Supporting Information for. Predicting the Stability of Fullerene Allotropes Throughout the Periodic Table MA 02139

Size: px
Start display at page:

Download "Supporting Information for. Predicting the Stability of Fullerene Allotropes Throughout the Periodic Table MA 02139"

Transcription

1 Supporting Information for Predicting the Stability of Fullerene Allotropes Throughout the Periodic Table Qing Zhao 1, 2, Stanley S. H. Ng 1, and Heather J. Kulik 1, * 1 Department of Chemical Engineering, Massachusetts Institute of Technology, Cambridge, MA Department of Mechanical Engineering, Massachusetts Institute of Technology, Cambridge, MA Contents Table S1 Distance cutoffs for A-B bonds Table S2 Electronegativity differences Table S3 Bond distances of A 36 B 36 fullerenes Figure S1 A 36 B 36 nanoparticles Table S4 CN of A 36 B 36 nanoparticles Figure S2 Stability analysis of A 36 B 36 fullerenes Method S1 Build A 72 fullerenes Figure S3 HOMO-LUMO gaps of A 36 B 36 fullerenes Table S5 Experimental band gap of crystals Figure S4 HOMO, LUMO of A 36 B 36 fullerenes Table S6 CB, VB of A 36 B 36 fullerenes Figure S5 PDOS of A 36 B 36 fullerenes Figure S6 HOMO LUMO gaps of A and B atoms versus A 36 B 36 fullerenes Figure S7 Charge of A 36 B 36 fullerenes Figure S8 Charge analysis of A 36 B 36 fullerenes Table S7 Bond distances of A 28 B 28 fullerenes Table S8 Bond distances of A 30 B 30 fullerenes Table S9 Energy of A 28 B 28, A 30 B 30 fullerenes Method S2 Build A 60 fullerenes Text S3 Summary of acronyms Page S2 Page S2 Page S2 Page S3 Page S3 Page S4 Page S5 Page S6 Page S6 Page S7 Page S8 Page S9 Page S10 Page S10 Page S11 Page S11 Page S12 Page S13 Page S13 Page S14 Supporting Information for Fullerene allotropes Page S1

2 Table S1. Distances cutoffs for different A-B bonds in A. III-V N P As II-VI S Se B Zn Al Cd Ga In Table S2. Unitless Pauling electronegativity differences. III-V N P As II-VI S Se B Zn Al Cd Ga In Table S3. Comparisons of bond distances of A 36 B 36 fullerenes in A before and after geometry optimizations. BN AlN GaN InN BP AlP GaP InP Before After BAs AlAs GaAs InAs ZnS CdS ZnSe CdSe Before After Supporting Information for Fullerene allotropes Page S2

3 Figure S1. Symmetric nanoparticle models for nitrogen-containing III-V group compounds (left) and symmetric nanoparticle models for phosphorus-, arsenic-containing III-V group and II-VI group compounds (right). Table S4. Coordination number of geometry-optimized A 36 B 36 spherical nanoparticles. III-V N P As II-VI S Se B Zn Al Cd Ga In Supporting Information for Fullerene allotropes Page S3

4 Figure S2. Relationship between relative energy per pair of AB atoms in kcal/mol of A 36 B 36 fullerenes and materials properties: sum of A and B atoms atomic numbers or covalent radii, A- B bond distances of geometry-optimized A 36 B 36 fullerenes, and Pauling electronegativity differences between B and A atoms of III-V (green cycles) and II-VI (orange cycles) materials. Supporting Information for Fullerene allotropes Page S4

5 Method S1. Details of computing the relative stabilities of the homogeneous A 72 (A=C, Si, Ge) fullerenes. We also used the B 36 N 36 fullerene geometry obtained with the CRYSTAL14 package as a starting point to generate all A 72 fullerenes, and the only difference is replacing both B and N atoms by A atoms. The A 72 spherical nanoparticles (NP) are cut from their bulk face-centered diamond-cubic crystal structures. We conducted geometry optimizations on both A 72 fullerenes and A 72 nanoparticles to get the local minimum structures. We define a relative energy per A 2 atoms in optimized A 72 fullerenes (E(FL)) with respect to those in the optimized NP (E(NP)), for consistency with per pair of A, B atoms in A 36 B 36 fullerenes: E per A2 = E(FL) 36 E(NP) 36 (1) Supporting Information for Fullerene allotropes Page S5

6 Figure S3. Comparison of HOMO-LUMO gaps (in ev) of geometry-optimized A 36 B 36 fullerenes from III-V and II-VI materials obtained with ωpbeh (blue cycles) and B3LYP (red cycles). The default B3LYP definition in TeraChem uses the VWN1-RPA form for the local density approximation component of the correlation. Table S5: experimental band gaps of III-V and II-VI bulk crystal structures in ev. N P As S Se B Zn Al Cd Ga In Supporting Information for Fullerene allotropes Page S6

7 Figure S4: Cation (red) and anion (blue) element dependence of the individual HOMO and LUMO eigenvalues. The gray box represents the symbols from light to heavy atoms. Supporting Information for Fullerene allotropes Page S7

8 Table S6. Contributions of s, p, d orbitals of cation (A) and anion (B) atoms in valence band (VB) and conduction band (CB) of A 36 B 36 fullerenes. VB CB A-s A-p A-d B-s B-p A-s A-p A-d B-s B-p BN BP BAs AlN AlP AlAs GaN GaP GaAs InN InP InAs ZnS ZnSe CdS CdSe Supporting Information for Fullerene allotropes Page S8

9 Figure S5. Total density of states (TDOS) (black line) and orbital projected density of states (PDOS) of A atom s orbital (red solid line), A atom p orbital (red dashed line), A atom d orbital (red dashdot line), B atom s orbital (blue solid line) and B atom p orbital (blue dashed line) for (a) A=aluminum (b) A=indium (c) B=arsenic (d) II-VI fullerenes. The dominant orbitals in valence band and conduction band are indicated with light blue and light red shaded regions. The gray solid lines, green and orange dashed lines show the shifts of TDOS peaks and dominant orbitals peaks in PDOS of both the CB and VB. The brown dashed lines indicate the positions of the HOMO and LUMO. Supporting Information for Fullerene allotropes Page S9

