VIRTUAL NANOLAB BY QUANTUMWISE

Slides:



Advertisements
Similar presentations
Exciton formation in graphene bilayer PHYSICAL REVIEW B 78, (2008) Raoul Dillenschneider, and Jung Hoon Han Presented by Wan-Ju Li 02/25/2009 PHYSICAL.
Advertisements

Working with Profiles in IX1D v 3 – A Tutorial © 2006 Interpex Limited All rights reserved Version 1.0.
1 After completing this lesson, you will be able to: Create a database. Create a table using the Table Wizard. Create and modify a table in Design view.
ECE : Nanoelectronics Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
Metals: Bonding, Conductivity, and Magnetism (Ch. 6)
USC Signal Integrity Lab Course 2 Ansoft High Frequency Structure Simulator (HFSS) ELCT 762 USC.
© 2013 Eric Pop, UIUCECE 340: Semiconductor Electronics ECE 340 Lecture 3 Crystals and Lattices Online reference:
Creating Rout Paths Using CAMMaster. Step 1 Import Gerber File. Import Gerber File. User Ctrl+W to window around data. User Ctrl+W to window around data.
Solid State Physics (1) Phys3710
Introduction to Solids. 3 Classes of Solids Amorphous – No long range order Polycrystalline – Order within grains Single Crystal – Regular, repeated pattern.
By Hrishikesh Gadre Session II Department of Mechanical Engineering Louisiana State University Engineering Equation Solver Tutorials.
Exam Study Practice Do all the reading assignments. Be able to solve all the homework problems without your notes. Re-do the derivations we did in class.
1 Motivation (Why is this course required?) Computers –Human based –Tube based –Solid state based Why do we need computers? –Modeling Analytical- great.
The effective mass Conductivity effective mass – determines mobility.
Gaxela N, Manaetja K.P, Mulaudzi S, Senosi R Supervisor: Dr V.L.Katkof.
ECE685 Nanoelectronics – Semiconductor Devices Lecture given by Qiliang Li.
Textbook: Electronic Devices and Circuit Theory Robert L.Boylested.
Microsoft Visual Basic 2005 CHAPTER 12 Cell Phone Applications and Web Services.
Network for Computational Nanotechnology (NCN) Purdue, Norfolk State, Northwestern, MIT, Molecular Foundry, UC Berkeley, Univ. of Illinois, UTEP DFT Calculations.
Data Analysis Using SPSS
Computational NanoEnginering of Polymer Surface Systems Aquil Frost, Environmental Engineering, Central State University John Lewnard, Mechanical Engineering,
VIRTUAL NANOLAB BY QUANTUMWISE
Sentaurus Introduction & Step-by-Step Manual
The H 2 O molecule: converging the size of the simulation box Objectives - study the convergence of the properties with the size of the unit cell.
Network for Computational Nanotechnology (NCN) Purdue, Norfolk State, Northwestern, MIT, Molecular Foundry, UC Berkeley, Univ. of Illinois, UTEP NEMO5.
Launch SpecE8 and React from GSS. You can use the chemical analyses in a GSS data sheet to set up and run SpecE8 and React calculations. Analysis → Launch…
Teacher’s Assessment Assistant Worksheet Builder Starting the Program
Network for Computational Nanotechnology (NCN) Purdue, Norfolk State, Northwestern, UC Berkeley, Univ. of Illinois, UTEP CNTbands First-Time User Guide.
Roy Downs University of Arkansas Faculty Mentor: Joe Rencis Graduate Student Mentor: Sachin Terdalkar.
- Compute and analyze the band structure of an ionic solid
Simulation of transport in silicon devices at atomistic level Introduction Properties of homogeneous silicon Properties of pn junction Properties of MOSFET.
Microsoft Visual Basic 2008 CHAPTER TWELVE Cell Phone Applications and Web Services.
Electronic Band Structures electrons in solids: in a periodic potential due to the periodic arrays of atoms electronic band structure: electron states.
Course ILT Forms and queries Unit objectives Create forms by using AutoForm and the Form Wizard, and add or modify form headers and footers Open and enter.
Electrical Potential When charges are within an electric field an electrical potential difference is created. Volt – unit of measurement for potential.
Tutorial for XFDTD Written by Cynthia Furse Utah State University.
APS -- March Meeting 2011 Graphene nanoelectronics from ab initio theory Jesse Maassen, Wei Ji and Hong Guo Department of Physics, McGill University, Montreal,
Calculations of Electronic Structure of Defective ZnO: the impact of Symmetry and Phonons A.V. Sorokin, D. Gryaznov, Yu.F. Zhukovskii, E.A. Kotomin, J.
Crystal Structures Crystal is constructed by the continuous repetition in space of an identical structural unit. Lattice: a periodic array of mathematical.
Quantum Mechanics Tirtho Biswas Cal Poly Pomona 10 th February.
05. Data from Bloomberg Add-in. Launch Bloomberg and Press GO.
Graphene-metal interface: an efficient spin and momentum filter
Band Structure Of Graphene Sheets and Carbon Nanotubes
EE105 - Spring 2007 Microelectronic Devices and Circuits
NEEP 541 Ionization in Semiconductors Fall 2002 Jake Blanchard.
4.12 Modification of Bandstructure: Alloys and Heterostructures Since essentially all the electronic and optical properties of semiconductor devices are.
Team work Majed AbdELSalam Nashaat,
Carrier generation and recombination A sudden increase in temperature increases the generation rate. An incident burst of photons increases the generation.
2/06/2015PHY 752 Spring Lecture 101 PHY 752 Solid State Physics 11-11:50 AM MWF Olin 107 Plan for Lecture 10: Reading: Chapter in MPM;
Active-HDL Server Farm Course 11. All materials updated on: September 30, 2004 Outline 1.Introduction 2.Advantages 3.Requirements 4.Installation 5.Architecture.
Tutorial of Practice #4 - Supercell & Defect formation energy -
Chapter 5 Armature Gap Sweep Workshop 4. Training Manual Electromagnetic Analysis in Workbench March 4, 2005 Inventory # Workshop #2: Armature.
Flat Band Nanostructures Vito Scarola
Address: 2401 East building Guanghua tower Phone: Magnetic and spin polarized transport properties.
Practice #2: Solid Yong-Hyun Kim NST551.
Photonic Systems Laboratory School of EE, Seoul National University Photonic Systems Lab School of EECS, S.N.U. Electro-Magnetic Fields I.
Isolated Si atoms.
Graphene Based Transistors-Theory and Operation; Development State
EE 315/ECE 451 Nanoelectronics I
Band structure of a cubic perovskite oxide:
Lecture 2 OUTLINE Important quantities
Spin-orbit interaction in a dual gated InAs/GaSb quantum well
Do all the reading assignments.
Energy Bands in Crystals
ECEE 302: Electronic Devices
Electronic properties in moiré superlattice
Observed by Photoemission
The Nuts and Bolts of First-Principles Simulation
VIRTUAL NANOLAB BY QUANTUMWISE
L.
Presentation transcript:

