INGENIA

ATM-31

Term degeneracy

Russell–Saunders term.

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Governing equation

g=(2S+1)(2L+1)g=(2S+1)(2L+1)

L∈[0,6]L \in \left[0, 6\right]

where

S
S (—)
L
L (—)
g
g (—)

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ATM-31 · spectrum
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①

Governing law — red

g=(2S+1)(2L+1)g=(2S+1)(2L+1)

L∈[0,6]L \in \left[0, 6\right]

L=0L = 0g=3g = 3

②

Domain of the variable — blue

Lmin⁡=0,Lmax⁡=6L_{\min} = 0,\quad L_{\max} = 6

L∈[0,6]L \in \left[0, 6\right]

L=0L = 0L=0L = 0

③

Response curve — green

g=(2S+1)(2L+1)g=(2S+1)(2L+1)

L∈[0,6]L \in \left[0, 6\right]

L=0L = 0g=3g = 3

④

Rate of change — amber

dgdL\frac{\mathrm{d}g}{\mathrm{d}L}

L∈[0,6]L \in \left[0, 6\right]

L=0.038L = 0.038g′=6g^{\prime} = 6

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-31 — Term degeneracy) is the form associated with term. Working symbols: SS, LL →\rightarrow gg. Russell–Saunders term.

Purpose

Purpose: compute gg from SS, LL in Atomic physics via g=(2S+1)(2L+1)g=(2S+1)(2L+1) Russell–Saunders term. 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=1.000 —S = 1.000\,\mathrm{—}, L=1.000 —L = 1.000\,\mathrm{—}, the governing relation g=(2S+1)(2L+1)g=(2S+1)(2L+1) yields g=9 —g = 9\,\mathrm{—}. Russell–Saunders term. Move a slider: the numbers are this situation, not a canned story.

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Outputs

  • g g9 —
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Narration of this film

Russell–Saunders term.

Russell–Saunders term.

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