10 Figure S6. Comparison of A 36 B 36 fullerene HOMO-LUMO gaps to the HOMO-LUMO gaps (all in ev) of individual A-type and B-type atoms following the same series as in Figure 5 in the main text. Figure S7. Charge on A (red) and B (blue) atoms from NBO analysis for A 36 B 36 fullerenes from III-V (dot) and II-VI (square) materials. Supporting Information for Fullerene allotropes Page S10

11 Figure S8. The relationship between the charge transfer from A atom to B atom of A 36 B 36 fullerenes given by NBO analysis from III-V (green dots) and II-VI (orange dots) materials. A linear best fit line (gray dashed) is also shown. Table S7. Comparisons of bond distances of A 28 B 28 fullerenes in A before and after geometry optimizations. BN AlN GaN InN BP AlP GaP InP Before After BAs AlAs GaAs InAs ZnS CdS ZnSe CdSe Before After Supporting Information for Fullerene allotropes Page S11

12 Table S8. Comparisons of bond distances of A 30 B 30 fullerenes in A before and after geometry optimizations. Before After A-B A-A B-B A-B BN BP BAs AlN AlP AlAs GaN GaP GaAs InN InP InAs ZnS ZnSe CdS CdSe Supporting Information for Fullerene allotropes Page S12

13 Table S9. Relative energy per pair of AB atoms in kcal/mol of geometry optimized A 28 B 28 fullerenes and A 30 B 30 fullerenes with respect to A 36 B 36 fullerenes from III-V and II-VI materials. BN BP BAs AlN AlP AlAs GaN GaP E(A 28 B 28 ) E(A 30 B 30 ) GaAs InN InP InAs ZnS ZnSe CdS CdSe E(A 28 B 28 ) E(A 30 B 30 ) Method S2. Details of obtaining the correlation between relative stabilities of the homogeneous A 60 (A=C, Si, Ge) fullerenes with respect to A 72 fullerenes and the ring-derived energy penalty differences. We used the C 60 fullerene geometry obtained from fullerene library as a starting point to generate all A 60 (A=C, Si, Ge) fullerenes, and screening the bond distances in the range of ±0.5 A around the experimental bond distances to get their optimal bond distances. We then conducted geometry optimizations on A 60 fullerenes to get the local minimum structures and defined a relative energy per A 2 atoms in optimized A 60 fullerenes (E(A 60 )) with respect to those in the optimized A 72 fullerenes we obtained before (E(A 72 )): E per A2 = E(A 60 ) 30 E(A 72 ) 36 (2) 4 The energy penalties of four-membered rings ( E penalty computed as follows: 5 ) and five-membered rings ( E penalty ) are 4 E penalty = 4 E(A H ) E(A 6 H 6 ) 6 (3), Supporting Information for Fullerene allotropes Page S13

14 5 E penalty = 5 E(A 5H 5 ) 5 E(A 6H 6 ) 6 (4) where E(A 4 H 4 ), E(A 5 H 5 ), and E(A 6 H 6 ) are the energies of optimized A 4 H 4 four-membered ring molecules, A 5 H 5 five-membered ring molecules, and A 6 H 6 six-membered ring molecules. The relative penalties for A 60 and A 72 fullerenes are calculated as a weighted difference in the number of unfavorable rings on a per-pair of atom basis: ΔE penalty = 12E 5 penalty 30 6E 4 penalty 36 (5) Method S3: Summary of acronyms A n B n : A is a cationic element (B, Al, Ga, or In in III-V materials), B is the anionic element (N, P, or As in III-V materials), and n is the number of atoms of each in materials described in this work. DFT: density functional theory LACVP*: A composite basis set from the Los Alamos LANLDZ effective core potential and the 6-31G* basis for lighter atoms. CNs: coordination numbers d cut (A B): cutoff for an A-b bond. A r cov : covalent (cov) radius of atom A. NBO: natural bond orbital NAO: natural atomic orbital PDOS: projected density of states σ: Gaussian broadening parameter in Hartrees (Ha). NPs: nanaoparticles Supporting Information for Fullerene allotropes Page S14

15 FL: fullerene E(FL): energy of a fullerene. Δχ B-A : unitless Pauling electronegativity difference. Δ-SCF: a method for computing band gaps from total energy differences after adding or removing an electron. HOMO: highest occupied molecular orbital LUMO: lowest unoccupied molecular orbital ω: range separation parameter in a hybrid functional ε HOMO : HOMO eigenvalue B3LYP: a hybrid exchange functional with Becke exchange and Lee-Yang-Parr correlation. ωpbeh: a range-separated hybrid with Perdew Burke Ernzerhof plus hybrid exchange PBE: Perdew Burke Ernzerhof functional 0D: isolated, not periodic system, e.g. a fullerene. CB: conduction band VB: valence band DOS: total density of states q A-B : charge transfer from A to B atoms. Bond A : extent of bonding character A atom contributes to A-B bonds. 4 E penalty : penalty for a four-membered ring model with respect to a six-membered ring model. n 4, n 5, n 6 are number of four-, five-, six-membered rings in the fullerenes. β: an overall descriptor (equation 11 main text). Supporting Information for Fullerene allotropes Page S15

Predicting the Stability of Fullerene Allotropes Throughout the Periodic Table

Predicting the Stability of Fullerene Allotropes Throughout the Periodic Table Predicting the Stability of Fullerene Allotropes Throughout the Periodic Table The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation

More information

Electronegativity is a very useful concept for the explanation or understanding of chemical reactivity throughout the periodic table.

