An alpha-squared dynamo generates a mean magnetic field using an alpha effect without requiring an additional large-scale shear coupling. For and a transverse mean field varying as , the growth rates are . A nonzero therefore allows growth for sufficiently long wavelengths, provided the domain and scale separation permit them.
For constant isotropic transport coefficients and zero mean flow, a divergence-free Fourier mode has two circular polarizations that diagonalize curl with eigenvalues . The mean induction equation therefore has the displayed growth rates. Growth requires an admissible with . Freely variable wavenumber gives , provided it respects mean-field scale separation. A uniform field has zero curl and cannot grow by constant alpha alone; boundaries fix the longest available spatial mode.
An alpha-squared dynamo may use a tensorial alpha effect rather than an isotropic coefficient. For constant alpha tensor and magnetic diffusivity , a steady nonzero Fourier mode with wavevector satisfies and . Anisotropy can change both the critical alpha magnitude and the preferred wavevector direction.
For , set , , and . A steady nonzero Fourier mode obeys the displayed condition when the denominator is nonzero. At fixed and , minimizing over gives and for ; for it gives and . This is a boundary-constrained threshold of an anisotropic alpha-squared dynamo.

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