scholarly journals Cardiovascular Imaging Using Two-Photon Microscopy

2008 ◽  
Vol 14 (6) ◽  
pp. 492-506 ◽  
Author(s):  
John A. Scherschel ◽  
Michael Rubart

AbstractTwo-photon excitation microscopy has become the standard technique for high resolution deep tissue and intravital imaging. It provides intrinsic three-dimensional resolution in combination with increased penetration depth compared to single-photon confocal microscopy. This article will describe the basic physical principles of two-photon excitation and will review its multiple applications to cardiovascular imaging, including second harmonic generation and fluorescence laser scanning microscopy. In particular, the capability and limitations of multiphoton microscopy to assess functional heterogeneity on a cellular scale deep within intact, Langendorff-perfused hearts are demonstrated. It will also discuss the use of two-photon excitation-induced release of caged compounds for the study of intracellular calcium signaling and intercellular dye transfer.

2008 ◽  
Vol 14 (6) ◽  
pp. 481-481
Author(s):  
Heide Schatten

Two-photon excitation microscopy (also referred to as multiphoton laser scanning microscopy) has gained increasing popularity during the past few years because of the distinct advantages over single-photon microscopy, which includes increased penetration depth and low out-of-focus photobleaching and photodamage. It allows superior imaging of thick specimen compared to single-photon microscopy, and it excels at imaging live cells either single or within intact tissue. This highly valuable tool has been used with great success to gain important new insights into brain tissue, embryos, whole organs, entire animals, and it has been most useful in numerous other applications.


2002 ◽  
Vol 68 (2) ◽  
pp. 901-909 ◽  
Author(s):  
Thomas R. Neu ◽  
Ute Kuhlicke ◽  
John R. Lawrence

ABSTRACT A major limitation for the use of two-proton laser scanning microscopy (2P-LSM) in biofilm and other studies is the lack of a thorough understanding of the excitation-emission responses of potential fluorochromes. In order to use 2P-LSM, the utility of various fluorochromes and probes specific for a range of biofilm constituents must be evaluated. The fluorochromes tested in this study included classical nucleic acid-specific stains, such as acridine orange (AO) and 4",6"-diamidino-2-phenylindole (DAPI), as well as recently developed stains. In addition, stains specific for biofilm extracellular polymeric substances (EPS matrix components) were tested. Two-photon excitation with a Ti/Sapphire laser was carried out at wavelengths from 760 to 900 nm in 10-nm steps. It was found that autofluorescence of phototrophic organisms (cyanobacteria and green algae) resulted in strong signals for the entire excitation range. In addition, the coenzyme F420-related autofluorescence of methanogenic bacteria could be used to obtain images of dense aggregates (excitation wavelength, 780 nm). The intensities of the emission signals for the nucleic acid-specific fluorochromes varied. For example, the intensities were similar for excitation wavelengths ranging from 780 to 900 nm for AO but were higher for a narrower range, 780 to 810 nm, for DAPI. In selective excitation, fading, multiple staining, and combined single-photon-two-photon studies, the recently developed nucleic acid-specific fluorochromes proved to be more suitable regardless of whether they are intended for living or fixed samples. Probes specific for proteins and glycoconjugates allowed two-photon imaging of polymeric biofilm constituents. Selective excitation-emission was observed for Calcofluor White M2R (780 to 800 nm) and SyproOrange (880 to 900 nm). In addition, fluor-conjugated concanavalin A lectins were examined and provided acceptable two-photon emission signals at wavelengths ranging from 780 to 800 nm. Finally, CellTracker, a fluorochrome suitable for long-term labeling of microbial eucaryote cells, was found to give strong emission at wavelengths ranging from 770 to 810 nm. If fluorochromes have the same two-photon excitation cross section, they are suitable for multiple staining and multichannel recording. Generally, if an appropriate excitation wavelength and fluorochrome were used, it was possible to obtain more highly resolved images for thick biofilm samples with two-photon laser microscopy than with conventional single-photon laser microscopy. Due to its potential for higher resolution in light-scattering tissue-like material, such as biofilms, and extremely localized excitation, 2P-LSM is a valuable addition to conventional confocal laser scanning microscopy with single-photon excitation. However, further development of the method and basic research are necessary to take full advantage of nonlinear excitation in studies of interfacial microbial ecology.