Electronegativity is a very useful concept for the explanation or understanding of chemical reactivity throughout the periodic table. 1.6. Review of Electronegativity (χ) CONCEPT: Electronegativity is a very useful concept for the explanation or understanding of chemical reactivity throughout the periodic table. There are many definitions

More information

Ga and P Atoms to Covalent Solid GaP

Ga and P Atoms to Covalent Solid GaP Ga and P Atoms to Covalent Solid GaP Band Gaps in Binary Group III-V Semiconductors Mixed Semiconductors Affect of replacing some of the As with P in GaAs Band Gap (ev) (nm) GaAs 1.35 919 (IR) GaP 2.24

More information

MO s in one-dimensional arrays of like orbitals

MO s in one-dimensional arrays of like orbitals MO s in one-dimensional arrays of like orbitals There will be as many MO s as orbitals in the array. Every molecular orbital is characterized by a specific pattern of nodes, The lowest energy orbital will

More information

The Periodic Table and Chemical Reactivity

The Periodic Table and Chemical Reactivity The and Chemical Reactivity Noble gases Less electronegative elements More electronegative elements Then what is electronegativity? The tendency of an atom to attract an electron (or electron density)

More information

Periodic Trends in Properties of Homonuclear

Periodic Trends in Properties of Homonuclear Chapter 8 Periodic Trends in Properties of Homonuclear Diatomic Molecules Up to now, we have discussed various physical properties of nanostructures, namely, two-dimensional - graphene-like structures:

More information

Chapter 1 Overview of Semiconductor Materials and Physics

Chapter 1 Overview of Semiconductor Materials and Physics Chapter 1 Overview of Semiconductor Materials and Physics Professor Paul K. Chu Conductivity / Resistivity of Insulators, Semiconductors, and Conductors Semiconductor Elements Period II III IV V VI 2 B

More information

Basic cell design. Si cell

Basic cell design. Si cell Basic cell design Si cell 1 Concepts needed to describe photovoltaic device 1. energy bands in semiconductors: from bonds to bands 2. free carriers: holes and electrons, doping 3. electron and hole current:

More information

Australian Journal of Basic and Applied Sciences

Australian Journal of Basic and Applied Sciences AENSI Journals Australian Journal of Basic and Applied Sciences ISSN:1991-8178 Journal home page: www.ajbasweb.com Theoretical Study for the Effect of Hydroxyl Radical on the Electronic Properties of Cyclobutadiene

More information

We have arrived to the question: how do molecular bonds determine the band gap? We have discussed that the silicon atom has four outer electrons.

We have arrived to the question: how do molecular bonds determine the band gap? We have discussed that the silicon atom has four outer electrons. ET3034Tux - 2.2.2 - Band Gap 2 - Electrons in Molecular Bonds We have arrived to the question: how do molecular bonds determine the band gap? We have discussed that the silicon atom has four outer electrons.

More information

Atomic Models for Anionic Ligand Passivation of Cation- Rich Surfaces of IV-VI, II-VI, and III-V Colloidal Quantum Dots

Atomic Models for Anionic Ligand Passivation of Cation- Rich Surfaces of IV-VI, II-VI, and III-V Colloidal Quantum Dots Electronic Supplementary Material (ESI) for ChemComm. This journal is The Royal Society of Chemistry 2016 Electronic Supplementary Information Atomic Models for Anionic Ligand Passivation of Cation- Rich

More information

Physical Properties of Mono-layer of

Physical Properties of Mono-layer of Chapter 3 Physical Properties of Mono-layer of Silicene The fascinating physical properties[ 6] associated with graphene have motivated many researchers to search for new graphene-like two-dimensional

More information

per unit cell Motif: Re at (0, 0, 0); 3O at ( 1 / 2, 0), (0, 0, 1 / 2 ) Re: 6 (octahedral coordination) O: 2 (linear coordination) ReO 6

per unit cell Motif: Re at (0, 0, 0); 3O at ( 1 / 2, 0), (0, 0, 1 / 2 ) Re: 6 (octahedral coordination) O: 2 (linear coordination) ReO 6 Lattice: Primitive Cubic 1ReO 3 per unit cell Motif: Re at (0, 0, 0); 3O at ( 1 / 2, 0, 0), (0, 1 / 2, 0), (0, 0, 1 / 2 ) Re: 6 (octahedral coordination) O: 2 (linear coordination) ReO 6 octahedra share

More information

Theoretical and experimental factors affecting measurements of semiconductor mean inner potentials

Theoretical and experimental factors affecting measurements of semiconductor mean inner potentials Journal of Physics: Conference Series Theoretical and experimental factors affecting measurements of semiconductor mean inner potentials Recent citations - Mapping Charge Distribution in Single PbS Core

More information

Pseudopotentials for hybrid density functionals and SCAN

Pseudopotentials for hybrid density functionals and SCAN Pseudopotentials for hybrid density functionals and SCAN Jing Yang, Liang Z. Tan, Julian Gebhardt, and Andrew M. Rappe Department of Chemistry University of Pennsylvania Why do we need pseudopotentials?

More information

DFT EXERCISES. FELIPE CERVANTES SODI January 2006

DFT EXERCISES. FELIPE CERVANTES SODI January 2006 DFT EXERCISES FELIPE CERVANTES SODI January 2006 http://www.csanyi.net/wiki/space/dftexercises Dr. Gábor Csányi 1 Hydrogen atom Place a single H atom in the middle of a largish unit cell (start with a

More information

Supporting Information: Local Electronic Structure of a Single-Layer. Porphyrin-Containing Covalent Organic Framework

Supporting Information: Local Electronic Structure of a Single-Layer. Porphyrin-Containing Covalent Organic Framework Supporting Information: Local Electronic Structure of a Single-Layer Porphyrin-Containing Covalent Organic Framework Chen Chen 1, Trinity Joshi 2, Huifang Li 3, Anton D. Chavez 4,5, Zahra Pedramrazi 2,

More information

New Volleyballenes: Y 20 C 60, La 20 C 60, and Lu 20 C 60

New Volleyballenes: Y 20 C 60, La 20 C 60, and Lu 20 C 60 New Volleyballenes: Y 20 C 60, La 20 C 60, and Lu 20 C 60 Jing Wang a and Ying Liu*,a,b a Department of Physics and Hebei Advanced Thin Film Laboratory, Hebei Normal University, Shijiazhuang 050016, Hebei,

More information

Valence bond theory accounts, at least qualitatively, for the stability of the covalent bond in terms of overlapping atomic orbitals.

