P460 - atoms1 Multi-Electron Atoms - Energy Levels and the Periodic Table can’t solve S.E. exactly --> use approximations Hartree theory (central field.

Slides:



Advertisements
Similar presentations

Advertisements

PY3P05 Lecture 8-9: Multi-electron atoms oAlkali atom spectra. oCentral field approximation. oShell model. oEffective potentials and screening. oExperimental.
Calculations of Characteristic X Ray Energies and Wavelengths and the PIXE Spectrum Physics 100 – PIXE – F06.
Physics 1161: Lecture 23 Models of the Atom Sections 31-1 –
CHAPTER 9 Beyond Hydrogen Atom
P460 - atoms II1 Energy Levels and Spectroscopic States in Atoms Only valence electrons need to be considered (inner “shield” nucleus) Filled subshells.
WAVE MECHANICS (Schrödinger, 1926) The currently accepted version of quantum mechanics which takes into account the wave nature of matter and the uncertainty.
P460 - Helium1 Multi-Electron Atoms-Helium He + - same as H but with Z=2 He - 2 electrons. No exact solution of S.E. but can use H wave functions and energy.
CHEMISTRY The Molecular Nature of Matter and Change 3 rd Edition CHAPTER 8 LECTURE NOTES Electron Configuration and Chemical Periodicity Chem Ken.
3D Schrodinger Equation
P460 - Helium1 Multi-Electron Atoms Start with Helium: He + - same as H but with Z=2 He - 2 electrons. No exact solution of S.E. but can use H wave functions.
Atomic physics PHY232 Remco Zegers Room W109 – cyclotron building
P461 - Molecules1 MOLECULES BONDS Ionic: closed shell (+) or open shell (-) Covalent: both open shells neutral (“share” e) Other (skip): van der Waals.
P460 - many particles1 Many Particle Systems can write down the Schrodinger Equation for a many particle system with x i being the coordinate of particle.
Chapter 41 Atomic Structure.
Tentative material to be covered for Exam 2 (Wednesday, October 27) Chapter 16Quantum Mechanics and the Hydrogen Atom 16.1Waves and Light 16.2Paradoxes.
Chapter 3 The Structure of the Atom In order to explain much of what is observed in chemistry, we need to adopt a model for the atom where the atom has.
Chapter 41 Atomic Structure
Atomic Structure and Periodicity. Atoms ProtonsNeutronsElectrons 1. Where are the electrons 2. Do they have different energies.
1 Chapter 7 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Quantum Theory and the Electronic Structure of.
Atomic Orbitals, Electron Configurations, and Atomic Spectra
Ch 9 pages Lecture 23 – The Hydrogen Atom.
P D S.E.1 3D Schrodinger Equation Simply substitute momentum operator do particle in box and H atom added dimensions give more quantum numbers. Can.
Quantum Theory and the Electronic Structure of Atoms Chapter 7 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
1 Chapter 7 Part 2 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Quantum Theory and the Electronic Structure.
1 Physical Chemistry III ( ) Chapter 3: Atomic Structure Piti Treesukol Kasetsart University Kamphaeng Saen Campus.
Bohr and Quantum Mechanical Model Mrs. Kay Chem 11A.
Department of Chemistry and Biochemistry CHM Reeves CHM 101 – Chapter Six The Wave Nature of Light Quantized Energy and Photons Line Spectra and.
Quantum Mechanics and Atomic Theory Wave models for electron orbitals.
LECTURE 21 THE HYDROGEN AND HYDROGENIC ATOMS PHYSICS 420 SPRING 2006 Dennis Papadopoulos.
7.1: Electromagnetic Radiation
Solid State Chemistry Chapter 3 Atomic Structure and Spectra.
CHAPTER 6: ELECTRONIC STRUCTURE. – The Nature of Light – Quantized Energy/Photons –Photoelectric Effect – Bohr’s Model of Hydrogen – Wave Behavior of.
Models of the Atom Physics 1161: Lecture 23 Sections 31-1 – 31-6.
Chem The Electronic Structure of Atoms Classical Hydrogen-like atoms: + - Atomic Scale: m or 1 Å Proton mass : Electron mass 1836 : 1 Problems.
Quantum Theory and the Electronic Structure of Atoms Chapter 7.
Quantum Atom. Problem Bohr model of the atom only successfully predicted the behavior of hydrogen Good start, but needed refinement.
Chapter 28:Atomic Physics
Atomic Quantum Mechanics - Hydrogen Atom ( ) Assuming an atom doesn’t move in space (translate), the SE is reduced to solving for the electrons.
Multi-Electron Atoms. Complete Description of a Ground State Wavefunction ψ A total of three quantum numbers appear from the solution of n = principal.
Last hour: Electron Spin Triplet electrons “avoid each other”, the WF of the system goes to zero if the two electrons approach each other. Consequence:
Atomic Structure and Atomic Spectra
Lecture 11. Hydrogen Atom References Engel, Ch. 9
Physics 361 Principles of Modern Physics Lecture 23.
Ch 10. Many-Electron Atoms MS310 Quantum Physical Chemistry - Schrödinger equation cannot be solved analytically - Schrödinger equation cannot be solved.
Section 3: Modern Atomic Theory
Quantum Theory and the Electronic Structure of Atoms Chapter 6.
Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Chemistry FIFTH EDITION Chapter 7 Atomic Structure and Periodicity.
CHM 108 SUROVIEC SPRING 2014 Periodic Properties of the Elements.
Lecture 9. Many-Electron Atoms
Part 2: Many-Electron Atoms and the Periodic Table.
So that k k E 5 = - E 2 = = x J = x J Therefore = E 5 - E 2 = x J Now so 631.
PHY 752 Solid State Physics
Chapter 41 Atomic Structure
Chapter 29 Atomic Physics.
What value of wavelength is associated with the Lyman series for {image} {image} 1. {image}
Identical Particles We would like to move from the quantum theory of hydrogen to that for the rest of the periodic table One electron atom to multielectron.
MOLECULES BONDS Ionic: closed shell (+) or open shell (-)
Electron Configuration
Chapter 41 Atomic Structure
Hartree-Fock Self Consistent Field Method
Multielectron Atoms The quantum mechanics approach for treating multielectrom atoms is one of successive approximations The first approximation is to treat.
Last hour: Hartree-Fock Self-Consistent Field (HF-SCF) Method
Chemistry Department of Fudan University
Section 3: Modern Atomic Theory
Hartree Self Consistent Field Method
Section 3: Modern Atomic Theory
Chapter 8: Periodic properties of the elements
Presentation transcript:

