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Waves, Light & Quanta. Tim Freegarde. Web Gallery of Art; National Gallery, London. Quantum mechanics. particles behave like waves , and vice-versa. energies and momenta can be quantized , ie measurements yield particular results. - PowerPoint PPT Presentation
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22
Quantum mechanics
1. particles behave like waves, and vice-versa
2. energies and momenta can be quantized, ie measurements yield particular results
3. all information about a particle is contained within a complex wavefunction, which determines the probabilities of experimental outcomes
4. deterministic evolution of the wavefunction is determined by a differential (e.g. Schrödinger) wave equation
5. 80 years of experiments have found no inconsistency with quantum theory
6. explanation of the ‘quantum measurement problem’ – the collapse of the wavefunction upon measurement – remains an unsolved problem• non-deterministic
process• Heisenberg’s uncertainty principle
33
Quantum measurement
• allowed energies 22
0
4 1
42 n
meE
en
erg y
0
hcR
4
hcR
n = 1
n = 3
n =
n = 2
1. measured energy must be one of allowed values
2. …but until measurement, any energy possible
3. after measurement, subsequent measurements will give same value
THE HYDROGEN ATOM
QUANTUM MEASUREMENT
44
The experiment with the two holes
x
0
s
a
y
• fringe maxima when
0sin ma a0 fringe spacing
• smallest visible feature size
a illumination wavelength
ahpy illumination momentum• equivalent to change in illumination angle and
hence by 0ppy
00
hp
a a
66
Uncertainty
HEISENBERG’S UNCERTAINTY PRINCIPLE
• certain pairs of parameters may not simultaneously be exactly determined• {position, momentum}
• {time, energy}
• {orientation, angular momentum}• {intensity, phase}
• {x, y}, {x, z}, {y, z} components of angular momentum
• {position, wavelength}
• {time, frequency}
• {linear, circular} polarization
• conjugate parameters cannot be simultaneously definite
1111
Terminology
UNCERTAINTY IN MEASUREMENT
• repeated experiment yields range of results
• expectation value = mean n
nan
a1
n
na aan
a222 1• uncertainty = standard
deviation
• before measurement, system was in a superposition
• probability of given result given bya 2a
1212
Uncertainty
• conjugate parameters cannot be simultaneously definite
QUANTUM MEASUREMENT
• measurement changes observed system so that parameter measured is subsequently definite
• process measure A, measure B not the same as measure B, measure A• measure A, measure B are not commutative / do not commute
• commutator [measure A, measure B] 0
HEISENBERG’S UNCERTAINTY PRINCIPLE
• certain pairs of parameters may not simultaneously be exactly determined• {position, momentum}
• {time, energy}
• {orientation, angular momentum}• {intensity, phase}
• {x, y}, {x, z}, {y, z} components of angular momentum
• {position, wavelength}
• {time, frequency}
• {linear, circular} polarization
1313
The LASER
by Stimulated Emission of Radiation
LIGHT AMPLIFICATION
• Theodore Maiman, 16 May 1960
beam splitter
flash tube
mirror
ruby
693.4 nm
light amplifier
optical resonator
1414
Absorption and emission of photons
ABSORPTION
en
erg y
0
hcR
4
hcR
n = 1
n = 3
n =
n = 2
absorption emission
EMISSIONSPONTANEOUS
ABSORPTIONEMISSION
STIMULATED
1121
d
dNB
t
N
1
2
1
2
1
1
2212
d
dNA
t
N
1515
Absorption and emission of photons
ABSORPTIONEMISSION
SPONTANEOUS
ABSORPTIONEMISSION
STIMULATED
1121
d
dNB
t
N
1
2
1
2
1
1
2212
d
dNA
t
N
2212
d
dANNNB
t
N
EINSTEIN EQUATIONS
NNN 21
• spontaneous emission stimulated by vacuum field
• amplification of light if atomic population is inverted i.e. 12 NN
• thermal equilibrium blackbody
spectrum
• Einstein A and B coefficients
1616
The ruby LASER
beam splitter
flash tube
mirror
ruby
693.4 nm
light amplifier
optical resonator
en
erg y
absorption emission
Cr3+
• Cr3+ ions in sapphire (Al2O3) absorb blue and green from flash light
• internal transitions to metastable state
metastable
• spontaneous emission is amplified by passage through ruby
• repeatedly reflected/amplified near-axial light builds up to form coherent laser beam
1717
Laser beam characteristics
beam splitter
flash tube
mirror
ruby
693.4 nm
• as initial source recedes down unfolded cavity, emission approaches that from distant point source
• long pulse continuous wave (c.w.)
• narrow linewidth for long pulses ( )
1 t• noise from spontaneous emission gives lower limit to
linewidth• nonlinear processes have various effects in detail
• divergence determined by diffraction by limiting aperture
• Hecht section 13.1
• focusable
• monochromatic
• constructive interference between reflections for certain wavelengths