Download presentation

Presentation is loading. Please wait.

Published byReed Neve Modified over 3 years ago

1
**DFT Density Functional theory and the description of Nature**

Edison Z. da Silva Instituto de Física "Gleb Wataghin", UNICAMP, Campinas - SP, Brazil

2
**Outline DFT, What it is, how it came about, what it is used for.....**

Solids and DFT Probing the Earth´s Inner Core Gold Nanowires

3
**We have a well defined system**

Nuclei + Electrons Molecules Atoms Solids Liquids

4
**DFT, theoretical framework**

Electrons are the “glue” which holds matter together DFT, theoretical framework Description of known materials, prediction of new materials, explanation of many questions

5
**Electromagnetic Forces**

Fundamental laws of electronic and nuclear motions well known Electromagnetic Forces + Quantum Mechanics H ( {ri , r} ) = ETOT ( {ri , r} ) ^ H = ( -½2i ) + ( -½ 2 ) + ( - ) + Z ri ___ i<j Ne i=1 ^ 1 rij =1 Nn < ZZ _____ r M Te ^ Tn ^ Ve-n ^ Ve-e ^ Vn-n ^

6
“There is an oral tradition that, shortly after Schrödinger’s equation for the electronic wavefunction had been put forward and spectacularly validated for small systems like He and H2, P. A. M. Dirac declared that chemistry had come to an end - its content was entirely contained in that powerful equation. Too bad, he is said to have added, that in almost all cases, this equation was far too complex to allow solution.” W. Kohn, Reviews of Modern Physics 71, 1253 (1999).

7
**Therefore, we have a well posed problem, but too complex and difficult to solve**

Impossible to have exact solution except in very few cases Need of approximations

8
**Born-Oppenheimer (1927) Approximation (Qualitatively)**

Based on the fact that nuclear masses are much larger than the electronic ones Therefore, electrons move on a different time-scale than the nuclei (nuclei move much more slowly) Thus, electrons follow the nuclei “instantaneously” This allows us to consider the nuclei fixed when solving for the electronic motion

9
**Helecaelec({ri};{r}) = Eaelec({r}) aelec({ri};{r})**

Born-Oppenheimer Approximation Helec = ( -½2i ) + ( - ) + Z ri ___ i<j Ne i=1 ^ 1 rij =1 Nn ZZ _____ r < Te ^ Ve-n ^ Ve-e ^ Vn-n ^ Helecaelec({ri};{r}) = Eaelec({r}) aelec({ri};{r}) ^ aelec({ri};{r}) depends explicitly on the electronic coordinates {ri} but only parametrically on the nuclear coordinates {r}, as does Eaelec({r})

10
**(r , Q) = a(Q) aelec(r;Q)**

Born-Oppenheimer Approximation As the {aelec(r;Q)}, for a fixed Q, form a complete orthonormalized set, one can write: (r , Q) = a(Q) aelec(r;Q) a [Tn + Ebelec(Q)] b(Q) + ba(Q) a(Q) = Etot b(Q) ^ a Roughly speaking, if the kinetic energy of the nuclei is small when compared to |Ebelec(Q) - Eaelec(Q)|, the non-diagonal terms ba can be neglected

11
**(r , Q) = b(Q) belec(r;Q)**

Born-Oppenheimer Approximation [Tn + Ebelec(Q)] b(Q) = Etot b(Q) ^ (r , Q) = b(Q) belec(r;Q) The total electronic energy Ebelec(Q) acts as a potential energy for the nuclear motion, which occurs in a single electronic state belec . The nuclear motion simply deforms the electronic distribution, and does not cause transitions between different electronic states.

12
**Born-Oppenheimer Approximation**

Important concepts: Molecular geometry

13
**Born-Oppenheimer Approximation**

Crystal structure Important concepts: Molecular geometry

14
**Born-Oppenheimer Approximation**

Important concepts: Molecular geometry Crystal structure Potential Energy Surface (PES) Geometrical coordinate PES Ex: Carbon Amorphous Graphite Diamond

15
**Two issues How to calculate (as accurately as possible) the PES**

electronic degrees of freedom How to sample the PES (or how to move the atoms) nuclear degrees of freedom

16
**How to solve Helecelec = Eelecelec**

Traditional way of thinking would be to describe the wavefunction as well as possible However, WF for a many electron system is a very complicated object!

