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Physics II

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Title: Physics II


1
Physics II
  • DeBroglie waves

2
Reference
  • Max Born, Atomic Physics, Dover, 1969

3
A prince of a fellow
  • Prince Debroglies (1929) Nobel lecture

4
An extraordinary thesis
5
Motivations
  • By 1925, the year of DeBroglies work
  • The wave-particle duality of light was well known
    (but still inexplicable)
  • Einsteins Special Theory of Relativity was
    well-known

6
DeBroglie leaned heavily on Einsteins work
  • Energy of photon E hf
  • Invariance of 4-vectors, esp. energy-momentum 4
    vector
  • (p, E)
  • p2c2 E2 invariant for a given system
  • Assign same dualism to particles that had been
    attached to light

7
Reasoning by analogy
  • For photon, E hf, so assign a frequency to a
    particle with energy E in the same fashion.
  • To be consistent with special relativity we argue
    that we can assign momentum by phk
  • Treat space and time on equal footing
  • Since f is number of vibrations in unit time,
    then k must be the number of waves per unit
    length
  • k 1/?
  • Then p h / ?
  • The famed DeBroglie wavelength

8
One-dimension DeBroglie waves
  • Plane wave of momentum p and energy E moving
    along the x axis
  • U(x,t) Aexp2pi(Et px)/h
  • U(x,t) A exp2pi(ft kx)

9
Phase velocity
  • The locus of waves of constant phase moves at
    the phase velocity
  • Constant phase ft kx constant
  • d (ft kx) / dt d (constant) / dt
  • f kdx/dt 0
  • dx / dt f/k ? / T f ?
  • Since frequency often depends on wavelength these
    waves show dispersion (ala white light passing
    through a prism)

10
Phase velocity is artificial
  • Phase velocity is a purely artificial concept
    since we cannot measure it (a positivist view)
  • We cannot mark an infinite plane wave of fixed
    frequency w/o superimposing another wave train on
    the plane wave to make a bump on it which we
    can follow
  • The bump moves at the group velocity

11
Group velocity
  • To the original wave we literally add a similar
    wave of slightly different frequency and
    wavelength (f and ?)
  • We will end up with a wave which has an amplitude
    that varies ala beat notes used in tuning
    guitars, etc.
  • We follow the maximum of this varying amplitude
    as our marker

12
Results
  • The resulting wave of superpositions moves at a
    phase velocity of (f f)/(k k)
  • If f and k are very near f and k, this is close
    to the original phase velocity f / k
  • The group (beat maximum) moves at a speed (f
    f) / (k k)
  • As superposed wave approaches identicality with
    original wave, this becomes df / dk
  • df /dk df / d(1/) - (1 / ? )2 df / d ?

13
Hokey justification to Bohrs quantum condition
  • Fit integral number of deBroglie waves into
    circumference of allowed circular orbits
  • To assure constructive interference
  • n ? 2pr
  • Plug in DeBroglie
  • nh/p 2pr
  • nh / (mv) 2pr
  • L mvr n (h / 2p )

14
Davison-Germer and GP Thomson
  • These gentlemen performed experiments
    demonstrating interference of electrons, as close
    as one can get to nailing down a wave nature of
    something.
  • GP got Nobel prize for showing electron is a wave
  • His daddy JJ won prize years earlier for showing
    electron is a particle
  • Sic transit gloria mundi

15

16
Group velocity
17
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