P460 - atoms1 Multi-Electron Atoms - Energy Levels and the Periodic Table can’t solve S.E. exactly --> use approximations Hartree theory (central field model) for n-electron at0ms. Need an antisymmetric wave function (1,2,3 are positions; i,j,k…are quantum states) while it is properly antisymmetric for any 1 j practically only need to worry about valence effects

P460 - atoms2 Schrod. Eq. For multi-electron have kinetic energy term for all electrons and (nominally) a complete potential energy: Simplify if look at 1 electron and sum over all the others --> ~spherically symmetric potential as filled subshells have no (theta,phi) dependence. Central- Field Model. Assume:

P460 - atoms3 Multi-electron Prescription “ignore” e-e potential….that is include this in a guess at the effective Z energy levels can depend on both n and L wavefunctions are essentially hydrogen-like 1guess at effective Z: Z e (r) 2solve (numerically) wave equation 3fill energy levels using Pauli principle 4use wavefunctions to calculate electrons’ average radii (radial distribution) 5redetermine Z e (r) 6go back to step 2

P460 - atoms4 First guess Look at electron proability P(r). Electrons will fill up “shells” (Bohr-like) assume all electrons for given n are at the same r with a V n for each n. Know number of electrons for each n. One can then smooth out this distribution to give a continuous Z(r) P(r) radius N=1 n=2 n=3 ZnZn radius Z-2 Z-8 Z-18

P460 - atoms5 Argon Z=18 First shell n=1 1S Z1 ~ 18-2 = 16 Second shell n=2 2S,2P Z2 ~ = 8 Third shell n=3 3S,3P Z3 ~ /4 = 4 for the outermost shell…good first guess is to assume half the electrons are “screening”. Will depend on where you are in the Periodic Table Use this to guess energy levels. ZnZn radius Z(r)

P460 - atoms6 Atomic Energy Levels After some iterations, get generalizations Afor the innermost shell: BOutermost shell atoms grow very slowly in size. The energy levels of the outer/valence electrons are all in the eV range

P460 - atoms7 Comment on X-ray Spectra If one removes an electron from an inner orbit of a high Z material, many transitions occur as other electrons “fall” as photon emitted, obey “large” energies so emit x-ray photons. Or need x- ray photons (or large temperature) to knock one of the electrons out can use the proportion of ionized atoms to measure temperature: Fe+ vs Fe++ vs Fe+++ vs Fe++++ study of photon energy gives effective Z for inner shells