There are also light-emitting diodes (LEDs) which generate white light in a process that involves the excitation of a phosphor. In that case, however, the actual LED produces blue rather than ultraviolet light, and this blue light is partly converted to red and green fluorescence light in the phosphor, and partly emitted by the device.

Substances emitting fluorescence, or sometimes just parts of larger molecules, are called fluorophores. Some artificial fluorophores may be added to samples in fluorescence spectroscopy.

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Fluorescence is a short-lived photoluminescence, excited by irradiation of a substance with light. The light hitting a sample puts atoms, ions or molecules in the sample into excited states (by absorption of photons), from where they decay into lower-lying states (e.g. their ground states) through spontaneous emission of fluorescence photons. This phenomenon is exploited for illumination, particularly in fluorescent lamps. It also occurs at a side effect in various kinds of optically pumped lasers and amplifiers, e.g. in solid-state doped-insulator lasers and amplifiers (including fiber lasers and fiber amplifiers), in optically pumped semiconductor lasers, and in dye lasers. The resulting radiation is called fluorescent light.

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For very long decay times, usually involving triplet states with forbidden transitions, such luminescence is called phosphorescence. Is also the phenomenon of delayed fluorescence, which can involve a weak intersystem crossing to a triplet state and later back to the original singlet state.

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Fluorescence effects can be quite disturbing under certain circumstances. For example, certain spectroscopic measurements can be disturbed by unwanted laser-induced fluorescence in glass windows or tubes. Such fluorescence often originates from certain impurities.

Fluorescent solar concentrators might be the basis for cheaper electricity from photovoltaic panels (solar modules), as they allow to collect radiation from a large area while requiring only relatively small photovoltaic cells.

Various processes can lead to pronounced non-exponential fluorescence decay, with a faster decay shortly after excitation and a slower decay later. For example, this can be caused by contributing atoms with different lifetimes, or by upconversion processes which are stronger for high level populations.

The quantum efficiency (or quantum yield) of fluorescence from some level is the average number of fluorescence photons obtained per ion which is put into the upper level. Solid-state gain media (e.g. laser crystals or rare-earth-doped fibers) often have laser transitions with a quantum efficiency very close to unity, whereas some levels (e.g. the lower laser level) exhibit virtually no fluorescence due to strong multi-phonon transitions.

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After excitation with a short pulse, the fluorescence decay is often of exponential nature with a decay constant which is called the fluorescence lifetime or upper-state lifetime ( because the fluorescence lifetime is identical to the lifetime of the population in the upper level of an electronic transition). For so-called allowed transitions, the fluorescence lifetime is typically of the order of a few nanoseconds. In solid-state laser gain media other than semiconductors, one is often dealing with weakly allowed transitions, where the fluorescence lifetime can be much longer, e.g. microseconds or even milliseconds. In any case, the upper-state lifetime can at most be the radiative lifetime (limited by fluorescence only), and possibly be shorter if there are additional non-radiative decay processes.

Fluorescence light can be useful, e.g. for direct use for optical measurements, such as for measuring the transmission spectra of optical devices. It is also the basis of fluorescence spectroscopy, fluorescence microscopy and of optical refrigeration. By combining multiple types of emitting rare earth ions in an optical fiber, very broadband radiation can be generated [1].

where <$\sigma_{ji}$> is the emission cross-section and <$N_j$> the density of ions in the starting level <$j$>. The given quantity <$I_{ji}(\nu)$> has units of J/m3, and multiplied with a small frequency interval <$\rm{d}\nu$> one arrives at W/m3 – consistent with the radiated optical power per unit volume.

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A special kind of fluorescence, which is not related to the excitation of atoms or ions in a substance, is parametric fluorescence in nonlinear crystal materials. This effect does not involve the excitation of electrons in the media, but rather a nonlinear interaction. Such fluorescence occurs only as long as some pump light propagates in the medium.

Cases with resonance fluorescence – most often with atoms or molecules – are those not involving additional transitions, where the interacting atoms or molecules can be considered as simple oscillators with a certain resonance frequency. The emission wavelengths are then close to the excitation wavelength.

