous Nitride Semiconductors II‐IV‐N<sub>2</sub> (II=Mg, Mn, Zn; IV=Si, Ge): Ammonothermal Synthesis and DFT Calculationscitations
- 2015[(Li0.8Fe0.2)OH]FeS and the ferromagnetic superconductors [(Li0.8Fe0.2)OH]Fe(S1−xSex) (0 < x ≤ 1)citations
- 2013Ce4Ag3Ge4O0.5 - chains of oxygen-centered OCe2Ce2/2] tetrahedra embedded in a CeAg3Ge4] intermetallic matrixcitations
- 2009The layered iron arsenide oxides Sr2CrO3FeAs and Ba2ScO3FeAscitations
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article
The kagomé metals RbTi3Bi5 and CsTi3Bi5
Abstract
<jats:title>Abstract</jats:title><jats:p>The kagomé metals RbTi<jats:sub>3</jats:sub>Bi<jats:sub>5</jats:sub> and CsTi<jats:sub>3</jats:sub>Bi<jats:sub>5</jats:sub> were synthesized both as polycrystalline powders by heating the elements in an argon atmosphere and as single crystals grown using a self-flux method. The compounds crystallize in the hexagonal crystal system isotypically to KV<jats:sub>3</jats:sub>Sb<jats:sub>5</jats:sub> (<jats:italic>P</jats:italic>6/<jats:italic>mmm</jats:italic>, <jats:italic>Z</jats:italic> = 1, CsTi<jats:sub>3</jats:sub>Bi<jats:sub>5</jats:sub>: <jats:italic>a</jats:italic> = 5.7873(1), <jats:italic>c</jats:italic> = 9.2062(1) Å; RbTi<jats:sub>3</jats:sub>Bi<jats:sub>5</jats:sub>: <jats:italic>a</jats:italic> = 5.773(1), <jats:italic>c</jats:italic> = 9.065(1) Å). The titanium atoms form a kagomé net with bismuth atoms in the hexagons as well as above and below the triangles. The alkali metal atoms are coordinated by 12 bismuth atoms and form AlB<jats:sub>2</jats:sub>-like slabs between the kagomé layers. Magnetic susceptibility measurements with CsTi<jats:sub>3</jats:sub>Bi<jats:sub>5</jats:sub> and RbTi<jats:sub>3</jats:sub>Bi<jats:sub>5</jats:sub> single crystals reveal Pauli-paramagnetism and traces of superconductivity caused by CsBi<jats:sub>2</jats:sub>/RbBi<jats:sub>2</jats:sub> impurities. Magnetotransport measurements reveal conventional Fermi liquid behavior and quantum oscillations indicative of a single dominant orbit at low temperature. DFT calculations show the characteristic metallic kagomé band structure similar to that of CsV<jats:sub>3</jats:sub>Sb<jats:sub>5</jats:sub> with reduced band filling. A symmetry analysis of the band structure does not reveal an obvious and unique signature of a nontrivial topology.</jats:p>