2006
DOI: 10.1134/s0021364006150124
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Energy relaxation of hot carriers in single-wall carbon nanotubes by surface optical phonons of the substrate

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Cited by 27 publications
(32 citation statements)
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“…Thermal broadening of the energy distribution is approximately k B T e ≈ 10 meV at T e = 120 K. The resulting energy of ≈ 30 meV is close to the 50 meV predicted threshold energy for the emission of surface polar phonons (SPPs) directly into the SiO 2 substrate. [21][22][23] 23 The difference in I s is likely the result of the differences between this modeled system and our measured sample. In particular, I s is strongly dependent on the tubesubstrate separation.…”
mentioning
confidence: 87%
“…Thermal broadening of the energy distribution is approximately k B T e ≈ 10 meV at T e = 120 K. The resulting energy of ≈ 30 meV is close to the 50 meV predicted threshold energy for the emission of surface polar phonons (SPPs) directly into the SiO 2 substrate. [21][22][23] 23 The difference in I s is likely the result of the differences between this modeled system and our measured sample. In particular, I s is strongly dependent on the tubesubstrate separation.…”
mentioning
confidence: 87%
“…where a q,q ⊥ ,ν is the annihilation operator for the ν-th surface phonon mode (not to be confused with the NT lattice phonons), and an explicit form of V ν k,q,q ⊥ was derived in Ref. [27]:…”
Section: Simulation Approachmentioning
confidence: 99%
“…The interactions of these SPP modes with charged carriers in the conduction channel was first explored in the context of inversion layer of semiconductor-oxide interface [24][25][26] . They have also been studied in other material systems such as carbon nanotubes [27][28][29] , where close proximity between charged carriers and the underlying substrate renders the SPP-phonon scattering more prominent. Similarly, in graphene, SPP was found to limit electronic transport properties [30][31][32][33][34][35][36][37][38][39] .…”
Section: Introductionmentioning
confidence: 99%