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PYL100 Electromagnetic Waves and Quantum Mechanics
Continuous Variables
• If I select a random person off the street, the probability that her age is
precisely 16 years, 4 hours, 27 minutes, and 3.333 ... seconds is zero.
• The only sensible thing to speak about is the probability that her age lies in
some interval-say, between 16 and 17.
• If the interval is sufficiently short, this probability is proportional to the
length of the interval.
probability density
The probability that x lies between a and b (a finite interval) is given by
the integral of (x):
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PYL100 Electromagnetic Waves and Quantum Mechanics
Continuous VariablesContinuousDiscrete
8/18/2019 PYL-100-2016-QMLect-02-ProbContEq
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PYL100 Electromagnetic Waves and Quantum Mechanics
Problem
Determine A
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PYL100 Electromagnetic Waves and Quantum Mechanics
NORMALIZATION
is the probability density for finding the particle at point x , at
time t
Is it consistent with Schrödinger equation ?
Schrödinger equation:
(x. t) is a solution A (x. t) is also a solution
You can choose A such that (x. t) satisfy the normalizing condition
Normalizing the
wave function
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PYL100 Electromagnetic Waves and Quantum Mechanics
NORMALIZATION
is the probability density for finding the particle at point x , at
time t
If the integral goes to Infinity or zero?
• Such non-normalizable solutions cannot represent particles, and
must be rejected.
Physically realizable states correspond to the square-integrable
solutions to Schrödinger equation
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PYL100 Electromagnetic Waves and Quantum Mechanics
TIME DEPENDENCE OF NORMALIZATION
is the probability density for finding the particle at point x, at
time t
Suppose I have normalized the wave function at time t = 0.
How do I know that it will stay normalized, as time goes on ?
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TIME DEPENDENCE OF NORMALIZATION
Schrödinger equation
Conjugate
8/18/2019 PYL-100-2016-QMLect-02-ProbContEq
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TIME DEPENDENCE OF NORMALIZATION
(x . t) must go to zero as x goes to () infinity-otherwise the
wave function would not be normalizable.
(x . t) is normalized at t = 0, it stays normalized for all future
time
• Schrödinger equation has the remarkable property that it
automatically preserves the normalization of the wave function.
• Without this crucial feature the Schrödinger equation would be
incompatible with the statistical interpretation, and the whole
theory would crumble
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Probability current
The probability of finding a particle in the range (a < x < b), at time t.
• J : the rate at which probability is "flowing" past the point x .
•
J has the dimensions 1/time, and units seconds−1
.
= (, )
, =
Define probability current
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PYL100 Electromagnetic Waves and Quantum Mechanics
Continuity Equation in Electrodynamics
Charge density Current density
Integrating over a small volume we have
• This shows that any decrease in the charge, in an infinitesimal
volume, must be accompanied by a flux of electric current out ofthe volume.
• In other words, charge has to be locally conserved.
• The total charge of a system is a constant independent of time
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PYL100 Electromagnetic Waves and Quantum Mechanics
Continuity Equation
The Schrödinger equation
in three-dimension
and its complex conjugate
Continuity equation in
Quantum mechanics
( )× Ψ∗
( )× Ψ
Subtracting we get,
Where,
Can be written asWhere, Position probability density
Probability current density
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PYL100 Electromagnetic Waves and Quantum Mechanics
Example
Find the probability current for the wave function:
Answer:
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PYL100 Electromagnetic Waves and Quantum Mechanics
Examples
Ψ , = (−)
, = →
= 0
Find probality current J (x, t)
=ℏ
2 =
ℏ
=
Plane wave function
Consistent with Electrodynamics
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PYL100 Electromagnetic Waves and Quantum Mechanics
Expectation Value
• is the average of measurements performed on particles
all in the state or the average of repeated measurements
on an ensemble of identically prepared (all in state )
systems
• It does not mean that if you measure the position of one
particle over and over again and the average is theexpectation value.
• It is not the most probable value.
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PYL100 Electromagnetic Waves and Quantum Mechanics
Expectation value of the velocity
Postulate: expectation value of the velocity is equal to the time derivative of the expectation
value of position
“Velocity" of ⟨⟩