The scaling down of Complementary Metal Oxide Semiconductor (CMOS) transistors to sub-100nm requires replacement of conventional Silicon dioxide layer with high dielectric constant (K) material for gate dielectric. Among the various high-K dielectrics that have been studied, HfO2 is found to be a promising candidate because of its high dielectric constant (~25), large band gap (5.68 eV), thermodynamic stability and good interface with Si. The HfO2 films have already been deposited using different growth techniques such as Atomic layer Deposition (ALD), Metalorgonic Chemical Vapor Deposition (MOCVD) and Pulsed Laser Deposition (PLD). Ion Assisted Deposition (IAD) is a novel technique that has been successfully employed to produce optical coatings of required quality. This growth technique presents many advantages over the other techniques such as formation from solid oxide sources, low growth temperatures (25-3000C) and film densification by ion bombardment. Hence this technique has been used to prepare HfO2 films in the present investigations. This thesis presents the structural, optical and electrical properties of HfO2 thin films prepared by Ion assisted deposition (IAD). The suitability of Ion assisted deposition process and the importance of investigations on the influence of process parameters on the film characteristics have been brought out in the process parameters-structure-composition and properties correlation presented in this thesis. The aim of this work is to process and characterize HfO2 films and investigate the influence of process parameters on the structure, composition and properties of the films to identify their suitability for CMOS gate applications. HfO2 films were deposited on p-type Si (100) wafers by Ion assisted deposition in an electron beam evaporation (Leybold,L-560) system. Pre-bombardment of the substrates with Argon ions has been done to remove any native oxide layer formation on Silicon by using a hallow cathode ion source (DENTON VACUUM CC103). During the film deposition a collimated oxygen ion beam, generated from the ion source is directed towards the substrate. The oxygen ion current is controlled by adjusting the voltage applied to the ion source and the oxygen flow through the ion source. The oxygen ions bombard the film as it grows and in that process improves its packing density as well as its stoichiometry. Keeping the deposition rate and thickness constant, HfO2 films have been deposited by varying Ion Current, Ion energy and substrate temperature. MOS capacitors were fabricated with Aluminum as gate electrode deposited by thermal evaporation. Ellipsometry techniques have been used to measure the optical thickness of the films. The interfacial layer (IL) formed at the HfO2/ Si interface was investigated by using Fourier transform Infrared spectroscopy (FT-IR). The structural characterization was carried out by X-ray diffraction technique. The high frequency capacitance-voltage and DC leakage current characteristics were measured to analyze the electrical characteristics of MOS capacitors. The effect of post deposition annealing (PDA) of the films at 600°C and 700ºC in Forming Gas (15%H2+85%N2) ambient and Post metallization annealing (PMA) at 400ºC in the same ambient was also investigated to observe the changes in electrical characteristics. The initial step of this work was to compare the characteristics of the films deposited by reactive evaporation and Ion assisted deposition which confirmed the superiority of the quality of IAD coatings and justified the need to proceed further with a more detailed study on the influence of various parameters on the properties of IAD coatings. HfO2 films deposited on substrates maintained at 1000C exhibited better structural, Optical and Electrical properties. The leakage current in these films were lower which has been attributed to silicate free interface as confirmed by XRD studies. Investigations on films deposited with oxygen ion beams of different currents in the range 20 to 40mA indicated that the films deposited at 20mA ion current showed better electrical properties. Better stoichiometry of these films as indicated by FT IR studies was one of the reasons for their improved performance. Annealing of these films at 6000C and 7000C in FGA medium resulted in creation of silicates and silicides at the interface thereby increasing the leakage currents and degraded the film properties. The films deposited with oxygen ion beams generated with a driving voltage 265V showed better structural and optical properties with silicate free interface compared with low and high driving voltages. Among all the films, the maximum dielectric constant of about 21.9 with a minimum EOT of 5.5 nm corresponding to a film deposited at ion current 20mA with PMA 400°C in FG ambient for 20minites is achieved. The lowest value of interface charge density achieved is 2.7 x1012 per cm-2 eV-1 corresponding to the sample deposited at substrate temperature 100°C with deposition rate of 0.5Å/sec followed by post metallization annealing at 400°C in forming gas for 20minutes. The range of Dit values that were obtained are varying from 2.7x 1012 – 16.7x1012 cm-2eV-1.It was also found that, the samples deposited at higher ion currents show lower Dit values than the samples deposited at lower ion currents. From the I−V analysis, the leakage current density is found to be comparatively less in IAD than in reactive evaporation. Leakage current increases with increase in substrate temperature and the same trend is observed with annealed films also. The lowest leakage current density of 1.05x10–8 A/cm2 at a gate bias of 1V was observed in the films deposited at substrate temperature 1000C. The present thesis focused on the suitability of the Ion Assisted deposition process for the preparation of HfO2 films for high-K gate dielectric application and the importance of investigations on the influence of process parameters on the film characteristics.

