Gives kinetic energy of the emitted particles.
Take a nucleus which can decay both ways, like potassium 40.
In case of positron emission, the difference between the masses of K-40 and Ar-40 is split between the 3 major components of
1) positron rest mass (511 keV)
2) positron kinetic energy
3) neutrino kinetic energy
and the minor components of
4) neutrino rest mass (unknown but small)
5) Ar-40 nucleus recoil
Eventually the positron is annihilated, emitting 2 or 3 photons whose combined energy shall be 1022 keV plus whatever the positron kinetic energy was.
If, however, the K-40 nucleus manages to capture an electron, then there is no positron emitted. But a neutrino is emitted.
The whole mass difference between K-40 and Ar-40 nuclei, plus the mass of electron (usually somewhat less than 511 keV), have to be carried away by the emitted neutrino. Only the recoil of the Ar-40 nucleus goes elsewhere.
It follows that the neutrinos emitted on electron capture are much more energetic than the neutrinos emitted by positron emission. The capture neutrinos have to take the 1022 keV of electron-positron pair energy, plus the positron´s share of kinetic energy.
Electron capture neutrinos also have a narrow line spectrum, because they cannot share their energy with positron.