Virtual laboratory/Physics/Atomic physics/The Zeeman effect — spectral lines in a magnetic field

The Zeeman effect — spectral lines in a magnetic field

An extension of the topic of atomic spectra and energy levels. Without a magnetic field an atom emits a single, sharp spectral line; in a magnetic field that line splits into several closely spaced lines, and the spacing between them grows with the field strength — proof that an atom's energy levels are tied to the magnetism of its electrons (Nobel Prize in Physics 1902, Lorentz and Zeeman).

The Zeeman effect — spectral lines in a magnetic field
Physics · Atomic physics · Zeeman effect (Nobel 1902)
Magnetic field strength BB0.0 T
When the magnetic field is switched on, the spectral line of the atom…
field B
0.0 T
spacing Δλ
0.0 pm
number of lines
1
spectrum
single
🎯 Challenge: hit the splitting
streak: 0

I'll give you a target spacing of the components Δλ — tune the magnetic field strength B to reach it. Δλ grows linearly with B.

What is the Zeeman effect?

You switched on field B, and one sharp spectral line broke into three closely spaced components. That is the Zeeman effect: the magnetic field splits the atom's energy levels, so instead of one transition the electron can make several transitions of slightly different energy — and you see several very closely spaced lines instead of one.

Energy splitting:

ΔE=ml gL μB B\Delta E = m_l \, g_L \, \mu_B \, B

— μ_B is the Bohr magneton (a constant tied to the electron's magnetic moment), g_L is the Landé factor (≈1 for the normal Zeeman effect), and m_l numbers the allowed levels. The stronger the field B, the larger the energy difference ΔE between the components.

Why study atomic spectra in a magnetic field?

The line spacing translates into a wavelength spacing: Δλ≈μBλ2hc B\Delta\lambda \approx \dfrac{\mu_B \lambda^2}{h c}\, B. For the yellow sodium line (λ ≈ 589 nm) this is only about 16 pm per 1 T — which is why the splitting is so hard to observe and requires very sensitive instruments (an interferometer) rather than an ordinary prism. By measuring this tiny spacing precisely, physicists read off the strength of the magnetic field in which the emitting atom was located.

How was it discovered?

In 1896 Pieter Zeeman observed that the spectral lines of sodium in a flame split into several components under a strong magnetic field. Hendrik Lorentz — based on his newly developed theory of the electron — gave the phenomenon a detailed theoretical interpretation. For their joint research on the influence of magnetism on radiation, both received the Nobel Prize in Physics in 1902.

What are its applications today?

The Zeeman effect was one of the first experimental proofs that an atom's energy levels are tied to the magnetic moment of the electrons orbiting the nucleus — that is, to the structure of the atom, later described by quantum mechanics. Today astronomers use it to measure the magnetic fields of stars and sunspots: by analysing the spacing of the split lines in the spectrum of light from a given region, one can calculate how strong the magnetic field is there.

Why you need this for the exam:

Remember the direction of the dependence: no field — one line; with a field — several lines, and their spacing grows with B. This is a classic proof of the quantisation (splitting) of an atom's energy levels under an external factor.

Remember: a magnetic field splits a spectral line into several closely spaced components, and their spacing grows linearly with the field strength B — that is the Zeeman effect.

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Theory & formulas

Splitting of the levels

In a magnetic field an atom's energy level splits into sublevels that depend on the magnetic quantum number mlm_l. Transitions between them give — instead of one — several closely spaced spectral lines.

Energy shift

The energy of a sublevel changes in proportion to the field strength: ΔE=ml μB B\Delta E = m_l\,\mu_B\,B where μB\mu_B is the Bohr magneton. The stronger the field BB, the larger the line spacing.

Frequency shift

From ΔE=h Δf\Delta E = h\,\Delta f it follows that: Δf=μB Bh\Delta f = \dfrac{\mu_B\,B}{h}

Application

By measuring the spacing of the split lines in the spectrum of a star or a sunspot, one determines the magnetic field present there.

Symbols: ΔE\Delta E — energy shift, mlm_l — magnetic quantum number, μB≈9.27⋅10−24 J/T\mu_B \approx 9{.}27\cdot10^{-24}\ \mathrm{J/T} — Bohr magneton, BB — magnetic flux density, hh — Planck constant, Δf\Delta f — frequency shift.

Frequently asked questions

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What is the Zeeman effect?

The splitting of an atom's spectral line into several components under the influence of a magnetic field.

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Why study atomic spectra in a magnetic field?

Because the splitting of the lines reveals how the electrons' energy levels are tied to their magnetic moment.

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What are the applications of the Zeeman effect?

To measure the strength of the magnetic fields of stars and sunspots from the splitting of the lines in their spectra.

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