We report on a novel silicon nanowire-based field effect transistor with integrated ferroelectric gate oxide. The concept allows tuning the carrier transport in a non-volatile approach by switching the polarization in the ferroelectric layer close to the source Schottky-junction. We interpret the results in terms of tuning the transmissibility of the Schottky-junction for charge carriers. The experimental results provide a first step towards the integration of memory-in-logic concepts with reconfigurable nanowire transistors.

During the last decade ferroelectrics based on doped hafnium oxide emerged as promising candidates for realization of ultra-low-power non-volatile memories. Two spontaneous polarization states occurring in the material that can be altered by applying electrical fields rather than forcing a current through and the materials compatibility to CMOS processing are the main benefits setting the concept apart from other emerging memories. 1T1C ferroelectric random access memories (FeRAM) as well as 1T FeFET concepts are under investigation. In this article the application of hafnium based ferroelectric memories in different flavours and their ranking in the memory landscape are discussed.

Im Fokus der vorliegenden Arbeit liegt das Widerstandsschalten von HfO2- und TiO2-Dünnschichten, wobei insbesondere auf den Einfluss der Kristallstruktur, der Stöchiometrie und der Elektrodenmaterialien ((inert, Pt) und (reaktiv, Ti/Pt)) eingegangen wurde. Die HfO2-Dünnschichten wurden mittels Atomlagenabscheidung (ALD) durch die Reaktion von Tetrakis(dimethylamido)hafnium mit Wasser bei Temperaturen von 100°C bis 350°C abgeschieden. Das beste ALD-Wachstum mit der geringsten Konzentration an Wasserstoff wurde für eine Temperatur von 300°C erhalten. Sowohl eine geringere als auch eine höhere Abscheidetemperatur führte durch parasitäre CVD-artige Prozesse bzw. durch die ungewollte thermische Zersetzung des Präkursors zu einer größeren Wasserstoffkonzentration. Des Weiteren wurde eine Korrelation zwischen der Wachstumsrate pro Zyklus, der Schichtdickenhomogenität und der Wasserstoffkonzentration in den HfO2-Schichten festgestellt. Das Widerstandsschalten wurde an amorphen (150°C) und polykristallinen (300°C) HfO2-Schichten mit unstrukturierten Rückelektroden und kreisförmigen Vorderseitenelektroden untersucht. Die Verwendung von symmetrischen Pt-Pt-Elektroden führte bei beiden Schichttypen zum unipolaren Schaltmodus. Der unipolare Schaltmodus wurde ebenfalls bei Verwendung von asymmetrischen Pt-Ti/Pt-Elektroden im Zusammenspiel mit der amorphen HfO2-Phase beobachtet. Eine Ausnahme stellt die Kombination von asymmetrischen Elektroden mit der polykristallinen HfO2-Phase dar. Dabei wurde nach der Elektroformierung mit positiv angelegter Spannung an die Vorderseitenelektrode der bipolare Schaltmodus erhalten. Eine Erklärung dafür liefert die Betrachtung der Filament-Wachstumsrichtung während der Elektroformierung. Die TiO2-Dünnschichten wurden durch reaktives Magnetronsputtern gewachsen. Die Stöchiometrie dieser Schichten wurde durch die Bestrahlung mit Ar-Ionen gezielt verändert. Dabei führt das bevorzugte Herausschlagen von Sauerstoff im Vergleich zum Titan zu einer an Sauerstoff verarmten TiOx-Schicht, welche sich durch die verwendete Ionenenergie von 2keV in oberflächennahen Bereichen befindet. Die Ausdehnung der TiOx-Schicht wurde mit einer TRIDYN-Simulation auf ca. 4nm bestimmt. Während sich zwischen einer