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Circulation Research. 2004;95:21-33
doi: 10.1161/01.RES.0000130529.18016.35
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(Circulation Research. 2004;95:21.)
© 2004 American Heart Association, Inc.


Reviews

Optical Imaging of the Heart

Igor R. Efimov, Vladimir P. Nikolski, Guy Salama

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 O’Rourke Guest Editor


*    Abstract
up arrowTop
*Abstract
down arrowIntroduction
down arrowGeneral Principles
down arrowNew Molecular Probes for...
down arrowCalibration of Optical...
down arrowNeed for Optical Mapping
down arrowProgress in Imaging Technology:...
down arrowDesign of Optical Mapping...
down arrowMapping of Activation and...
down arrowMapping of Stimulation and...
down arrowMapping of the Impulse...
down arrowMapping of Atrial and...
down arrowMultiparametric Optical Mapping:...
down arrowMapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
Optical techniques have revolutionized the investigation of cardiac cellular physiology and advanced our understanding of basic mechanisms of electrical activity, calcium homeostasis, and metabolism. Although optical methods are widely accepted and have been at the forefront of scientific discoveries, they have been primarily applied at cellular and subcellular levels and considerably less to whole heart organ physiology. Numerous technical difficulties had to be overcome to dynamically map physiological processes in intact hearts by optical methods. Problems of contraction artifacts, cellular heterogeneities, spatial and temporal resolution, limitations of surface images, depth-of-field, and need for large fields of view (ranging from 2x2 mm2 to 3x3 cm2) have all led to the development of new devices and optical probes to monitor physiological parameters in intact hearts. This review aims to provide a critical overview of current approaches, their contributions to the field of cardiac electrophysiology, and future directions of various optical imaging modalities as applied to cardiac physiology at organ and tissue levels.


Key Words: optical mapping • fluorescent probes • electrophysiology • arrhythmia • defibrillation


*    Introduction
up arrowTop
up arrowAbstract
*Introduction
down arrowGeneral Principles
down arrowNew Molecular Probes for...
down arrowCalibration of Optical...
down arrowNeed for Optical Mapping
down arrowProgress in Imaging Technology:...
down arrowDesign of Optical Mapping...
down arrowMapping of Activation and...
down arrowMapping of Stimulation and...
down arrowMapping of the Impulse...
down arrowMapping of Atrial and...
down arrowMultiparametric Optical Mapping:...
down arrowMapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
Mammalian physiology has an ingrained hierarchy with molecular and cellular physiology at its base, followed by the interactions of large populations of cells and organ systems, and finally the integration of multiple organ functions of an entire animal. For the past 4 decades, cardiovascular physiology has been dominated by a "reductionist" approach, focusing on cellular mechanisms. Major strides have been accomplished in our understanding of cellular mechanisms, including metabolism, intracellular signaling, trafficking, ion channel structure, function, and expression. With a greater understanding of cellular mechanisms came the growing realization that organs such as the heart are composed of several types of interacting cells with significant and important heterogeneities of properties, cell-to-cell coupling, and function within each group. Thus, an understanding of molecular and cellular mechanisms must still be integrated to explain the more complex organ system while taking into account spatial and temporal heterogeneities of cell functions throughout the organ.

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
up arrowTop
up arrowAbstract
up arrowIntroduction
*General Principles
down arrowNew Molecular Probes for...
down arrowCalibration of Optical...
down arrowNeed for Optical Mapping
down arrowProgress in Imaging Technology:...
down arrowDesign of Optical Mapping...
down arrowMapping of Activation and...
down arrowMapping of Stimulation and...
down arrowMapping of the Impulse...
down arrowMapping of Atrial and...
down arrowMultiparametric Optical Mapping:...
down arrowMapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
Optical imaging modalities are based on physical principles of wavelength-dependent light-tissue interaction, including photon scattering, total internal reflection, absorption, reflectance, and fluorescence. The physical interactions of photons with tissue, namely, intrinsic tissue absorption and light scattering, limit the depth of penetration and spatiotemporal resolution of images that can be obtained from bulk tissue. However, recent advances in optical contrast agents, optical probes of physiological parameters, light transport theory, light sources, and optical detectors have created conditions for major breakthroughs in optical imaging at the organ level. Novel imaging modalities with expanding areas of application have emerged, including optical diffusion tomography,8,9 optical coherence tomography,10 and various confocal fluorescence imaging approaches. These new technologies have encouraged the development of new fluorescence or absorption contrast agents and probes of physiological parameters, and the combination of new instruments and probes will most likely propel a new era of multidimensional and multiparametric imaging in organ system physiology.

