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Ain Shams U' Faculty of Engineering Mathematics and Engineering Physics Department Quantum Mechanics

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Title: Ain Shams U' Faculty of Engineering Mathematics and Engineering Physics Department Quantum Mechanics


1
Ain Shams U.Faculty of EngineeringMathematics
and Engineering Physics DepartmentQuantum
Mechanics 2
  • ?. ???? ???????
  • ?????? 2004

2
Contents
  • Applications of Schrödinger equation
  • Hydrogen atom
  • Summary of Bohr model.
  • Quantum mechanical solution.
  • Particle in infinite potential well
  • Introduction to band theory
  • What is a quantum well.
  • Solution of Schrödinger equation for the particle
    in infinite quantum well.

3
Websites
  • http//www.colorado.edu/physics/2000/quantumzone/b
    ohr.html
  • http//www.launc.tased.edu.au/online/sciences/phys
    ics/brhydrogen.html
  • http//www.falstad.com/mathphysics.html
  • http//www.physics.nwu.edu/ugrad/vpl/atomic/hydrog
    en.html
  • http//www.falstad.com/qmatom/

4
Atomic spectroscopy
  • What is the problem ?
  • If an atom is exited through heat or bombardment
    with high speed electrons, electromagnetic
    radiation is generated from this atom.
  • When this electromagnetic radiation is analyzed
    (for example through a prism), one finds that it
    is composed of discrete wavelengths.
  • Each element in the periodic table has a unique
    line spectrum.
  • The Hydrogen atom is the simplest case to model
    since it is composed of a single proton and a
    single electron. (applet)

5
Hydrogen atom (Rutherford)
  • Rutherford (1911) proved that the atomic system
    is a miniature solar system, but didnt know why
    the electron orbits should take certain radii.

6
Hydrogen atom (Bohrs assumptions)
  • In addition to the fixed orbits proposed by
    Rutherford, Bohr proposed that
  • The orbits are defined such that the angular
    momentum (mvr) is quantized
  • Electromagnetic radiation occur when an electron
    goes from one allowed orbit to another of lower
    energy

7
Hydrogen atom (Bohrs model results)
  • With a complete classical model (using Coulomb's
    and Newtons laws), Bohr succeeded
  • in calculating the electron energy rotating in
    each orbit. (applet)
  • in calculating the orbits radii

8
Hydrogen atom (Bohrs model results)
  • In calculating all spectrum lines of the Hydrogen
    atom as measured experimentally.

9
Hydrogen atom (Bohrs model failure)
  • This model visualizes the Hydrogen atom as a
    planar system, not a 3-D one.
  • While this model is successful in describing
    other single electron systems such as He and
    Li, it failed to explain systems with multiple
    electrons.

10
Hydrogen atom (QM)
Time independent SE in spherical coordinates
(note the 3-D nature of the problem)
11
Hydrogen atom (QM)
  • Using separation of variable
  • Substituting in SE, one can find an expression
    for R(r),? (?), and ? (?) where each function is
    associated with a unique quantum number,
    resulting in 3 quantum numbers1 quantum number
    for spin.
  • All s states have no angular (?) or azimuthal
    (?) dependence.

12
Hydrogen atom (QM)
13
Hydrogen atom (QM)
  • 2s state

14
  • (applet)

1s state
2s state
15
Hydrogen atom (QM)
  • The probability of finding the electron in a
    spherical shell dV at a distance r from the
    nucleus
  • We define the radial probability density P(r) as

16
Hydrogen atom (QM)
ro
5ro
17
Hydrogen atom (QM)
18
Hydrogen atom (QM)
  • Electron cloud instead of specific orbits.
  • 3-D model for the atom.
  • Applicable for all atomic systems, molecules.

19
Band theory
20
Band theory
  • If N sodium atoms are brought together, each
    atomic level splits into N new level, each level
    accommodates 2 electrons of opposite spin.
  • If one atomic state are fully occupied in all N
    atoms, the corresponding band is full.
  • Since the 3s state in sodium atom has just one
    electron, the corresponding 3s band is half full

21
Band theory
  • The conduction band is partially filled

22
Quantum well
Conduction band
Electrons confined in a finite quantum well
Energy gap
Valence band
23
Finite QW
Energy
  • Electron in a finite quantum well.

24
Infinite QW
?
?
Energy
Distance
Electron in an infinite quantum well.
25
Quantum well Potential well
Particle in a quantum well Particle in a box
26
Infinite potential well
  • This is a problem in 1D space.

27
Infinite potential well
  • In the region 0ltxlta

28
Infinite potential well
B0
29
Infinite potential well
  • Applying the 2nd boundary condition

kan? n1,2,3,
30
Infinite potential well
  • The energy is quantized

31
Infinite potential well
  • Normalization

32
Infinite potential well
  • Normalization

33
Infinite potential well
34
Infinite potential well
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