A fluorescence molecule is usually excited by absorbing a single photon of a particular energy, corresponding to a particular wavelength. However, excitation is also possible by simultaneous absorption of two (n) photons, each of half (1/n) the energy and therefore twice (n times) the wavelength. Because this requires all the absorbed photons to be in the vicinity of the molecule within a limited time frame, the chance for a multi-photon excitation event to occur is much lower than the chance for a single photon event. The chance of a single photon event is proportional to the number of photons 'hitting' the molecule, and therefore proportional to the intensity. The chance of two photons hitting the molecule in a short interval is proportional to the square of this hit rate, so proportional to the square of the intensity.
Raising the photon probability distribution to the n-th power reduces de Point Spread Function and increases the resolution and the Band Width, thus the Nyquist Rate for ideal sampling changes accordingly.
Importantly, the 3D shape of the band-pass volume is very different: while the Wide Field Microscope area has a wedge at the center causing the large widefield blur cones, the multi-photon bandpass volume has no such defects.
Multi-photon excitation reduces the Bleaching Effects.
See this article to find out how to use Huygens with your multi-photon microscope.
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Laapersveld 63
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Laapersveld 63
1213 VB Hilversum
The Netherlands
Phone: +31 (0)35 64216 26
E-mail: info at svi.nl