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 field–induced reorientation of the dye molecule in the plasma membrane (solvatochromic theory16).


*    New Molecular Probes for Optical Recordings of Electrical Activity
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
*New Molecular Probes for...
down arrowCalibration of Optical...
down arrowNeed for Optical Mapping
down arrowProgress in Imaging Technology:...
down arrowDesign of Optical Mapping...
down arrowMapping of Activation and...
down arrowMapping of Stimulation and...
down arrowMapping of the Impulse...
down arrowMapping of Atrial and...
down arrowMultiparametric Optical Mapping:...
down arrowMapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
In tests of over 1500 different compounds, several useful classes of chromophores have emerged, including merocyanine, oxonol, and styryl dyes. Styryl dyes represent the most popular family of dyes; RH-421 and di-4-ANEPPS being the most important members of this family. The spectroscopic properties of these dyes have been shown to linearly change with membrane potential changes in the normal physiological range of transmembrane voltages.13,17,18

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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Figure 1. Optical recordings of cardiac action potentials. A, Simultaneous fluorescent (Vf) and microelectrode (Ve) recordings of action potentials in the frog heart stained with Merocyanine-540. Recordings show a faithful reproduction of transmembrane potential by the fluorescence signals. Upstroke of optical action potential is typically slower than that of the microelectrode, due to spatial averaging of a propagating wavefront. B, Optical recording of action potentials from different regions of the heart stained with di-4-ANEPPS: ventricular and atrial working myocardium, AV node, and Crista terminalis.

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.24–26 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
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
*Calibration of Optical...
down arrowNeed for Optical Mapping
down arrowProgress in Imaging Technology:...
down arrowDesign of Optical Mapping...
down arrowMapping of Activation and...
down arrowMapping of Stimulation and...
down arrowMapping of the Impulse...
down arrowMapping of Atrial and...
down arrowMultiparametric Optical Mapping:...
down arrowMapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
It is important to note that fast voltage-sensitive dyes do not provide an absolute measurement of transmembrane potential but merely track the changes in membrane potential with high temporal fidelity. Initial studies calibrated optical action potential by simultaneously recording fluorescence and microelectrode signals from the same region of the heart.12 The linearity and kinetics of the voltage-dependent merocyanine dye signals were characterized in heart muscles under sucrose-gap voltage clamp conditions.13 More recent studies have concentrated on application of ratiometry approach for quantitative measurements of transmembrane potential with newer and better dyes. Initially these methods were developed on neuroblastoma cells.28 The early experiments have not been repeated to confirm the linearity of these dyes in artificial planar bilayers or cardiac cells. Simultaneous ratiometric optical and microelectrode recordings of transmembrane potential in perfused hearts confirmed excellent correlation and linearity of optical recordings.26


*    Need for Optical Mapping
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
up arrowCalibration of Optical...
*Need for Optical Mapping
down arrowProgress in Imaging Technology:...
down arrowDesign of Optical Mapping...
down arrowMapping of Activation and...
down arrowMapping of Stimulation and...
down arrowMapping of the Impulse...
down arrowMapping of Atrial and...
down arrowMultiparametric Optical Mapping:...
down arrowMapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
The spread of electrical activity is important for our understanding of the mechanisms responsible for the normal cardiac rhythm and for the initiation and maintenance of arrhythmias. Although much has been learned regarding the ionic basis of the cardiac action potential using intracellular microelectrodes, single cell impalements cannot be practically used to simultaneously record action potentials from hundreds of recording sites. The generally used methods to map activation and repolarization are based on surface unipolar and bipolar electrograms measured with arrays of electrodes.29,30 Although surface electrodes can describe the spread of excitation and repolarization, interpretation of data in some cases is uncertain.29,31 For instance, activation sequences were difficult to interpret during rapid synchronous depolarization, as after electric shock application, and during slowly changing, low-level depolarization, as in ischemia. Repolarization measured with an electrogram often does not coincide with the actual repolarization at the recording site.31,32


