'Lattice point' presentation slideshows

Solid State Physics (1) Phys3710 Crystal Structure 3 Lecture 3

Solid State Physics (1) Phys3710 Crystal Structure 3 Lecture 3. Department of Physics. Dr Mazen Alshaaer Second semester 2013/2014. Ref.: Prof. Charles W. Myles, Department of Physics, Texas Tech University.

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Homework 3, X-ray diffraction

Homework 3, X-ray diffraction. Homework for chapter 6 (due Monday, Feb. 21). If not stated otherwise, assume l = 0.154 nm (CuK a -radiation) van Holde 6.1 van Holde 6.2a van Holde 6.5 van Holde 6.6 van Holde 6.10

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Homework 3, X-ray diffraction

Homework 3, X-ray diffraction. Homework for chapter 6 (due Monday, Feb. 21). If not stated otherwise, assume l = 0.154 nm (CuK a -radiation) van Holde 6.1 van Holde 6.2a van Holde 6.5 van Holde 6.6 van Holde 6.10

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Lecture 2 The Crystal Structure of Solids

DMT 234 SEMICONDUCTOR PHYSICS & DEVICE. Lecture 2 The Crystal Structure of Solids. Nor Roshidah 2012. SUBTOPIC. Point defect. Line defect. CZ. FZ. Crystal Growth. Si, Ge. Elementary. Frenkel defect. Imperfection Impurities. S/c material. GaAs, GaN InGaN, AlGaAs.

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THIN FILM CHARACTERIZATION TECHNIQUES

THIN FILM CHARACTERIZATION TECHNIQUES. * Optical techniques refers to all regions of the electromagnetic spectrum from IR to X-rays. THIN FILM CHARACTERIZATION TECHNIQUES. Mass, energy, or wavelength of reflected or transmitted particles are measured

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Typical Crystal Structures

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Lecture 2 The Crystal Structure of Solids

DMT 234 Semiconductor Physic & Device. Lecture 2 The Crystal Structure of Solids. Mnorhafiz 2011. DMT 234 Semiconductor Physic & Device. Preview. This topic expalin about basic properties and characteristics of semicondcutor material. Mnorhafiz 2011. DMT 234 Semiconductor Physic & Device.

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Lattice-Based Cryptography

Lattice-Based Cryptography. Cryptographic Hardness Assumptions. Factoring is hard Discrete Log Problem is hard Diffie-Hellman problem is hard Decisional Diffie-Hellman problem is hard Problems involving Elliptic Curves are hard Many assumptions. Why Do We Need More Assumptions?.

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Discrepancy Minimization by Walking on the Edges

Discrepancy Minimization by Walking on the Edges. Raghu Meka (IAS & DIMACS) Shachar Lovett (IAS). Discrepancy. Subsets Color with or - to minimize imbalance. 1 2 3 4 5. 1 2 3 4 5. 3. 1. 1. 0. 1. Discrepancy Examples. Fundamental combinatorial concept.

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MILLER INDICES

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Physical Metallurgy 2nd Lecture

Physical Metallurgy 2nd Lecture. MS&E 410 D.Ast dast@ccmr.cornell.edu 255 4140. Review: Ionic Bonding => electron transfer => ion => Coulomb Covalent => shared electron => localized => directional => exchange interaction

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Space Symmetry I

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Solid state physics

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PH0101 UNIT 4 LECTURE 4

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The Wigner-Seitz Method to Construct a Primitive Cell

A simple, geometric method to construct a Primitive Cell is called the Wigner-Seitz Method . The procedure is:. The Wigner-Seitz Method to Construct a Primitive Cell. 1. Choose a starting lattice point . 2. Draw lines to connect that point to its nearest neighbors.

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Crystal Structure Continued!

Crystal Structure Continued!. NOTE !!

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Introduction to Stochastic Models

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1. Crystal Structure

1. Crystal Structure. Issues that are addressed in this chapter include: Periodic array of atoms Fundamental types of lattices Index system for crystal planes Simple crystal structures Imaging of atomic structure Non-ideal structures. 1.1 Periodic Array of Atoms.

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1. Crystal Structure

1. Crystal Structure. Issues that are addressed in this chapter include: Periodic array of atoms Fundamental types of lattices Index system for crystal planes Simple crystal structures Imaging of atomic structure Non-ideal structures. 1.1 Periodic Array of Atoms.

805 views • 16 slides

Electrostatic Interactions in Proteins Involved in any process where there is movement of charge

Electrostatic Interactions in Proteins Involved in any process where there is movement of charge. Folding Ligand and Ion Binding Ion conduction Proton transfer (pKa) Salt effects, e.g in protein-DNA binding Electron transfer Spectroscopic Transitions.

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