MRS Meetings and Events

 

EL11.12.09 2023 MRS Fall Meeting

Schottky Barrier Diode and MESFET based on Ge-Doped α-Ga2O3 Thin Film Grown by Mist-CVD

When and Where

Nov 30, 2023
4:00pm - 4:15pm

Hynes, Level 2, Room 210

Presenter

Co-Author(s)

Takeru Wakamatsu1,Yuki Isobe1,Hitoshi Takane1,Kentaro Kaneko1,2,Katsuhisa Tanaka1

Kyoto University1,Ritsumeikan University2

Abstract

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).

Keywords

chemical vapor deposition (CVD) (deposition)

Symposium Organizers

Stephen Goodnick, Arizona State University
Robert Kaplar, Sandia National Laboratories
Martin Kuball, University of Bristol
Yoshinao Kumagai, Tokyo University of Agriculture and Technology

Symposium Support

Silver
Taiyo Nippon Sanson

Publishing Alliance

MRS publishes with Springer Nature