Reviews |
From the Case Western Reserve University (I.R.E., V.P.N.), Cleveland, Ohio; and the University of Pittsburgh (G.S.), Pittsburgh, Pa.
Correspondence to Dr Igor R. Efimov, Case Western Reserve University, 10900 Euclid Ave, Cleveland, OH 44106-7207. E-mail efimov{at}case.edu
This Review is part of a thematic series on Imaging of Cardiovascular Cells and Tissues, which includes the following articles:
Use of Chimeric Fluorescent Proteins and Fluorescence Resonance Energy Transfer to Monitor Cellular Responses
Imaging Microdomain Ca2+ in Muscle Cells
Optical Imaging of the Heart
Examining Intracellular Organelle Function Using Fluorescent Probes
Two-Photon Microscopy of Cells and Tissue
Brian ORourke Guest Editor
| Abstract |
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Key Words: optical mapping fluorescent probes electrophysiology arrhythmia defibrillation
| Introduction |
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Unfortunately, experimental methodologies available for studies at the organ level are not as abundant as at the cellular scale. Nonoptical imaging modalities, including positron emission tomography, magnetic resonance, and ultrasound imaging have only started to bridge molecular and organ physiology using novel contrast agents.1 On the other hand, optical modes of imaging, in combination with parameter-sensitive probes have already demonstrated their ability to overcome the problem of spatiotemporal resolution in two dimensions for a wide range of applications from single molecular events to in vivo whole animal physiology.
Fluorescence has been used to measure a wide range of physiological parameters in cells and tissues. For instance, cellular metabolic state can be monitored through (1) the intrinsic fluorescence changes of NADH or flavoproteins,2 (2) the differential absorption changes of mitochondrial cytochromes, which report on the oxidative phosphorylation redox state, or (3) the oxygen content of blood and cardiac muscle through the absorption changes of oxy to deoxy hemoglobin and myoglobin, respectively.3,4 More recent has been the development of probes to selectively measure functional parameters such as membrane potential, intracellular concentrations of free calcium, magnesium, sodium and potassium, pH, nitric oxide, oxygen tension, and sulfhydryl redox sate. Of these, optical probes of membrane potential and intracellular free calcium ([Ca2+]i) indicators have had the most impact in cardiovascular physiology. The development of optical recordings of membrane potential was driven by the need to overcome many obstacles in electrophysiology and the promise of a technology "for measuring membrane potential in systems where, for reasons of scale, topology, or complexity, the use of electrodes is inconvenient or impossible."5 Specific to cardiac electrophysiology, there was also the need to record transmembrane voltage changes during or immediately after the firing of electric shocks used for defibrillation. Optical mapping techniques and potentiometric probes have now made major contributions to our understanding of nerve network behavior and cardiac electrophysiology in ways that could not have been accomplished by other approaches. Advances in neuroscience driven by optical mapping have been extensively reviewed.6,7 Although there is considerable overlap in the instruments used for optical mapping of neuronal and cardiac tissues, there are also important differences, and this review will focus on instrumentation, optical probes, major findings, and future directions of optical imaging as it applies to the heart.
| General Principles |
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The ionic basis of cellular electrophysiology, intercellular coupling, and electrical propagation are understood with considerable detail. Although intracellular and patch-clamp microelectrode techniques have been used to elucidate the physiology of excitable cells, an understanding of the behavior of cardiac tissues have been more difficult to attain by conventional electrode techniques. More than 30 years ago, investigators discovered molecular probes that bind to the plasma membrane of neuronal11 and cardiac cells12 and exhibited changes in fluorescence and/or absorption that tracked changes in transmembrane potential.
Several optical properties of membrane-bound dyes have been used to measure membrane potential changes; namely, fluorescence, absorption, dichroism, birefringence, fluorescence resonance energy transfer, nonlinear second harmonic generation, and resonance Raman absorption. However, most studies in cardiac cells or tissues have relied on the fluorescence mode that tends to yield higher fractional changes in signal compared with the other modes and because fluorescence signals tend to be considerably less sensitive to movement artifacts generated by muscle contractions.12,13
Several mechanisms have been proposed to explain voltage-dependent changes in fluorescence and/or absorption of dye molecules based on interactions of the electric field with dye molecules resulting in intra- and extramolecular rearrangements of the dye in the membrane. Cohen and Salzberg7 introduced a simple classification of voltage-sensitive dyes into two groups, fast and slow dyes, based on their response times and presumed molecular mechanism of voltage sensitivity. Only the fast probes are used in cardiac electrophysiology, due to their ability to follow voltage changes on a time scale of microseconds.14 The precise mechanisms underlying the voltage-dependent spectroscopic properties of fast voltage-sensitive dyes are still not fully understood. Spectral shift in the properties of chromophore is thought to be related to the changes in excitation-induced intramolecular relocation of electronic charge along the electric field gradient (electrochromic theory15) or to electric fieldinduced reorientation of the dye molecule in the plasma membrane (solvatochromic theory16).
| New Molecular Probes for Optical Recordings of Electrical Activity |
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Initial studies were performed with a class of molecules called merocyanine dyes, which exhibited 1% fractional changes in fluorescence in cardiac tissue.12,13,17 As shown in Figure 1A, action potentials were simultaneously recorded through the fluorescence changes of the potentiometric dye and with an intracellular microelectrode. The fluorescence action potentials were recorded from frog ventricular tissue stained with merocyanine 540 from a 2-mm diameter excitation spot and compared with microelectrode recording from one of the cells excited by the incident light beam. The two techniques show excellent correlation between the two signals. In the intact heart, surface or volume electrograms are also in excellent correlation with optical recordings. But unlike electrode recordings, optical signals can be easily recorded from different regions of the heart by simply displacing the optical paths. Figure 1B shows examples of optical action potentials from different regions of atrial and ventricular rabbit myocardium.
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Early studies faced marked phototoxic effects of potentiometric probes in some preparations.11,17 These initial obstacles were resolved through the development of better probes with reduced phototoxic effects and greater sensitivity to potential changes. A.S. Waggoner, L.A. Ernst, and G. Salama (unpublished data, 2003) have recently developed and tested new potentiometric dyes in search of probes with greater fractional fluorescence changes per action potential and longer peak excitation and emission wavelengths, with large Stoke shifts. The longer wavelengths would be particularly desirable for optical recordings from deep inside the myocardial wall as light absorption and scattering diminishes with longer wavelengths. One of these new dyes, PGH1 (Pittsburgh 1), was found to yield excellent signal-to-noise ratio and stability when applied to the whole heart with an excitation wavelength of 690 nm and an emission at 850 nm. Although initial tests of PGH1 by several groups were highly positive in heart (B.-R. Choi, University of Pittsburgh, Pa, and R.A. Gray, University of Alabama), experiments on isolated cells reported up to 30% fractional fluorescence change per action potential, but a high level of photobleaching or phototoxicity (E. Entcheva, Stony Brook University, G. Smith, University of Glasgow, personal communication). Further modifications of successful potentiometric probes and better staining procedures are likely to yield improvements in voltage sensitivity, depth penetration of the signals, and the opportunity to detect increasingly smaller potential changes from smaller areas of membrane stained with dye.
