2017
DOI: 10.1103/physrevb.96.195165
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Polaron-induced phonon localization and stiffening in rutile TiO2

Abstract: Small polaron formation in transition metal oxides, like the prototypical material rutile TiO 2 , remains a puzzle and a challenge to simple theoretical treatment. In our combined experimental and theoretical study, we examine this problem using Raman spectroscopy of photo-excited samples and real-time time-dependent density functional theory (RT-TDDFT), which employs Ehrenfest dynamics to couple the electronic and ionic subsystems. We observe experimentally the unexpected stiffening of the A 1g phonon mode un… Show more

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Cited by 10 publications
(1 citation statement)
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“…5,6,[38][39][40][41][42][43][44][45] However, Nb doping turns the metallic character of TiO 2 into a thermally-activated electrical conduction which is commonly assumed to originate from the polaronic nature of the Ti 3+ centers, the transport of which transport is characterized by effective masses as large as a hundred times the free electron mass. 19,26,[45][46][47][48][49][50] On the other side of the solid solution, NbO 2 adopts a distorted rutile structure which transforms into an undistorted rutile phase at about 1000 K. [51][52][53] Simultaneously, a large increase in electrical conductivity is observed suggestive of a non-metal to metal transition. [54][55][56] The mechanism of the structural/electronic transition is best understood in terms of metal-metal bonding between Nb ions, which paired along the c-axis as a result of a Peierls instability.…”
Section: Introductionmentioning
confidence: 99%
“…5,6,[38][39][40][41][42][43][44][45] However, Nb doping turns the metallic character of TiO 2 into a thermally-activated electrical conduction which is commonly assumed to originate from the polaronic nature of the Ti 3+ centers, the transport of which transport is characterized by effective masses as large as a hundred times the free electron mass. 19,26,[45][46][47][48][49][50] On the other side of the solid solution, NbO 2 adopts a distorted rutile structure which transforms into an undistorted rutile phase at about 1000 K. [51][52][53] Simultaneously, a large increase in electrical conductivity is observed suggestive of a non-metal to metal transition. [54][55][56] The mechanism of the structural/electronic transition is best understood in terms of metal-metal bonding between Nb ions, which paired along the c-axis as a result of a Peierls instability.…”
Section: Introductionmentioning
confidence: 99%