*    Progress in Imaging Technology: Advances in Light Detectors
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
up arrowCalibration of Optical...
up arrowNeed for Optical Mapping
*Progress in Imaging Technology:...
down arrowDesign of Optical Mapping...
down arrowMapping of Activation and...
down arrowMapping of Stimulation and...
down arrowMapping of the Impulse...
down arrowMapping of Atrial and...
down arrowMultiparametric Optical Mapping:...
down arrowMapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
Current imaging technology presents several approaches for fast imaging, including photomultipliers (PMT), laser scanning,33 charge-coupled device (CCD) cameras, and photodiode arrays (PDA). Currently, only CCD cameras and PDA detectors are predominantly used in heart imaging applications.19,34–37 Complementary metal-oxide semiconductor (CMOS) cameras represent another emerging candidate. Combination of PMT devices with a laser scanning technique failed to overcome spatiotemporal limitations imposed by sequential nature of recordings.38,39

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.43–45

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
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
up arrowCalibration of Optical...
up arrowNeed for Optical Mapping
up arrowProgress in Imaging Technology:...
*Design of Optical Mapping...
down arrowMapping of Activation and...
down arrowMapping of Stimulation and...
down arrowMapping of the Impulse...
down arrowMapping of Atrial and...
down arrowMultiparametric Optical Mapping:...
down arrowMapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
Any optical imaging system consists of a 2D optical sensor and a stable light source, such as a laser or DC-powered tungsten-halogen lamp, mercury source, or light-emitting diodes. Figure 2 describes a typical single-lens design. It consists of a PDA, 256-channel signal conditioner/amplifier, analog-to-digital converter, and a computer. An excitation beam is passed through 520±30-nm interference filters and focused on the surface of a perfused preparation placed in a tissue chamber. A camera lens collects the fluorescence light, directs it to a 610-nm long pass filter and focuses an image of a chosen region of the heart on the surface of PDA.



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Figure 2. Schematics of a typical optical mapping system.


*    Mapping of Activation and Repolarization
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
up arrowCalibration of Optical...
up arrowNeed for Optical Mapping
up arrowProgress in Imaging Technology:...
up arrowDesign of Optical Mapping...
*Mapping of Activation and...
down arrowMapping of Stimulation and...
down arrowMapping of the Impulse...
down arrowMapping of Atrial and...
down arrowMultiparametric Optical Mapping:...
down arrowMapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
Figure 3 shows a map of action potentials optically recorded from the anterior surface of a Langendorff-perfused guinea pig heart. An optical trace at the right illustrates that the quality of optical recordings approaches that of the gold standard: microelectrode recordings. When movement artifacts are a concern, activation and repolarization times can be still be determined by calculating the maximum first derivative of the action potential upstroke and the maximum second derivative of the downstroke, respectively19 (Figure 3). Alternatively, these times could be determined from the time point at which the upstroke reaches 50% or recovers to 90% of its maximum amplitude,46,47 respectively. Recently, phase-mapping techniques were introduced for an analysis of quasiperiodic electrical activity in the heart.48 These techniques determine the specific phase of electrical activity that corresponds to each moment of the action potential. The algorithms used are based on analysis of phase-space trajectories, which result from a plot of a measured variable (optical action potential) against a transform of the same variable (time-delay,48 first derivative, Hilbert transformation49). Activation and repolarization data are usually presented as isophasic or isochronal maps (see Figure 3)4,19,37,50–52 or a vector field of conduction in the cardiac muscle (see Figure 3),53,54 allowing quantitative assessment of spread of activation and repolarization in highly anisotropic heart muscle under normal and pathological conditions.54–56



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Figure 3. Maps of optical action potentials and methods of analysis (left to right, top to bottom): schematic diagram of anterior epicardium of the guinea pig heart and the imaging field of view. Maps of optical action potentials: detection of activation and repolarization time points using first (dF/dt) and second (d2F/dt2) derivatives of fluorescence (F). Maps of activation: conduction velocity vectors and repolarization. See text for detail.

