At the high-frequency limit (meaning optical frequencies), the complex permittivity is commonly referred to as (or sometimes ). At the plasma frequency and below, dielectrics behave as ideal metals, with electron gas behavior. The static permittivity is a good approximation for alternating fields of low frequencies, and as the frequency increases a measurable phase difference emerges between and . The frequency at which the phase shift becomes noticeable depends on temperature and the details of the medium. For moderate field strength (), and remain proportional, and