17
**YES Is there another way to solve the problem (ab initio)?**

Electronic density e(r) as the fundamental object (and not wavefunction elec)

18
**Density Functional Theory (DFT)**

Proc. Cambridge Philos. Soc. 26, 376 (1930) Roots in the works of Thomas (1926), Fermi (1928), Dirac (1930), Slater, etc. Chemistry Nobel prize Formally well founded in the works of W. Kohn P. Hohenberg and W. Kohn, Phys. Rev 136, 864B (1964) W. Kohn and L. J. Sham, Phys. Rev. 140, 1133A (1965)

19
**DFT - Two basic theorems P. Hohenberg and W. Kohn, Phys**

DFT - Two basic theorems P. Hohenberg and W. Kohn, Phys. Rev 136, 864B (1964) Let’s consider a system of N interacting electrons in the ground-state associated with an external potential v(r) 1) The ground state density 0e(r) uniquely determines the potential v(r) Since with v(r) the full electronic Hamiltonian is known, 0e(r) completely determines all properties of the system 2) There exists a functional E[e(r)] which has its minimum for the ground-state density 0e(r) Can use this variational principle to calculate 0e(r)

20
**DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev**

DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev. 140, 1133A (1965) E[e] = v(r) e(r) d3r + T[e] + U[e] I don’t know how to solve this problem, but I know how to solve the following problem: If I had a system of non-interacting electrons, in an external potential veff(r), then: Es[e] = veff(r) e(r) d3r + Ts[e] Ts[e] = kinetic energy of a non-interacting system with density e

21
**DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev**

DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev. 140, 1133A (1965) The ground-state wavefunction in this case is a Slater determinant of N orbitals i (i=1,N), which satisfy the equations: [-½ 2 + veff(r)] i(r) = i i(r) And the ground-state density can be written as: 0e(r) = |i(r)|2 lowest N i

22
**DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev**

DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev. 140, 1133A (1965) However, from the Hohenberg-Kohn theorem, a completely equivalent way of calculating 0e(r) would be through the minimization of E[e(r)]: e(r) Es[e] - e(r’) d3r’ = 0 + veff(r) - = 0 Ts[e] e(r) 0e(r) = |i(r)|2 i Gives same density as

23
**DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev**

DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev. 140, 1133A (1965) Application of the Hohenberg-Kohn theorem to E[e] gives e(r) E[e] - e(r’) d3r’ = 0 Ts[e] + v(r’) e(r’) d3r’ + UH[e] + EXC[e] - e(r’) d3r’ e(r) = 0 + v(r) + d3r’e(r’)/|r-r’| + Ts[e] e(r) EXC[e] - = 0

24
**DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev**

DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev. 140, 1133A (1965) Comparison with similar equation for non-interacting electrons gives: + v(r) + d3r’e(r’)/|r-r’| + Ts[e] e(r) EXC[e] - = 0 Interacting electrons + veff(r) - = 0 Ts[e] e(r) Non-interacting electrons v(r) + d3r’e(r’)/|r-r’| + EXC[e] e(r) veff(r) =

25
**DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev**

DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev. 140, 1133A (1965) We can, therefore, calculate exactly (in principle) the problem of the interacting electrons through the solution of the following equations: [-½ 2 + veff(r)] i(r) = i i(r) 0e(r) = |i(r)|2 lowest N i v(r) + d3r’e(r’)/|r-r’| + EXC[e] e(r) veff(r) =

26
**DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev**

DFT - How to calculate 0e W. Kohn and L. J. Sham, Phys. Rev. 140, 1133A (1965) Problem of many-electrons mapped exactly (in principle) into the problem of non-interacting electrons subjected to an effective potential! v(r) + d3r’e(r’)/|r-r’| + EXC[e] e(r) veff(r) = However, we don’t know how to calculate this effective potential: We need approximations for EXC[e] and vXC[e] = EXC[e] e(r)

27
**DFT - Local Density Approximation (LDA)**

Let’s consider the exchange-correlation energy, per particle, for a homogeneous electron gas, ehXC This quantity can be calculated very accurately (Quantum Monte Carlo) Let’s imagine the real system divided in small cells: Ni Vi i = Ni / Vi i