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.60–62


*    Mapping of Stimulation and Defibrillation
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
up arrowCalibration of Optical...
up arrowNeed for Optical Mapping
up arrowProgress in Imaging Technology:...
up arrowDesign of Optical Mapping...
up arrowMapping of Activation and...
*Mapping of Stimulation and...
down arrowMapping of the Impulse...
down arrowMapping of Atrial and...
down arrowMultiparametric Optical Mapping:...
down arrowMapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
Optical mapping is an especially powerful tool in studies of electrostimulation therapy. Due to overwhelming stimulus-induced artifacts, the conventional electrode techniques are not able to record electrical activity during and after stimuli. In contrast, optical recordings provide an accurate account of transmembrane potential changes during stimulation and defibrillation. Dillon20 demonstrated the prolongation of action potential duration by strong electric shocks applied during the refractory period. Optical mapping explained the mechanisms of epicardial unipolar63 and bipolar pacing.64 Optical mapping also provided the experimental basis for the new theory of stimulus-induced arrhythmogenesis and the related theory of success and failure of defibrillation based on virtual electrode effects,34,65,66 which are also known as secondary source effects.44,67 Figure 468 presents experimental evidence of a virtual electrode-induced phase singularity mechanism of shock-induced arrhythmogenesis.66 Optical recordings for the first time allowed faithful dynamic registration of maps of transmembrane potential before, during, and after shock application. Figure 4B illustrates the typical pattern of virtual electrode polarization mapped as a distribution of transmembrane potential seen immediately after the application of a shock. Virtual electrode patterns are characterized by the presence of both positive and negative polarizations, which are induced by the virtual cathode and anode, respectively. As a result, a shock-induced wavefront of break-excitation can form a reentrant pattern around the virtual electrode-induced phase singularity.66,69,70



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Figure 4. Optical imaging of shock-induced arrhythmogenesis and defibrillation. A, Preparation. B, Shock-induced polarization. C, Shock-induced conduction pattern. D, Optical recording of transmembrane potential during normal action potential, T-wave shock, and shock-induced arrhythmia.


*    Mapping of the Impulse Generation and Conduction System of the Heart
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
up arrowCalibration of Optical...
up arrowNeed for Optical Mapping
up arrowProgress in Imaging Technology:...
up arrowDesign of Optical Mapping...
up arrowMapping of Activation and...
up arrowMapping of Stimulation and...
*Mapping of the Impulse...
down arrowMapping of Atrial and...
down arrowMultiparametric Optical Mapping:...
down arrowMapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
Optical mapping has made a significant contribution to functional studies of the fundamental mechanisms of impulse generation in the SA and AV nodes, and impulse propagation in the conduction system of the heart. Kamino’s group pioneered optical mapping techniques in the brain and heart, investigating the genesis of spontaneous electrical activity in the embryonic heart.71–74 Optical mapping was also instrumental in the identification of nonradial spread of activation via preferential pathways from the SA node toward the AV node.75,76 Our groups applied optical mapping to studies of AV nodal conduction,22,76,77 AV nodal reentrant arrhythmias,78,79 and AV junctional rhythm.80 Finally, Morley and colleagues54,56 pioneered the application of optical mapping to investigate mechanisms of conduction in the Purkinje system, which was unattainable by electrode-based techniques.

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 ({circ}), the compact AV node ({bullet}), 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 {circ}, in Figure 5A and 5B) of the AV junction, whereas the second component represents electrical activity of the deeper NH layer ({bullet} in Figure 5A and 5B).



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Figure 5. Three-dimensional (multilayer) imaging of the conduction through the atrioventricular (AV) junction. AV junctional preparation was paced at atrial septum with a cycle length S1S1=280 ms (A, top) and 274 ms (A, bottom), which caused Wenckebach AV block. Bipolar electrograms were recorded from Crista terminalis (CrT) and bundle of His. Optical traces (OAP) represent the superimposition of signals from the septum and the distal AV nodal areas. B, Masson Trichrome stained section through the distal AV node. Places of microelectrode recordings (MAP) are marked with black and white circles. See text for detail.


