States of an atom in spectral notation

In summary, the possible states of an atom with a closed core and one d electron can be expressed in spectral notation as 2 D 5/2 and 2 D 3/2. The total angular momentum quantum number (J) can be calculated by adding the orbital angular momentum quantum number (L) and the spin angular momentum quantum number (S) and then finding the absolute difference between them. The number of possible states for a given value of J can differ by steps of one.
  • #1
Amith2006
427
2

Homework Statement



1)Give in spectral notation the possible states of an atom which has a closed core plus one d electron.


Homework Equations





The Attempt at a Solution



I solved in the following way:
For d electron,
Orbital angular momentum quantum number(L)=2
Spin angular momentum quantum number(S)=1/2
Possible values of total angular momentum quantum number(J)= L+S,| L+S-1|,…,|L+S|
Hence,
J= (2+1/2), |2+1/2-1|,|2-1/2|
J= 5/2,3/2,1/2
Possible states of the atom in spectral notation are,
2 D 5/2, 2 D 3/2, 2 D ½
But the answer given in my book is 2 D 5/2, 2 D 3/2.
 
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  • #2
Amith2006 said:

Homework Statement



1)Give in spectral notation the possible states of an atom which has a closed core plus one d electron.


Homework Equations





The Attempt at a Solution



I solved in the following way:
For d electron,
Orbital angular momentum quantum number(L)=2
Spin angular momentum quantum number(S)=1/2
Possible values of total angular momentum quantum number(J)= L+S,| L+S-1|,…,|L+S|
Hence,
J= (2+1/2), |2+1/2-1|,|2-1/2|
J= 5/2,3/2,1/2
thisis where your mistake is...

(2+1/2) = 5/2

|2+1/2-1| = 3/2

|2-1/2| = 3/2
 
  • #3
nrqed said:
thisis where your mistake is...

(2+1/2) = 5/2

|2+1/2-1| = 3/2

|2-1/2| = 3/2

Sorry,I meant J=|L+S-2| =|2+1/2-2|=1/2 instead of J=|L+S-1|=3/2
Is there something to do with the multiplicity of states given by 2S+1 = 2 so that for a given value of J there are only 2 possible values L+S and L-S?
 
Last edited:
  • #4
Amith2006 said:
Sorry,I meant J=|L+S-2| =|2+1/2-2|=1/2 instead of J=|L+S-1|=3/2
Is there something to do with the multiplicity of states given by 2S+1 = 2 so that for a given value of J there are only 2 possible values L+S and L-S?

I think you misunderstand the rule. You calculate L+S and then you calculate |L-S|. J may take any value between those two extremes, differing by steps of one.

In your example, L+S = 5/2 and |L-S| = |2-1/2| = 3/2.

So the possible values of J are 3/2 and 5/2. J=1/2 is not possible.

Of course, you can check that the number of states comes out right. L=2 has 5 states and S=1/2 has two states so the total number of states is 10.

Now, J=5/2 has 6 states and J=3/2 has 4 states so the total number checks out.
 
  • #5
Thats cool!Thanx.
 

1. What is the definition of spectral notation?

Spectral notation is a type of shorthand used to represent the various energy states of an atom. It uses letters, numbers, and subscripts to indicate the energy level, orbital type, and number of electrons in an atom.

2. How do you determine the energy level of an atom using spectral notation?

The energy level of an atom can be determined by the letter associated with it in spectral notation. The letter "K" represents the first energy level, "L" represents the second energy level, and so on.

3. What do the subscripts in spectral notation represent?

The subscripts in spectral notation represent the number of electrons in each energy level and orbital type. For example, the subscript "2" in the notation 2p6 indicates that there are 6 electrons in the p orbital of the second energy level.

4. How does spectral notation differ from electron configuration notation?

Spectral notation is a simplified version of electron configuration notation. While electron configuration notation provides a detailed breakdown of the electrons in an atom, spectral notation only shows the number of electrons in each energy level and orbital type.

5. Why is spectral notation useful in studying atoms?

Spectral notation is useful because it allows scientists to quickly and easily represent the energy states of atoms without having to write out the full electron configuration. It also helps to visually show the distribution of electrons in an atom, which can aid in understanding its properties and behavior.

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