Find spin quantum number s and multiplicity fast. Compute S(S+1), ms options, and g factor. Understand fermions, bosons, and selection rules clearly with tables.
| Mode | Input | Expected s | Expected multiplicity (2s+1) | Allowed ms |
|---|---|---|---|---|
| From multiplicity | M = 2 | 0.5 | 2 | −0.5, +0.5 |
| From multiplicity | M = 3 | 1 | 3 | −1, 0, +1 |
| From unpaired electrons | n = 2 | 1 | 3 | −1, 0, +1 |
| From s directly | s = 1.5 | 1.5 | 4 | −1.5, −0.5, +0.5, +1.5 |
The spin quantum number s describes intrinsic angular momentum. Unlike orbital motion, spin is an internal property of particles. It sets the total spin magnitude through |S| = √(s(s+1)) ħ, which is why s(s+1) appears in spectroscopy and angular momentum algebra.
Spin comes in integer or half-integer steps. Particles with half-integer spin are fermions, such as electrons, protons, and neutrons (s = 1/2). Integer-spin particles are bosons, such as photons (s = 1). This distinction matters because it controls statistical behavior and state occupancy.
For a given s, the number of spin states is M = 2s + 1. For example, an electron has M = 2 (a doublet), while s = 1 gives M = 3 (a triplet). In atoms and molecules, multiplicity is written as 2S+1, where S is the total spin.
The projection along a chosen axis is ms = −s, −s+1, …, +s. These values differ by exactly 1, so a half-integer s produces half-integer ms. The calculator lists every allowed ms state so you can verify degeneracy quickly.
Spin contributes to magnetic moment. A common spin-only estimate is μ = g √(s(s+1)) μB. For electrons, g is close to 2, so s = 1/2 gives μ ≈ 1.732 μB using this magnitude form. Real materials can deviate due to orbital contributions and coupling.
In many chemistry and atomic cases, total spin can be estimated from unpaired electrons: S = n/2. One unpaired electron gives S = 1/2 and multiplicity 2. Two parallel unpaired electrons can give S = 1 and multiplicity 3, which is often observed as a triplet state.
The splitting of spin states in a magnetic field underlies the Stern–Gerlach picture and electron spin resonance. The count of discrete deflections corresponds to 2s+1. Transition rules, line intensities, and Zeeman splitting patterns are strongly shaped by the set of available ms values.
If you enter multiplicity, (M−1)/2 should be a multiple of 0.5. If you enter s, your result list should contain exactly 2s+1 values of ms. For spin-only cases, verify that the unpaired-electron mode matches your expected multiplicity.
s sets the total intrinsic spin magnitude. ms is the component along a chosen axis and can take values from −s to +s in steps of 1.
The projection ms has equally spaced values from −s to +s. Counting them gives 2s+1 possible orientations, which is the degeneracy of the spin degree of freedom.
No. By definition, s is a non‑negative quantum number. Negative values appear only for projections (ms), not for the total spin quantum number itself.
It provides a common spin-only estimate from unpaired electrons using S = n/2. Exact atomic term symbols can require coupling rules and quantum mechanical addition of angular momenta.
For a basic electron spin-only estimate, g ≈ 2 is widely used. In solids and molecules, effective g can differ due to bonding, crystal fields, and relativistic effects.
Quantum angular momentum has magnitude |S| = √(s(s+1)) ħ. Using this magnitude form gives a rotationally invariant estimate, independent of the chosen axis.
These labels refer to multiplicity. Singlet means 2S+1 = 1 so S = 0. Triplet means 2S+1 = 3 so S = 1, giving three ms states.
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