Mode volume may refer to figures of merit used either to characterise optical and microwave cavities or optical fibers.
In electromagnetic cavities The mode volume (or modal volume) of an optical or microwave cavity is a measure of how concentrated the electromagnetic energy of a single cavity mode is in space, expressed as an effective volume in which most of the energy associated with an electromagentic mode is confined. Various expressions may be used to estimate this volume:
The volume that would be occupied by the mode if its electromagnetic energy density was constant and equal to its maximum value
V m = ∫ ϵ | E | 2 d V m a x ( ϵ | E | 2 ) o r V m = ∫ ( | B | 2 / μ ) d V m a x ( | B | 2 / μ ) {\displaystyle V_{m}={\frac {\int \epsilon |E|^{2}dV}{\rm {{max}(\epsilon |E|^{2})}}}\;\;\;{\rm {{or}\;\;\;V_{m}={\frac {\int (|B|^{2}/\mu )\;dV}{\rm {{max}(|B|^{2}/\mu )}}}}}}
The volume over which the electromagnetic energy density exceeds some threshold (e.g., half the maximum energy density)
V m = ∫ ( | E | 2 > | E m a x | 2 2 ) d V {\displaystyle V_{m}=\int \left(|E|^{2}>{\frac {|E_{max}|^{2}}{2}}\right)dV}
The volume that would be occupied by the mode if its electromagnetic energy density was constant and equal to a weighted average value that emphasises higher energy densities.
V m = ( ∫ | E | 2 d V ) 2 ∫ | E | 4 d V o r V m = ( ∫ | B | 2 d V ) 2 ∫ | B | 4 d V {\displaystyle V_{m}={\frac {(\int |E|^{2}dV)^{2}}{\int |E|^{4}dV}}\;\;\;{\rm {{or}\;\;\;V_{m}={\frac {(\int |B|^{2}dV)^{2}}{\int |B|^{4}dV}}}}}
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