28
**DFT - Local Density Approximation (LDA)**

If we consider that the density is approximately homogeneous inside cell i, then we can write for the XC energy in cell i EiXC ehXC (i) Ni = ehXC (i) Ni (Vi / Vi) = = ehXC (i) (Ni / Vi) Vi = ehXC (i) i Vi i Ni Vi i = Ni / Vi

29
**DFT - Local Density Approximation (LDA)**

Summing over all the cells i will give for the total XC energy EXC ehXC(i) i Vi i EXC ehXC((r)) (r) d3r = ELDAXC i Ni Vi i = Ni / Vi

30
**DFT - Local Density Approximation (LDA)**

And from this we can get the XC potential vLDAXC ELDAXC e vLDAXC = = ehXC((r)) (r) d3r e = ehXC() d d e i Ni Vi i = Ni / Vi

31
**DFT - Self-consistency cycle**

Still a problem: veff depends one ande depends on veff Solution: self-consistency cycle 1. Choose an initial density 0e and determine the effective potential veff (0e) 2. Solve the Kohn-Sham equations [-½ 2 + veff(r)] i(r) = i i(r) 3. Calculate the density 1e(r) = |i(r)|2 lowest N i 4. Check if 1e = 0e. If yes, end of cycle. If not, go back to 2. (with 0e = 1e)

32
**Crystal - Bloch functions**

veff has the periodicity of the crystal According to Bloch’s theorem, the i will have the following form: (n,k)(r) = exp(i k•r) u(n,k)(r) The function u(n,k) also has the periodicity of the crystal Therefore, it can be expanded in a discrete set of plane waves whose wave vectors are reciprocal lattice vectors of the crystal u(r) = cGexp(i G•r) G

33
**Crystal - Bloch functions**

Therefore (n,k)(r) = cnk+G exp[i (k+G)•r] G For a crystal, the density will be given by e(r) = |i(r)|2 = 2 |(n,k)(r)|2 lowest N i occ. bands n k BZ

34
**Crystal - Bloch functions**

Two approximations: 1) Maximum value of G=GC number of basis function (plane wave) (n,k)(r) = cnk+G exp[i (k+G)•r] G Gc To determine GC one gives the kinetic energy associated with the GC Cutoff energy EC = GC2/2m 2) Number of Brillouin-zone points - set of “special points” e(r) = 2 |(n,k)(r)|2 occ. bands n k SP

35
**Strong oscillations in the core region**

Crystal - Bloch functions Strong oscillations in the core region All electron valence WF

36
These strong oscillations are bad for plane-wave expansion (large value of GC to describe small features in real space) Either use a different basis function in the core region, or change the function in the core region

37
**Pseudopotentials Valence electrons are the chemically relevant ones**

Removes the core electrons and replaces them and the strong potential by an effective, weaker potential that acts on the valence electrons rc r V,

38
All electron Pseudo

39
**Si, The credibility of DFT**

40
**How to solve the KS equations**

After all these approximations, I have to find the cnk+G through the self-consistent solution of the KS equations HKS i(r) = i i(r) (n,k)(r) = cnk+G exp[i (k+G)•r] G Gc

41
**= c HKS Traditional method - diagonalization**

Write the matrix for the KS Hamiltonian in the plane wave basis set and diagonalize it HKSk+G,k+G’ cnk+G’ = nk+G cnk+G G’ HKS c =

42
Perfect crystal

43
Crystal with a defect

44
** Crystal with a defect **

45
** Crystal with a defect **

46
Surfaces

47
Surfaces

48
Surfaces

49
**Applications Understanding the Earth´s inner core**

Breaking of Gold nanowires

50
**Elasticity of Iron at the temperature of the Earth´s inner core**

G. Stainle-Neumann, L. Stixrude, R. Cohen & O. Gulseren Nature, 413, 57 (2001)

51
General picture

52
**Seismological Studies:**

Compressional waves travel faster along polar paths than in equatorial plane. Earth´s center, 2,440 km across is nearly pure Iron At high temperatures and pressures iron goes to an hcp phase called e-phase

53
**Iron at Temperatures and pressures of the Earth´s core.**

Crystal structure distorts unexpectedly Inner core believed to be made up of Iron crystals in hcp structure Observed seismic anisotropy must arise from differences in elastic response of hcp Iron Densities for iron 7.87 Mg m atmospheric pressure 13.04 Mg m-3 at Earth´s core pressures