Another significant limitation of optical mapping of the heart is artifact introduced by the muscle contractions. These "movement" artifacts distort optical action potentials, preventing accurate recordings of repolarization phase. Several methods have been used in the past to minimize the effect of movement artifact. Mechanical restriction of the movement can successfully restrict the artifact without affecting physiology of the heart.19 This method works particularly well with small hearts such as mice, rats, and guinea pig. Alternatives include various pharmacological approaches, such as calcium channel blockers,20 2,3-butanedione monoxime,21,22 or cytochalasin D.23 Another approach to reduce movement artifacts is to apply a ratiometric technique.24,25 This method is based on simultaneous measurements of fluorescent signal at two different wavelength ranges: one where the dye exhibits a largest voltage-dependent response and the other at a wavelength where the potentiometric dye exhibits an inverted or no voltage-dependent response. The ratio or difference of these two signals would then result in an optical signal free of, or with significantly reduced, motion artifacts.2426 Unfortunately, this method works well with relatively weak contractions and with biphasic action spectra of fluorescent and/or absorption dyes.27
| Calibration of Optical Recordings |
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| Need for Optical Mapping |
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| Progress in Imaging Technology: Advances in Light Detectors |
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PDA technology was first developed by Centronix.40,41 Now PDAs are available from Hamamatsu. WuTech42 produces custom arrays of arbitrary size and shape made of individual photodiodes.43
CCD technology has a significant advantage of higher spatial resolution due to the large number of pixels on a CCD sensor. However, the rate of data acquisition is usually lower. This can be increased by pixel binning; however, this defeats the major advantage of CCD technology because binning reduces spatial resolution. For example, a camera from DALSA has 128x128 pixels at 490 frames/sec.
Theoretically, CCD technology should provide significant advantages with respect to signal-to-noise ratio, particularly at low-light applications, due to the right combination of high quantum efficiency and low background noise level. It is important to emphasize that an optical mapping experiment on a whole heart or a multicellular preparations tends not to be light-limited but deals with conditions where the greater the fluorescence intensity from the preparation, the greater the absolute amplitude of the fractional fluorescence change. The dynamic range of CCD cameras is constrained by the accuracy of A/D conversion and the saturation of the sensor at light levels readily detected from heart tissue; a dynamic range of 103 is not easily achieved. Thus, for practical purposes the majority of single cell and cell culture optical mapping studies has been done using PDA.4345
Improvements in CMOS technology produced a family of novel image sensors with high-speed image acquisition while retaining the quantum efficiency of CCD. MiCAM Ultima CMOS camera from SciMedia was recently tested on a perfused guinea pig heart at 10 000 frames/sec and 100x100 pixels. High signal-to-noise ratio allowed detection of activation times from the first derivative of optical signals during ventricular fibrillation without spatial averaging. CMOS cameras are more costly than CCD or PDA cameras. However, due to clear advantages these CMOS cameras will become competitive soon.
| Design of Optical Mapping System |
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| Mapping of Activation and Repolarization |
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Conventional high-resolution multielectrode mapping was successful in assessing activation sequences. However, repolarization was generally beyond the capabilities of electrode mapping.32 Only a monophasic action potential (MAP) technique57 was able to reliably measure repolarization and action potential duration. However, MAP cannot be used for multisite mapping. Optical mapping provides a tool with the unique ability to overcome limitations of electrode-based techniques and to reliably and faithfully record action potentials. However, it typically requires the use of mechanical or pharmacological immobilization techniques to suppress the motion artifacts.
In particular, optical mapping has made a significant contribution to our understanding of the role of intrinsic myocardial heterogeneities in the normal repolarization processes in normal heart;19,55 of dynamic concordant and discordant alternans in the onset of ventricular tachyarrhythmias;58,59 and the role of the slope of the restitution curve in the transition from ventricular tachycardia to fibrillation.6062
| Mapping of Stimulation and Defibrillation |
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| Mapping of the Impulse Generation and Conduction System of the Heart |
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In addition to contributing to our understanding of mechanisms of impulse generation and conduction, these studies demonstrated the ability of optical techniques to assess electrical activity in three dimensions. Figure 5 presents22,80 an example of optical (OAP) and microelectrode (MAP) action potential recordings and histology from the distal AV junctional area of the rabbit heart. Figure 5B shows histology of this area in another preparation from the apical area of the triangle of Koch,80 which clearly shows multilayered morphology of the AV junction. One can see the thin layer of AN transitional tissue (
), the compact AV node (
), and loosely coupled deeper layer of NH transitional cells. Optical action potentials (OAPs) recorded during conducted beats contained two components, representing electrical activity in the two layers. OAPs recorded during AV block contained only one component. Microelectrode recordings conducted simultaneously provides evidence that the first component of optical recording corresponds to the superficial transitional AN layer (see
, in Figure 5A and 5B) of the AV junction, whereas the second component represents electrical activity of the deeper NH layer (
in Figure 5A and 5B).
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| Mapping of Atrial and Ventricular Tachyarrhythmias |
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Jalifes group pioneered the application of optical mapping to study arrhythmogenesis8184 and made numerous significant contributions to our understanding of mechanisms of both atrial83 and ventricular arrhythmias.48,84 Since that time, many groups presented optical mapping data supporting reentrant nature of ventricular tachycardia66,81,85,86 and fibrillation.48,87,88 Furthermore, optical mapping presented evidence for 3D nature of ventricular reentry, which is sustained by scroll waves.86,89
Despite the success of dynamic optical imaging of wavefronts and phase singularities during arrhythmias, there is still no agreement on the mechanisms that induce and sustain ventricular and atrial fibrillation.90 Two competing dominant theories are being tested: the so-called "mother rotor"9193 and "break-up"9498 hypotheses. According to the mother rotor hypothesis, ventricular fibrillation is maintained by a single or limited number of leading centers of reentrant nature, ie, mother rotors. These centers occupy regions of myocardium that are capable of sustaining the highest possible frequency of reentrant activity.9193 Disorganized activity observed throughout the heart, in regions beyond those of the mother rotor(s) results from conduction blocks between the regions encompassed by the mother rotor and regions with longer refractory periods. In contrast, the break-up theory proposes that fibrillation is perpetuated by dynamic or anatomic heterogeneities in the myocardium sustained through constant creation and annihilation of waves.94,9698 Profound complexity of conduction patterns during fibrillation makes quantitative analysis of wavefronts and wavebreaks a formidable task.35,99 Therefore, frequency analysis of optical data was adopted98,100 following the pioneering work of Wiggers.101 As presented in Figure 6A, according to one school of thought,100 during fibrillation, dominant frequencies of electrical activity are distributed in a stationary pattern. This appears to support the mother rotor hypothesis. On the other hand, as presented in Figure 6B and 6C,98 another group of investigators presents evidence of constantly changing pattern of frequencies of electrical activity without clear dominant frequency. This issue remains controversial as evidence in support of both theories continues to appear in the literature.
