Selective excitation of fluorescent proteins on the basis of the two-photon absorption spectrum measurement

2006 ◽  
Author(s):  
M. Tanaka ◽  
J. Tada ◽  
F. Kannari ◽  
H. Kawano ◽  
H. Mizuno ◽  
...  
1984 ◽  
Vol 9 (3) ◽  
pp. 82 ◽  
Author(s):  
F. Arqueros ◽  
P. E. LaRocque ◽  
M. S. O’Sullivan ◽  
B. P. Stoicheff

1968 ◽  
Vol 28 (4) ◽  
pp. 305-306 ◽  
Author(s):  
K. Park ◽  
H.S. Waff

1979 ◽  
Vol 57 (12) ◽  
pp. 2143-2154 ◽  
Author(s):  
B. P. Stoicheff ◽  
E. Weinberger

Doppler-free, two-photon spectroscopy has been used to investigate the transitions n2S ← 52S and n2D ← 52S of atomic rubidium, from n = 9 to 116 and n = 7 to 124, respectively, only 7.3 cm−1 from the ionization limit. Wavelengths of these transitions have been measured to an accuracy of 1 part in 107, and series formulae computed for term values and quantum defects. Hyperfine structure splittings in the 92S to 132S levels have also been measured.


2022 ◽  
Vol 23 (2) ◽  
pp. 770
Author(s):  
Mikhail Drobizhev ◽  
Rosana S. Molina ◽  
Jacob Franklin

Red fluorescent proteins and biosensors built upon them are potentially beneficial for two-photon laser microscopy (TPLM) because they can image deeper layers of tissue, compared to green fluorescent proteins. However, some publications report on their very fast photobleaching, especially upon excitation at 750–800 nm. Here we study the multiphoton bleaching properties of mCherry, mPlum, tdTomato, and jREX-GECO1, measuring power dependences of photobleaching rates K at different excitation wavelengths across the whole two-photon absorption spectrum. Although all these proteins contain the chromophore with the same chemical structure, the mechanisms of their multiphoton bleaching are different. The number of photons required to initiate a photochemical reaction varies, depending on wavelength and power, from 2 (all four proteins) to 3 (jREX-GECO1) to 4 (mCherry, mPlum, tdTomato), and even up to 8 (tdTomato). We found that at sufficiently low excitation power P, the rate K often follows a quadratic power dependence, that turns into higher order dependence (K~Pα with α > 2) when the power surpasses a particular threshold P*. An optimum intensity for TPLM is close to the P*, because it provides the highest signal-to-background ratio and any further reduction of laser intensity would not improve the fluorescence/bleaching rate ratio. Additionally, one should avoid using wavelengths shorter than a particular threshold to avoid fast bleaching due to multiphoton ionization.


Pramana ◽  
1995 ◽  
Vol 45 (3) ◽  
pp. 271-278
Author(s):  
I B Singh ◽  
S B Rai ◽  
D K Rai

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