INGENIA

ATM-12

Spin–orbit interval

E_{SO} = (A/2) [J(J+1) − L(L+1) − S(S+1)]. Landé interval rule.

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StructureSpin–orbit

Governing equation

E=A2[J(J+1)−L(L+1)−S(S+1)]E=\dfrac{A}{2}\bigl[J(J+1)-L(L+1)-S(S+1)\bigr]

J∈[0,5]J \in \left[0, 5\right]

where

A
Interval A (cm^{-1})
L
L (—)
S
S (—)
J
J (—)
E_{SO}
Fine-structure energy (cm^{-1})

The figure, part by part

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ATM-12 · spectrum
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①

Governing law — red

E=A2[J(J+1)−L(L+1)−S(S+1)]E=\dfrac{A}{2}\bigl[J(J+1)-L(L+1)-S(S+1)\bigr]

J∈[0,5]J \in \left[0, 5\right]

J=0J = 0ESO=−27.5E_{SO} = -27.5

②

Domain of the variable — blue

Jmin⁡=0,Jmax⁡=5J_{\min} = 0,\quad J_{\max} = 5

J∈[0,5]J \in \left[0, 5\right]

J=0J = 0J=0J = 0

③

Response curve — green

E=A2[J(J+1)−L(L+1)−S(S+1)]E=\dfrac{A}{2}\bigl[J(J+1)-L(L+1)-S(S+1)\bigr]

J∈[0,5]J \in \left[0, 5\right]

J=0J = 0ESO=−27.5E_{SO} = -27.5

④

Rate of change — amber

dESOdJ\frac{\mathrm{d}E_{SO}}{\mathrm{d}J}

J∈[0,5]J \in \left[0, 5\right]

J=0.031J = 0.031ESO′=10.63E_{SO}^{\prime} = 10.63

Lecture brief

Historical brief

Balmer, Rydberg, Bohr (1913), fine structure, Zeeman and Stern–Gerlach built the spectrum of one atom. The lab computes levels, selection and magnetic splitting. This sheet (ATM-12 — Spin–orbit interval) is the form associated with Spin–orbit. Working symbols: AA, LL, SS, JJ →\rightarrow ESOE_{SO}. A ∝ Z⁴ α² Rydberg. Fine-structure splitting of alkali D lines is this plus core penetration.

Purpose

Purpose: compute ESOE_{SO} from AA, LL, SS, JJ in Atomic physics via E=A2[J(J+1)−L(L+1)−S(S+1)]E=\dfrac{A}{2}\bigl[J(J+1)-L(L+1)-S(S+1)\bigr] E_{SO} = (A/2) [J(J+1) − L(L+1) − S(S+1)]. Landé interval rule. Use it when a real atomic physics question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given A=20.000 cm−1A = 20.000\,\mathrm{cm^-1}, L=1.000 —L = 1.000\,\mathrm{—}, S=0.500 —S = 0.500\,\mathrm{—}, J=1.500 —J = 1.500\,\mathrm{—}, the governing relation E=A2[J(J+1)−L(L+1)−S(S+1)]E=\dfrac{A}{2}\bigl[J(J+1)-L(L+1)-S(S+1)\bigr] yields ESO=10.000 cm−1E_{SO} = 10.000\,\mathrm{cm^-1}. A term that splits into J levels. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Fine-structure energy E_{SO}10.000 cm^{-1}
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ATM-12 · spectrum
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Narration of this film

A term that splits into J levels.

A ∝ Z⁴ α² Rydberg. Fine-structure splitting of alkali D lines is this plus core penetration.

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