TiO2-Schicht und einer Pt-Elektrode ein Schottky-Kontakt ausbildet, führt das Einbringen einer TiOx-Schicht zu einem ohmschen Kontakt. Für die Charakterisierung des Widerstandsschaltens an den mit Ar-Ionen bestrahlten TiO2-Schichten wurde somit auf symmetrische Pt-Pt-Elektroden zurückgegriffen. Im Bereich der getesteten Fluenzen von 1 x 10^13 Ar+/cm2 bis 1 x 10^16 Ar+/cm2 wurde mit einer Fluenz von 1 x 10^14 Ar+/cm2 sowohl die beste Ausbeute als auch die größten Endurance-Werte erzielt. / The work focuses on the resistive switching of HfO2 and TiO2 thin films. Especially the influence of crystal structure, stoichiometry and electrode materials ((inert, Pt) and (reactive, Ti/Pt)) have been examined. HfO2 thin films have been grown at temperatures ranging from 100°C to 350°C through the process of atomic layer deposition (ALD) by the reaction of tetrakis(dimethylamido)-hafnium with water. The best ALD growth with the lowest concentration of hydrogen was achieved at a temperature of 300°C. Both lower and higher deposition temperatures caused higher hydrogen concentrations due to parasitic CVD-like processes or thermal decomposition of the precursor. Moreover a correlation between the growth rate per cycle, the layer thickness uniformity and the hydrogen concentration in the HfO2 films was observed. Resistive switching was examined in amorphous (150°C) and polycrystalline (300°C) HfO2 films with unstructured bottom electrodes and circular structured top electrodes. The use of symmetric Pt-Pt-electrodes caused the unipolar switching mode in both layer types. The unipolar switching mode was also observed when asymmetric Pt-Ti/Pt-electrodes were used with an amorphous phase of the HfO2 layer. An exception is the use of asymmetric electrodes with the polycrystalline phase of the HfO2 layer. In this case electroforming with the application of positive voltage to the top electrode resulted in the bipolar switching mode. This is explained when looking at the filament growth direction during electroforming. TiO2 thin films were grown by reactive magnetron sputtering. The stoichiometry of these layers was modified by irradiation with Ar-ions. The preferential sputtering of oxygen compared to titanium causes a surface-near oxygen deficient TiOx layer due to the used ion energy of 2 keV. The depth of the TiOx layer was estimated to be 4 nm by using a TRIDYN simulation. While a Schottky contact formed between a TiO2 layer and a Pt-electrode, the use of a TiOx layer led to an ohmic contact. Symmetric Pt-Pt-electrodes were used to characterize resistive switching of TiO2 layers which have been irradiated with Ar-ions. The tested fluences ranged from 1×10^13 Ar+/cm2 to 1 × 10^16 Ar+/cm2. A fluence of 1 × 10^14 Ar+/cm2 resulted in the best yield and highest endurance.

Ferroelectric HfO₂ attracts a huge amount of attention not only for memory and negative capacitance, but also for programmable logic including memory-in-logic and neuromorphic applications. However, the understanding of material fundamentals still needs to be improved. This paper gives material fundamentals and new insights to this ferroelectric material for future device applications. In particular, the key role of dopants, effects of the interface on the ferroelectric phase, and a detailed discussion of the switching kinetics are of central focus. Based on material properties newly obtained, we discuss opportunities of ferroelectric HfO₂ for device applications.