54
**Iron at Temperatures and pressures of the Earth´s core.**

DFT calculations of elastic constants Thermodynamics given by the Helmholtz free energy F(V,T) = E0(V) + Eel(V,T) -T Sel(V,T) + Fvib(V,T) E0(V) static total energy Eel(V,T) due to thermal excitations Sel(V,T) electronic entropy Fvib(V,T) phonon contribution (particle in a cell )

55
r(Mg m-3) 12.52 13.04 13.62 Equilibrium structure of hcp iron over a range of densities and temperatures of the Earth´s core. Computing F for different c/a and finding the minima

56
Elastic constants Elasticity of hcp iron for a density Mgm-3

57
**Velocity Acoustic properties of iron for the Earth´s core.**

Adiabatic bulk modulus (KS) and shear modulus (m) as function of temperature compared with inner core at the same density Mgm-3 Travel time anomaly Solid line , model with 1/3 of crystals with basal planes aligned with rotation axis

58
**Conclusions Seismological Studies:**

Compressional waves travel faster along polar paths than in equatorial plane. At high temperatures and pressures iron goes to an hcp phase called e -phase. With c/a = 1.7 seismic waves travel 12 % faster in the ab plane. This anisotropy is too strong, if crystals are aligned it accounts for the experimental findings.

59
**Breaking of Gold Nanowires: A Computer Simulation study**

E. Z. da Silva Instituto de Física "Gleb Wataghin", UNICAMP, Campinas - SP, Brazil

60
**Participants, motivation...**

Theory Antonio José R. da Silva(IF-USP) Adalberto Fazzio (IF-USP) Frederico D. Novaes (PhD-IF-USP) Experimental motivation Daniel Ugarte (LNLS) Varlei Rodrigues

61
**When we get to the very, very small**

world - say circuits of seven atoms - we have a lot of new things that would happen that represent completelly new opportunities for design. Atoms on a small scale behave like nothing on the large scale, for they satisfy the laws of quantum mechanics. Richard Feynman Plenty of Room at the Bottom(1959)

62
**Program Why study Au nanowires? Experiments Theory TBMD simulations**

Impurities Conclusions

63
**Why study Au nanowires? Gold nanowires are produced in the lab!**

Understanding of its properties is fundamental. Gold is the electrical contact in nanotechnology. When Gold nanowires become very thin, interesting surprises are found: Conductivity is quantized. Possibility of helical structures. One-atom thick wires are produced.

64
Gold in devices J Reichert, et al., Phys. Rev. Lett., 88, (2002)

65
**Experiments, How it all started!**

Pin-plate experiment: nanowire formed conductance during elongation and contraction U.Landman, W.D.Luedtke, B.E.Salisbury, and R.L.Whetten, Phys. Rev. Lett. 77, 1362, (1996)

66
**Theoretical Predictions**

Computer simulations with a “glue” type empirical many-body potential (for Al and Pb) predicted: As the diameter decrease, thin metal wires develop exotic stable noncrystalline structures: Existence of critical diameter Formation of helical, spiral-structured wires O. Gulseren, F Ercolessi, and E. Tosatti, Phys. Rev. Lett. 80, 3775, (1998)

67
**Theory Weird Nanowires**

O. Gulseren, F Ercolessi, and E. Tosatti, Phys. Rev. Lett. 80, 3775, (1998)

68
How to make a wire

69
**Theorist´s view: production and imaging process!**

70
**Y. Kondo and K. Takayanagi, Phys. Rev. Lett. 79, 3455, (1997)**

Stable Au Nanowires from surface structures Production Au thin films (3nm) in UHVTEM electron beam irradiation (100 A/cm2) produced many holes nanowires Imaging Straight nanowires images produced with electron beam irradiation (5 A/cm2) Y. Kondo and K. Takayanagi, Phys. Rev. Lett. 79, 3455, (1997)

71
**Interpretation of the Experiments**

1-7 4-11 6-13 1-7-14 1-8-15

72
**Folding of a (111) plane Cylindrical folding of a**

triangular lattice for an (m, n) tube, with views of several coaxial tube nanowires. Each atom is pictured as a sphere of atomic radius. The (7, 3) gold nanowire (note its chirality) was reported to be magic in (3).

