Apparent magnitude is a calibrated description of the observed radiative flux received from an astronomical source. It answers how bright the source appears in a specified photometric passband, rather than how much luminosity the source emits. Define as the measurement assigned zero apparent magnitude by the chosen magnitude zero point. ThenHere is the positive passband measurement, with the same units and response convention as . For an energy-weighted detector this measures received radiative flux through its response; for a photon-counting detector use the corresponding calibrated count rate for both quantities. Actual photometric passbands include the instrument's response across wavelength, so naming the photometric system is part of reporting an apparent magnitude. [ref]
https://www.cosmos.esa.int/web/gaia/edr3-passbands. ESA/Gaia/DPAC: Passbands and zero points
. [ref]https://xmm-tools.cosmos.esa.int/external/xmm_calibration/calib/documentation/CALHB/node597.html. ESA XMM-Newton calibration handbook: Count rate to magnitude
.As toy examples in one photometric passband, gives , gives , and gives . A negative apparent magnitude therefore means more received radiative flux than the reference; it is physically allowed. Zero apparent magnitude does not mean zero radiative flux. The ordinary logarithm formula requires .
A small apparent magnitude alone cannot distinguish a nearby faint source from a distant source with large luminosity: this is the flux-distance degeneracy. Stellar parallax supplies independent distance information, while a calibrated standard candle supplies intrinsic brightness. Interstellar extinction also changes the received radiative flux and hence the measured apparent magnitude.
Apparent magnitude is a measure of the brightness of a celestial object as seen from Earth. It quantifies how bright an object appears to an observer, regardless of its actual distance from the observer or its intrinsic luminosity. The scale of apparent magnitude is logarithmic: a difference of 5 magnitudes corresponds to a brightness factor of 100. This means that a difference of 1 magnitude corresponds to a brightness factor of about 2.5.
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