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In the context of lasers, fluorescence in the laser crystal (or other gain medium) by spontaneous emission is lost for the laser operation because only a tiny fraction of it goes into the laser resonator mode. The fluorescence lifetime for fluorescence from the upper laser level is usually called the upper-state lifetime. Fluorescence is the most fundamental reason why a certain laser threshold has to be overcome to achieve lasing (exception: thresholdless lasers). Note also that when the pump source of a laser is turned on, laser action normally starts from a tiny amount of fluorescence in the laser resonator mode, amplified to high levels in many resonator round trips.

Fluorescence of the single atoms, ions or molecules of a sample usually occurs in an uncoordinated manner, i.e., uniformly in all spatial directions and without temporal correlations between the emitted photons. However, certain conditions lead to amplified spontaneous emission (superluminescence) or superfluorescence, where this is no longer the case.

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The optical spectrum of fluorescence light (see e.g. Figure 1) generally differs from that of the light which initially caused the excitation of the medium. A significant Stokes shift (difference in photon energies of absorbed and emitted light) can occur because a part of the excitation energy is converted to heat in the medium. For example, the excited atoms or ions may first undergo an optical or a non-radiative transition to some intermediate level, before emitting fluorescence light in a transition to the ground state, or to some higher-lying energy level. It is also possible that a cascade of emission processes occurs, i.e., a cascade of transitions to lower-lying energy levels; in that case, more than one fluorescence photon can be emitted for one absorbed photon.

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Fluorescence in transparent polymer sheets, which are doped with some luminescent species, can be used for luminescent (or fluorescent) solar concentrators [2]. Sunlight hitting the polymer sheets from any direction can be absorbed and efficiently transformed into fluorescent light, which is partly trapped in the sheets and thus sent to the edges, where solar cells receive the concentrated radiation. Potentially suitable luminescent agents can be certain organic dyes and quantum dots. Further research is required to optimize the still limited lifetime of dyes under irradiation with sunlight and the quantum efficiency of quantum dots.

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In solid-state laser gain media, phonons lead to very fast thermalization within Stark level manifolds. As the emission occurs on a much longer time scale, the spectral shape of the emission spectrum does not depend on the exact wavelength of the exciting light. It depends only on the spectral dependence of the emission cross-sections, combined with some other factors. The frequency-dependent fluorescence intensity (actually a power spectral density) related to spontaneous emission from some level <$j$> to level <$i$> is given by [3]:

Upconversion processes lead to the population in relatively high-lying energy levels, from where blue and even ultraviolet light is emitted. Such fibers are suitable for lasing in the blue spectral region near 480 nm. (The weak peaks around 700 nm are artifacts, caused by second-order diffraction of ultraviolet light in the spectrograph. Data taken by R. Paschotta.)

In optical amplifiers, fluorescence can be even more important. In the form of amplified spontaneous emission (ASE), it may extract significant power and thus limit the achievable gain. It also determines much of the quantum noise contributions to laser noise and amplifier noise.

In many cases, there are non-radiative processes which compete with fluorescence and reduce or even fully suppress it (→ quenching). In particular, multi-phonon transitions are very strong for level pairs with an energy distance which is at most a few times the maximum phonon energy of the host material. In other cases, energy transfer processes can deplete the population in a metastable level.

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Fluorescence is widely used in fluorescent tubes for illumination purposes. The most common fluorescent lamps contain mercury vapor inside a glass tube, where an electric discharge excites the mercury atoms to emit mostly ultraviolet light. A fluorescent material (called the phosphor) on the inner surface of the tube absorbs the ultraviolet light and converts it into fluorescence light, mostly in the visible spectral region. The phosphor contains several substances mixed in such a way that the overall emission spectrum corresponds to white light (with the color tone adjusted according to the envisaged application). Although part of the energy of the ultraviolet light is lost in the phosphor, fluorescence lights are still several times more energy-efficient than incandescent lamps.