73
**V. Rodrigues and D. Ugarte, Phys. Rev. B 63, 073405-1, (2001)**

Real time imaging of one-atom-thick Au nanowires The film irradiation technique from Kondo and Takayanagi produced stable one-atom-thick Au- nanowires. Time sequence of formation, elongation and fracture of a chain of gold atoms. V. Rodrigues and D. Ugarte, Phys. Rev. B 63, , (2001)

74
**Dynamical Simulations of Gold nanowires**

Is it possible to simulate the evolution of a gold nanowire under stress with a reliable electronic structure method? Wire under tension. It forms, starts to thin ( atoms going to the wire edges) neck is produced (one atom constriction). Atoms from the wire,( near the tips) are draw back and are incorporated into the one -atom thick neck. This thin neck grows to 4-5 atoms The wire finally breaks

75
**(three orders of magnitude faster)**

Ab Initio DFT Methods (costly in terms of computer time!) NRL-TBMD keeps the electrons (three orders of magnitude faster) Number of atoms ACCURACY MD with Classical Potentials Embedded-atom, Effective medium, Finnis-Sinclair, Second Moment(TB) (No electrons!)

76
**The Tight -Binding Method**

Slater and Koster proposed in 1954 a modified combination of atomic orbitals (LCAO) as a interpolation scheme to determine energy bands. In 1986 Papaconstantopoulos published a handbook of SK parameters for most elements in the periodic table. As DFT ab initio methods improve, so does the Papaconstantopoulos TB fits with updates the of SK parameters for most elements in the periodic table.

77
**The NRL tight-binding method**

Procedure, The method fits TB parameters to reproduce ab initio total energies (DFT) calculated with full-potential linear aumented plane wave method. Slater-Koster parameters are fitted to LAPW bands and total energies as function of volume for 10 fcc structures, 6 bcc structures and 5 sc structures. Perdue-Wang parametrization to LDA M.J.Mehl and D. A.Papacontantopoulos, Phys. Rev. B 54, 4519 (1996)

78
**Tight-binding and Molecular Dynamics**

TB basis set The Slater-Koster (SK) parameters Tight-binding Fit of the ab initio Potential energy surface Ab initio molecular dynamics

79
**TB basis set Minimum basis set of atomic like orbitals,**

for transition metals; Number of basis functions per atom N0. Number of atoms Na, dimension space spanned by this basis set Nb = N0 Na. States are expressed as linear combinations of these orbitals:

80
**The Slater-Koster parameters**

Matrix elements of the Hamiltonian and overlap gives: Hopping terms Overlap terms SK-parameters

81
**Tight-Binding Fit of the ab initio Potential energy surface**

Formalism Parametrization

82
**Complicated Transition Metal-Mn**

Manganese crystallizes in the -Mn structure with 29 atoms Above 710 0C, Mn transforms to the -Mn with 20 atoms Calculated TB total energy

83
**Fitting Procedure for Au, using the static TB code**

Equation of state How good is the TB parametrization for fcc bulk Au? Data basis: 10 fcc structures, 6 bcc structures, 5 sc structures. Phonon dispersion, T = 0 Fcc structure, lowest energy F.Kirchhhoff et al. Phys. Rev. B, (2001)

84
**Ab initio molecular dynamics steps of the simulation**

Input, Ri, positions of the atoms H the Hamiltonian The electronic ground state of the system is calculated. Eigenvectors Forces on the atoms. Forces (EOM) integrated and new positions found. Where states are expanded using the TB orbitals

85
**Electronic DOS for Au, using TBMD code**

Solid, T dependence MD simulations: Microcanonical ensemble, EM with Verlet algo, t = 2 fs, point sampling. Liquid Au, T = 1773 K F.Kirchhhoff et al. Phys. Rev. B, (2001)

86
**Au-nanowires, simulations E. Z. da Silva. A J. R. da Silva and A**

Au-nanowires, simulations E. Z. da Silva. A J. R.da Silva and A. Fazzio, Phys. Rev. Lett., 87 , (2001) Front view Starting structures: nanowire along the along the(111) direction - 10 atom planes - 7atoms in each plane. Top view

87
**Simulation Protocol EM integrated using Verlet algo, t =1 fs**

The system is heated to T = 600 K, MD steps, 7ps Elongation of the wire by L = 0.5 Å The system is heated to T = 400 K, 4000 MD steps, 4ps Previous two steps are repeated Procedure done for Å < LW < 44.0 Å

