Takeru Wakamatsu1,Yuki Isobe1,Hitoshi Takane1,Kentaro Kaneko1,2,Katsuhisa Tanaka1
Kyoto University1,Ritsumeikan University2
Takeru Wakamatsu1,Yuki Isobe1,Hitoshi Takane1,Kentaro Kaneko1,2,Katsuhisa Tanaka1
Kyoto University1,Ritsumeikan University2
Gallium oxide (Ga<sub>2</sub>O<sub>3</sub>), which is one of the ultra-wide bandgap semiconductors, has attracted considerable attention because of its potential applications for power electronics. Among polymorphs of Ga<sub>2</sub>O<sub>3</sub>, β-Ga<sub>2</sub>O<sub>3</sub> is the most stable phase. Although β-Ga<sub>2</sub>O<sub>3</sub>-based devices such as Schottky barrier diode (SBD), MESFET and MOSFET have been reported thus far, the fact that β-Ga<sub>2</sub>O<sub>3</sub> substrate is expensive and has a low thermal conductivity is a problem from a point of view of practical applications. On the other hand, α-Ga<sub>2</sub>O<sub>3</sub>, which is one of the metastable phases, can be grown on a sapphire substrate by heteroepitaxial growth techniques such as mist-CVD, HVPE and MEB. The sapphire substrate is cost-effective and has a high thermal conductivity, which is preferable for device applications. Nonetheless, there are not so many reports on the α-Ga<sub>2</sub>O<sub>3</sub>-based devices including SBD, MESFET and MOSFET. This is partly because the control of carrier density and achievement of high mobility are not so easy compared with β-Ga<sub>2</sub>O<sub>3</sub>. Recently, we successfully obtained Ge-doped α-Ga<sub>2</sub>O<sub>3</sub> thin films by using mist-CVD method with the wider carrier density ranging from 10<sup>16</sup> to 10<sup>19</sup> cm<sup>-3</sup> and the higher mobility 65.9 cm<sup>2</sup>V<sup>-1</sup>s<sup>-1</sup> than previous reported Sn-doped α-Ga<sub>2</sub>O<sub>3</sub>.<sup>[1]</sup> In this work, we report on the fabrication of SBD and MESFET based on the Ge-doped α-Ga<sub>2</sub>O<sub>3</sub> thin films and confirm that the resultant devices exhibit rather high performance.<br/>Ge-doped α-Ga<sub>2</sub>O<sub>3</sub> thin films were grown on <i>m</i>-plane sapphire substrates by mist-CVD method. An α-Ga<sub>2</sub>O<sub>3 </sub>n<sup>+</sup> layer (900-1000 nm thick, the donor density, <i>N</i><sub>d</sub> = 1×10<sup>19</sup> cm<sup>3</sup>) and an α-Ga<sub>2</sub>O<sub>3 </sub>n<sup>−</sup> drift layer (500-600 nm thick, UID) were grown on the <i>m</i>-plane sapphire substrate for SBD. To make a mesa structure, the n<sup>−</sup> layer was etched by ICP-RIE following photolithography. As an ohmic electrode, Ti/Au (20 nm/100 nm thick) or Ti/Al/Ti/Au (30 nm/100 nm/30 nm/ 30 nm thick) was deposited on the n<sup>+</sup> layer by electron beam (EB) deposition. After that, the samples were annealed at 400, 450, 470 and 500 °C for 1 min in an N<sub>2</sub> atmosphere. Then, Ti/Au (20/100 nm thick) Schottky electrode was formed by EB deposition. The <i>I</i>-<i>V</i> characteristic of the resultant SBDs was measured and analyzed in terms of the thermionic emission model. The <i>n</i> value and the barrier height are 1.06-1.19 and 0.95-1.13 eV, respectively. The on-resistance decreases as the annealing temperature is increased. The lowest on-resistance is 3.7 mΩcm<sup>2</sup> achieved for the device with Ti/Au/Ti/Au ohmic electrode annealed at 500 °C.<br/>Also, we prepared MESFET as follows. First, Fe-doped buffer layer (800 nm thick), Ge-doped channel layer (300 nm thick) and n<sup>+</sup> layer (30 nm thick) were grown on an <i>m</i>-plane sapphire substrate. For the mesa device isolation, 500 nm-thick α-Ga<sub>2</sub>O<sub>3</sub> was etched by ICP-RIE. A Ti/Au (20/100 nm thick) was deposited as source and drain electrodes. The n<sup>+</sup> layer on the channel layer was etched by ICP-RIE. A Ni/Au (30/100 nm thick) was deposited as a gate electrode. From the Hall effect measurements, the carrier concentration, the sheet carrier density, and the electron mobility were evaluated to be 2.1×10<sup>17</sup> cm<sup>-3</sup>, 4.9×10<sup>12</sup> cm<sup>-2</sup> and 44 cm<sup>2</sup>V<sup>-1</sup>s<sup>-1</sup>, respectively. The <i>I</i>−<i>V</i> measurements were conducted for the device with <i>L</i><sub>GS</sub>/<i>L</i><sub>G</sub>/<i>L</i><sub>GD</sub> = 3/3/12 μm, where <i>L</i><sub>GS</sub>, <i>L</i><sub>G</sub>, and <i>L</i><sub>GD</sub> are gate-to-source, gate and gate-to-drain lengths, respectively. From the output curve (<i>V</i><sub>DS</sub>−<i>I</i><sub>D</sub> characteristic), the maximum <i>I</i><sub>D</sub> and the on-resistance were estimated to be 24 mA/mm and 587 Ωmm (at <i>V</i><sub>GS</sub> = 2 V), respectively. The break down voltage is 364 V (at <i>V</i><sub>GS</sub> = -10 V). From the transfer curve (<i>I</i><sub>D</sub>−<i>V</i><sub>GD</sub> characteristic), the threshold voltage, the subthreshold slope and the on-off ratio were evaluated to be -9 V, 164 mV/dec and 10<sup>9</sup>, respectively. These values are superior compared to a-Ga<sub>2</sub>O<sub>3</sub>-based MESFET reported previously, for which the break down voltage, the on-off ratio and the maximum <i>I</i><sub>D</sub> are 48 V, 2×10<sup>7</sup> and 35 mA.<sup>[2]</sup><br/>[1]<i>Phys. status solidi A</i> <b>217</b>, 1900632 (2020). [2]<i>IEEE Trans. Electron Devices</i> <b>62</b>, 3640 (2015).