2021
DOI: 10.1039/d1ta01920a
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Localized vibration and avoided crossing in SrTi11O20 for oxide thermoelectrics with intrinsically low thermal conductivity

Abstract: The localized vibration in SrTi11O20 forms low-lying optical phonon bands that distort acoustic phonon branches through the avoided crossing effect. The electrical and thermal transport are decoupled to achieve phonon-glass electron-crystal behaviour.

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Cited by 13 publications
(4 citation statements)
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“…67 To address this issue, a novel thermoelectric oxide SrTi O 20 is presented, where the TiO 6 octahedra form a network creating an irregular polyhedron for the loosely bonded Sr ions and thus obtain an extremally low κ lat ∼1.7 W m −1 K −1 even comparable with PbTe. 89 Very recently, Light element H − substitution in SrTiO 2.784 H 0.216 largely reduces its κ lat to 3.5 W m −1 K −1 . 80 Importantly, the given Sr−H bonding energy is 164 kJ mol much lower than Sr−O bond even PbTe, 67 which implies that selective introduction of lowenergy bonds by reference to the chemical bond energy is an effective way to weakened the bond and thus inhibit κ lat .…”
Section: Weakened Bondmentioning
confidence: 99%
See 1 more Smart Citation
“…67 To address this issue, a novel thermoelectric oxide SrTi O 20 is presented, where the TiO 6 octahedra form a network creating an irregular polyhedron for the loosely bonded Sr ions and thus obtain an extremally low κ lat ∼1.7 W m −1 K −1 even comparable with PbTe. 89 Very recently, Light element H − substitution in SrTiO 2.784 H 0.216 largely reduces its κ lat to 3.5 W m −1 K −1 . 80 Importantly, the given Sr−H bonding energy is 164 kJ mol much lower than Sr−O bond even PbTe, 67 which implies that selective introduction of lowenergy bonds by reference to the chemical bond energy is an effective way to weakened the bond and thus inhibit κ lat .…”
Section: Weakened Bondmentioning
confidence: 99%
“…Note that the SrTiO 3 shows a high κ lat ∼9 W m −1 K −1 at 300 K because of the high bonding energy 426.3 kJ mol of Sr−O bond 67 . To address this issue, a novel thermoelectric oxide SrTi 11 O 20 is presented, where the TiO 6 octahedra form a network creating an irregular polyhedron for the loosely bonded Sr ions and thus obtain an extremally low κ lat ∼1.7 W m −1 K −1 even comparable with PbTe 89 . Very recently, Light element H − substitution in SrTiO 2.784 H 0.216 largely reduces its κ lat to 3.5 W m −1 K −1 80 .…”
Section: Lattice Thermal Conductivity Suppression Strategiesmentioning
confidence: 99%
“…In Figure 4, we visualized such a low-frequency molecular optical modes by red arrows: the first two modes involve specific rotations of the butyl groups, and the third involves the rotation of the whole tert-butyl isocyanate molecule. The phonon-crossing phenomenon, identified in various structures, [30][31][32] are usually correlated with a noteworthy decrease in acoustic phonon group velocities and a corresponding strong increases of the vibrational anharmonicity, ultimately resulting in a further decrease of thermal conductivity. [33] Figure 5 shows the corresponding group velocities of the acoustic (and quasi-acoustic for structure (a)) phonon modes (see Figure 5).…”
Section: Systemmentioning
confidence: 99%
“…The mixing phenomenon between acoustic and optical phonons introduced anharmonicity effects in the crystal structure. This mechanism caused the flattening of the phonon modes and suppression of acoustic group velocity [364]. You et al observed the dynamic behavior of Cu-ion doped in the PbSe matrix, providing more charge carriers with the increasing temperature.…”
Section: Phonon Engineeringmentioning
confidence: 99%