Ulis 2003 4th European Workshop on ULtimate Integration of Silicon Theoretical investigation of hole phonon-velocity in strained Si inversion layer F.

Slides:



Advertisements
Présentations similaires
European Commission DG DEV B2 CONDITIONALITY REFORMULATED THE BURKINA FASO PILOT CONDITIONALITY REFORMULATED THE BURKINA FASO PILOT.
Advertisements

Laboratoire de lIntégration du Matériau au Système CNRS UMR ICECS 2010 A 65nm CMOS Fully Integrated 31.5dBm Triple SFDS Power Amplifier dedicated.
What is the time Mr. Wolf? LObjectif At the end of the lesson, you will be able to: 1.Say quarter past and quarter to the hour.
Présenté par : AHMED Toufik Université de Versailles - France
Branche Développement Cnet La communication de ce document est soumise à autorisation du Cnet © France Télécom - (Nom du fichier) - D1 - 11/01/2014 Diffusion.
Environmental Data Warehouse Cemagref, UR TSCF, TR MOTIVE 2011 – projet Miriphyque.
L A H C Activités en Opto-Microondes au LAHC - Université de Savoie Optoélectronique ultrarapide.
La R&D industrielle autour des DSP en France Texas Instruments : - Villeneuve-Loubet centre R&D Motorola : - Saclay centre R&D - Toulouse centre R&D +
Université Des Sciences Et De La Technologie DOran Mohamed Boudiaf USTO République Algérienne Démocratique et Populaire Département de linformatique Projet.
External Communication Plan Energy Europe Division March 2009
Créons des questions! -mot interrogatif (question word) -est-ce que (except in short questions such as with être) OR -inversion (reverse the subject and.
Groupe de Recherche en Economie Théorique et appliquée – UMR CNRS 5113 An evolutionary modelling of recycling and product-life extension EMAEE 2007 Globalisation,
Contours dénergie constante. 2 Drude Oscillations de Bloch.
J. Duchesne1, P. Raimbault2 and C. Fleurant1
Passé Composé Teagan Ringstad.
Modifications of working conditions in the host states Report on the AT Board held on 18 April 2000 New minimum wages in Switzerland Impact of the 35-hour.
The Solar Orbiter A high-resolution mission to the Sun and inner heliosphere.
Ce document est la propriété d ’EADS CCR ; il ne peut être communiqué à des tiers et/ou reproduit sans l’autorisation préalable écrite d ’EADS CCR et son.
Information Theory and Radar Waveform Design Mark R. bell September 1993 Sofia FENNI.
What is the nanotechnology History applications of nanotechnology Conclusion.
Etudes statistiques de la puissance des ondes à la magnétopause et à son voisinage (Traversées Cluster). Corrélations avec la pression du vent solaire.
Les Monstres Due Next Class: A day- Tuesday B day- Wednesday.
Sensitivity improvement of non- linearities measurements using binary diffractive optics Thomas Godin M. Fromager, E. Cagniot, B. Païvänranta, N. Passilly,
Energy optimization in a manufacturing plant Journée GOThA Ordonnancement avec contraintes d’énergie et/ou de ressources périssables LAAS-CNRS Toulouse.
Modélisation d’un dopage
Observation des concentrations et flux d’azote atmosphériques
PAPRIKA WP4: MODELLING THE INTERACTION BETWEEN SNOWPACK, RADIATION, AND THE ABSORBING MATERIAL DEPOSITED IN THE SNOW Hans-Werner Jacobi
Ottawa – News release January 2007 Nouvelle effective en Janvier 2007 Massive federal government tax surplus this year will make a tax rebate possible.
ELI Nuclear Physics meeting, Bucarest Feb1-2, 2010 Interferometric beam combination Gérard Mourou.
Ordre des cours d’eau et zones humides : application à la dynamique spatio-temporelle des nitrates Sous-titre : De la nécessité de travailler à différentes.
January 26 th 2015 European Organization for Nuclear Research CLIC WORKSHOP 26/01/2015 CLIC WORKSHOP 2015, Geneva, Switzerland Optics Design and Beam Dynamics.
Astroparticle Physics in Provence Wednesday 7 July Presentation Amphitheatre CPPM 10: Welcome (John Carr) Introduction to neutrino.
Français 2, 2 septembre 2012 Dessinez le vocabulaire, page 51. What's the difference between a teacher and a train? Drôle – funny. Tu en fais une drôle.