2000 ◽  
Vol 6 (S2) ◽  
pp. 808-809
Author(s):  
F. J. Kao ◽  
B. L. Lin ◽  
P. C. Cheng

Considering its non-linear nature, two-photon excitation may generate very different spectral response in samples when compared with single photon excitation. It is thus necessary to measure the two-photon spectra of samples, so that the two-photon fluorescence microscopic images can be properly interpreted. Fluorescence spectra obtained from bulk samples may not provide useful information for microscopy. For instance, due to the relatively small contribution to the total fluorescence intensity, a small number of fluorescent particles in a generally fluorescing specimen may escape detection when the spectrum of the specimen as a whole is obtained. Under two-photon excitation, the background noise can be greatly reduced due to the naturally limited excitation volume of focused laser beam. In addition, signals resulted from second harmonic generation (SHG) may be mixed with low level broad-band background autofluorescence which is commonly found in biological specimen. Therefore, measuring fluorescence spectrum from a micro-focused volume is essential for the proper interpretation of multi-photon fluorescence images.


Author(s):  
David W. Piston ◽  
James H. Strickler ◽  
Watt W. Webb

The non-linear optical technique of two-photon excitation of fluorescence and photochemical reactions makes possible new applications that are not possible using linear one-photon excitation in laser scanning confocal microscopy. The two-photon excitation effect arises from the simultaneous absorption of two red photons, which causes the transition to an excited electronic state with its normal absorption in the ultraviolet. In our fluorescence experiments, this excited state is the same singlet state, S1, that is populated during a conventional fluorescence experiment, and thus exhibits the same emission properties (e.g. wavelength shifts, environmental sensitivity) that are observed in typical biological microscopy studies. Likewise, photochemical reactions such as light induced polymerization and photolytic uncaging that are normally catalyzed by UV light can be generated using two-photon excitation. In practice, twophoton excitation is made possible by the very high local instantaneous intensity that is provided by a combination of the diffraction limited focusing in the microscope and the temporal concentration of a subpicosecond mode-locked laser.


2003 ◽  
Vol 284 (6) ◽  
pp. C1654-C1668 ◽  
Author(s):  
Michael Rubart ◽  
Exing Wang ◽  
Kenneth W. Dunn ◽  
Loren J. Field

The ability to image calcium signals at subcellular levels within the intact depolarizing heart could provide valuable information toward a more integrated understanding of cardiac function. Accordingly, a system combining two-photon excitation with laser-scanning microscopy was developed to monitor electrically evoked [Ca2+]itransients in individual cardiomyocytes within noncontracting Langendorff-perfused mouse hearts. [Ca2+]itransients were recorded at depths ≤100 μm from the epicardial surface with the fluorescent indicators rhod-2 or fura-2 in the presence of the excitation-contraction uncoupler cytochalasin D. Evoked [Ca2+]i transients were highly synchronized among neighboring cardiomyocytes. At 1 Hz, the times from 90 to 50% ( t 90–50%) and from 50 to 10% ( t 50–10%) of the peak [Ca2+]i were (means ± SE) 73 ± 4 and 126 ± 10 ms, respectively, and at 2 Hz, 62 ± 3 and 94 ± 6 ms ( n = 19, P < 0.05 vs. 1 Hz) in rhod-2-loaded cardiomyocytes. [Ca2+]i decay was markedly slower in fura-2-loaded hearts ( t 90–50% at 1 Hz, 128 ± 9 ms and at 2 Hz, 88 ± 5 ms; t 50–10% at 1 Hz, 214 ± 18 ms and at 2 Hz, 163 ± 7 ms; n = 19, P < 0.05 vs. rhod-2). Fura-2-induced deceleration of [Ca2+]i decline resulted from increased cytosolic Ca2+ buffering, because the kinetics of rhod-2 decay resembled those obtained with fura-2 after incorporation of the Ca2+ chelator BAPTA. Propagating calcium waves and [Ca2+]i amplitude alternans were readily detected in paced hearts. This approach should be of general utility to monitor the consequences of genetic and/or functional heterogeneity in cellular calcium signaling within whole mouse hearts at tissue depths that have been inaccessible to single-photon imaging.


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