- #1
SSJVegetto
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Reflection at a surface takes place under the condition that the field amplitude is zero at the reflecting surface. As a result, the axial modes i of wavelength λi inside a laser cavity can be defined by their number ni of sine-wave half cycles that fit exactly into the laser cavity. The optical gain curve of the active medium of a crystalline solid-state laser has a wavelength range of typically 10-100 nm, so that many (~104) axial modes inside a few-cm long cavity fall within the optical gain curve and may therefore start lasing.
Can someone explain why nevertheless only one axial mode starts lasing in a homogeneously broadened gain medium at pump threshold?
Can someone explain the phenomenen of spectral hole burning?
Another question is, is there someone who can help me with a few other questions that i send a pm with a pdf file?
Can someone explain why nevertheless only one axial mode starts lasing in a homogeneously broadened gain medium at pump threshold?
Can someone explain the phenomenen of spectral hole burning?
Another question is, is there someone who can help me with a few other questions that i send a pm with a pdf file?