Valence bond theory accounts, at least qualitatively, for the stability of the covalent bond in terms of overlapping atomic orbitals. Molecular Orbital Theory Valence bond theory accounts, at least qualitatively, for the stability of the covalent bond in terms of overlapping atomic orbitals. Using the concept of hybridization, valence

More information

Density Functional Theory (DFT) modelling of C60 and

Density Functional Theory (DFT) modelling of C60 and ISPUB.COM The Internet Journal of Nanotechnology Volume 3 Number 1 Density Functional Theory (DFT) modelling of C60 and N@C60 N Kuganathan Citation N Kuganathan. Density Functional Theory (DFT) modelling

More information

Linking electronic and molecular structure: Insight into aqueous chloride solvation. Supplementary Information

Linking electronic and molecular structure: Insight into aqueous chloride solvation. Supplementary Information Linking electronic and molecular structure: Insight into aqueous chloride solvation Ling Ge, Leonardo Bernasconi, and Patricia Hunt Department of Chemistry, Imperial College London, London SW7 2AZ, United

More information

Density Functional Theory Calculation of the Electronic Structure for C 20 Cage Fullerene حسابات نظرية دالة الكثافة للتركيب االلكتروني للفوليرين C 20

Density Functional Theory Calculation of the Electronic Structure for C 20 Cage Fullerene حسابات نظرية دالة الكثافة للتركيب االلكتروني للفوليرين C 20 Density Functional Theory Calculation of the Electronic Structure for C 20 Cage Fullerene حسابات نظرية دالة الكثافة للتركيب االلكتروني للفوليرين C 20 محمد اف ارح هادي هاشم نضال هادي طالب ليث عبيس اب ارهيم

More information

Cohesive energy of zinc blende (A III B V and A II B VI ) structured solids

Cohesive energy of zinc blende (A III B V and A II B VI ) structured solids Cohesive energy of zinc blende (A III B V and A II B VI ) structured solids A. S. Verma *,1, B. K. Sarkar 2 and V. K. Jindal 1 1 Department of Physics, Panjab University, Chandigarh, (India), 160014 2

More information

Introduction to Chemical Bonding Chemical Bond

Introduction to Chemical Bonding Chemical Bond Introduction to Chemical Bonding Chemical Bond Mutual attraction between the and electrons of different atoms that binds the atoms together. Ionic Bond o that results from the attraction between large

More information

Improved Electronic Structure and Optical Properties of sp-hybridized Semiconductors Using LDA+U SIC

Improved Electronic Structure and Optical Properties of sp-hybridized Semiconductors Using LDA+U SIC 286 Brazilian Journal of Physics, vol. 36, no. 2A, June, 2006 Improved Electronic Structure and Optical Properties of sp-hybridized Semiconductors Using LDA+U SIC Clas Persson and Susanne Mirbt Department

More information

Midterm I Results. Mean: 35.5 (out of 100 pts) Median: 33 Mode: 25 Max: 104 Min: 2 SD: 18. Compare to: 2013 Mean: 59% 2014 Mean: 51%??

Midterm I Results. Mean: 35.5 (out of 100 pts) Median: 33 Mode: 25 Max: 104 Min: 2 SD: 18. Compare to: 2013 Mean: 59% 2014 Mean: 51%?? Midterm I Results Mean: 35.5 (out of 100 pts) Median: 33 Mode: 25 Max: 104 Min: 2 SD: 18 Compare to: 2013 Mean: 59% 2014 Mean: 51%?? Crystal Thermodynamics and Electronic Structure Chapter 7 Monday, October

More information

Rodhwan Salem D.S Idkhil (Magister of Physics/ Faculty of Sciences/ Brawijaya University, Malang, Indonesia)

Rodhwan Salem D.S Idkhil (Magister of Physics/ Faculty of Sciences/ Brawijaya University, Malang, Indonesia) IOSR Journal of Applied Physics (IOSR-JAP) e-issn: 2278-4861.Volume 7, Issue 1 Ver. III (Jan.-Feb. 2015), PP 11-17 www.iosrjournals.org Study Electronic And Mechanical Properties Of Carbon, Silicon, And

More information

Crystals, packings etc.

Crystals, packings etc. Crystals, packings etc. Ram Seshadri MRL 2031, x6129, seshadri@mrl.ucsb.edu These notes complement chapter 6 of Anderson, Leaver, Leevers and Rawlings Bond Distances We have seen that in the P-cubic structure,

More information

Supplemental Material: Experimental and Theoretical Investigations of the Electronic Band Structure of Metal-Organic Framework of HKUST-1 Type

Supplemental Material: Experimental and Theoretical Investigations of the Electronic Band Structure of Metal-Organic Framework of HKUST-1 Type Supplemental Material: Experimental and Theoretical Investigations of the Electronic Band Structure of Metal-Organic Framework of HKUST-1 Type Zhigang Gu, a Lars Heinke, a,* Christof Wöll a, Tobias Neumann,

More information

need another quantum number, m s it is found that atoms, substances with unpaired electrons have a magnetic moment, 2 s(s+1) where {s = m s }

need another quantum number, m s it is found that atoms, substances with unpaired electrons have a magnetic moment, 2 s(s+1) where {s = m s } M polyelectronic atoms need another quantum number, m s it is found that atoms, substances with unpaired electrons have a magnetic moment, 2 s(s+1) where {s = m s } Pauli Exclusion Principle no two electrons

More information

Journal of Computational Methods in Molecular Design, 2013, 3 (1):1-8. Scholars Research Library (

Journal of Computational Methods in Molecular Design, 2013, 3 (1):1-8. Scholars Research Library ( Journal of Computational Methods in Molecular Design, 2013, 3 (1):1-8 Scholars Research Library (http://scholarsresearchlibrary.com/archive.html) ISSN : 2231-3176 CODEN (USA): JCMMDA Theoretical study

More information

EECS143 Microfabrication Technology

EECS143 Microfabrication Technology EECS143 Microfabrication Technology Professor Ali Javey Introduction to Materials Lecture 1 Evolution of Devices Yesterday s Transistor (1947) Today s Transistor (2006) Why Semiconductors? Conductors e.g

More information

ELEMENTARY BAND THEORY

ELEMENTARY BAND THEORY ELEMENTARY BAND THEORY PHYSICIST Solid state band Valence band, VB Conduction band, CB Fermi energy, E F Bloch orbital, delocalized n-doping p-doping Band gap, E g Direct band gap Indirect band gap Phonon

More information

Electronic Supplementary Information

Electronic Supplementary Information Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2014 Electronic Supplementary Information Rational modifications on champion porphyrin

More information

Earth Materials I Crystal Structures

Earth Materials I Crystal Structures Earth Materials I Crystal Structures Isotopes same atomic number, different numbers of neutrons, different atomic mass. Ta ble 1-1. Su mmar y of quantu m num bers Name Symbol Values Principal n 1, 2,

More information

Explaining the apparent arbitrariness of the LDA-1/2 self-energy. correction method applied to purely covalent systems

Explaining the apparent arbitrariness of the LDA-1/2 self-energy. correction method applied to purely covalent systems Explaining the apparent arbitrariness of the LDA-1/2 self-energy correction method applied to purely covalent systems Kan-Hao Xue, 1,2 Leonardo R. C. Fonseca, 3 and Xiang-Shui Miao 1,2 1 School of Optical

More information

Lecture 2: Bonding in solids

Lecture 2: Bonding in solids Lecture 2: Bonding in solids Electronegativity Van Arkel-Ketalaar Triangles Atomic and ionic radii Band theory of solids Molecules vs. solids Band structures Analysis of chemical bonds in Reciprocal space

More information

1. Binary III-V compounds 2 p From which atoms are the 16 binary III-V compounds formed?...column III B, Al, Ga and In...column V N, P, As and Sb...