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| Multiparametric Optical Mapping: Imaging of Voltage and Intracellular Calcium |
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The first techniques for measuring changes in cytosolic [Ca2+]i concentration of coronary-perfused hearts involved 19F nuclear magnetic resonance,106,107 fluorescent Ca2+ indicator Indo-1,108 and a bioluminescent Ca2+ indicator aequorin.109 Later, other fluorescent Ca2+ indicators (Fluo 3110 and Rhod 2111,112) were successfully used for heart imaging. Simultaneous Ca2+ and voltage imaging of the heart has also been achieved by costaining with RH421 and Rhod-2,113 RH237, and Rhod-2,59,114 with RH237 and Fluo-4/Oregon Green BARTA 1,25 with di-4-ANEPPS and Fluor3/4,115 and with di-4-ANEPPS and Indo-1.116
Figure 7 shows the optical system for simultaneous recording voltage and [Ca2+]i signals from perfused hearts stained with RH237 and Rhod-2.59 It uses two PDAs (Figure 7A). RH237 and Rhod-2 dyes can be excited at the same wavelength but fluoresce at different wavelengths, allowing the separation of the Vm and [Ca2+]i signals. Rhod-2 was found to be an excellent Ca2+ indicator for perfused hearts because of its rapid association/dissociation with Ca2+, fast loading into myocytes of perfused hearts, and long-term stability or low levels of exocytosis.59 The independence of Vm and [Ca2+]i recordings is illustrated in Figure 7C through 7E. First, signals from both Vm and [Ca2+]i arrays were recorded when the heart was stained with one of the two dyes but not both dyes. Second, after staining with both dyes, Vm and [Ca2+]i signals were recorded before and after the addition of ryanodine, known to markedly inhibit [Ca2+]i transients.
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Multiparametric optical mapping is still in its infancy. Other probes are being synthesized and evaluated for simultaneous recordings from the same tissue, stained with multiple fluorescent probes. This exciting progress is likely to bring about a better understanding of cellular physiology at a tissue and organ level.
| Mapping Transgenic Mouse Models |
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Dominant-negative transgenic mice that overexpress an N-terminal fragment of the K+ channel Kv1.1 were shown to exhibit prolonged action potential duration due to the loss of a slowly inactivating 4-aminopyrydine sensitive current, Islow, which is likely to be encoded by Kv1.5.118 These mice were found to have long-QT intervals, spontaneous nonsustained ventricular tachycardia (VT) during ambulatory telemetry monitoring and inducible polymorphic VT during programmed stimulation in anesthetized open chest preparations.118,119 Optical mapping demonstrated a 2-fold increase in action potential durations and enhanced dispersion of repolarization from apex to base in dominant-negative transgenic mice.120 In dominant-negative transgenic mice, a premature impulse applied at the apex of the heart produced sustained reentrant VT that did not occur with stimulation at any location in controls hearts.120 Direct injection of adenoviral vectors expressing wild-type Kv1.5 (AV-Kv1.5) in the myocardium of these Kv1 dominant-negative transgenic mice resulted in the overexpression of Kv1.5, a shortening of APD, shortened the QT interval, decreased dispersion of repolarization, and increased the heart rate. These changes were consistent with a physiological reversal of the arrhythmogenic phenotype by the adenoviral induced expression of Kv1.5 in Kv1 dominant-negative mice.121
Transgenic mice overexpressing the inflammatory cytokine tumor necrosis factor
(TNF-
) develop a progressive heart failure (HF) phenotype characterized by biventricular dilatation, decreased ejection fraction, and ventricular arrhythmias on ambulatory telemetry and decreased survival compared with control liter mates. Optical maps of action potentials and [Ca2+]i transients showed that TNF-
hearts had prolonged action potential durations, no change in dispersion of repolarization, elevated diastolic, depressed systolic, and prolonged [Ca2+]i compared with controls.114 Premature beats had lower action potential amplitudes, slower conduction velocities, and elicited reentrant beats. Increasing heart rate produced [Ca2+]i alternans in TNF-
but not in control hearts. In this model, anomalies of both AP and [Ca2+]i contributed to arrhythmias.
Gap junction channels are essential for cell-to-cell coupling and impulse propagation. Changes in channel conductance may underlie the development and maintenance of lethal arrhythmias in pathological conditions.122124 Null mutations of connexin 43 (Cx43) in mice, the predominant gap junction channel proteins in ventricular tissue, was lethal in homozygous (Cx43/) mice but seemingly normal in heterozygous (Cx43+/) mice. Measurements of conduction velocity from the same line of Cx43+/ mice produced conflicting results depending on the optical mapping technique. Using a CCD camera, Morley et al125 found no significant difference in conduction velocity between heterozygous Cx43+/ mice and controls, whereas Eloff et al126 found a 23% to 35% slowing of conduction velocity using a photodiode array (PDA) to map action potentials. The different findings perhaps reflect the differences in temporal resolution of the CCD and PDA technology because the same line of Cx43+/ mice was used in both studies.
| Mapping Developing Myocardium |
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| Emerging Optical Imaging Modalities |
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To overcome the depth limitation, Hooks et al140 developed an elegant optrode-based method. This method extends the idea of a plunge needle electrode.141 Plunge optrodes present a unique possibility for multisite intramural recordings of transmembrane potential,140,142 yet cause damage of the myocardium.
Depth restriction is due to light absorption and scattering on intrinsic differences of tissue optical properties (endogenous contrast). Absorption occurs primarily at endogenous chromospheres of hemoglobin, melanin, fat, and water. Scattering is usually due to refractive index differences of extra- and intracellular structures. These properties are strongly wavelength-dependent. Baxter et al143 proposed an original method that takes advantage of this wavelength dependence to visualize excitation waves within the cardiac muscle. Light in the 700- to 900-nm range is known as the "therapeutic window," due to low intrinsic tissue absorbance and high scattering of photons dominates in this range of wavelengths. This window opened an opportunity for tomographic reconstruction of 3D structures using novel biophotonics imaging modalities, such as optical coherence tomography.137,144
Optical coherence tomography (OCT) exploits the heart tissue scattering heterogeneity and at present can reconstruct through 2- to 3-mm depth of cardiac tissue with up to 1-µm resolution. The latter characteristics make tomography a method of choice for in situ analysis of embryonic heart morphology,136,137 AV nodal multilayer structures (Figure 8),145 or complex 3D geometry of trabeculated structures of myocardium and the Purkinje network146 (Figure 8). Presently available OCT technology is limited to structural imaging only. However, emerging second harmonic OCT technique147,148 could directly resolve the 2D limitations of conventional optical mapping. Alternatively, 3D limitations could potentially be addressed with confocal,149 Nipkow disk, or Ronchi grating150 approaches. Another promising direction relies on the possibility of solving the inverse problem for light diffusion/scattering in the tissue.9 This could numerically separate the optical signal collected from the heart surface into individual components related to signals from the different layers of the tissue.