*    Mapping of Atrial and Ventricular Tachyarrhythmias
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
up arrowCalibration of Optical...
up arrowNeed for Optical Mapping
up arrowProgress in Imaging Technology:...
up arrowDesign of Optical Mapping...
up arrowMapping of Activation and...
up arrowMapping of Stimulation and...
up arrowMapping of the Impulse...
*Mapping of Atrial and...
down arrowMultiparametric Optical Mapping:...
down arrowMapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
Optical mapping techniques presented a unique opportunity to study the mechanisms of supraventricular and ventricular arrhythmias because of unprecedented spatiotemporal resolution and the ability to map all phases of electrical activity, including activation and repolarization.

Jalife’s group pioneered the application of optical mapping to study arrhythmogenesis81–84 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"91–93 and "break-up"94–98 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.91–93 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.94,96–98 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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Figure 6. Frequency analysis of optically recorded electrical activity during ventricular fibrillation. A, FFT spectra with a single dominant frequency and maps with static frequency domains,100 support the mother-rotor hypothesis of fibrillation. B and C, Complex FFT spectra and dynamic frequency domains98 support the multiple wave-breaks hypothesis of fibrillation. See text for details.


*    Multiparametric Optical Mapping: Imaging of Voltage and Intracellular Calcium
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
up arrowCalibration of Optical...
up arrowNeed for Optical Mapping
up arrowProgress in Imaging Technology:...
up arrowDesign of Optical Mapping...
up arrowMapping of Activation and...
up arrowMapping of Stimulation and...
up arrowMapping of the Impulse...
up arrowMapping of Atrial and...
*Multiparametric Optical Mapping:...
down arrowMapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
Calcium cycling is arguably the single most important component of cardiac excitation-contraction coupling. The action potential elicits an influx of Ca2+ through the activation of L-type voltage-gated Ca2+ channels that trigger a release of Ca2+ from intracellular stores called the sarcoplasmic reticulum (SR) resulting in a contraction.102 Ca2+ release from the SR occurs via Ca2+ release channels or ryanodine receptors that are activated by a local elevation of intracellular Ca2+ ([Ca2+]i) by a process called Ca2+-induced Ca2+ release (CICR).103 Normally, depolarization triggers [Ca2+]i transients, but in pathological conditions, abnormalities in [Ca2+]i handling may activate Ca2+-dependent currents that influence the time course of the AP and trigger a spontaneous membrane depolarization.104,105 Abnormalities in [Ca2+]i handling have been implicated as the underlying mechanism in a number of pathologies that promote arrhythmias such as ischemia, reperfusion-arrhythmias, the generation of early and delayed afterdepolarizations, and torsades de pointes that occurs in patients with the long QT syndrome. [Ca2+]i overload has been implicated in triggering electromechanical alternans and in increasing the steepness of APD restitution curves, which are both associated with promotion of arrhythmias. Thus, one cannot overstate the importance of simultaneous measurements of APs and [Ca2+]i transients in intact hearts to address fundamental questions regarding the spatiotemporal relationship of voltage and [Ca2+]i and their interplay in arrhythmias.

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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Figure 7. Multiparametric optical imaging: simultaneous optical recordings of transmembrane potential and intracellular calcium transients. A, Experimental setup with 2 16x16 photodiode arrays. Hearts were stained with voltage-sensitive dye RH 237 and Ca2+ indicator Rhod-2. B, Optically recorded action potentials (AP) and calcium transients (Cai) at 252 points of mapped region. C and D, Effects of Ryanodine on AP and Cai recordings. To verify that the Rhod-2 signal is a measure of Cai released from the sarcoplasmic reticulum via ryanodine receptors and was impervious to changes in Vm, ryanodine (10 µmol/L) was added to the perfusate to test the selectivity of its actions on Cai versus the AP. E, Superposition of an AP and Cai transient recorded from the same region of myocardium. AP and Cai were simultaneously recorded at a sampling rate of 4000 frames/sec for each array. AP upstroke preceded the rise of Cai by 10.4±0.4 ms.