1. Binary III-V compounds 2 p From which atoms are the 16 binary III-V compounds formed?...column III B, Al, Ga and In...column V N, P, As and Sb... PROBLEMS part B, Semiconductor Materials. 2006 1. Binary III-V compounds 2 p From which atoms are the 16 binary III-V compounds formed?...column III B, Al, Ga and In...column V N, P, As and Sb... 2. Semiconductors

More information

Electronic structures of one-dimension carbon nano wires and rings

Electronic structures of one-dimension carbon nano wires and rings IOP Publishing Journal of Physics: Conference Series 61 (2007) 252 256 doi:10.1088/1742-6596/61/1/051 International Conference on Nanoscience and Technology (ICN&T 2006) Electronic structures of one-dimension

More information

Earth Solid Earth Rocks Minerals Atoms. How to make a mineral from the start of atoms?

Earth Solid Earth Rocks Minerals Atoms. How to make a mineral from the start of atoms? Earth Solid Earth Rocks Minerals Atoms How to make a mineral from the start of atoms? Formation of ions Ions excess or deficit of electrons relative to protons Anions net negative charge Cations net

More information

Ionic Bonding. Example: Atomic Radius: Na (r = 0.192nm) Cl (r = 0.099nm) Ionic Radius : Na (r = 0.095nm) Cl (r = 0.181nm)

Ionic Bonding. Example: Atomic Radius: Na (r = 0.192nm) Cl (r = 0.099nm) Ionic Radius : Na (r = 0.095nm) Cl (r = 0.181nm) Ionic Bonding Ion: an atom or molecule that gains or loses electrons (acquires an electrical charge). Atoms form cations (+charge), when they lose electrons, or anions (- charge), when they gain electrons.

More information

Valence Bond Theory Considers the interaction of separate atoms brought together as they form a molecule. Lewis structures Resonance considerations

Valence Bond Theory Considers the interaction of separate atoms brought together as they form a molecule. Lewis structures Resonance considerations CHEM 511 chapter 2 page 1 of 11 Chapter 2 Molecular Structure and Bonding Read the section on Lewis dot structures, we will not cover this in class. If you have problems, seek out a general chemistry text.

More information

Statistical learning for alloy design from electronic structure calculations

Statistical learning for alloy design from electronic structure calculations Graduate Theses and Dissertations Iowa State University Capstones, Theses and Dissertations 2009 Statistical learning for alloy design from electronic structure calculations Scott Broderick Iowa State

More information

Relation Between Refractive Index, Micro Hardness and Bulk Modulus of A II B VI and A III B V Semiconductors

Relation Between Refractive Index, Micro Hardness and Bulk Modulus of A II B VI and A III B V Semiconductors International Journal of Pure and Applied Physics ISSN 0973-1776 Volume 5, Number 3 (2009), pp. 271-276 Research India Publications http://www.ripublication.com/ijpap.htm Relation Between Refractive Index,

More information

Introduction to Engineering Materials ENGR2000. Dr.Coates

Introduction to Engineering Materials ENGR2000. Dr.Coates Introduction to Engineering Materials ENGR2000 Chapter 18: Electrical Properties Dr.Coates 18.2 Ohm s Law V = IR where R is the resistance of the material, V is the voltage and I is the current. l R A

More information

Memorize: Understand: Know how to:

Memorize: Understand: Know how to: NAME: CLASS PERIOD: REVIEW FOR HONORS CHEMISTRY SEMESTER 1 EXAM Memorize: Understand: Know how to: 1 SI units for different measurements (length, volume, number, mass, temperature, density) Definition

More information

NH 3 H 2 O N 2. Why do they make chemical bonds? Molecular Orbitals

NH 3 H 2 O N 2. Why do they make chemical bonds? Molecular Orbitals N 2 NH 3 H 2 O Why do they make chemical bonds? 5 Molecular Orbitals Why do they make chemical bonds? Stabilization Bond energy Types of Chemical Bonds Metallic Bond Ionic Bond Covalent Bond Covalent Bond

More information

: Bond Order = 1.5 CHAPTER 5. Practice Questions

: Bond Order = 1.5 CHAPTER 5. Practice Questions CAPTER 5 Practice Questions 5.1 5.3 S 5.5 Ethane is symmetrical, so does not have a dipole moment. owever, ethanol has a polar group at one end and so has a dipole moment. 5.7 xygen has the valence electron

More information

with cubic symmetry Supplementary Material

with cubic symmetry Supplementary Material Prediction uncertainty of density functional approximations for properties of crystals with cubic symmetry Supplementary Material Pascal Pernot,,, Bartolomeo Civalleri, Davide Presti, and Andreas Savin,

More information

Teoría del Funcional de la Densidad (Density Functional Theory)

Teoría del Funcional de la Densidad (Density Functional Theory) Teoría del Funcional de la Densidad (Density Functional Theory) Motivation: limitations of the standard approach based on the wave function. The electronic density n(r) as the key variable: Functionals

More information

Unified theory of the direct or indirect bandgap nature of. conventional semiconductors

Unified theory of the direct or indirect bandgap nature of. conventional semiconductors Unified theory of the direct or indirect bandgap nature of conventional semiconductors Lin-Ding Yuan 1,2, Hui-Xiong Deng 1,2, Shu-Shen Li 1,2,3, Jun-Wei Luo 1,2,3*, and Su-Huai Wei 4* 1 State key laboratory

More information

Which of the following chemical elements corresponds to the symbol Cu?