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| Conclusion |
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| Acknowledgments |
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| Footnotes |
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| References |
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2. Chance B, Salkovitz IA, Kovach AG. Kinetics of mitochondrial flavoprotein and pyridine nucleotide in perfused heart. Am J Physiol. 1972; 223: 207218.
3. Chance B. On the mechanism of the reaction of cytochrome oxidase with oxygen. Ann N|Y Acad Sci. 1975; 244: 163173.[Medline] [Order article via Infotrieve]
4. Salama G, Lombardi R, Elson J. Maps of optical action potentials and NADH fluorescence in intact working hearts. Am J Physiol. 1987; 252: H384H394.[Medline] [Order article via Infotrieve]
5. Cohen LB, Lesher, S. Optical monitoring of membrane potential: methods of multisite optical measurement. In: Optical Methods in Cell Physiology. De Weer P, Salzberg BM, eds. New York: Wiley-Interscience; 1986.
6. Zochowski M, Wachowiak M, Falk CX, Cohen LB, Lam YW, Antic S, Zecevic D. Imaging membrane potential with voltage-sensitive dyes. Biol Bull. 2000; 198: 121.[Abstract]
7. Cohen LB, Salzberg BM. Optical measurement of membrane potential. Rev Physiol Biochem Pharmacol. 1978; 83: 3588.[Medline] [Order article via Infotrieve]
8. Dehghani H, Delpy DT, Arridge SR. Photon migration in non-scattering tissue and the effects on image reconstruction. Phys Med Biol. 1999; 44: 28972906.[CrossRef][Medline] [Order article via Infotrieve]
9. Arridge SR, Schweiger M. Image reconstruction in optical tomography. Philos Trans R Soc Lond B Biol Sci. 1997; 352: 717726.
10. Huang D, Swanson EA, Lin CP, Schuman JS, Stinson WG, Chang W, Hee MR, Flotte T, Gregory K, Puliafito CA. Optical coherence tomography. Science. 1991; 254: 11781181.
11. Davila HV, Salzberg BM, Cohen LB, Waggoner AS. A large change in axon fluorescence that provides a promising method for measuring membrane potential. Nat New Biol. 1973; 241: 159160.[Medline] [Order article via Infotrieve]
12. Salama G, Morad M. Merocyanine 540 as an optical probe of transmembrane electrical activity in the heart. Science. 1976; 191: 485487.
13. Morad M, Salama G. Optical probes of membrane potential in heart muscle. J Physiol (Lond). 1979; 292: 267295.
14. Lev-Ram V, Grinvald A. Ca2+- and K+-dependent communication between central nervous system myelinated axons and oligodendrocytes revealed by voltage- sensitive dyes. Proc Natl Acad Sci U S A. 1986; 83: 66516655.
15. Loew LM, ed. Spectroscopic Membrane Probes. Boca Raton, Fla: CRC Press; 1988.
16. Clarke RJ, Zouni A, Holzwarth JF. Voltage sensitivity of the fluorescent probe RH421 in a model membrane system. Biophys J. 1995; 68: 14061415.[Medline] [Order article via Infotrieve]
17. Ross WN, Salzberg BM, Cohen LB, Grinvald A, Davila HV, Waggoner AS, Wang CH. Changes in absorption, fluorescence, dichroism, and birefringence in stained giant axons: optical measurement of membrane potential. J Membr Biol. 1977; 33: 141183.[CrossRef][Medline] [Order article via Infotrieve]
18. Salama G. Optical Measurements of Transmembrane Potential in Heart. In: Spectroscopic Membrane Probes. Loew LM, ed. Boca Raton, Fla: CRC Press; 1988.
19. Efimov IR, Huang DT, Rendt JM, Salama G. Optical mapping of repolarization and refractoriness from intact hearts. Circulation. 1994; 90: 14691480.
20. Dillon SM. Optical recordings in the rabbit heart show that defibrillation strength shocks prolong the duration of depolarization and the refractory period. Circ Res. 1991; 69: 842856.
21. Li T, Sperelakis N, Teneick RE, Solaro RJ. Effects of diacetyl monoxime on cardiac excitation-contraction coupling. J Pharmacol Exp Ther. 1985; 232: 688695.
22. Efimov IR, Mazgalev TN. High-resolution three-dimensional fluorescent imaging reveals multilayer conduction pattern in the atrioventricular node. Circulation. 1998; 98: 5457.
23. Wu J, Biermann M, Rubart M, Zipes DP. Cytochalasin D as excitation-contraction uncoupler for optically mapping action potentials in wedges of ventricular myocardium. J Cardiovasc Electrophysiol. 1998; 9: 13361347.[Medline] [Order article via Infotrieve]
24. Rohr S, Kucera JP. Optical recording system based on a fiber optic image conduit: assessment of microscopic activation patterns in cardiac tissue. Biophys J. 1998; 75: 10621075.[Medline] [Order article via Infotrieve]
25. Kong W, Walcott GP, Smith WM, Johnson PL, Knisley SB. Emission ratiometry for simultaneous calcium and action potential measurements with coloaded dyes in rabbit hearts: reduction of motion and drift. J Cardiovasc Electrophysiol. 2003; 14: 7682.[CrossRef][Medline] [Order article via Infotrieve]
26. Knisley SB, Justice RK, Kong W, Johnson PL. Ratiometry of transmembrane voltage-sensitive fluorescent dye emission in hearts. Am J Physiol. 2000; 279: H1421H1433.
27. Salama G. Merocyanine Dyes as Optical Probes of Membrane Potential in Heart. PhD thesis. University of Pennsylvania; 1977.
28. Zhang J, Davidson RM, Wei MD, Loew LM. Membrane electric properties by combined patch clamp and fluorescence ratio imaging in single neurons. Biophys J. 1998; 74: 4853.[Medline] [Order article via Infotrieve]
29. Ideker RE, Smith WM, Blanchard SM, Reiser SL, Simpson EV, Wolf PD, Danieley ND. The assumptions of isochronal cardiac mapping. Pacing Clin Electrophysiol. 1989; 12: 456478.[CrossRef][Medline] [Order article via Infotrieve]
30. Josephson ME, Horowitz LN, Farshidi A. Continuous local electrical activity. A mechanism of recurrent ventricular tachycardia. Circulation. 1978; 57: 659665.
31. Haws CW, Lux RL. Correlation between in vivo transmembrane action potential durations and activation-recovery intervals from electrograms: effects of interventions that alter repolarization time. Circulation. 1990; 81: 281288.
32. Steinhaus BM. Estimating cardiac transmembrane activation and recovery times from unipolar and bipolar extracellular electrograms: a simulation study. Circ Res. 1989; 64: 449462.
33. Dillon S, Morad M. A new laser scanning system for measuring action potential propagation in the heart. Science. 1981; 214: 453456.
34. Banville I, Gray RA, Ideker RE, Smith WM. Shock-induced figure-of-eight reentry in the isolated rabbit heart. Circ Res. 1999; 85: 742752.
