<p>The in-plane thermal conductivity (<i>k</i>) of ultrathin films is of great scientific and engineering importance as the ultrafine thickness will cause remarkable energy carrier scattering. However, the in-plane <i>k</i> is extremely difficult to measure as the in-plane heat conduction is highly overshadowed by the substrate. To date, very rare experimental data and understanding have been reported. Here we report an advanced differential transient electro-thermal (TET) technique to characterize the in-plane <i>k</i> of supported nm-thin Iridium films down to &lt; 2&#xa0;nm thickness. The ultrathin (500&#xa0;nm) organic substrate and its low <i>k</i> makes it possible to distinguish the in-plane <i>k</i> of the film with high confidence. The radiation effect is rigorously treated and subtracted from the measured <i>k</i>. Also measurements under different temperature rise levels allow us to determine the <i>k</i> at the zero temperature rise limit. All these physics treatments lead to high accuracy determination of the in-plane <i>k</i>, and understanding of the strong structural effects. The <i>k</i> of ultrathin Ir films supported on polyethylene terephthalate is determined to be 11.7 W·m<sup>−1</sup>·K<sup>−1</sup>, 20.1 W·m<sup>−1</sup>·K<sup>−1</sup>, 23.5 W·m<sup>−1</sup>·K<sup>−1</sup>, and 34.3 W·m<sup>−1</sup>·K<sup>−1</sup> for thicknesses of 1.83&#xa0;nm, 3.11&#xa0;nm, 5.86&#xa0;nm, and 9.16&#xa0;nm, respectively. This is more than one order of magnitude reduction from the bulk’s <i>k</i> of 147 W·m<sup>−1</sup>·K<sup>−1</sup>. The film’s electrical conductivity is found to have more than two orders of magnitude reduction from that of bulk Ir (1.96 × 10<sup>7</sup> Ω<sup>−1</sup>·m<sup>−1</sup>). The Lorenz number of the studied Ir films increases significantly with decreased film thickness, and is upto 14-fold higher (3.97 × 10<sup>–7</sup> W·Ω·K<sup>−2</sup>) than that of bulk Ir (2.54 × 10<sup>–8</sup> W·Ω·K<sup>−2</sup>). It underscores the significant and deviated influence of structure and film dimension on heat and electrical conductions and provides invaluable knowledge for future applications in nanoelectronics.</p>

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Characterization of the In-plane Thermal Conductivity of Sub-10 nm Ir Films on a Flexible Substrate

  • Qusai Alahmad,
  • Huan Lin,
  • Jing Liu,
  • Mahya Rahbar,
  • Todd A. Kingston,
  • Xinwei Wang

摘要

The in-plane thermal conductivity (k) of ultrathin films is of great scientific and engineering importance as the ultrafine thickness will cause remarkable energy carrier scattering. However, the in-plane k is extremely difficult to measure as the in-plane heat conduction is highly overshadowed by the substrate. To date, very rare experimental data and understanding have been reported. Here we report an advanced differential transient electro-thermal (TET) technique to characterize the in-plane k of supported nm-thin Iridium films down to < 2 nm thickness. The ultrathin (500 nm) organic substrate and its low k makes it possible to distinguish the in-plane k of the film with high confidence. The radiation effect is rigorously treated and subtracted from the measured k. Also measurements under different temperature rise levels allow us to determine the k at the zero temperature rise limit. All these physics treatments lead to high accuracy determination of the in-plane k, and understanding of the strong structural effects. The k of ultrathin Ir films supported on polyethylene terephthalate is determined to be 11.7 W·m−1·K−1, 20.1 W·m−1·K−1, 23.5 W·m−1·K−1, and 34.3 W·m−1·K−1 for thicknesses of 1.83 nm, 3.11 nm, 5.86 nm, and 9.16 nm, respectively. This is more than one order of magnitude reduction from the bulk’s k of 147 W·m−1·K−1. The film’s electrical conductivity is found to have more than two orders of magnitude reduction from that of bulk Ir (1.96 × 107 Ω−1·m−1). The Lorenz number of the studied Ir films increases significantly with decreased film thickness, and is upto 14-fold higher (3.97 × 10–7 W·Ω·K−2) than that of bulk Ir (2.54 × 10–8 W·Ω·K−2). It underscores the significant and deviated influence of structure and film dimension on heat and electrical conductions and provides invaluable knowledge for future applications in nanoelectronics.