Solid State Magnetism: Calculating N2/N1 and T for 99% Ground State Population

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Homework Help Overview

The discussion revolves around a problem in solid state magnetism, specifically concerning the calculation of the relative concentration of electron states population for V^{4+} ions in a magnetic field at low temperature. Participants are tasked with determining the ratio \(\frac{N_2}{N_1}\) and the temperature required for 99% of ions to be in the ground state.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the definitions of quantum numbers S, L, and J, questioning the values provided in a referenced solution. There is a focus on the implications of the electronic configuration 3d^1 and the appropriate values for angular momentum in this context.

Discussion Status

The discussion is ongoing, with participants expressing skepticism about the values of J and L in the provided solution. Some suggest that the solution may contain errors, while others are attempting to clarify the definitions and assumptions regarding the quantum states involved.

Contextual Notes

There is uncertainty regarding the interpretation of L as it relates to the d orbital configuration and whether it should be considered frozen in the crystal structure. The original poster references a book solution that may not align with the participants' understanding.

Petar Mali
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Homework Statement


On crystal which containing ions V^{4+}, electronic configuration 3d^1, was applied magnetic field B_0=2,5T.

If the temperature is 1K, find the relative concentration of electron states population \frac{N_2}{N_1}.

In what temperature we should expect 99% ions in ground state?

Homework Equations


m_J=\pm J

E=\pm \mu_B B_0

\frac{N_2}{N_1}=e^{-\frac{\Delta E}{k_B T}

g=1+\frac{J(J+1)+S(S+1)-L(L+1)}{2J(J+1)}

The Attempt at a Solution



I have some solution of this problem but I don't understand it.

In solution

S=\frac{1}{2}, L=3, J=\frac{1}{2}
Why?

They get g=2

If I have configuration 3d^1

then

z=1, l=2

S=S_{max}=\frac{z}{2}=\frac{1}{2}

L=L_{max}=S_{max}(2l+1-z)=2

J=|L-S|=\frac{3}{2}

And the basic term is

^2D_{\frac{3}{2}}

How they get L=3,J=\frac{1}{2}?
\frac{N_2}{N_1}=e^{-\frac{\Delta E}{k_BT}}=e^{-\frac{2\mu_BB_0}{k_BT}}=0,035

From the text of problem - In what temperature we should expect 99% ions in ground state?

\frac{N_2}{N_1}=0,01

ln(\frac{N_2}{N_1})=-\frac{\Delta E}{k_B T}

T=-\frac{\Delta E}{k_B ln(\frac{N_2}{N_1})}=0,7K

So my fundamental problem is how they get

S=\frac{1}{2}, L=3, J=\frac{1}{2}

Thanks for your answer!
 
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Where did you get that solution? I don't think it is possible to have J=1/2, when S=1/2 and L=3. The only possible J's are J = 5/2 and 7/2 for that choice of S and L.

Also, you never say what the N2 and N1 states are.
 
Last edited:
From some book. They write L=3 but I suppose they use L=0 but I don't know why? That they use for d orbital. They say something like L is frosen?!
 
Does this book solution have more than one electron? I believe the L=2 like you said originally, not sure what solution you are reading.
 
You have text of problem in my first post. In solution in book is mistake I think.

They write in solution

S=\frac{1}{2}

L=3 (L is frosen in crystal)

and they write then

J=\frac{1}{2}

In solution they do like this only for d orbitals.
 

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