35. Zaitsev AV, Guha PK, Sarmast F, Kolli A, Berenfeld O, Pertsov AM, de Groot JR, Coronel R, Jalife J. Wavebreak formation during ventricular fibrillation in the isolated, regionally ischemic pig heart. Circ Res. 2003; 92: 546553.
36. Sidorov VY, Woods MC, Wikswo JP. Effects of elevated extracellular potassium on the stimulation mechanism of diastolic cardiac tissue. Biophys J. 2003; 84: 34703479.[Medline] [Order article via Infotrieve]
37. Laurita KR, Rosenbaum DS. Implications of ion channel diversity to ventricular repolarization and arrhythmogenesis: insights from high resolution optical mapping. Can J Cardiol. 1997; 13: 10691076.[Medline] [Order article via Infotrieve]
38. Clark DM, Pollard AE, Ideker RE, Knisley SB. Optical transmembrane potential recordings during intracardiac defibrillation-strength shocks. J Interv Card Electrophysiol. 1999; 3: 109120.[CrossRef][Medline] [Order article via Infotrieve]
39. Knisley SB, Neuman MR. Simultaneous electrical and optical mapping in rabbit hearts. Ann Biomed Eng. 2003; 31: 3241.[CrossRef][Medline] [Order article via Infotrieve]
40. Fujii S, Hirota A, Kamino K. Action potential synchrony in embryonic precontractile chick heart: optical monitoring with potentiometric dyes. J Physiol (Lond). 1981; 319: 529541.
41. Salama G, Sanger T, Cohen LB. Optical recordings of action potential propagation in intact heart. Biological Bulletin. 1981; 61: 316.[CrossRef]
42. Sakai T. Optical mapping of the spread of excitation in the isolated rat atrium during tachycardia-like excitation. Pflugers Arch. 2003; 447: 280288.[CrossRef][Medline] [Order article via Infotrieve]
43. Rohr S, Salzberg BM. Multiple site optical recording of transmembrane voltage (MSORTV) in patterned growth heart cell cultures: assessing electrical behavior, with microsecond resolution, on a cellular and subcellular scale. Biophys J. 1994; 67: 13011315.[Medline] [Order article via Infotrieve]
44. Fast VG, Rohr S, Gillis AM, Kleber AG. Activation of cardiac tissue by extracellular electrical shocks: formation of secondary sources at intercellular clefts in monolayers of cultured myocytes. Circ Res. 1998; 82: 375385.
45. Windisch H, Ahammer H, Schaffer P, Muller W, Platzer D. Optical multisite monitoring of cell excitation phenomena in isolated cardiomyocytes. Pflugers Archiv Euro J Physiol. 1995; 430: 508518.[CrossRef]
46. Gray RA, Jalife J, Panfilov A, Baxter WT, Cabo C, Davidenko JM, Pertsov AM. Nonstationary vortexlike reentrant activity as a mechanism of polymorphic ventricular tachycardia in the isolated rabbit heart. Circulation. 1995; 91: 24542469.
47. Fast VG, Kleber AG. Block of impulse propagation at an abrupt tissue expansion: evaluation of the critical strand diameter in 2- and 3- dimensional computer models. Cardiovasc Res. 1995; 30: 449459.[CrossRef][Medline] [Order article via Infotrieve]
48. Gray RA, Pertsov AM, Jalife J. Spatial and temporal organization during cardiac fibrillation. Nature. 1998; 392: 7578.[CrossRef][Medline] [Order article via Infotrieve]
49. Bray MA, Wikswo JP. Considerations in phase plane analysis for nonstationary reentrant cardiac behavior. Phys Rev E Stat Nonlin Soft Matter Phys. 2002; 65: 051902.[Medline] [Order article via Infotrieve]
50. Efimov IR, Ermentrout B, Huang DT, Salama G. Activation and repolarization patterns are governed by different structural characteristics of ventricular myocardium: experimental study with voltage-sensitive dyes and numerical simulations. J Cardiovasc Electrophysiol. 1996; 7: 512530.[Medline] [Order article via Infotrieve]
51. Choi BR, Burton F, Salama G. Cytosolic Ca2+ triggers early afterdepolarizations and Torsade de Pointes in rabbit hearts with type 2 long QT syndrome. J Physiol. 2002; 543: 615631.
52. Rosenbaum DS, Kaplan DT, Kanai A, Jackson L, Garan H, Cohen RJ, Salama G. Repolarization inhomogeneities in ventricular myocardium change dynamically with abrupt cycle length shortening. Circulation. 1991; 84: 13331345.
53. Salama G, Kanai A, Efimov IR. Subthreshold stimulation of Purkinje fibers interrupts ventricular tachycardia in intact hearts: experimental study with voltage-sensitive dyes and imaging techniques. Circ Res. 1994; 74: 604619.
54. Morley GE, Vaidya D, Samie FH, Lo C, Delmar M, Jalife J. Characterization of conduction in the ventricles of normal and heterozygous Cx43 knockout mice using optical mapping. J Cardiovasc Electrophysiol. 1999; 10: 13611375.[Medline] [Order article via Infotrieve]
55. Kanai A, Salama G. Optical mapping reveals that repolarization spreads anisotropically and is guided by fiber orientation in guinea pig hearts. Circ Res. 1995; 77: 784802.
56. Tamaddon HS, Vaidya D, Simon AM, Paul DL, Jalife J, Morley GE. High-resolution optical mapping of the right bundle branch in connexin40 knockout mice reveals slow conduction in the specialized conduction system. Circ Res. 2000; 87: 929936.
57. Franz MR. Method and theory of monophasic action potential recording. Prog Cardiovasc Dis. 1991; 33: 347368.[CrossRef][Medline] [Order article via Infotrieve]
58. Pastore JM, Girouard SD, Laurita KR, Akar FG, Rosenbaum DS. Mechanism linking T-wave alternans to the genesis of cardiac fibrillation. Circulation. 1999; 99: 13851394.
59. Choi BR, Salama G. Simultaneous maps of optical action potentials and calcium transients in guinea-pig hearts: mechanisms underlying concordant alternans. J Physiol. 2000; 529 Pt 1: 171188.
60. Laurita KR, Girouard SD, Rudy Y, Rosenbaum DS. Role of passive electrical properties during action potential restitution in intact heart. Am J Physiol. 1997; 273: H1205H1214.[Medline] [Order article via Infotrieve]
61. Banville, E. Gray, R. A. Effect of cytochalasin D on action potential duration restitution. Pacing Clin Electrophysiol. 2000; 23: 609.
