Hauptseite > Publikationsdatenbank > High-k rare-earth oxides on GaN and ferroelectric properties of hafnia based thin films > print |
001 | 862553 | ||
005 | 20210130001447.0 | ||
024 | 7 | _ | |a 2128/22160 |2 Handle |
037 | _ | _ | |a FZJ-2019-02847 |
100 | 1 | _ | |a Tromm, Thomas Carl Ulrich |0 P:(DE-Juel1)165625 |b 0 |e Corresponding author |
245 | _ | _ | |a High-k rare-earth oxides on GaN and ferroelectric properties of hafnia based thin films |f - 2019-03-01 |
260 | _ | _ | |c 2019 |
300 | _ | _ | |a 133 p. |
336 | 7 | _ | |a Output Types/Dissertation |2 DataCite |
336 | 7 | _ | |a DISSERTATION |2 ORCID |
336 | 7 | _ | |a PHDTHESIS |2 BibTeX |
336 | 7 | _ | |a Thesis |0 2 |2 EndNote |
336 | 7 | _ | |a Dissertation / PhD Thesis |b phd |m phd |0 PUB:(DE-HGF)11 |s 1557161850_5873 |2 PUB:(DE-HGF) |
336 | 7 | _ | |a doctoralThesis |2 DRIVER |
502 | _ | _ | |a Dissertation, RWTH Aachen University, 2014 |c RWTH Aachen University |b Dissertation |d 2014 |
520 | _ | _ | |a The continuous improvement of the transistors is the basis for the increase of computing power. For enhanced metal-oxide-semiconductor (MOS) field-effect-transistors(FETs) and other devices suitable gate dielectrics are required, that exhibit a high relative permittivity, good insulating properties like a large band gap, and a goodlayer quality. Additionally, new device structures like negative capacitance FET (NCFET) are developed.In this thesis the ternary rare-earth oxides GdScO3 (GSO), LaLuO3 (LLO) and SmScO3 (SSO) are grown on GaN by pulsed laser deposition (PLD). Those oxidesreveal a hexagonal phase, that has been discovered few years ago. The oxides have a large lattice mismatch to the GaN and are not at thermodynamic equilibrium,according to ab-initio calculations. The hexagonal ternary rare-earth oxides reveal a permittivity of 30 (GSO) and of 32 (LLO) and a bandgap above 5 eV. To understandthe growth mechanism of the rare-earth oxides, the layer and especially the interface are investigated. First of all hexagonal GSO reveals a decomposition of Scand Gd at the interface, so that it exhibits twice as much Sc than Gd, which reduces the length of the in-plane axis of the GSO and subsequently the lattice mismatch.Secondly, the grains are tilted in-plane, revealing a fibre texture with the c-axis as fibre axis perpendicular to the interface. Thirdly, the distance of the lattice planesat the interface is enhanced, revealing a distance of 3.1 Å. The SSO also reveals a fibre texture and an enhanced interface distance, thought the decomposition of theSm and the Sc occurs in places. The hexagonal LLO reveals a fibre texture and a small decomposition.For a novel NCFET a ferroelectric is placed in between the gate metal and the oxide of a MOSFET. The ferroelectric should exhibit a negative capacitance and inthis way cause a voltage amplification, resulting in a subthreshold slope (SS) below 60 mV/dec. PLD grown ferroelectric HfO2 with 5% Gd and HfO2 with 5% Lu(HfLuO) reveal a remanent polarization of 12 μC/cm2, while the HfO2 with 5% Y, grown by atomic layer deposition, reveals one of 20 μC/cm2 and a steeper hysteresis.HfLuO exhibits a pinched hysteresis at the initial state, if the sample is annealed at 500 °C, which could be related to an antiferroelectric phase. At an annealingtemperature of 700 °C the HfLuO layer becomes ferroelectric. |
536 | _ | _ | |a 521 - Controlling Electron Charge-Based Phenomena (POF3-521) |0 G:(DE-HGF)POF3-521 |c POF3-521 |f POF III |x 0 |
856 | 4 | _ | |y OpenAccess |u https://juser.fz-juelich.de/record/862553/files/Dissertation%20Tromm.pdf |
856 | 4 | _ | |y OpenAccess |x pdfa |u https://juser.fz-juelich.de/record/862553/files/Dissertation%20Tromm.pdf?subformat=pdfa |
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910 | 1 | _ | |a Forschungszentrum Jülich |0 I:(DE-588b)5008462-8 |k FZJ |b 0 |6 P:(DE-Juel1)165625 |
913 | 1 | _ | |a DE-HGF |b Key Technologies |l Future Information Technology - Fundamentals, Novel Concepts and Energy Efficiency (FIT) |1 G:(DE-HGF)POF3-520 |0 G:(DE-HGF)POF3-521 |2 G:(DE-HGF)POF3-500 |v Controlling Electron Charge-Based Phenomena |x 0 |4 G:(DE-HGF)POF |3 G:(DE-HGF)POF3 |
914 | 1 | _ | |y 2019 |
915 | _ | _ | |a OpenAccess |0 StatID:(DE-HGF)0510 |2 StatID |
920 | _ | _ | |l yes |
920 | 1 | _ | |0 I:(DE-Juel1)PGI-9-20110106 |k PGI-9 |l Halbleiter-Nanoelektronik |x 0 |
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