Which of the following chemical elements corresponds to the symbol Cu? Which of the following chemical elements corresponds to the symbol Cu? A) copper B) gold C) lead D) silver E) none of the above Which of the following chemical elements corresponds to the symbol Cu? A)

More information

Supporting Information. Don-Hyung Ha, Liane M. Moreau, Clive R. Bealing, Haitao Zhang, Richard G. Hennig, and. Richard D.

Supporting Information. Don-Hyung Ha, Liane M. Moreau, Clive R. Bealing, Haitao Zhang, Richard G. Hennig, and. Richard D. Supporting Information The structural evolution and diffusion during the chemical transformation from cobalt to cobalt phosphide nanoparticles Don-Hyung Ha, Liane M. Moreau, Clive R. Bealing, Haitao Zhang,

More information

3/23/2010 More basics of DFT Kieron Burke and friends UC Irvine Physics and Chemistry References for ground-state DFT ABC of DFT, by KB and Rudy Magyar, http://dft.uci.edu A Primer in Density Functional

More information

Valence electrons octet rule. Lewis structure Lewis structures

Valence electrons octet rule. Lewis structure Lewis structures Lewis Dot Diagrams Valence electrons are the electrons in the outermost energy level of an atom. An element with a full octet of valence electrons has a stable configuration. The tendency of bonded atoms

More information

Worksheet 5 - Chemical Bonding

Worksheet 5 - Chemical Bonding Worksheet 5 - Chemical Bonding The concept of electron configurations allowed chemists to explain why chemical molecules are formed from the elements. In 1916 the American chemist Gilbert Lewis proposed

More information

Ceramic Bonding. CaF 2 : large SiC: small

Ceramic Bonding. CaF 2 : large SiC: small Recall ceramic bonding: - Mixed ionic and covalent. - % ionic character ( f ) increases with difference in electronegativity Large vs small ionic bond character: Ceramic Bonding CaF : large SiC: small

More information

Name PRACTICE Unit 3: Periodic Table

Name PRACTICE Unit 3: Periodic Table 1. Compared to the atoms of nonmetals in Period 3, the atoms of metals in Period 3 have (1) fewer valence electrons (2) more valence electrons (3) fewer electron shells (4) more electron shells 2. On the

More information

Electron Emission from Diamondoids: a DMC Study. Neil D. Drummond Andrew J. Williamson Richard J. Needs and Giulia Galli

Electron Emission from Diamondoids: a DMC Study. Neil D. Drummond Andrew J. Williamson Richard J. Needs and Giulia Galli Electron Emission from Diamondoids: a DMC Study Neil D. Drummond Andrew J. Williamson Richard J. Needs and Giulia Galli October 18, 2005 1 Semiconductor Nanoparticles for Optoelectronic Devices (I) The

More information

Chem 115: Chapter 9 Dr. Babb

Chem 115: Chapter 9 Dr. Babb Periodic Properties of the Atom Properties that depend on position of element in the periodic table. Factors that affect the periodic properties: 1. Principal quantum number of valence shell (n valence

More information

LN 3 IDLE MIND SOLUTIONS

LN 3 IDLE MIND SOLUTIONS IDLE MIND SOLUTIONS 1. Let us first look in most general terms at the optical properties of solids with band gaps (E g ) of less than 4 ev, semiconductors by definition. The band gap energy (E g ) can

More information

Practical calculations with the GW approximation and Bethe-Salpeter equation in BerkeleyGW

Practical calculations with the GW approximation and Bethe-Salpeter equation in BerkeleyGW Practical calculations with the GW approximation and Bethe-Salpeter equation in BerkeleyGW David A. Strubbe Department of Physics, University of California, Merced Benasque, Spain 23 August 2018 Band gaps:

More information

Biotech 2: Atoms and Molecules OS Text Reading pp Electron cloud Atoms & Nucleus 2e Subatomic Particles Helium Electron cloud

Biotech 2: Atoms and Molecules OS Text Reading pp Electron cloud Atoms & Nucleus 2e Subatomic Particles Helium Electron cloud 9/4/017 Biotech : Atoms and Molecules OS Text Reading pp. 34-4 Atoms & Subatomic Particles Nucleus Helium e cloud cloud e Protons Neutrons Mass number = 4 s Nucleus Carbon atomic number = # of protons

More information

Chapter 6 Chemical Bonding

Chapter 6 Chemical Bonding Chapter 6 Chemical Bonding Section 6-1 Introduction to Chemical Bonding Chemical Bonds Valence electrons are attracted to other atoms, and that determines the kind of chemical bonding that occurs between

More information

Semiconductor Device Physics

Semiconductor Device Physics 1 Semiconductor Device Physics Lecture 1 http://zitompul.wordpress.com 2 0 1 3 2 Semiconductor Device Physics Textbook: Semiconductor Device Fundamentals, Robert F. Pierret, International Edition, Addison

More information

Journal of Chemical and Pharmaceutical Research

Journal of Chemical and Pharmaceutical Research Available on line www.jocpr.com Journal of Chemical and Pharmaceutical Research ISSN No: 0975-7384 CODEN(USA): JCPRC5 J. Chem. Pharm. Res., 2011, 3(4): 589-595 Altering the electronic properties of adamantane

More information

The GW Approximation. Manish Jain 1. July 8, Department of Physics Indian Institute of Science Bangalore 1/36

The GW Approximation. Manish Jain 1. July 8, Department of Physics Indian Institute of Science Bangalore 1/36 1/36 The GW Approximation Manish Jain 1 Department of Physics Indian Institute of Science Bangalore July 8, 2014 Ground-state properties 2/36 Properties that are intrinsic to a system with all its electrons

More information

Re-evaluating CeO 2 Expansion Upon Reduction: Non-counterpoised Forces, Not Ionic Radius Effects, are the Cause

Re-evaluating CeO 2 Expansion Upon Reduction: Non-counterpoised Forces, Not Ionic Radius Effects, are the Cause Re-evaluating CeO 2 Expansion Upon Reduction: Non-counterpoised Forces, Not Ionic Radius Effects, are the Cause Christopher L. Muhich, a* a ETH Zurich, Department of Mechanical and Process Engineering,

More information

Introduction. Atom is made up of protons, electrons and neutrons. Electrons revolving in concentric circles around nucleus in fixed orbitals

