postulates of Quantum mechanics (2 and 3)
In our previous meeting we discussed the postulate # 1 of Quantum mechanics, In this blog we will further our understanding about postulate # 2 and postulate # 3.
Postulate #
2
Statement:
Allowed
values of the measurements of observable “a” are given by eigenvalues of
operator “A” associated with the observable.
Explanation:
When an operator is applied on any
observable and if it gives back the same observable times a constant, then the
constant will be called the value of the observable.
The constant
is also called the eigenvalue of the equation. And the equation as a whole is
called eigenvalue equation.
Mathematically:
Ậ (f(x)) = c f(x)
------------- (2)
Where
Ậ
is any operator
f(x) is any function
c is a constant, this is called
eigenvalue.
we see in equation (2) that we are getting the same original function f(x) even after applying the operator on L.H.S of the equation. we are getting a constant as an additional term.
we see in equation (2) that we are getting the same original function f(x) even after applying the operator on L.H.S of the equation. we are getting a constant as an additional term.
Equation (2) is called the eigenvalue
equation as it contains the eigenvalue of the observable.
Postulate 3:
Statement:
For every system, there exists a state function
“ᴪ” that contains all the information about the
system.
Facts about ᴪ:
The symbol ᴪ has impressed me when I was enrolled as an
undergraduate student . here are few important point which are obligatory , (I
should say), to know, these are
· ᴪ is called the wave function.
·
ᴪ is a function of spatial coordinates
·
ᴪ can be a complex number.
_ __ _ ___ ___ __ _
Your
feedback and question will be appreciated.
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