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the total energy of matter related to the frequency ν of the wave is
E=hν
the momentum of matter related to the wavelength λ of the wave is
p=h/λ
3.1 Matter wave: de Broglie
Ex: (a) the de Broglie wavelength of a baseball moving at a speed v=10m/s, and m=1kg. (b) for a electron K=100 eV.
)baseball()electron(
2.1106.1100101.92/106.6
2// (b)
106.6106.6)101/(106.6/ (a)
193134
253534
o
o
A
mKhph
Amph
Chapter 3 de Broglie’s postulate: wavelike properties of particles
Chapter 3 de Broglie’s postulate: wavelike properties of particles
The experiment of Davisson and Germer
(1) A strong scattered electron beam is detected at θ=50o for V=54 V.
(2) The result can be explained as a constructive interference of waves scattered by the periodic arrangement of the atoms into planes of the crystal.
(3) The phenomenon is analogous to the Bragg-reflections (Laue pattern).
1927, G. P. Thomson showed the diffraction of electron beams passing through thin films confirmed the de Broglie relation λ=h/p. (Debye-Scherrer method)
Bragg reflection:
Chapter 3 de Broglie’s postulate: wavelike properties of particles
constructive interference:
)wavelength (electron
65.1106.154101.92/106.6
2/
eV 54 electronfor
)wavelength ray-(X
65.165sin91.02sin2
1for
652/90 and 50 , 91.0
sin2
193134o
oo
oooo
A
mKh
K
Ad
n
Ad
nd
consistent
Chapter 3 de Broglie’s postulate: wavelike properties of particles
Debye-Scherrer diffraction
X-ray diffraction: electron diffraction : zirconium oxide crystal gold crystal
Laue pattern of X-ray (top) and neutron (bottom) diffraction for sodium choride crystal
3.2 The wave-particle duality
Chapter 3 de Broglie’s postulate: wavelike properties of particles
Bohr’s principle of complementarity: The wave and particle models are complementary; if a measurement proves the wave character of matter, then it is impossible to prove the particle character in the same measurement, and conversely
Einstein’s interpretation: for radiation (photon) intensity
is a probability measure of photon density
)/1( 220 NNhcI
2
Max Born: wave function of matter is just as satisfies wave equation
is a measure of the probability of finding a particle in unit volume at a
given place and time. Two superposed matter waves obey a principle of
superposition of radiation.
),( tx
2
Chapter 3 de Broglie’s postulate: wavelike properties of particles
3.3 The uncertainty principle
Heisenberg uncertainty principle: Experiment cannot simultaneously determine the exact value of momentum and its corresponding coordinate.
2/
2/
tE
xpx
Bohr’s thought experiment2/2
)/(/
2/22/ (2)
2/2sin/sin)/2(
)/ ( sin/
sin)/2(sin2 (1)
2
''
'
''
hxptE
ptxEtxvtvx
pvmppEmpE
hhxp
ax
hpp
x
xxx
xxxxx
x
x
Bohr’s thought experiment:
a diffraction apparatus
Chapter 3 de Broglie’s postulate: wavelike properties of particles
3.4 Properties of matter wave
wave propagation velocity:
Why? 2
2/)()(
2
vwv
mv
mv
p
E
h
E
p
hw
a de Broglie wave of a particle
)(2sin),(
1/set )/(2sin),(
txtx
txtx
(1) x fixed, at any time t the amplitude is one, frequency is ν.
(2) t fixed, Ψ(x,t) is a sine function of x.
(3) zeros of the function are at
these nodes move along x axis with a velocity
it is the node propagation velocity (the oscillation velocity)
tnxtnx
nntx
nn
n
)/(2/2/
,.......2,1,0 )(2
// dtdxw n
modulate the amplitude of the waves
Chapter 3 de Broglie’s postulate: wavelike properties of particles
2/
2/ is wave the of velocity group the (2)
/ is wave individual the of velocity the (1)
)(2sin]22
cos[2 ),(2 and 2for
]2
)2(
2
)2([2sin]
22cos[2),(
])()[(2sin),( ),(2sin),(
),(),(),(
21
21
d
dν
dκ
dνg
w
txtd
xd
txdd
td
xd
td
xd
tx
tdxdtxtxtx
txtxtx
group velocity of waves equal to moving velocity of particles
vg
vdp
dEmvdvdEmvpmvE
dp
dE
hdp
hdE
d
dg
h
dpd
h
p
h
dEd
h
E
2
1
/
/
1
2
Chapter 3 de Broglie’s postulate: wavelike properties of particles
The Fourier integral can prove the following universal properties
of all wave. 4/1 and ,1/for 4/1 tx
:wavematter for hphp //1/
2/
)/1()/(/
2/
4/1)/1()/(
tE
EthhEthEhE
xp
pxhhpxx
uncertainty principle
uncertainty principle
the consequence of duality
Ex: An atom can radiate at any time after it is excited. It is found that in a typical case the average excited atom has a life-time of about 10-8 sec. That is, during this period it emit a photon and is deexcited. (a) What is the minimum uncertainty in the frequency of the photon? (b) Most photons from sodium atoms are in two spectral lines at about . What is the fractional width of either line, (c) Calculate the uncertainty in the energy of the excited state of the atom. (d) From the previous results determine, to within an accuracy , the energy E of the excited state of a sodium atom, relative to its lowest energy state, that emits a photon whose wavelength is centered at
Chapter 3 de Broglie’s postulate: wavelike properties of particles
o
A5890?/ E
eV 1.2)//(//hh/ (d)
state the of width theeV 103.3104
1063.6
4
4/ (c)
line spectral the of width natural 106.1101.5/108/
sec 101.5105890/103/ (b)
sec 1084/14/1 (a)
88
34
8146
-114810
-16
EEEEt
h
t
hE
c
tt
E o
A 5890
uncertainty principle in a single-slit diffraction
for a electron beam:
Chapter 3 de Broglie’s postulate: wavelike properties of particles
2
sin
sin ,sin
hyy
hyp
y
pppp
p
p
y
y
yy
y
Chapter 3 de Broglie’s postulate: wavelike properties of particles
Ex: Consider a microscopic particle moving freely along the x axis. Assume that at the instant t=0 the position of the particle is measured and is uncertain by the amount . Calculate the uncertainty in the measured position of the particle at some later time t.
0x
xtxx
xmtvtx
xmmpv
xp
x
xx
x
or
2/t timeAt
2//
2/0tAt
0
0
0
0
Dirac’s relativistic quantum mechanics of electron: 420
22 cmpcE
Dirac’s assumption: a vacuum consists of a sea of electrons in
negative energy levels which are normally filled at all points in space.
Some consequences of the uncertainty principle:
(1) Wave and particle is made to display either face at will but not both
simultaneously.
(2) We can observe either the wave or the particle behavior of radiation;
but the uncertainty principle prevents us from observing both together.
(3) Uncertainty principle makes predictions only of probable behavior of
the particles.
Chapter 3 de Broglie’s postulate: wavelike properties of particles
The philosophy of quantum theory:
(1) Neil Bohr: Copenhagen interpretation of quantum mechanics.
(2) Heisenberg: Principally, we cannot know the present in all details.
(3) Albert Einstein: “God does not play dice with the universe”
The belief in an external world independent of the perceiving subject is
the basis of all natural science.