Introduction. Atom is made up of protons, electrons and neutrons. Electrons revolving in concentric circles around nucleus in fixed orbitals Chemistry of life Introduction Atom is made up of protons, electrons and neutrons Electrons revolving in concentric circles around nucleus in fixed orbitals Electron Orbital (energy level) Chemical bonding

More information

Lecture 4: Band theory

Lecture 4: Band theory Lecture 4: Band theory Very short introduction to modern computational solid state chemistry Band theory of solids Molecules vs. solids Band structures Analysis of chemical bonding in Reciprocal space

More information

CHEM 101: CHAPTER 11: CHEMICAL BONDS: THE FORMATION OF COMPOUNDS FROM ATOMS

CHEM 101: CHAPTER 11: CHEMICAL BONDS: THE FORMATION OF COMPOUNDS FROM ATOMS 1 CHEM 101: CHAPTER 11: CHEMICAL BONDS: THE FORMATION OF COMPOUNDS FROM ATOMS PERIODIC TRENDS: See pages 214-216, 221 Table 11.3, and 227 + 228 of text. Lewis Structures of Atoms: The Lewis Dot Diagram

More information

College of Science, Xi an University of Science and Technology, Xi an *Corresponding author

College of Science, Xi an University of Science and Technology, Xi an *Corresponding author 2016 International Conference on Advanced Manufacture Technology and Industrial Application (AMTIA 2016) ISBN: 978-1-60595-387-8 The Study of Coordination Adsorption Effect that CO Adsorption on 4H-SiC

More information

Lewis Dot Symbols. The Octet Rule ATOMS TEND TO GAIN, LOSE, or SHARE ELECTRONS to ATTAIN A FILLED OUTER SHELL of 8 ELECTRONS.

Lewis Dot Symbols. The Octet Rule ATOMS TEND TO GAIN, LOSE, or SHARE ELECTRONS to ATTAIN A FILLED OUTER SHELL of 8 ELECTRONS. Chapter 9, Part 1 Models of Chemical Bonding Recall Chapter 2: Chemical bonds hold atoms together in a compound. transfer of electrons, forming cations and anions, results in ionic bonding sharing of electron

More information

Trends in Atomic Size. Atomic Radius-one half the distance between the nuclei of two atoms of the same element when the atoms are joined

Trends in Atomic Size. Atomic Radius-one half the distance between the nuclei of two atoms of the same element when the atoms are joined Periodic trends Trends in Atomic Size Atomic Radius-one half the distance between the nuclei of two atoms of the same element when the atoms are joined Trends in Atomic Size Group Trend: Atomic radii of

More information

Lecture. Ref. Ihn Ch. 3, Yu&Cardona Ch. 2

Lecture. Ref. Ihn Ch. 3, Yu&Cardona Ch. 2 Lecture Review of quantum mechanics, statistical physics, and solid state Band structure of materials Semiconductor band structure Semiconductor nanostructures Ref. Ihn Ch. 3, Yu&Cardona Ch. 2 Reminder

More information

Organic Electronic Devices

Organic Electronic Devices Organic Electronic Devices Week 2: Electronic Structure Lecture 2.1: Atomic and Molecular Orbitals Bryan W. Boudouris Chemical Engineering Purdue University 1 Lecture Overview and Learning Objectives Concepts

More information

CO Adsorption Site Preference on Platinum: Charge Is the Essence

CO Adsorption Site Preference on Platinum: Charge Is the Essence Supporting Information CO Adsorption Site Preference on Platinum: Charge Is the Essence G.T. Kasun Kalhara Gunasooriya, and Mark Saeys *, Laboratory for Chemical Technology, Ghent University, Technologiepark

More information

Chem 121 Exam 4 Practice Exam

Chem 121 Exam 4 Practice Exam Chem 121 Exam 4 Practice Exam 1. What is the correct electron configuration for bromine? b. 1s 2 2s 2 2p 6 3s 2 3p 6 3d 9 4s 2 4p 6 c. 1s 2 2s 2 2p 6 3s 2 3p 6 3d 10 4s 2 4p 5 d. 1s 2 2s 2 2p 6 3s 2 3p

More information

Lecture 8 January 24, 2013 GaAs crystal surfaces, n-p dopants Si

Lecture 8 January 24, 2013 GaAs crystal surfaces, n-p dopants Si Lecture 8 January 24, 2013 Ga crystal surfaces, n-p dopants Si Nature of the Chemical Bond with applications to catalysis, materials science, nanotechnology, surface science, bioinornic chemistry, and

More information

FULL POTENTIAL LINEARIZED AUGMENTED PLANE WAVE (FP-LAPW) IN THE FRAMEWORK OF DENSITY FUNCTIONAL THEORY

FULL POTENTIAL LINEARIZED AUGMENTED PLANE WAVE (FP-LAPW) IN THE FRAMEWORK OF DENSITY FUNCTIONAL THEORY FULL POTENTIAL LINEARIZED AUGMENTED PLANE WAVE (FP-LAPW) IN THE FRAMEWORK OF DENSITY FUNCTIONAL THEORY C.A. Madu and B.N Onwuagba Department of Physics, Federal University of Technology Owerri, Nigeria

More information

How to generate a pseudopotential with non-linear core corrections

How to generate a pseudopotential with non-linear core corrections How to generate a pseudopotential with non-linear core corrections 14 12 AE core charge AE valence charge PS core charge PS valence charge 10 8 6 4 2 Objectives 0 0 0.5 1 1.5 2 2.5 3 Check whether the

More information

Aqeel Mohsin Ali. Molecular Physics Group, Department of Physics, College of Science, University of Basrah, Basrah, Iraq

Aqeel Mohsin Ali. Molecular Physics Group, Department of Physics, College of Science, University of Basrah, Basrah, Iraq Journal of Physical Science, Vol. 23(2), 85 90, 2012 Theoretical Investigation for Neon Doping Effect on the Electronic Structure and Optical Properties of Rutile TiO 2 for Photocatalytic Applications

More information

Structure, Electronic and Nonlinear Optical Properties of Furyloxazoles and Thienyloxazoles

