Polarization dependence of resonant multiphoton ionizations on 1S0 and 1,3D2 states in atomic mercury

1988 ◽  
Vol 66 (1) ◽  
pp. 1-6
Author(s):  
K. R. Mah ◽  
F. W. Dalby ◽  
C. W. Barnard

The polarization dependences of some resonant multiphoton ionizations in atomic mercury have been measured with a broadband (bandwidth ≈ 1.5 cm−1) multimode dye laser at moderate light intensities (≈ 500 MW∙cm−2). The multiphoton processes studied were the absorption of four photons to a resonant 1S0, 1D2, or 3D2 level by one-photon ionization. Complete saturation of the one-photon ionization step results in the ionization of all atoms excited to the resonant level. Because of the saturation of the ionization step, the polarization dependence of the four-photon excitation to the resonant level is measured. The theory developed by Dalby et al. is shown to give good agreement with the experiment when it is used to calculate the polarization dependence of the multiphoton transition to the resonant level. For the 6d1D2 resonance, distortions in the polarization dependence and an unusual linewidth dependence on the light polarization were observed. We relate these observations to the alternating current Stark effect and to the production of the third harmonic of the laser light in the focal volume.

1984 ◽  
Vol 62 (5) ◽  
pp. 419-430
Author(s):  
F. W. Dalby ◽  
M. H. L. Pryce ◽  
J. H. Sanders

The polarization dependences of a number of resonant multiphoton ionizations in atomic Hg have been studied experimentally and theoretically. Good agreement between theory and experiment is found from which quantitive information about relative ionization cross sections from excited states has been deduced.


1997 ◽  
Vol 3 (S2) ◽  
pp. 305-306
Author(s):  
David W. Piston

Two-photon excitation microscopy (TPEM) provides attractive advantages over confocal microscopy for three-dimensionally resolved fluorescence imaging and photochemistry. It provides three-dimensional resolution and eliminates background equivalent to an ideal confocal microscope without requiring a confocal spatial filter, whose absence enhances fluorescence collection efficiency. This results in inherent submicron optical sectioning by excitation alone. In practice, TPEM is made possible by the very high local instantaneous intensity provided by a combination of diffraction-limited focusing of a single laser beam in the microscope and the temporal concentration of 100 femtosecond pulses generated by a mode-locked laser. Resultant peak excitation intensities are 106 times greater than the CW intensities used in confocal microscopy, but the pulse duty cycle of 10−5 limits the average input power to less than 10 mW, only slightly greater than the power normally used in confocal microscopy. Because of the intensity-squared dependence of the two-photon absorption, the excitation is limited to the focal volume.


2015 ◽  
Vol 17 (5) ◽  
pp. 053011 ◽  
Author(s):  
Lukas Medišauskas ◽  
Felipe Morales ◽  
Alicia Palacios ◽  
Alberto González-Castrillo ◽  
Lev Plimak ◽  
...  

1977 ◽  
Vol 55 (5) ◽  
pp. 434-435 ◽  
Author(s):  
C. Tai ◽  
F. W. Dalby

Strong photoionization spectra have been observed in atomic mercury following absorption of laser light. In the frequency range 25 500 to 27 800 cm−1 many resonances corresponding to coherent three-photon absorption followed by one-photon ionization are reported.


2002 ◽  
Vol 65 (15) ◽  
Author(s):  
C. K. Choi ◽  
J. B. Lam ◽  
G. H. Gainer ◽  
S. K. Shee ◽  
J. S. Krasinski ◽  
...  

2019 ◽  
Vol 21 (43) ◽  
pp. 23916-23921 ◽  
Author(s):  
Martina Perić ◽  
Željka Sanader Maršić ◽  
Isabelle Russier-Antoine ◽  
Hussein Fakhouri ◽  
Franck Bertorelle ◽  
...  

The effects of explicit ligands and of aqueous solvent on optical properties and in particular on the one- and two-photon excitation fluorescence of zwitterion functionalized gold nanoclusters have been studied.


2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Paul J. Marchand ◽  
Xuecong Lu ◽  
Cong Zhang ◽  
Frédéric Lesage

Abstract We present a validation of red blood cell flux and speed measurements based on the passage of erythrocytes through the OCT’s focal volume. We compare the performance of the so-called RBC-passage OCT technique to co-localized and simultaneously acquired two-photon excitation fluorescence microscopy (TPEF) measurements. Using concurrent multi-modal imaging, we show that fluctuations in the OCT signal display highly similar features to TPEF time traces. Furthermore, we demonstrate an overall difference in RBC flux and speed of 2.5 ± 3.27 RBC/s and 0.12 ± 0.67 mm/s (mean ± S.D.), compared to TPEF. The analysis also revealed that the OCT RBC flux estimation is most accurate between 20 RBC/s to 60 RBC/s, and is severely underestimated at fluxes beyond 80 RBC/s. Lastly, our analysis shows that the RBC speed estimations increase in accuracy as the speed decreases, reaching a difference of 0.16 ± 0.25 mm/s within the 0–0.5 mm/s speed range.


1997 ◽  
Vol 3 (S2) ◽  
pp. 299-300
Author(s):  
W. W. Webb

Multiphoton molecular excitation by the strongly focused femtosecond pulses of infrared light generated as an 80 MHZ pulse train by a mode locked laser provides intrinsic submicron three dimensional spatial resolution of fluorescence excitation and photochemistry for laser scanning fluorescence microscopy. Because two-photon excitation requires simultaneous (∼10-16 seconds), absorption of two-photons focused laser intensities of about 1022 photons/cm2s are required. Since the rate of absorption is proportional to the square of the intensity, excitation is limited to the focal volume and is negligible elsewhere along the double cone of the focused illumination. Therefore, out of focus photodamage and fluorescence are generally negligible and laser scanning fluorescence microscopy with multiphoton excitation is intrinsically three dimensionally resolved with no out of focus background. Since the appropriate wave lengths are infrared for multiphoton excitation of ultraviolet or visible absorbing molecules, out of focus photodamage is eliminated. This allows imaging of useful ultraviolet absorbing indicators, vital DNA stains and autofluorescence in living cells with minimal, but not necessarily negligible, photodamage.


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