88
**Au nanowire, 6 (111) planes of 7 Au atoms,**

unrelaxed structure relaxed structure

89
**Similarities for the breaking the one-atom necklace**

Experiment 2.99 2.98 2.89 2.74 2.63 2.91 2.61 2.89 Simulation

90
**Evolution and breaking**

Atomic configurations (in Å) (a) 25.5, (b) 33.0, (c) 37.0 (a) 38.0, (b) 40.5, (d) 41.0

91
**Defect structure, one atom neck**

(i) Defect structure (iii) 4-5 atoms planes (iv) atoms planes (v) one atom neck

92
Forces Saw-tooth behavior

93
**Before breaking the one-atom necklace**

The nanowire develops a one-atom thick necklace with five atoms in its final structure. Just before breaking, the apex-apex distance gets to da-a ~ Å.

94
**Animation of the simulation**

See this animation at

95
**Pending problems Are TBMD results reproducible using ab initio DFT.**

Large Au-Au distances seen in the experiments

96
**Real time imaging of one-atom-thick Au nanowires**

HRTEM image of atom chain with three gold atoms. Atomic positions are the dark spots Large Au-Au distances!!!! Schematic representation V. Rodrigues and D. Ugarte, Phys. Rev. B 63, , (2001)

97
**Simulations give shorter Au-Au distances**

Before breaking: one-atom necklace Simulations give shorter Au-Au distances

98
**Ab initio DFT (Siesta) Fully self-consistent DFT LCAO**

Extremely fast simulation using minimal basis set Kohn-Sham equations Exchange-correlation (GGA) Norm conserving pseudopotentials (Troullier-Martins) Total energy Forces

99
**Ab initio evolution Starting structure Before breaking**

Au-Au distance 3.0 Å After breaking

100
**Large distances, Impurities?**

The statistics The Images Au-Au distances 3.6±0.2 (Au-Au)Max 3.1 Å (Au-X-Au)Max 3.6 Å X = ? Legoas,Galvão, Rodrigues , Ugarte , PRL, 88, , (2002)

101
**Reasoning for impurities**

Structure simulation TEM simulation 2.9 2.8 3.6 3.1

102
**Carbon, structure right before breaking**

Carbon in Au nanowire Carbon, initial structure Au-nanowire Carbon intermediate structure, 3.73 Carbon, structure right before breaking Quebra

103
**Considered the effect of the impurities, H, B, C, N, O and S **

Impurities and the Au-Au Bond Length Frederico D. Novaes, A.J.R. da Silva, E.Z. da Silva and A.Fazzio, Phys. Rev. Lett. 90, (2003)22 january Use ab initio DFT to study contamination of the pure Au nanowire by impurities. Considered the effect of the impurities, H, B, C, N, O and S Experiment gives Au-?-Au = 3.6 Å Au-??-Au = 4.8 Å

104
**Contamination by H and S**

105
**H Impurities? 3.5 3.5 4.9 Our simulation Experiments:**

Legoas,Galvão, Rodrigues , Ugarte , PRL, 88, , (2002) 4.9 3.5

106
**General Conclusions Future: Importance of Gold nanowires.**

Simulations can help understand the dynamical evolution and finally the breaking of metal nanowires. TBMD is reliable and fast. Can be used to study dynamical evolution of metal nanowires. Future: Study of other directions for wire formation. Investigation of nanowires of other metals (Ag, Pt etc..) Use nanowires and their tips to design devices.

107
Conclusions DFT, A effective way of studying and projecting interesting materials. Solids and DFT Probing the Earth´s Inner Core Gold Nanowires

Similar presentations

OK

Mrs. Minna Turrell Room 153 Hours 1, 3, 5. It’s this or Chemistry Improves problem-solving skills, math skills, standardized-test scores Encourages logical.

Mrs. Minna Turrell Room 153 Hours 1, 3, 5. It’s this or Chemistry Improves problem-solving skills, math skills, standardized-test scores Encourages logical.

© 2017 SlidePlayer.com Inc.

All rights reserved.

Ads by Google

Ppt on power distribution in india Funny ppt on human resource management Ppt on non biodegradable waste materials Ppt on social networking and youth Ppt on solar energy satellite Ppt on needle chest decompression Ppt on rabindranath tagore life Ppt on corbett national park Convert pptx file into ppt online Ppt on youth leadership