Ferroelectricity in hafnium oxide thin films is known to be induced by various doping elements and in solid-solution with zirconia. While a wealth of studies is focused on their basic ferroelectric properties and memory applications, thorough studies of the related pyroelectric properties and their application potential are only rarely found. This work investigates the impact of Si doping on the phase composition and ferro- as well as pyroelectric properties of thin film capacitors. Dynamic hysteresis measurements and the field-free Sharp-Garn method were used to correlate the reported orthorhombic phase fractions with the remanent polarization and pyroelectric coefficient. Maximum values of 8.21 µC cm−2 and −46.2 µC K−1 m−2 for remanent polarization and pyroelectric coefficient were found for a Si content of 2.0 at%, respectively. Moreover, temperature-dependent measurements reveal nearly constant values for the pyroelectric coefficient and remanent polarization over the temperature range of 0 °C to 170 °C, which make the material a promising candidate for IR sensor and energy conversion applications beyond the commonly discussed use in memory applications.

The ferroelectricity in fluorite structure based hafnium oxide (HfO2) material expanded the horizon for realizing nonvolatile ferroelectric memory concepts. Due to the excellent HfO2 ferroelectric film properties, CMOS compatibility, and scalability; the material is foreseen as a replacement of the lead based ferroelectric materials with a big game changing potential for the emerging ferroelectric memories. In this thesis, the development of novel memory concepts based on the ferroelectric or antiferroelectric HfO2 material is reported. The ferroelectric field effect transistor (FeFET) memory concept offers a low power, high-speed, nonvolatile, and one cell memory solution ideal for embedded memory realization. As an emerging concept based on a novel ferroelectric material, the FeFET is challenged with key performance aspects intrinsic to the underlying physics of the device. A central part of this thesis is the development of FeFET through material and gate stack engineering, in turn leading to innovative novel device concepts. The conceptual innovation, process development, and electrical assessment are explored for an ferroelectric or antiferroelectric HfO2 based nonvolatile memories with focus on the underlying device physics. The impact of the ferroelectric material on the FeFET physics is explored via the screening of different HfO2 based ferroelectric materials, thicknesses, and the film doping concentration. The impact of material interfaces and substrate doping conditions are explored on the stack engineering level to achieve a low power and reliable FeFET. The material optimization leads to the concept of ferroelectric lamination, i.e. a dielectric interlayer between multi ferroelectric ones, to achieve a novel multilevel data storage in FeFET at reduced device variability. Toward a low power FeFET, the stack structure tuning and dual ferroelectric layer integration are explored through an MFM and MFIS integration in a single novel FeFET stack. The charge trapping effect during the FeFET switching captures the dynamics of the hysteresis polarization switching inside the stack with direct impact on the interfacial layer field. Even though manifesting as a clear drawback in FeFET operation, it can be utilized in Flash, leading to a novel hybrid low power and high-speed antiferroelectric based charge trap concept. Furthermore, the FeFET reliability is studied covering the role of operating temperature and the ferroelectric wakeup phenomenon observed in the FeFET. The temperature modulated operation, role of the high-temperature pyroelectric effect, and the temperature induced endurance and retention reliability are studied.:Table of Contents Abstract Table of Contents 1. Introduction 2. Fundamentals 2.1. Basics of Ferroelectricity 2.2. The FeFET Operation Principle and Gate Stack Theory 2.3. Structure and Outline of the PhD Thesis 3. The Emerging Memory Optimization Cycle: From Conceptual Design to Fabrication 3.1. The FeFET Conceptual Design and Layout Implementation 3.2. Gate First FeFET Fabrication: Material and Gate Stack Optimization 3.3. Novel Gate First based Memory Concepts: Device Integration and Stack Optimization 3.4. Device Characterization: Electrical Testing Schemes 4. The Emerging FeFET Memory: Material and Gate Stack Optimization 4.1. Material Aspect of FeFET Optimization: Role of the FE Material Properties 4.2. The Stack Aspect of FeFET Optimization: Role of the Interface Layer Properties 4.3. The Stack Aspect of FeFET Optimization: Role of the Substrate Implant Doping 4.4. Summary 5. A Novel Multilevel Cell FeFET Memory: Laminated HSO and HZO Ferroelectrics 5.1. The Laminate MFM and Stack Characteristics 5.2. The Laminate based FeFET Memory Switching 5.3. The Laminate FeFET Multilevel Coding Operation (1 bit, 2 bit, 3 bit/cell) 5.4. The Maximum Laminate FeFET MW Dependence on FE Stack Thickness 5.5. The Role of Wakeup and Charge Trapping 5.6. The Laminate MLC FeFET Area Dependence 5.7. The Laminate MLC Retention and Endurance 5.8. Impact of Pass Voltage Disturb on Laminate based NAND Array Operation 5.9. The Laminate FeFET based Synaptic Device 5.10. Summary 6. A Novel Ferroelectric MFMFIS FeFET: Toward Low Power and High-Speed NVM 6.1. The MFMFIS FeFET P-E and FET Characteristics 6.2. The MFMFIS based Memory Characteristics 6.3. The Impact of MFMFIS Stack Structure Tuning 6.4. The Maximum MFMFIS FeFET Memory Window 6.5. The Role of Device Scalability and Variability 6.6. The MFMFIS Area Tuning for Low Power Operation 6.7. The MFMFIS based FeFET Reliability 6.8. The Synaptic MFMFIS based FeFET 6.9. Summary 7. A Novel Hybrid Low Power and High-Speed Antiferroelectric Boosted Charge Trap Memory 7.1. The Hybrid Charge Trap Memory Switching Characteristics 7.2. The Role of Polarization Switching on Optimal Write Conditions 7.3. The Impact of FE/AFE Properties on the Charge Trap Maximum Memory Window 7.4. The Hybrid AFE Charge Trap Multi-level Coding and Array Operation 7.5. The Global Variability and Area Dependence of the Charge Trap Memory Window 7.6. The AFE Charge Trap Reliability 7.7. The Hybrid AFE Charge Trap based Synapse 7.8. Summary 8. The Emerging FeFET Reliability: Role of Operating Temperature and Wakeup Effect 8.1. The FeFET Temperature Reliability: A Temperature Modulated Operation 8.2. The FeFET Temperature Reliability: Role of the Pyroelectric Effect 8.3. The FeFET Temperature Reliability: Endurance and Retention 8.4. The Impact of Ferroelectric Wakeup on the FeFET Memory Reliability 8.5. Summary 9. Closure: What this Thesis has Solved? 9.1. How material selection/development influence the FeFET? 9.2. Why the FeFET Still Operates at High Write Conditions? 9.3. Why the FeFET Endurance is still a Challenge? 9.4. Can the FeFET become Multi-bit Storage Memory? 9.5. How the Scalability Determine FeFET Chances? 10. Summary 11. Bibliography List of symbols and abbreviations List of Publications Acknowledgment Erklärung

