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1-5: The Meaning of the Wave Function |
As learned on
the page 1-3,
the fundamental equation
of quantum mechanics
is the Schroedinger equation.
It was introduced
as a wave equation
which did not contradict
the relation between
the energy and the momentum
of a particle
in classical mechanics.
As a result,
the wave function
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became a complex number.
This looked quite strange,
because using a complex number
for a physical quantity
could not be accepted.
Then, what does
the wave function mean?
As for the interpretation
of the wave function,
various ideas were proposed.
Among them,
the probability interpretation
proposed by
M. Born
(Germany, UK, 1882 - 1970)
has been accepted
to be the most orthodox,
and all the theories
of quantum mechanics are constructed
on the basis
of this interpretation.
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[The Probability Interpretation of the Wave Function]
Suppose a small volume
(box)
dV = dx dy dz
with three edges of
dx ,
dy ,
and
dz
at a coordinate point
r = (x , y , z )
in a three-dimensional space.
(See the figure below.)
Let the probability
that a particle
will be found in this volume
at a time t
be
P (x,y,z,t )dxdydz.
The function
P (x,y,z,t )
is considered as the probability
in the unit volume
in the neighborhood
of the point
(x,y,z),
and is sometimes called
the probability density.
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[N.B.]
In the above discussion,
the word, "probability"
was used.
This however does not mean
that the particle,
e.g. an electron,
exists in a form
of a "particle" or "corpuscle"
and this particle moves
in accordance with
the degree of probability.
An electron is
neither mere "particle"
nor mere "wave".
An electron exists
with particle-wave
duality.
The word "probability" used
above denotes the chance
that the particle
will be found
in the volume
dV
when it is detected.
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Born's probability
interpretation claims that
the probability density
that a particle
will be found
is equal to the square
of the absolute value
of the wave function.
Namely, the probability
that the particle will be found
in the small volume
dV
shown in the above figure
is considered to be
Although the wave function
is a complex number in general,
the square of the absolute value of it
is always positive (or zero),
and we have no difficulty.
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[Normalization of the Wave Function]
At an arbitrary time,
the particle should exist
somewhere in the whole space.
The total probability
that the particle
will be found somewhere
must therefore be 100 %.
This total probability
is obtained by integrating
Eq. (1) over the whole space.
Accordingly,
the wave function
should satisfy
the normalization condition
A solution of the
Schroedinger equation,
does not always satisfy
this normalization condition
(2).
We therefore have to
normalize the wave function
so that it satisfies
the normalization condition.
Let
be a solution of the
Schroedinger equation.
A function obtained
by multiplying
an arbitrary non-zero constant
C
to the
,
i.e.,
,
is also a wave function
satisfying the same
Schroedinger equation.
Therefore we can normalize
the wave function
by arranging the normalization constant
C
to make
satisfy the normalization condition
(2).
It is easy to see
that the normalization constant
is given by
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On the one hand,
in the classical theory,
we can precisely
determine the
orbit (or trajectory)
and the momentum of a particle
all over the time
by using Newtonian
equation of motion.
On the other hand,
the Schroedinger equation
in quantum mechanics
determines the
wave function
from which we
can derive only
the probability
that a particle
will be found somewhere.
You may feel
that this is not
entirely satisfactory.
However, this is necessary
and sufficient
in order to describe
the microscopic world.
This is enough
from the point of view
of Heisenberg's
uncertainty principle.
You will gradually
be able to understand this
through this Seminar.
A typical proof of
the correctness
of the probability interpretation
of the wave function
will be shown
in the following page.
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