Search Results

Now showing 1 - 2 of 2
Loading...
Thumbnail Image
Item

Shallow and Undoped Germanium Quantum Wells: A Playground for Spin and Hybrid Quantum Technology

2019, Sammak, Amir, Sabbagh, Diego, Hendrickx, Nico W., Lodari, Mario, Wuetz, Brian Paquelet, Tosato, Alberto, Yeoh, LaReine, Bollani, Monica, Virgilio, Michele, Schubert, Markus Andreas, Zaumseil, Peter, Capellini, Giovanni, Veldhorst, Menno, Scappucci, Giordano

Buried-channel semiconductor heterostructures are an archetype material platform for the fabrication of gated semiconductor quantum devices. Sharp confinement potential is obtained by positioning the channel near the surface; however, nearby surface states degrade the electrical properties of the starting material. Here, a 2D hole gas of high mobility (5 × 10 5 cm 2 V −1 s −1 ) is demonstrated in a very shallow strained germanium (Ge) channel, which is located only 22 nm below the surface. The top-gate of a dopant-less field effect transistor controls the channel carrier density confined in an undoped Ge/SiGe heterostructure with reduced background contamination, sharp interfaces, and high uniformity. The high mobility leads to mean free paths ≈ 6 µm, setting new benchmarks for holes in shallow field effect transistors. The high mobility, along with a percolation density of 1.2 × 10 11 cm −2 , light effective mass (0.09m e ), and high effective g-factor (up to 9.2) highlight the potential of undoped Ge/SiGe as a low-disorder material platform for hybrid quantum technologies. © 2019 The Authors. Published by WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim

Loading...
Thumbnail Image
Item

Structural and optical properties of (112̅2) InGaN quantum wells compared to (0001) and (112̅0)

2016, Pristovsek, Markus, Han, Yisong, Zhu, Tongtong, Oehler, Fabrice, Tang, Fengzai, Oliver, Rachel A., Humphreys, Colin J., Tytko, Darius, Choi, Pyuck-Pa, Raabe, Dierk, Brunner, Frank, Weyers, Markus

We benchmarked growth, microstructure and photo luminescence (PL) of (112-2) InGaN quantum wells (QWs) against (0001) and (112-0). In incorporation, growth rate and the critical thickness of (112-2) QWs are slightly lower than (0001) QWs, while the In incorporation on (112-0) is reduced by a factor of three. A small step-bunching causes slight fluctuations of the emission wavelength. Transmission electron microscopy as well as atom probe tomography (APT) found very flat interfaces with little In segregation even for 20% In content. APT frequency distribution analysis revealed some deviation from a random InGaN alloy, but not as severe as for (112-0). The slight deviation of (112-2) QWs from an ideal random alloy did not broaden the 300 K PL, the line widths were similar for (112-2) and (0001) while (112-0) QWs were broader. Despite the high structural quality and narrow PL, the integrated PL signal at 300 K was about 4 lower on (112-2) and more than 10 lower on (112-0).