●OPERATOR :-
Operator is a function over the state of system OR operator is mathematical rule in physics , when it apply on a state |Ψ > then it can be change and provide same value of state , An observable ca be represented by ' ^ ' to convert into operator ,
x = x^
●Types of operator :-
Generally operator are many types , we discussed about few important types ,
1. Linear operator :-
If two operator A^ and B^ are following such relation
( A^ +B^ )|Ψ> = A^| Ψ > + B^| Ψ >
2. Null operator :-
If a operator O^ apply on a state |Ψ > then we get zero of its value .
O^ | Ψ > = 0
3. Unit operator :-
If an operator I^ apply on a state | Ψ > After operating operator it state remains same and it gives unit value then this operator is known as unit operator . It is represented by -
I^ | Ψ > = | Ψ >
4. Hermitian operator :-
Ifan operator following such relation then it's operator known as hermitian operator .
(A^)+ = A^
A+ is represented degar of operator A^
Two operator A^ and B^ are Hermitian operator then there product A^B^ is also Hermitian operator if and only if A^ and B^ commute.
Given , A^ is Hermitian operator
( A^)+ = A^ -----( 1 )
B^ is Hermitian operator
(A^)+ = A^ -----( 2 )
( A^B^ )+ = A^B^ ---------( 3 )
Now take L. H. S. From equation ( 3 )
( A^B^ )+ = (B^+) (A^+)
( A^B^ )+ = B^A^ ---------( 4 )
Condition , ( A^ and B^ commute) !
Then , [ A^ B^ ] = 0
[ A^B^ - B^A^ ] = 0
A^B^ = B^A^ ---------( 5 )
Put value in equation ( 4 ) from ( 5 ).
(A^B^)+ = A^B^ = R.H.S.
5. Anti Hermitian operator :-
If operator A^ is following such relation .
A+ = -A
A+ is represented degar of operator A^
6. projection operator :-
If an operator P^ following such relation .
(P^)+ = p^
(P^)² = P^
Then P^ is known as projection operator .
(P^)+ = degar of operator P^
7. Unitary operator :-
An operator U^ is such that ,
(U^)+ = ( U^) inverse ( power -1 )
Then U is known as unitary operator.
U+ is represented degar of operator U^
8. Inverse operator :-
If operator B^ is following such relation .
BA = AB = I^
then B is known as inverse operator of A^ and it can written as
A = B inverse
If operator A is define in matrix form. Then,
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