VIRTUAL NANOLAB BY QUANTUMWISE Presentation by: Sheng Yu Supervisor: Prof. Qiliang Li

Outline: 2. MoS2 monolayer (1) Build structure 1. Download and install Virtual NanoLab 2. MoS2 monolayer (1) Build structure (2) Optimize the structure (3) Change your unit cell (4) Simulate your structure (5) Analyze your results 3. IV curve for MoS2 nanoribbon

Installation http://quantumwise.com/free-trial 1. TRIAL LICENSE

2. DOWNLOAD 3. Installation

Manual for installation http://www.quantumwise.com/documents/manuals/latest/InstallationGuide /InstallationGuide.pdf

2. Simulation on MoS2 monolayer (1) Build your own structure. ① Jobs command window ② The jobs you have already finished ③ The jobs you are going to analyze ④ Analysis window

Find your crystal Unit cell of 3D MoS2

Drag to select right 3 atoms, Press Delete.

Press Ctrl + R: Stretch the unit cell ● Increasing the separation between neighboring layers Press Ctrl + R: (Make the unit cell in the central window)

Center the atoms in the central simulation box The unit cell of 2D MoS2 monolayer

Important! Change your lattice type back into Hexagonal ●Unit cell: the simulation box composes the whole structure. ●Hexagonal: the simulation box repeats infinitely in Hexagonal route.

(2) Optimize your structure Go to Script Generator

Due to 2D nature in A,B direction K-point Sampling nA=9 nB=9 nC=1, Due to 2D nature in A,B direction Spin: Unpolarized (No energy level separation) Polarized (The energy level separation in valence band)

Do not constrain cell Save your Job

Run it!

(3) Change your unit cell ● Changing unit cell is for better later simulation and results display. ● Changing unit cell do not means changing the lattice structure. Drag your structure into Builder

Change the supercell (Coordinate vector) ●Make it into rectangular coordinate Swap Axes ●Make it more transparent appearance

Center your atoms in the simulation box Press Ctrl + R:

Important! Change your lattice type into Simple orthorhombic ● Simple orthorhombic is for rectangular box.

(4) Simulate your structure Go to Script Generator Add your items. ● Physical properties you are interested.

K-point Sampling nA=1 nB=9 nC=9, Due to 2D nature in B, C direction

K space route: G, Y, Z, G ● G(0,0,0) ● Y(0,1,0) ● Z(0,0,1) ● Do not add X(1,0,0) due to 2D nature in B,C direction

(5) See your simulation results!

Band structure for monolayer MoS2 Density of states for monolayer MoS2

Chemical potential for monolayer MoS2 Electron density for monolayer MoS2

Effective mass

Effective mass Direction: [0, 1, 0]: zigzag [0, 0, 1]: armchair Relative band index: 0: Electrons -1: Holes Drag your nc file into Effective Mass Box

3. IV curve for MoS2 nanoribbon Repeat unit cell 5×9 ● Make it into nanoribbon Add electrodes

Device structure Go to Script Generator

Choose: New Calculator Transmission Spectrum 1st New Calculator: K-points 1×1×50 Bias voltage: 0.01V

Increase Maximum steps to 1000 ● Assure Converging

Set the boundary condition: Periodic Dirichlet: The electric potential continues at the boundary Neumann: The electric field continues at the boundary

For the 2ND New Calculator, set the same parameters but different electrode voltage: 0.02V Save and Run!

See your results Your results in Window 3 See your results

Drag your nc file into I-V Curve box

Your results: ● Transmission Spectrum ● Current vs. Voltage Calculated by non-equilibrium Greens function (NEGF)

Transmission spectrum of perfect sheets of graphene and MoS2: http://www.quantumwise.com/publications/tutorials/mini-tutorials/167 Opening a band gap in silicene and bilayer graphene with an electric field: http://www.quantumwise.com/publications/tutorials/mini-tutorials/209 Effective mass of electrons in silicon: http://www.quantumwise.com/publications/tutorials/mini-tutorials/135 Sheng Yu Email: syu12@gmu.edu Phone number: 7036470780 Engineering Building 2602