Structure, Electronic and Nonlinear Optical Properties of Furyloxazoles and Thienyloxazoles Journal of Physics: Conference Series PAPER OPEN ACCESS Structure, Electronic and Nonlinear Optical Properties of Furyls and Thienyls To cite this article: Ozlem Dagli et al 6 J. Phys.: Conf. Ser. 77 View

More information

3/30/2015. Third energy level. Second energy level. Energy absorbed. First energy level. Atomic nucleus. Energy released (as light)

3/30/2015. Third energy level. Second energy level. Energy absorbed. First energy level. Atomic nucleus. Energy released (as light) Chapter 2 An Introduction Chemistry Lecture 2: Energy Levels and Chemical Bonding Electrons are always moving Outside the nucleus in atomic orbitals Maybe usually Average distance from nucleus (size of

More information

PART CHAPTER2. Atomic Bonding

PART CHAPTER2. Atomic Bonding PART O N E APTER2 Atomic Bonding The scanning tunneling microscope (Section 4.7) allows the imaging of individual atoms bonded to a material surface. In this case, the microscope was also used to manipulate

More information

Structure and Bonding. Dr. Sapna Gupta

Structure and Bonding. Dr. Sapna Gupta Structure and Bonding Dr. Sapna Gupta Origins of Organic Chemistry Initially thought to be chemicals that were obtained from plants and animals only. Thought to have a vital force as they from natural

More information

Review Package #3 Atomic Models and Subatomic Particles The Periodic Table Chemical Bonding

Review Package #3 Atomic Models and Subatomic Particles The Periodic Table Chemical Bonding Chemistry 11 Review Package #3 Atomic Models and Subatomic Particles The Periodic Table Chemical Bonding 1. Atomic Models and Subatomic Particles: A. Subatomic Particles and Average Atomic Mass: - Subatomic

More information

Flatbands in 2D boroxine-linked covalent organic frameworks

Flatbands in 2D boroxine-linked covalent organic frameworks Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 215 Supplementary Material Flatbands in 2D boroxine-linked covalent organic frameworks

More information

CHAPTER 6. ELECTRONIC AND MAGNETIC STRUCTURE OF ZINC-BLENDE TYPE CaX (X = P, As and Sb) COMPOUNDS

CHAPTER 6. ELECTRONIC AND MAGNETIC STRUCTURE OF ZINC-BLENDE TYPE CaX (X = P, As and Sb) COMPOUNDS 143 CHAPTER 6 ELECTRONIC AND MAGNETIC STRUCTURE OF ZINC-BLENDE TYPE CaX (X = P, As and Sb) COMPOUNDS 6.1 INTRODUCTION Almost the complete search for possible magnetic materials has been performed utilizing

More information

Chapter 7: Chemical Bonding and Molecular Structure

Chapter 7: Chemical Bonding and Molecular Structure Chapter 7: Chemical Bonding and Molecular Structure Ionic Bond Covalent Bond Electronegativity and Bond Polarity Lewis Structures Orbital Overlap Hybrid Orbitals The Shapes of Molecules (VSEPR Model) Molecular

More information

Supporting Information for Ultra-narrow metallic armchair graphene nanoribbons

Supporting Information for Ultra-narrow metallic armchair graphene nanoribbons Supporting Information for Ultra-narrow metallic armchair graphene nanoribbons Supplementary Figure 1 Ribbon length statistics. Distribution of the ribbon lengths and the fraction of kinked ribbons for

More information

Section 12: Lewis Structures

Section 12: Lewis Structures Section 12: Lewis Structures The following maps the videos in this section to the Texas Essential Knowledge and Skills for Science TAC 112.35(c). 12.01 Electronegativity Chemistry (5)(C) 12.02 Electron

More information

Modelowanie Nanostruktur

Modelowanie Nanostruktur Chair of Condensed Matter Physics Institute of Theoretical Physics Faculty of Physics, Universityof Warsaw Modelowanie Nanostruktur, 2012/2013 Jacek A. Majewski Semester Zimowy 2012/2013 Wykad Modelowanie

More information

Intermediate DFT. Kieron Burke and Lucas Wagner. Departments of Physics and of Chemistry, University of California, Irvine, CA 92697, USA

Intermediate DFT. Kieron Burke and Lucas Wagner. Departments of Physics and of Chemistry, University of California, Irvine, CA 92697, USA Intermediate DFT Kieron Burke and Lucas Wagner Departments of Physics and of Chemistry, University of California, Irvine, CA 92697, USA October 10-19th, 2012 Kieron (UC Irvine) Intermediate DFT Lausanne12

More information

XYZ of ground-state DFT

XYZ of ground-state DFT XYZ of ground-state DFT Kieron Burke and Lucas Wagner Departments of Physics and of Chemistry, University of California, Irvine, CA 92697, USA January 5-9th, 2014 Kieron (UC Irvine) XYZ of ground-state

More information

Solid State Electronics EC210 Arab Academy for Science and Technology AAST Cairo Fall Lecture 10: Semiconductors

Solid State Electronics EC210 Arab Academy for Science and Technology AAST Cairo Fall Lecture 10: Semiconductors Solid State Electronics EC210 Arab Academy for Science and Technology AAST Cairo Fall 2014 Lecture 10: Semiconductors Lecture Notes Prepared by: Dr. Amr Bayoumi, Dr. Nadia Rafat These PowerPoint color

More information

Its Bonding Time. Chemical Bonds CH 12

Its Bonding Time. Chemical Bonds CH 12 Its Bonding Time Chemical Bonds CH 12 What is a chemical bond? Octet Rule: Chemical compounds tend to form so that each atom, by gaining, losing, or sharing electrons, has an octet of electrons in its

More information

Problem 1 (2 points) Lone pair on N may donate to an empty p orbital of B on another molecule of aminoborane, leading to oligomers.

Problem 1 (2 points) Lone pair on N may donate to an empty p orbital of B on another molecule of aminoborane, leading to oligomers. Problem 1 (2 points) B N Lone pair on N may donate to an empty p orbital of B on another molecule of aminoborane, leading to oligomers. B N x 3 B N 3 3x 2 + (BN) x MW( 3 B N 3 ) = 30.87 g/mol MW( 2 ) =

More information

Ionic Bonding. Chem

Ionic Bonding. Chem Whereas the term covalent implies sharing of electrons between atoms, the term ionic indicates that electrons are taken from one atom by another. The nature of ionic bonding is very different than that

More information