3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)3.012 Fund of Mat Sci: Bonding – Lecture 13THE DANCE OF SHIVASource: Wikipedia3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Homework for Mon Oct 31• Study:18.1 (quantum oscillator), 28.1 and 28.2 (symmetry)• Read 18.6 (classical harmonic oscillator)3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Last time: 1. Diagonalization in a basis2. Huckel model for conjugated and aromatic polymers1,nnkncϕψ==∑HCC CCCCHHHHHπππππ π bondingπFigure by MIT OCW.Energyπ5π4π2π1π6π3Figure by MIT OCW.3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Matrix Formulation1,nnkncϕψ==∑ˆmn nmHHϕϕ=11 1 1221...........0.........kkkkkHE H cHEHHEc−⎛⎞⎛⎞⎜⎟⎜⎟−⎜⎟⎜⎟⎜⎟⎜⎟⋅=⎜⎟⎜⎟⎜⎟⎜⎟⎜⎟⎜⎟−⎝⎠⎝⎠O3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)The Quantization of Vibrations• Electrons are much lighter than nuclei (mproton/melectron~1800)• Electronic wave-functions always rearrange themselves to be in the ground state (lowest energy possible for the electrons), even if the ions are moving around• Born-Oppenheimer approximation: electrons in the instantaneous potential of the ions (so, electrons can not be excited – FALSE in general)3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Nuclei have some quantum action…• Go back to Lecture 1 – remember the harmonic oscillatorGraph of Potential energy, V(x), as a function of the bond length, x, for a diatomic molecule. Removed for copyright reasons.See Engel, T., and P. Reid. Physical Chemistry. Single volume ed. San Francisco, CA: Benjamin Cummings, 2005, p. 378, figure 18.1.StationaryobjectSpringMassEquilibriumposition ofmasszz0A mass on a spring. This system can berepresented by a harmonic oscillator.Figure by MIT OCW.3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)The quantum harmonic oscillator2222() 1() ()22dzkz z E zMdzϕϕϕ−+=hkmω=kma =h3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)The quantum harmonic oscillator (II)12Enω⎛⎞=+⎜⎟⎝⎠hFigure by MIT OCW.543210xV(x)n = 2n = 3n = 4n = 1n = 0E (in units of hνo)3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Quantum Oscillator Applet3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Quantized atomic vibrationsPhoto courtesy of Malene Thyssen, www.mtfoto.dk/malene/Figure by MIT OCW.Image removed for copyright reasons. See http://w3.rz-berlin.mpg.de/%7Ehermann/hermann/Phono1.gif.3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Specific Heat of Graphite (Dulong and Petit)0050050010001000150015002000200025002500Temperature (K)CP (J.K-1.kg-1)Figure by MIT OCW.3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Structure3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Symmetry• Symmetry operations: actions that transform an object into a new but undistinguishable configuration• Symmetry elements: geometric entities (axes, planes, points…) around which we carry out the symmetry operations3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Figure 17.1bImages of the symmetry elements of the allene (CH2CCH2) and PCl5 molecules removed for copyright reasons.See Engel, T., and P. Reid. Physical Chemistry. Single volume ed. San Francisco, CA: Benjamin Cummings, 2005, p. 658, figure 28.1.3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Table 28.1Table of symmetry elements and their corresponding operations removed for copyright reasons.See Engel, T., and P. Reid. Physical Chemistry. Single volume ed. San Francisco, CA: Benjamin Cummings, 2005, p. 658, table 28.1.3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Group Therapy…A group G is a finite or infinite set of elements A, B, C, D…together with an operation “☼” that satisfy the four properties of:1. Closure: If A and B are two elements in G, then A☼B is also in G.2. Associativity: For all elements in G, (A☼B) ☼C==A☼ (B☼C).3. Identity: There is an identity element I such that I☼A=A☼I=A for every element A in G.4. Inverse: There is an inverse or reciprocal of each element. Therefore, the set must contain an element B=inv(A) such that A☼inv(A)=inv(A) ☼A=I for each element of G.3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Examples• Integer numbers, and addition• Integer numbers, and multiplication• Real numbers, and multiplication• Rotations around an axis by 360/nFigure 17.3Image of mirror planes in a water molecule removed for copyright reasons.See Engel, T., and P. Reid. Physical Chemistry. Single volume ed. San Francisco, CA: Benjamin Cummings, 2005, p. 663, figure 28.3.3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Figure by MIT OCW.3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Figure by MIT OCW.3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)Table 17.3Multiplication Table for Operators of the C2VGroup removed for copyright reasons. See Engel, T., and P. Reid. Physical Chemistry. Single volume ed. San Francisco, CA: Benjamin Cummings, 2005, p. 666, table 28.3.3.012 Fundamentals of Materials Science: Bonding - Nicola Marzari (MIT, Fall 2005)D2h(dihedral)Image of the Symmetry elements of the D2hgroup in ethene removed for copyright reasons. See Engel, T., and P. Reid. Physical Chemistry. Single volume ed. San Francisco, CA: Benjamin Cummings, 2005, p. 682, figure
View Full Document
Unlocking...