INGENIA

ATM-09

Term degeneracy

A term ²ˢ⁺¹L_J has multiplicity 2S+1 and (2J+1) magnetic sublevels.

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SpectraTerm symbols

Governing equation

g=2J+1,M=2S+1g=2J+1,\quad M=2S+1

J∈[0,8]J \in \left[0, 8\right]

where

S
Spin S (—)
J
J (—)
2S+1
Multiplicity (—)
2J+1
Degeneracy (—)

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ATM-09 · spectrum
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①

Governing law — red

g=2J+1,M=2S+1g=2J+1,\quad M=2S+1

J∈[0,8]J \in \left[0, 8\right]

J=0J = 02S+1=12S+1 = 1

②

Domain of the variable — blue

Jmin⁡=0,Jmax⁡=8J_{\min} = 0,\quad J_{\max} = 8

J∈[0,8]J \in \left[0, 8\right]

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

③

Response curve — green

g=2J+1,M=2S+1g=2J+1,\quad M=2S+1

J∈[0,8]J \in \left[0, 8\right]

J=0J = 02S+1=12S+1 = 1

④

Rate of change — amber

d2S+1dJ\frac{\mathrm{d}2S+1}{\mathrm{d}J}

J∈[0,8]J \in \left[0, 8\right]

J=0.05J = 0.052S+1′=22S+1^{\prime} = 2

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-09 — Term degeneracy) is the form associated with Term symbols. Working symbols: SS, JJ →\rightarrow 2S+12S+1, 2J+12J+1. L = 0,1,2,… → S,P,D. J runs from |L−S| to L+S. Hund fills the ground term.

Purpose

Purpose: compute 2S+12S+1, 2J+12J+1 from SS, JJ in Atomic physics via g=2J+1,M=2S+1g=2J+1,\quad M=2S+1 A term ²ˢ⁺¹L_J has multiplicity 2S+1 and (2J+1) magnetic sublevels. 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 S=0.500 —S = 0.500\,\mathrm{—}, J=1.500 —J = 1.500\,\mathrm{—}, the governing relation g=2J+1,M=2S+1g=2J+1,\quad M=2S+1 yields 2S+1=2 —2S+1 = 2\,\mathrm{—}, 2J+1=4 —2J+1 = 4\,\mathrm{—}. A term label, a degeneracy bar. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Multiplicity 2S+12 —
  • Degeneracy 2J+14 —
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ATM-09 · spectrum
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Narration of this film

A term label, a degeneracy bar.

L = 0,1,2,… → S,P,D. J runs from |L−S| to L+S. Hund fills the ground term.

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