62. Weiss JN, Chen PS, Qu Z, Karagueuzian HS, Lin SF, Garfinkel A. Electrical restitution and cardiac fibrillation. J Cardiovasc Electrophysiol. 2002; 13: 292295.[CrossRef][Medline] [Order article via Infotrieve]
63. Wikswo JP, Lin SF, Abbas RA. Virtual electrodes in cardiac tissue: a common mechanism for anodal and cathodal stimulation. Biophys J. 1995; 69: 21952210.[Medline] [Order article via Infotrieve]
64. Nikolski V, Efimov IR. Virtual electrode polarization of ventricular epicardium during bipolar stimulation. J Cardiovasc Electrophysiol. 2000; 11: 605.[Medline] [Order article via Infotrieve]
65. Efimov IR, Cheng YN, Biermann M, Van Wagoner DR, Mazgalev T, Tchou PJ. Transmembrane voltage changes produced by real and virtual electrodes during monophasic defibrillation shock delivered by an implantable electrode. J Cardiovasc Electrophysiol. 1997; 8: 10311045.[Medline] [Order article via Infotrieve]
66. Efimov IR, Cheng Y, Van Wagoner DR, Mazgalev T, Tchou PJ. Virtual electrode-induced phase singularity: a basic mechanism of failure to defibrillate. Circ Res. 1998; 82: 918925.
67. Gillis AM, Fast VG, Rohr S, Kleber AG. Mechanism of ventricular defibrillation : the role of tissue geometry in the changes in transmembrane potential in patterned myocyte cultures. Circulation. 2000; 101: 24382445.
68. Efimov IR, Aguel F, Cheng Y, Wollenzier B, Trayanova N. Virtual electrode polarization in the far field: implications for external defibrillation. Am J Physiol. 2000; 279: H1055H1070.
69. Lin S-F, Roth BJ, Wikswo J. P. Quatrefoil reentry in myocardium: an optical imaging study of the induction mechanism. J Cardiovasc Electrophysiol. 1999; 10: 574586.[Medline] [Order article via Infotrieve]
70. Efimov IR, Gray RA, Roth BJ. Virtual electrodes and de-excitation: new insights into fibrillation induction and defibrillation. J Cardiovasc Electrophysiol. 2000; 11: 339353.[Medline] [Order article via Infotrieve]
71. Fujii S, Hirota A, Kamino K. Optical recording of development of electrical activity in embryonic chick heart during early phases of cardiogenesis. J Physiol (Lond). 1981; 311: 147160.
72. Hirota A, Fujii S, Kamino K. Optical monitoring of spontaneous electrical activity of 8-somite embryonic chick heart. Jpn J Physiol. 1979; 29: 635639.[Medline] [Order article via Infotrieve]
73. Hirota A, Sakai T, Fujii S, Kamino K. Initial development of conduction pattern of spontaneous action potential in early embryonic precontractile chick heart. Dev Biol. 1983; 99: 517523.[CrossRef][Medline] [Order article via Infotrieve]
74. Sawanobori T, Hirota A, Fujii S, Kamino K. Optical recording of conducted action potential in heart muscle using a voltage-sensitive dye. Jpn J Physiol. 1981; 31: 369380.[Medline] [Order article via Infotrieve]
75. Sakai T, Hirota A, Momose-Sato Y, Sato K, Kamino K. Optical mapping of conduction patterns of normal and tachycardia-like excitations in the rat atrium. Jpn J Physiol. 1997; 47: 179188.[CrossRef][Medline] [Order article via Infotrieve]
76. Efimov IR, Fahy GJ, Cheng YN, Van Wagoner DR, Tchou PJ, Mazgalev TN. High resolution fluorescent imaging of rabbit heart does not reveal a distinct atrioventricular nodal anterior input channel (fast pathway) during sinus rhythm. J Cardiovasc Electrophysiol. 1997; 8: 295306.[Medline] [Order article via Infotrieve]
77. Choi BR, Salama G. Optical mapping of atrioventricular node reveals a conduction barrier between atrial and nodal cells. Am J Physiol. 1998; 274: H829H845.[Medline] [Order article via Infotrieve]
78. Nikolski V, Efimov IR. Fluorescent imaging of a dual-pathway conduction system of the AV-node. Circulation. 2000; 102: 3.
79. Nikolski VP, Jones SA, Lancaster MK, Boyett MR, Efimov IR. Cx43 and the dual-pathway electrophysiology of the AV node and AV nodal reentry. Circ Res. 2003; 92: 469475.
80. Dobrzynski H, Nikolski VP, Sambelashvili AT, Greener ID, Yamamoto M, Boyett MR, Efimov IR. Site of origin and molecular substrate of atrioventricular junctional rhythm in the rabbit heart. Circ Res. 2003; 93: 11021110.
81. Davidenko JM, Kent PF, Chialvo DR, Michaels DC, Jalife J. Sustained vortex-like waves in normal isolated ventricular muscle. Proc Natl Acad Sci U S A. 1990; 87: 87858789.
82. Davidenko JM, Pertsov AV, Salomonsz R, Baxter W, Jalife J. Stationary and drifting spiral waves of excitation in isolated cardiac muscle. Nature. 1992; 355: 349351.[CrossRef][Medline] [Order article via Infotrieve]
83. Gray RA, Ayers G, Jalife J. Video imaging of atrial defibrillation in the sheep heart. Circulation. 1997; 95: 10381047.
84. Gray RA, Jalife J, Panfilov AV, Baxter WT, Cabo C, Davidenko JM, Pertsov AM. Mechanisms of cardiac fibrillation. Science. 1995; 270: 12221223;discussion 12245.
85. Girouard SD, Pastore JM, Laurita KR, Gregory KW, Rosenbaum DS. Optical mapping in a new guinea pig model of ventricular tachycardia reveals mechanisms of multiple wavelengths in a single reentrant circuit. Circulation. 1996; 93: 603613.
86. Efimov IR, Sidorov VY, Cheng Y, Wollenzier B. Evidence of 3D scroll waves with ribbon-shaped filament as a mechanism of ventricular tachycardia in the isolated rabbit heart. J Cardiovasc Electrophysiol. 1999; 10: 14521462.[Medline] [Order article via Infotrieve]
87. Witkowski FX, Leon LJ, Penkoske PA, Giles WR, Spano ML, Ditto WL, Winfree AT. Spatiotemporal evolution of ventricular fibrillation. Nature. 1998; 392: 7882.[CrossRef][Medline] [Order article via Infotrieve]
88. Valderrabano M, Lee MH, Ohara T, Lai AC, Fishbein MC, Lin SF, Karagueuzian HS, Chen PS. Dynamics of intramural and transmural reentry during ventricular fibrillation in isolated swine ventricles. Circ Res. 2001; 88: 839848.
89. Bray MA, Wikswo JP. Examination of optical depth effects on fluorescence imaging of cardiac propagation. Biophys J. 2003; 85: 41344145.[Medline] [Order article via Infotrieve]
90. Chen PS, Wu TJ, Ting CT, Karagueuzian HS, Garfinkel A, Lin SF, Weiss JN. A tale of two fibrillations. Circulation. 2003; 108: 22982303.
91. Lewis T. The Mechanism and Graphic Registration of the Heart Beat. London, UK: Shaw and sons; 1925.
92. Gurvich NL. The Main Principles of Cardiac Defibrillation. Moscow: Medicine; 1975.
93. Jalife J, Berenfeld O, Mansour M. Mother rotors and fibrillatory conduction: a mechanism of atrial fibrillation. Cardiovasc Res. 2002; 54: 204216.
