2012
DOI: 10.1209/0295-5075/100/26004
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Low-temperature thermal conductivity in polycrystalline graphene

Abstract: The low-temperature thermal conductivity in polycrystalline graphene is theoretically studied.The contributions from three branches of acoustic phonons are calculated by taking into account scattering on sample borders, point defects and grain boundaries. Phonon scattering due to sample borders and grain boundaries is shown to result in a T α -behaviour in the thermal conductivity where α varies between 1 and 2. This behaviour is found to be more pronounced for nanosized grain boundaries.

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Cited by 12 publications
(9 citation statements)
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“…It should also be mentioned that T o characterizes the temperature when the wavelength of an incident phonon becomes comparable with the size of the GB. T GB decreases with an increase of the packing coefficient, the misorientation angle and/or sample size, while T o depends on the grain boundary length only [94]. Using non-equilibrium molecular dynamics simulations, it was shown that the boundary conductance on the tilt GBs are in the range 1.5 × 10 10 -4.5 × 10 10 W m −2 K −1 , which is significantly higher than that of any other thermoelectric interfaces reported in the literature [95].…”
Section: Thermal Transportmentioning
confidence: 98%
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“…It should also be mentioned that T o characterizes the temperature when the wavelength of an incident phonon becomes comparable with the size of the GB. T GB decreases with an increase of the packing coefficient, the misorientation angle and/or sample size, while T o depends on the grain boundary length only [94]. Using non-equilibrium molecular dynamics simulations, it was shown that the boundary conductance on the tilt GBs are in the range 1.5 × 10 10 -4.5 × 10 10 W m −2 K −1 , which is significantly higher than that of any other thermoelectric interfaces reported in the literature [95].…”
Section: Thermal Transportmentioning
confidence: 98%
“…Theoretical calculations predict two distinct temperature ranges, below and above T * , a crossover temperature at low temperatures. T * ≈ T o /2, where T o is governed by the dominant phonon mode [94]. Above T * the thermal conductivity behaves like T 2 , while below T * the behavior is acutely sensitive to T GB , it behaves like T α , where α values range from 1 to 2 with increasing T GB .…”
Section: Thermal Transportmentioning
confidence: 99%
“…In pristine systems, the main phonon scattering mechanism is anharmonicity, manifested in three-phonon processes, and graphene owes its high thermal conductivity to the high density of states of its flexural phonon branch at low energies, together with a symmetry-induced selection rule for three-phonon scattering processes [48]. Several theoretical studies have also addressed the broader problem of thermal transport in defect-laden graphene [49][50][51][52][53][54][55] and graphene nanostructures [56][57][58]. However, in general those studies use either classical molecular dynamics or simple parametric models, both of which fail to give a detailed insight into the phonon physics underpinning the complex transport behavior in these systems.…”
Section: Introductionmentioning
confidence: 99%
“…Similar to the case of 2D graphene samples, the power in the power-law dependence of thermal conductivity on temperature is reduced due to the presence of domain walls (cf. [5]). At higher temperatures the grain boundary scattering results in constant mean free path and reducing the role of exural ZA phonon mode, reducing the magnitude of heat conductivity and leaving the power-law temperature dependence intact.…”
Section: Resultsmentioning
confidence: 99%