Thin film metal–insulator–metal capacitors with undoped HfO₂ as the insulator are fabricated by sputtering from ceramic targets and subsequently annealed. The influence of film thickness and annealing temperature is characterized by electrical and structural methods. After annealing, the films show distinct ferroelectric properties. Grazing incidence X-ray diffraction measurements reveal a dominant ferroelectric orthorhombic phase for thicknesses in the 10–50 nm range and a negligible non-ferroelectric monoclinic phase fraction. Sputtering HfO₂ with additional oxygen during the deposition decreases the remanent polarization. Overall, the impact of oxygen vacancies and interstitials in the HfO₂ film during deposition and annealing is correlated to the phase formation process.

This article corrects the following: 'Origin of Ferroelectric Phase in Undoped HfO2 Films Deposited by Sputtering' Advanced Materials Interfaces 6(11) 2019, first Published online: April 29, 2019

The discovery of the ferroelectric orthorhombic phase in doped hafnia films has sparked immense research efforts. Presently, a major obstacle for hafnia's use in high-endurance memory applications like nonvolatile random-access memories is its unstable ferroelectric response during field cycling. Different mechanisms are proposed to explain this instability including field-induced phase change, electron trapping, and oxygen vacancy diffusion. However, none of these is able to fully explain the complete behavior and interdependencies of these phenomena. Up to now, no complete root cause for fatigue, wake-up, and imprint effects is presented. In this study, the first evidence for the presence of singly and doubly positively charged oxygen vacancies in hafnia–zirconia films using thermally stimulated currents and impedance spectroscopy is presented. Moreover, it is shown that interaction of these defects with electrons at the interfaces to the electrodes may cause the observed instability of the ferroelectric performance.