94. Moe GK. A conceptual model of atrial fibrillation. J Electrocardiol. 1968; 1: 145146.[Medline] [Order article via Infotrieve]
95. Allessie MA, Lammers WJEP, Bonke FIM, Hollen J. Experimental evaluation of Moes multiple wavelet hypothesis of atrial fibrillation. In: Cardiac Electrophysiology and Arrhythmias. Zipes DP, Jalife J, eds. Orlando, Fla: Grune & Stratton; 1985.
96. Koller ML, Riccio ML, Gilmour RFJ. Dynamic restitution of action potential duration during electrical alternans and ventricular fibrillation. Am J Physiol. 1998; 275: H1635H1642.[Medline] [Order article via Infotrieve]
97. Garfinkel A, Kim YH, Voroshilovsky O, Qu Z, Kil JR, Lee MH, Karagueuzian HS, Weiss JN, Chen PS. Preventing ventricular fibrillation by flattening cardiac restitution. Proc Natl Acad Sci U S A. 2000; 97: 60616066.
98. Choi BR, Nho W, Liu T, Salama G. Life span of ventricular fibrillation frequencies. Circ Res. 2002; 91: 339345.
99. Cheng Y, Mowrey KA, Nikolski V, Tchou PJ, Efimov IR. Mechanisms of shock-induced arrhythmogenesis during acute global ischemia. Am J Physiol. 2002; 282: H2141H2151.
100. Zaitsev AV, Berenfeld O, Mironov SF, Jalife J, Pertsov AM. Distribution of excitation frequencies on the epicardial and endocardial surfaces of fibrillating ventricular wall of the sheep heart. Circ Res. 2000; 86: 408417.
101. Wiggers CJ. The mechanism and nature of ventricular fibrillation. Am Heart J. 1940; 20: 399412.[CrossRef]
102. Berg D. Excitation-Contraction Coupling and Cardiac Contractile Force. Dordrecht, The Netherlands: Kluwer; 1991.
103. Fabiato A, Fabiato F. Use of chlorotetracycline fluorescence to demonstrate Ca2+-induced release of Ca2+ from the sarcoplasmic reticulum of skinned cardiac cells. Nature. 1979; 281: 146148.[CrossRef][Medline] [Order article via Infotrieve]
104. Laflamme MA, Becker PL. Ca2+-induced current oscillations in rabbit ventricular myocytes. Circ Res. 1996; 78: 707716.
105. Lakatta EG, Guarnieri T. Spontaneous myocardial calcium oscillations: are they linked to ventricular fibrillation? J Cardiovasc Electrophysiol. 1993; 4: 473489.[Medline] [Order article via Infotrieve]
106. Marban E, Kitakaze M, Kusuoka H, Porterfield JK, Yue DT, Chacko VP. Intracellular free calcium concentration measured with 19F NMR spectroscopy in intact ferret hearts. Proc Natl Acad Sci U S A. 1987; 84: 60056009.
107. Steenbergen C, Murphy E, Levy L, London RE. Elevation in cytosolic free calcium concentration early in myocardial ischemia in perfused rat heart. Circ Res. 1987; 60: 700707.
108. Lee HC, Mohabir R, Smith N, Franz MR, Clusin WT. Effect of ischemia on calcium-dependent fluorescence transients in rabbit hearts containing indo1: correlation with monophasic action potentials and contraction. Circulation. 1988; 78: 10471059.
109. Kihara Y, Grossman W, Morgan JP. Direct measurement of changes in intracellular calcium transients during hypoxia, ischemia, and reperfusion of the intact mammalian heart. Circ Res. 1989; 65: 10291044.
110. Knisley SB. Mapping intracellular calcium in rabbit hearts with fluo3. In: Proceedings of the 17th Annual International Conference, IEEE Engineering in Medicine and Biology Society; Piscataway, NJ: IEEE Engineering in Medicine and Biology Society. 1995: 455456Abstract.
111. del Nido PJ, Glynn P, Buenaventura P, Salama G, Koretsky AP. Fluorescence measurement of calcium transients in perfused rabbit heart using rhod2. Am J Physiol. 1998; 274: H728H741.[Medline] [Order article via Infotrieve]
112. MacGowan GA, Du C, Glonty V, Suhan JP, Koretsky AP, Farkas DL. Rhod-2 based measurements of intracellular calcium in the perfused mouse heart: cellular and subcellular localization and response to positive inotropy. J Biomed Opt. 2001; 6: 2330.[CrossRef][Medline] [Order article via Infotrieve]
113. Efimov, I. R., Rendt, J. M., Salama, G. Optical maps of intracellular [Ca2+]i transients and action potentials from the surface of perfused guinea pig hearts. Circulation. 1994; 90: 632.
114. London B, Baker LC, Lee JS, Shusterman V, Choi BR, Kubota T, McTiernan CF, Feldman AM, Salama G. Calcium-dependent arrhythmias in transgenic mice with heart failure. Am J Physiol Heart Circ Physiol. 2003; 284: H431H441.
115. Johnson PL, Smith W, Baynham TC, Knisley SB. Errors caused by combination of Di-4 ANEPPS and Fluo3/4 for simultaneous measurements of transmembrane potentials and intracellular calcium. Ann Biomed Eng. 1999; 27: 563571.[CrossRef][Medline] [Order article via Infotrieve]
116. Laurita KR, Singal A. Mapping action potentials and calcium transients simultaneously from the intact heart. Am J Physiol Heart Circ Physiol. 2001; 280: H2053H2060.
117. London B. Cardiac arrhythmias: from (transgenic) mice to men. J Cardiovasc Electrophysiol. 2001; 12: 10891091.[CrossRef][Medline] [Order article via Infotrieve]
118. London B, Jeron A, Zhou J, Buckett P, Han X, Mitchell GF, Koren G. Long QT and ventricular arrhythmias in transgenic mice expressing the N terminus and first transmembrane segment of a voltage-gated potassium channel. Proc Natl Acad Sci U S A. 1998; 95: 29262931.
119. Jeron A, Mitchell GF, Zhou J, Murata M, London B, Buckett P, Wiviott SD, Koren G. Inducible polymorphic ventricular tachyarrhythmias in a transgenic mouse model with a long Q-T phenotype. Am J Physiol Heart Circ Physiol. 2000; 278: H1891H1898.
120. Baker LC, London B, Choi BR, Koren G, Salama G. Enhanced dispersion of repolarization and refractoriness in transgenic mouse hearts promotes reentrant ventricular tachycardia. Circ Res. 2000; 86: 396407.
121. Brunner M, Kodirov SA, Mitchell GF, Buckett PD, Shibata K, Folco EJ, Baker L, Salama G, Chan DP, Zhou J, Koren G. In vivo gene transfer of Kv1.5 normalizes action potential duration and shortens QT interval in mice with long QT phenotype. Am J Physiol Heart Circ Physiol. 2003; 285: H194H203.