E2Phi Nantes Aug S.Deleonibus LETI/D2NT
Questions: -W-W-W-What are their main tasks? - What skills should laboratory technicians have? (quote at least 6) -W-W-W-Why is it important for a lab.
Formation de la précipitation
Effets sur la santé des champs électromagnétiques basse fréquence
Marseille, 22 November 2007 MINISTRY OF ECONOMY & FINANCE
PhD student: Salvatore Danzeca EN/STI/ECE
Français Deux L’accord au passé (agreement of the past participle)
The BMV project : axion search with a pulsed magnet Status of the experiment Rémy Battesti Laboratoire National des Champs Magnétiques Pulsés Université.
ECASA.org.uk Ecosystem approach for a sustainable aquaculture STREP (FP6, Priority 8)
8ème édition des JNRDM Paris Mai 2005 Propriétés hyperfréquences et de bruit des filières conventionnelles de transistors MOS à grille sub-100 nm.
G. Ladier DAS Systèmes Embarqués, Electronique & Logiciel (SE²L) - Programme Fédérateur Intégration des Systèmes Embarqués Electroniques (ISEE) Journée.
Modèles d’interaction et scénarios
Proposals/Propositions Organisation of Union Events together with National Events Members will recall that in recent years, the level of participation.
« © CEA [2006]. Tous droits réservés. Toute reproduction totale ou partielle sur quelque support que ce soit ou utilisation du contenu de ce document est.
Telling time in French. To ask for and give the time:  Quelle heure est-il?  Il est ___ heure(s).
Effets nucléaires « froids »: discussion Marie-Pierre COMETS IPN Orsay Journées QGP-France, Etretat, 3-5 juillet 2006.
University of Ottawa - Bio 4118 – Applied Biostatistics © Antoine Morin and Scott Findlay 24/07/2015 2:29 PM Bootstrap et permutations.
NAME: Abdul Saleem Mir Enrollment Number: 49/2010 7th ELECTRICAL
%mass %volume Composition of concrete Concrete cement water sand
Bienvenue! Instructions: Take out your “smiley face paper” and study your notes for two minutes. We will be reviewing all of the vocabulary today for body.
1 THE GESTRANS PROJECT Taking into account changing alluvial channels in flood risk assessment N° ANR-09-RISK-004/GESTRANS.
Fabien Plassard December 4 th European Organization for Nuclear Research ILC BDS MEETING 04/12/2014 ILC BDS MEETING Optics Design and Beam Dynamics Modeling.
GDR SURGECO, Montpellier, 3-5 March 2008 D Mangelinck, K Hoummada, F Haidara, C Perrin, A Portavoce, M-C Record, B Duployer Institut Matériaux, Microélectronique.
LISBP Laboratoire d’Ingénierie des Systèmes Biologiques et des Procédés Page 1 The Dale Edmondson Conference, July 2013, Atlanta MAOs and P450s Philipp.
CHAPTER 4 CONDUCTION IN SEMICONDUCTORS Prof. Dr. Beşire GÖNÜL.
Accélérateur laser – plasma
Concrete as a construction material. What Is Concrete Used For? Construction Material Art Work.
TP3
Monte Carlo Algorithm for simulation of phonon transport in silicium nanowires Scattering mechanism 18 June 2013 Jérôme LARROQUE.
Quantum Computer A New Era of Future Computing Ahmed WAFDI ??????
The consequences of the.
Project title: Olympic Energy: Tipping the scale towards Bio-CNG for European Transport starts in TEN-T Core Urban Node Paris! CEF Transport Blending 2017.
Project title: Olympic Energy: Tipping the scale towards Bio-CNG for European Transport starts in TEN-T Core Urban Node Paris! CEF Transport Blending 2017.
Répondez aux 5 questions – Travaillez à deux
FROM THE NEAR FIELD OF NANO- ANTENNAS TO THE FAR FIELD OF METASURFACES Thesis Supervisor: Dr. Yannick De Wilde Co-supervisor: Dr. Patrick Bouchon.
Insights on V2X Technology ARCHI - Symposium Applied Research on Charging Infrastructure 24th January, Amsterdam Sara González Villafranca.
Transcription de la présentation:

Ulis th European Workshop on ULtimate Integration of Silicon Theoretical investigation of hole phonon-velocity in strained Si inversion layer F. Payet (1,2), N. Cavassilas (1), J.L. Autran (1) (1) Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - (2) ST Microelectronics Crolles

