The mm-th Fourier harmonic of a one-dimensional periodic function is its component f^(m)eimθ\widehat f(m)e^{im\theta}, for an angular coordinate of period 2π2\pi. The term harmonic can also refer to the eimθe^{im\theta} itself. For real-valued functions, the mm and m-m components combine to a real sinusoidal component.

Several frequencies

On a unit dd-torus the harmonic index is mZdm\in\mathbb Z^d, and the component is f^(m)e2πimx\widehat f(m)e^{2\pi i m\cdot x}. In an ansatz ameikmΦa_m e^{ikm\Phi}, the integer harmonic multiplier mm is distinct from a chosen carrier parameter kk. Fourier harmonics are frequency components; they are generally not harmonic functions in the sense Δf=0\Delta f=0.