122. Saffitz JE, Davis LM, Darrow BJ, Kanter HL, Laing JG, Beyer EC. The molecular basis of anisotropy: role of gap junctions. J Cardiovasc Electrophysiol. 1995; 6: 498510.[Medline] [Order article via Infotrieve]
123. Jalife J, Morley GE, Vaidya D. Connexins and impulse propagation in the mouse heart. J Cardiovasc Electrophysiol. 1999; 10: 16491663.[Medline] [Order article via Infotrieve]
124. Kanno S, Saffitz JE. The role of myocardial gap junctions in electrical conduction and arrhythmogenesis. Cardiovasc Pathol. 2001; 10: 169177.[CrossRef][Medline] [Order article via Infotrieve]
125. Morley GE, Vaidya D, Jalife J. Characterization of conduction in the ventricles of normal and heterozygous Cx43 knockout mice using optical mapping. J Cardiovasc Electrophysiol. 2000; 11: 375377.[Medline] [Order article via Infotrieve]
126. Eloff BC, Lerner DL, Yamada KA, Schuessler RB, Saffitz JE, Rosenbaum DS. High resolution optical mapping reveals conduction slowing in connexin43 deficient mice. Cardiovasc Res. 2001; 51: 681690.
127. Kamino K, Komuro H, Sakai T, Hirota A. Functional pacemaking area in the early embryonic chick heart assessed by simultaneous multiple-site optical recording of spontaneous action potentials. J Gen Physiol. 1988; 91: 573591.
128. Sakai T, Hirota A, Kamino K. Video-imaging assessment of initial beating patterns of the early embryonic chick heart. Jpn J Physiol. 1996; 46: 465472.[CrossRef][Medline] [Order article via Infotrieve]
129. Rentschler S, Vaidya DM, Tamaddon H, Degenhardt K, Sassoon D, Morley GE, Jalife J, Fishman GI. Visualization and functional characterization of the developing murine cardiac conduction system. Development. 2001; 128: 17851792.[Abstract]
130. Vaidya D, Tamaddon HS, Lo CW, Taffet SM, Delmar M, Morley GE, Jalife J. Null mutation of connexin43 causes slow propagation of ventricular activation in the late stages of mouse embryonic development. Circ Res. 2001; 88: 11961202.
131. Fast VG, Kleber AG. Microscopic conduction in cultured strands of neonatal rat heart cells measured with voltage-sensitive dyes. Circ Res. 1993; 73: 914925.
132. Rohr S, Salzberg BM. Characterization of impulse propagation at the microscopic level across geometrically defined expansions of excitable tissue: multiple site optical recording of transmembrane voltage (MSORTV) in patterned growth heart cell cultures. J Gen Physiol. 1994; 104: 287309.
133. Fast VG, Ideker RE. Simultaneous optical mapping of transmembrane potential and intracellular calcium in myocyte cultures. J Cardiovasc Electrophysiol. 2000; 11: 547556.[Medline] [Order article via Infotrieve]
134. Thomas SP, Kucera JP, Bircher-Lehmann L, Rudy Y, Saffitz JE, Kleber AG. Impulse propagation in synthetic strands of neonatal cardiac myocytes with genetically reduced levels of connexin43. Circ Res. 2003; 92: 12091216.
135. Reckova M, Rosengarten C, DeAlmeida A, Stanley CP, Wessels A, Gourdie RG, Thompson RP, Sedmera D. Hemodynamics is a key epigenetic factor in development of the cardiac conduction system. Circ Res. 2003; 93: 7785.
136. Yelbuz TM, Choma MA, Thrane L, Kirby ML, Izatt JA. Optical coherence tomography: a new high-resolution imaging technology to study cardiac development in chick embryos. Circulation. 2002; 106: 27712774.
137. Boppart SA, Tearney GJ, Bouma BE, Southern JF, Brezinski ME, Fujimoto JG. Noninvasive assessment of the developing Xenopus cardiovascular system using optical coherence tomography. Proc Natl Acad Sci U S A. 1997; 94: 42564261.
138. Schaffer P, Ahammer H, Muller W, Koidl B, Windisch H. Di-4-ANEPPS causes photodynamic damage to isolated cardiomyocytes. Pflugers Arch. 1994; 426: 548551.[CrossRef][Medline] [Order article via Infotrieve]
139. Cheng YN, Mazgalev T, Van Wagoner DR, Tchou PJ, Efimov IR. Voltage-sensitive dye RH421 increases contractility of cardiac muscle. Can J Physiol Pharmacol. 1998; 76: 11461150.[CrossRef][Medline] [Order article via Infotrieve]
140. Hooks DA, LeGrice IJ, Harvey JD, Smaill BH. Intramural multisite recording of transmembrane potential in the heart. Biophys J. 2001; 81: 26712680.[Medline] [Order article via Infotrieve]
141. Chen PS, Wolf PD, Dixon EG, Danieley ND, Frazier DW, Smith WM, Ideker RE. Mechanism of ventricular vulnerability to single premature stimuli in open-chest dogs. Circ Res. 1988; 62: 11911209.
142. Fast VG, Sharifov OF, Cheek ER, Newton JC, Ideker RE. Intramural virtual electrodes during defibrillation shocks in left ventricular wall assessed by optical mapping of membrane potential. Circulation. 2002; 106: 10071014.
143. Baxter WT, Mironov SF, Zaitsev AV, Jalife J, Pertsov AM. Visualizing excitation waves inside cardiac muscle using transillumination. Biophys J. 2001; 80: 516530.[Medline] [Order article via Infotrieve]
144. Fujimoto JG. Optical coherence tomography for ultrahigh resolution in vivo imaging. Nat Biotechnol. 2003; 21: 13611367.[CrossRef][Medline] [Order article via Infotrieve]
145. Gupta M, Rollins AM, Izatt JA, Efimov IR. Imaging of the atrioventricular node using optical coherence tomography. J Cardiovasc Electrophysiol. 2002; 13: 95.[CrossRef][Medline] [Order article via Infotrieve]
146. Jenkins MW, Pederson CJ, Wade RS, Nikolski VP, Cheng Y, Efimov IR, Rollins AM. Three-dimensional OCT imaging of endocardial architecture. Photonics West: Technical Summary Digest: 129- 2004; 61.
147. Millard AC, Jin L, Lewis A, Loew LM. Direct measurement of the voltage sensitivity of second-harmonic generation from a membrane dye in patch-clamped cells. Opt Lett. 2003; 28: 12211223.[Medline] [Order article via Infotrieve]
148. Jiang Y, Tomov I, Wang Y, Chen Z. Second-harmonic optical coherence tomography. Opt Lett. 2004; 29: 13.[CrossRef]
149. Loew LM. Confocal microscopy of potentiometric fluorescent dyes. Meth Cell Biol. 1993; 38: 195209.[Medline] [Order article via Infotrieve]
150. Lagerholm BC, Vanni S, Taylor DL, Lanni F. Cytomechanics applications of optical sectioning microscopy. Methods Enzymol. 2003; 361: 175197.[CrossRef][Medline] [Order article via Infotrieve]
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