scholarly journals Two-photon excitation in scattering media by spatiotemporally shaped beams and their application in optogenetic stimulation

2013 ◽  
Vol 4 (12) ◽  
pp. 2869 ◽  
Author(s):  
Aurélien Bègue ◽  
Eirini Papagiakoumou ◽  
Ben Leshem ◽  
Rossella Conti ◽  
Leona Enke ◽  
...  
Keyword(s):  
Scattering Media ◽  
Two Photon ◽  
Optogenetic Stimulation ◽  
Photon Excitation ◽  
Two Photon Excitation

Spatially localized ballistic two-photon excitation in scattering media

1998 ◽  
Vol 4 (5) ◽  
pp. 303-310 ◽  
Author(s):  
Henryk Szmacinski ◽  
Ignacy Gryczynski ◽  
Joseph R. Lakowicz
Keyword(s):  
Scattering Media ◽  
Two Photon ◽  
Photon Excitation ◽  
Two Photon Excitation

Two-Photon Microscopy of Single Molecules

2000 ◽  
Vol 6 (S2) ◽  
pp. 804-805
Author(s):  
R. Yuste ◽  
A. Majewska ◽  
K. Holthoff ◽  
K. Holthoff
Keyword(s):  
Dendritic Spines ◽  
Pyramidal Neurons ◽  
Calcium Influx ◽  
Pyramidal Cells ◽  
Scattering Media ◽  
Decay Kinetics ◽  
Two Photon ◽  
Photon Excitation ◽  
Cortical Pyramidal Neurons ◽  
Two Photon Excitation

Two-photon excitation has enabled investigators to image living cells in highly scattering media like the central nervous system (1). We have used a custom-built two-photon microscope to image dendritic spines from living cortical pyramidal neurons. Pyramidal cells form the majority of the neuron in the mammalian cortex and they receive practically all their synaptic contacts through dendritic spines. Dendritic spines are small (<1 μm diameter) appendages that have been practically inaccessible to physiological measurements until the application of two-photon excitation to their study (2). We have concentrated in two questions:A- Calcium compartmentalization of spines: Mechanisms of calcium decay kinetics.Dendritic spines can compartmentalize calcium (2). Although the mechanisms of calcium influx into spines have been explored (3), it is unknown what determines the calcium decay kinetics in spines. We investigate calcium dynamics in spines from rat CA1 pyramidal neurons in slices.

Two-photon excitation microscopy in cellular biophysics

1995 ◽  
Vol 53 ◽  
pp. 62-63
Author(s):  
David W. Piston ◽  
Brian D. Bennett ◽  
Robert G. Summers
Keyword(s):  
Confocal Microscopy ◽  
Laser Beam ◽  
Duty Cycle ◽  
Excited Electronic State ◽  
Input Power ◽  
Two Photon ◽  
Simultaneous Absorption ◽  
Photon Excitation ◽  
Very High ◽  
Two Photon Excitation

Two-photon excitation microscopy (TPEM) provides attractive advantages over confocal microscopy for three-dimensionally resolved fluorescence imaging and photochemistry. Two-photon excitation arises from the simultaneous absorption of two photons in a single quantitized event whose probability is proportional to the square of the instantaneous intensity. For example, two red photons can cause the transition to an excited electronic state normally reached by absorption in the ultraviolet. In practice, two-photon excitation 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 maintains the average input power on the order of 10 mW, only slightly greater than the power normally used in confocal microscopy.

Two-photon excitation fluorescence microscopy in living systems

1993 ◽  
Vol 51 ◽  
pp. 154-155 ◽  
Author(s):  
David W. Piston
Keyword(s):  
Confocal Microscopy ◽  
Fluorescence Microscopy ◽  
Singlet State ◽  
Excited Electronic State ◽  
Input Power ◽  
Two Photon ◽  
Simultaneous Absorption ◽  
Photon Excitation ◽  
Very High ◽  
Two Photon Excitation

Two-photon excitation fluorescence microscopy provides attractive advantages over confocal microscopy for three-dimensionally resolved fluorescence imaging. Two-photon excitation arises from the simultaneous absorption of two photons in a single quantitized event whose probability is proportional to the square of the instantaneous intensity. For example, two red photons can cause the transition to an excited electronic state normally reached by absorption in the ultraviolet. In our fluorescence experiments, the final excited state is the same singlet state that is populated during a conventional fluorescence experiment. Thus, the fluorophore exhibits the same emission properties (e.g. wavelength shifts, environmental sensitivity) used in typical biological microscopy studies. In practice, two-photon excitation 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 maintains the average input power on the order of 10 mW, only slightly greater than the power normally used in confocal microscopy.

Two‐photon excitation fluorescence microscopy using a semiconductor laser

Bioimaging ◽  
1995 ◽  
Vol 3 (2) ◽  
pp. 70-75 ◽  
Author(s):  
Pekka E Hänninen ◽  
Martin Schrader ◽  
Erkki Soini ◽  
Stefan W Hell
Keyword(s):  
Fluorescence Microscopy ◽  
Semiconductor Laser ◽  
Two Photon ◽  
Photon Excitation ◽  
Two Photon Excitation

Two-Photon Excitation Imaging of Glucose Metabolism in Living Tissue

1997 ◽  
Vol 3 (S2) ◽  
pp. 305-306
Author(s):  
David W. Piston
Keyword(s):  
Confocal Microscopy ◽  
Collection Efficiency ◽  
Three Dimensional ◽  
Spatial Filter ◽  
Input Power ◽  
Photon Absorption ◽  
Focal Volume ◽  
Two Photon ◽  
Photon Excitation ◽  
Two Photon Excitation

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.

Sign in / Sign up

Export Citation Format

Share Document