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Physics 250-06 “Advanced Electronic Structure” Earlier Electronic Structure Methods Contents: 1. Solution for a Single Atom 2. Solution for Linear Atomic.

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Presentation on theme: "Physics 250-06 “Advanced Electronic Structure” Earlier Electronic Structure Methods Contents: 1. Solution for a Single Atom 2. Solution for Linear Atomic."— Presentation transcript:

1 Physics “Advanced Electronic Structure” Earlier Electronic Structure Methods Contents: 1. Solution for a Single Atom 2. Solution for Linear Atomic Chain 3. LCAO Method and Tight-Binding Representation 4. Tight-Binding with BandLab

2 Solving Schrodinger’s equation for solids Solution of differential equation is required Properties of the potential

3 Atomic potential (spherically symmetric) Properties of Solution for a Single Atom

4  Property of solution for symmetric potential Discrete set of levels is obtained. While degeneracy with respect to m remains, degeneracy with respect to l is now lifted since V V(r) is different from –Ze2/r. We can label the levels by main quantum number and orbital quantum number. For given l, n=l+1,l+2,... which is the property of the solution. For l=0 we have the states E1s, E2s,E3s,E4s,... For l=1 we have the states E2p, E3p,E4p,E5p,... For l=2 we have the states E3d, E4d,E5d,E6d,... No artificial degeneracy as in the hydrogen atom case: E2s=E2p,E3s=E3p=E3d,E4s=E4p=E4d=E4f… At some point, level Enl becomes above zero, i.e the spectrum changes from discrete to continuous. Note also that this spectrum of levels is a functional of V(r), i.e. it is different for a given atom with a given number of electrons N.

5 We can interpret different solutions as wave functions with different numbers of nodes. For example, for l=2, there are solutions of the equations with no nodes, with one node, with two nodes, etc. Number of nodes = n-l-1. If n runs from l+1, l+2,..., nodes =0,1,2,3...

6  Periodic table of elements The one-electron approximation is very useful as it allows to understand what happens if we have many electrons accommodated over different levels. Let us take atom with N electrons. Lets us find all discrete levels E1s

7  Hunds rules For a given l shell, the electrons will occupy the slots to maximize the total spin For a given l shell, the electrons will maximize the total spin and total angular momentum Hunds rules cannot be understood on the basis of one-electron self-consistent approximation. However, for atomic system, the many body problem for N electrons moving in the Coulomb potential can be solved where En is the set of many body energy levels. Hunds rules follow from this Hamiltonian

8 Bringing atoms together: what to expect? Properties of the solutions: Core Levels Energy Bands

9 Illustration: Periodic array of potential wells placed at distance L between the wells. Solution for a Linear Atomic Chain Basic property of the potential V(x+l)=V(x), and of the Hamiltonian H(x+l)=H(x) Solving variationally:

10 We obtain infinite system of equations If overlap is only between nearest wells, we simplify it to be This is infinite set of equations. At first glance it seems that we cannot solve it. But we can do it indeed.

11 Since Hamitonian is periodical function, all wells are equivalent for the electron. That would mean that the probability to find the electron in each of the well should be the same. That is possible if where u(x) is a periodical function: introduce periodic boundary condition where n is any integer number and phase is frequently called the wave vector k_n

12 Once we understand the form for the wave function, we already see one problem with the representation Each term in this expansion is not a periodical function, only the entire sum is periodical. The question is if we can construct another linear combinations of those basis functions so that each of the terms obeys the periodicity condition. In other words, we would like to have such combinations of with some coefficients c_n so that the combination obeys the periodicity condition automatically

13 For this to happen or, the coefficient is equal to where n can be any integer. So we can label those combinations with index k_n which automatically obey the periodicity condition for wave function (Bloch theorem)

14 What we want is to is to use those linear combinations in finding the solutions The advantage of this formulation is seen because all off-diagonal matrix elements disappear. This is seen because F(x) is periodical function, therefore Therefore, we automatically obtain the diagonalized Hamiltonian That mean that the spectrum is known to us In other words, we are able to solve the problem completely!

15 Let us analyze the solutions We see that we can draw the solutions as a cosine centered around h as a function of wave number k. That is a band. Due to periodicity of cos, it is sufficient to draw it within –pi

16 Summary: Bloch Property for a Local Basis Differential equation using expansion where is a basis set satisfying Bloch theorem To force the Bloch property we now use instead of plane waves : Linear combinations of local orbitals

17 Apply Variational Principle Variational principle leads us to solve matrix eigenvalue problem where is hamiltonian matrix is overlap matrix

18 Linear Combination of Atomic Orbitals (LCAO) to be used in variational principle Tailored to atomic potential LCAO Method

19 Hamiltonian of LCAO Method: Hoppings between the orbitals

20 Tight-Binding Parametrization In LCAO Method, the Hamitonain is parameterized via on site energies of the orbitals and nearest-neighbor hopping integrals between the orbitals. In many situations symmetry plays an important role since for many orbitals hoppings intergrals between them are automatically equal zero.

21 Thinking of Cubic Harmonics - unitary transformation

22 Hoppings between various orbitals ss,sp,sd hoppings pp,pd hoppings dd hoppings

23 Illustration, CuO2 plane It is clear that levels are non-bonding and are all occupied. The same is true for level of copper, and for orbitals. The active degrees of freedom here are orbitals which have hopping rate. Using the active degrees of freedom as the basis the hamiltonian has the form

24 Let us introduce another basis set of bonding (b), antibonding (a), and non-bonding (n) orbitals Within this basis set, the Hamiltonian becomes The bands are now seen as the bonding band below and the antibonding band above. The non--bonding band is also present.

25 MINDLab Software

26 Understanding s-electron band structure. Tight-binding parameterization for Na. s level position and hopping rate for s electrons.

27 Understanding s-d electron band structure. Tight-binding parameterization for Cu. s level position and hopping rate for s electrons. d level position and narrow d-bands. s-d hybridization

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