INGENIA

ATM-23

Landé g-factor

g_J = 1 + [J(J+1)+S(S+1)−L(L+1)] / [2 J(J+1)]. Anomalous Zeeman g.

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StructureLandé

Governing equation

gJ=1+J(J+1)+S(S+1)−L(L+1)2J(J+1)g_J=1+\dfrac{J(J+1)+S(S+1)-L(L+1)}{2J(J+1)}

J∈[0.5,6]J \in \left[0.5, 6\right]

where

L
L (—)
S
S (—)
J
J (—)
g_J
Landé g (—)

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ATM-23 · spectrum
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①

Governing law — red

gJ=1+J(J+1)+S(S+1)−L(L+1)2J(J+1)g_J=1+\dfrac{J(J+1)+S(S+1)-L(L+1)}{2J(J+1)}

J∈[0.5,6]J \in \left[0.5, 6\right]

J=0.5J = 0.5gJ=0.667g_J = 0.667

②

Domain of the variable — blue

Jmin⁡=0.5,Jmax⁡=6J_{\min} = 0.5,\quad J_{\max} = 6

J∈[0.5,6]J \in \left[0.5, 6\right]

J=0.5J = 0.5J=0.5J = 0.5

③

Response curve — green

gJ=1+J(J+1)+S(S+1)−L(L+1)2J(J+1)g_J=1+\dfrac{J(J+1)+S(S+1)-L(L+1)}{2J(J+1)}

J∈[0.5,6]J \in \left[0.5, 6\right]

J=0.5J = 0.5gJ=0.667g_J = 0.667

④

Rate of change — amber

dgJdJ\frac{\mathrm{d}g_J}{\mathrm{d}J}

J∈[0.5,6]J \in \left[0.5, 6\right]

J=0.535J = 0.535gJ′=1.931g_J^{\prime} = 1.931

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-23 — Landé g-factor) is the form associated with Landé. Working symbols: LL, SS, JJ →\rightarrow gJg_J. g = 2 for a pure spin, g = 1 for a pure orbit. Alkali D2 has g = 4/3 for ²P_{3/2}.

Purpose

Purpose: compute gJg_J from LL, SS, JJ in Atomic physics via gJ=1+J(J+1)+S(S+1)−L(L+1)2J(J+1)g_J=1+\dfrac{J(J+1)+S(S+1)-L(L+1)}{2J(J+1)} g_J = 1 + [J(J+1)+S(S+1)−L(L+1)] / [2 J(J+1)]. Anomalous Zeeman g. 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 L=1.000 —L = 1.000\,\mathrm{—}, S=0.500 —S = 0.500\,\mathrm{—}, J=1.500 —J = 1.500\,\mathrm{—}, the governing relation gJ=1+J(J+1)+S(S+1)−L(L+1)2J(J+1)g_J=1+\dfrac{J(J+1)+S(S+1)-L(L+1)}{2J(J+1)} yields gJ=1.3333 —g_J = 1.3333\,\mathrm{—}. Three quantum numbers, a g bar. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Landé g g_J1.3333 —
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ATM-23 · spectrum
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Narration of this film

Three quantum numbers, a g bar.

g = 2 for a pure spin, g = 1 for a pure orbit. Alkali D2 has g = 4/3 for ²P_{3/2}.

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