2D MATERIALS

Pioneering 2D Materials for Semiconductor Industry

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This webinar, hosted by the Graphene Flagship's 2D-EPL, will examine encapsulation and dielectric interfaces in the integration of 2D materials for the semiconductor industry.

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On Demand
Time:

On Demand

Duration:

2 hours 10 minutes

Language:

English

Businesses:

Plasma Technology

In Partnership With

Agenda

Time (BST)

Talk Title

Presenter

14:00-14:15

2D Experimental Pilot Line update

Gordon Rinke

14:15-14:45

The Quest for the Perfect Insulator for 2D Materials

Tibor Grasser

14:45-15:25

Damage-free plasma ALD on graphene: enabled by in-situ-prepared protective seed layer

Harm Knoops

15:25-15:55

Panel Discussion

Ravi Sundaram (moderator)

Abstracts

2D Experimental Pilot Line update
Dr Gordon Rinke, AMO GMBH

Announcing the call for applications to participate in the 2D-Experimental Pilot Line's first Multi-Project Wafer (MPW) run.


The Quest for the Perfect Insulator for 2D Materials
Dr Tibor Grasser, Head of Institute for Microelectronics

Despite the breathtaking progress already achieved for 2D electronic devices, they are still far from exploiting their predicted performance potential. This is in part due to the lack of scalable insulators, which would go along with 2D materials as nicely as SiO2 goes with silicon. As a result, there is still no commercially competitive 2D transistor technology available today. The selection of suitable insulators for 2D nanoelectronics represents an enormous challenge. However, this problem is of key importance, since scaling of 2D semiconductors towards sub-10nm channel lengths is only possible with gate insulators scalable down to sub-1nm equivalent oxide thicknesses (EOT). In order to achieve competitive device performance, these insulators need to meet stringent requirements regarding (i) low gate leakage currents, (ii) low density of interface traps, (iii) low density of border insulator traps and (iv) high dielectric strength.

The insulators typically used for 2D electronic devices are amorphous 3D oxides known from Si technologies (SiO2, HfO2, Al2O3), while native 2D oxides (MO3, WO3 and Bi2SeO5), layered 2D crystals (hBN, mica) and ionic 3D crystals (CaF2 and other fluorides like SrF2, MgF2) have received increasing attention. 3D oxides form poor quality interfaces with 2D semiconductors and contain border traps which severely perturb stable device operation. Native oxides, on the other hand, are often non-stoichiometric due to the lack of well-adjusted oxidation methods and thus have a limited dielectric stability and inherently narrow bandgaps. As the most popular candidate, the layered 2D insulator hBN forms excellent van der Waals interfaces with 2D semiconductors, but has mediocre dielectric properties resulting in excessive leakage currents for sub-1nm EOT. The potential of other 2D insulators (e.g. mica) is currently unclear, in part due to the absence of scalable growth techniques. Finally, very promising insulators for 2D electronics are 3D ionic crystals like CaF2 which form well-defined interfaces to 2D channel materials. In contrast to hBN, fluorides have good dielectric properties and thus exhibit low gate leakage currents. This talk will address the current state of the art and summarize the main problems together with potential solutions.


Damage-free plasma ALD on graphene: enabled by in-situ-prepared protective seed layer
Dr Harm Knoops, Oxford Instruments Plasma Technology

A key challenge to realising graphene’s potential in emerging electronics and optoelectronics is the development of scalable, high-quality integration of dielectric materials as functional layers and encapsulation. We describe a novel method to deposit high-κ dielectrics on graphene through an in-situ-prepared protective seed-layer using the Oxford Instruments Atomfab system. For the development of graphene-based devices, such as transistors, photodetectors, or optical modulators, a deposition of a high-quality dielectric film on graphene is required. However, this deposition is challenging because nucleation on pristine graphene is difficult. While defect induced nucleation, for example through plasma exposure, improves nucleation, it also decreases the quality of the graphene layer.

Recently we reported dielectric deposition using remote plasma ALD, without observable damage, by protecting the graphene by hexagonal boron nitride (hBN). However, using hBN involves additional transfer processes, which may complicate the fabrication and introduce contamination, defects, and wrinkles. Inspired by this process, we developed a new process using an in-situ deposited seed-layer to protect the graphene effectively, enabling plasma assisted deposition of Al2O3 without damaging the graphene.

Speakers

Dr Gordon Rinke - AMO GmbH
Deputy Head of the Graphene Electronics Group

Dr Gordon Rinke obtained his PhD in Materials Science from the EPFL Lausanne, Switzerland in 2013. After spending over 6 years ...

Dr Tibor Grasser - TU Wien
Head of Institute for Microelectronics

Prof. Tibor Grasser is an IEEE Fellow and head of the Institute for Microelectronics at TU Wien. He has edited various books, e...

Dr Harm Knoops - Oxford Instruments Plasma Technology
Atomic Scale Segment Specialist

Dr Harm Knoops is the Atomic Scale Segment Specialist at Oxford Instruments Plasma Technology and holds a part-time assistant p...

Dr Ageeth Bol - University of Michigan
Professor of Chemistry and Applied Physics

Ageeth Bol is Professor of Chemistry and Applied Physics at the University of Michigan - Ann Arbor, MI. She received her MSc an...

Dr Ravi Sundaram - Oxford Instruments Plasma Technology
Head of strategic R&D Markets

Dr Ravi Sundaram is the Head of strategic R&D Markets at Oxford Instruments Plasma Technology responsible for leading the marke...


 

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