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Outline  Strained Silicon Deformed Si lattice Strain contribution on the valence band Strain consequences on transport properties  Strained Silicon inversion layer Strained Si MOSFET Tensile strain and quantization effects Transport results  Conclusion  Strained Silicon Deformed Si lattice Strain contribution on the valence band Strain consequences on transport properties  Strained Silicon inversion layer Strained Si MOSFET Tensile strain and quantization effects Transport results  Conclusion

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles The System Strained Si on SiGe [001] [100] [010] Two strain contributions: Hydrostatic Uniaxial → lower lattice symmetry Si 1-x Ge x strainedSi a SiGe (x) a (x) a // (x) a  (x) a SiGe (x) a // (x)

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Tensile Strain Contribution on Band Structure

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Tensile Strain Contribution on Band Structure Band Structure

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Strain Contribution on the Valence Band Unstrained Si Si/SiGe LH BandHH Band phonon [100] [010] [110] [100] [010] [110]

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Strain Consequences on Transport Properties < 1 % in HH ≈ 86 % in HH F= 30 kV/cm

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Strain Consequences on Transport Properties Hole Drift Velocity LH Band HH Band F = 50 kV/cm Distribution Functions F kyky kxkx F F kyky kxkx kyky kxkx

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Strain Consequences on Transport Properties F = 50 kV/cm Distribution Functions F kyky kxkx F F kyky kxkx kyky kxkx LH Band HH Band Hole Drift Velocity

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Strain Consequences on Transport Properties F = 50 kV/cm Distribution Functions F kyky kxkx F F kyky kxkx kyky kxkx LH Band HH Band Hole Drift Velocity

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Strain Consequences on Transport Properties F = 50 kV/cm Distribution Functions F kyky kxkx F F kyky kxkx kyky kxkx LH Band HH Band Hole Drift Velocity

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Strain Consequences on Transport Properties F = 50 kV/cm Distribution Functions F kyky kxkx F F kyky kxkx kyky kxkx LH Band HH Band Hole Drift Velocity

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Strain Consequences on Transport Properties F = 50 kV/cm Distribution Functions F kyky kxkx F F kyky kxkx kyky kxkx LH Band HH Band Hole Drift Velocity

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Strain Consequences on Transport Properties F = 50 kV/cm Distribution Functions F kyky kxkx F F kyky kxkx kyky kxkx LH Band HH Band Hole Drift Velocity

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Strain Consequences on Transport Properties F = 50 kV/cm Distribution Functions F kyky kxkx F F kyky kxkx kyky kxkx LH Band HH Band Hole Drift Velocity

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Strain Consequences on Transport Properties F = 50 kV/cm Distribution Functions F kyky kxkx F F kyky kxkx kyky kxkx LH Band HH Band Hole Drift Velocity

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Strained Si MOSFET Depth (m) Energy (eV) Hole Density (u.a.) Strained Si Relaxed SiGe CB VB LH sub-Band HH sub-Band Energy Levels Non Localised in the Strained Si Channel Depth (m) Energy (eV) Hole Density (u.a.) Strained Si Relaxed SiGe CB VB LH sub-Band HH sub-Band Energy Levels Non Localised in the Strained Si Channel

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Tensile Strain and Quantization Effects Strain and Confinement in [001] direction

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Transport Results: Strain effects Hole Velocity versus Time Tsi = 10 nm F = 50 kV/cm

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Transport Results: Quantization Effects Hole Velocity versus Electric Field

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles Transport Results Hole Mobility Enhancement versus Strain

Laboratoire Matériaux et Microélectronique de Provence UMR CNRS Marseille/Toulon (France) - ST Microelectronics Crolles ConclusionConclusion  Strain-induced effects increase hole transport performances in silicon.  Quantization in MOSFET inversion layer tends to decrease the splitting between LH and HH band.  Holes must be localized in the strained channel.  As a consequence, device structure should be carefully optimized:  tsi ≥ 10nm  [Ge] ≥ 30%  Strain-induced effects increase hole transport performances in silicon.  Quantization in MOSFET inversion layer tends to decrease the splitting between LH and HH band.  Holes must be localized in the strained channel.  As a consequence, device structure should be carefully optimized:  tsi ≥ 10nm  [Ge] ≥ 30%