I Why normal Zeeman effect contains three components?

misko
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Can someone explain to me why normal Zeeman effect splits spectral line into three components and not into 4, 5 or any other number?
 
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Do you know the selection rule for the magnetic quantum number?
 
Yes, it can be changed by +1, -1, 0.
 
In normal Zeeman effect, states with different ##m## split, accordingly the transition lines also split according to their value of ##\Delta m##.
 
I know that normal Zeeman effect happens when total spin of electrons in an atom is S=0.
This means that energy levels splitting in external magnetic field is done only on orbital angular momentum.

So for example P orbital will split into three sub-levels with slightly different energies. Now, it make sense to me that if there is transition from P orbital (L=1) to S orbital (L=0) there will be splitting to three components because P is split to three sub-levels and S orbital has no splitting.
But what about transition from say, D to P orbital? D orbital will be split into 5 sub-levels and P orbital will be split to 3 sub-levels so that gives many more combinations for transitions, even when selection rule for magnetic moment is taken into account.
So, (assuming total spin is zero), for D orbital we have J = 2,1,0,-1,-2 and for P orbital there is J=1,0,-1.
Possible transitions are then:
##D_2 \rightarrow P_1##
##D_1 \rightarrow P_1##
##D_0 \rightarrow P_1##

##D_1 \rightarrow P_0##
##D_0 \rightarrow P_0##
##D_{-1} \rightarrow P_0##

##D_0 \rightarrow P_{-1}##
##D_{-1} \rightarrow P_{-1}##
##D_{-2} \rightarrow P_{-1}##

So there are 9 lines here, each respecting the selection rule for magnetic quantum number.
What is wrong in this logic, where is my error in understanding?
 
The formula for the transition energy under Zeeman effect is
$$
\Delta E = \Delta E_0 + \mu_B B \Delta m
$$
where ##\Delta E_0## is the energy difference without magnetic field. As you see the energy difference in the presence of magnetic field only depends on ##\Delta m##. In your example the lines ##d_2 \to p_1## and ##d_1 \to p_0## coincide.
 
I think I am starting to get it now...

So in my example there are 9 transitions but they are grouped such that only 3 different lines are present, right?
If I group transitions that belong to the same line they would be like this:
line 1:
##D_2 \rightarrow P_1##
##D_1 \rightarrow P_0##
##D_0 \rightarrow P_{-1}##

line 2:
##D_1 \rightarrow P_1##
##D_0 \rightarrow P_0##
##D_{-1} \rightarrow P_{-1}##

line 3:
##D_0 \rightarrow P_1##
##D_{-1} \rightarrow P_0##
##D_{-2} \rightarrow P_{-1}##

Is this correct?

Btw, This formula you gave me, it is valid only for normal Zeeman effect right? I mean g-factor is 1 in the formula which applies to singlet states with total spin equal to zero.
 
misko said:
Is this correct?
Yes.

misko said:
This formula you gave me, it is valid only for normal Zeeman effect right? I mean g-factor is 1 in the formula which applies to singlet states with total spin equal to zero.
Yes.
 
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