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
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
up arrowCalibration of Optical...
up arrowNeed for Optical Mapping
up arrowProgress in Imaging Technology:...
up arrowDesign of Optical Mapping...
up arrowMapping of Activation and...
up arrowMapping of Stimulation and...
up arrowMapping of the Impulse...
up arrowMapping of Atrial and...
up arrowMultiparametric Optical Mapping:...
*Mapping Transgenic Mouse Models
down arrowMapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
Molecularly engineered mice are increasingly used to genetically alter a specific component of a complex signaling process and to develop models of human diseases. Transgenic and knockout mice are used as models for various cardiac diseases and offer an effective strategy to elucidate the mechanisms underlying arrhythmias, metabolic diseases, the pathology of heart failure, and altered ion channel and gap junction expression.117 A limitation of mouse models is the rapid heart rate and small size of the heart, which makes it difficult to study changes in contractility, electrophysiology, and arrhythmias vulnerability. The challenge of studying cardiac phenotypes in mice has been effectively tackled by optical mapping of action potentials and [Ca2+]i transients.

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 {alpha} (TNF-{alpha}) 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-{alpha} 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-{alpha} 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.122–124 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
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
up arrowCalibration of Optical...
up arrowNeed for Optical Mapping
up arrowProgress in Imaging Technology:...
up arrowDesign of Optical Mapping...
up arrowMapping of Activation and...
up arrowMapping of Stimulation and...
up arrowMapping of the Impulse...
up arrowMapping of Atrial and...
up arrowMultiparametric Optical Mapping:...
up arrowMapping Transgenic Mouse Models
*Mapping Developing Myocardium
down arrowEmerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
In embryonic hearts and neonatal cell cultures, the ability to optically record simultaneously from multiple sites is making important contributions to our understanding of the developing heart. Optical mapping was applied to study the patterning and organization of the conduction system and working myocardium in the developing avian127,128 and mammalian129,130 hearts. Optical mapping of action potentials and [Ca2+]i in combination with patterned cultured neonatal rat131–133 mouse134 and genetically modified mice is bound to make major contributions to our understanding of propagation in the adult and developing heart. Optical mapping has contributed to investigation of the important role of mechanoelectrical coupling in shaping the working myocardium and the conduction system of chick heart.135 Combination of optical mapping of electrical activity with structural 3D mapping of developing hearts is especially exciting new opportunity.136,137


*    Emerging Optical Imaging Modalities
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
up arrowCalibration of Optical...
up arrowNeed for Optical Mapping
up arrowProgress in Imaging Technology:...
up arrowDesign of Optical Mapping...
up arrowMapping of Activation and...
up arrowMapping of Stimulation and...
up arrowMapping of the Impulse...
up arrowMapping of Atrial and...
up arrowMultiparametric Optical Mapping:...
up arrowMapping Transgenic Mouse Models
up arrowMapping Developing Myocardium
*Emerging Optical Imaging...
down arrowConclusion
down arrowReferences
 
Imaging with voltage-sensitive probes has several limitations. Pharmacological effects of the dye include phototoxicity138 and increased contractility.139 Yet, arguably, the major limitation of organ-level optical imaging is its restricted depth of penetration.

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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Figure 8. Optical coherence tomography of the AV junction. A, Optical coherence tomography 3D reconstruction of the triangle of Koch area in a rabbit heart: N indicates compact node; His, His Bundle; CS, coronary sinus. B, OCT section along the black line in A. C, 3D OCT image of the 3x4-mm region of right ventricular epicardium of the rabbit heart with network of Purkinje fibers.


*    Conclusion
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
up arrowCalibration of Optical...
up arrowNeed for Optical Mapping
up arrowProgress in Imaging Technology:...
up arrowDesign of Optical Mapping...
up arrowMapping of Activation and...
up arrowMapping of Stimulation and...
up arrowMapping of the Impulse...
up arrowMapping of Atrial and...
up arrowMultiparametric Optical Mapping:...
up arrowMapping Transgenic Mouse Models
up arrowMapping Developing Myocardium
up arrowEmerging Optical Imaging...
*Conclusion
down arrowReferences
 
Optical imaging of cardiac electrical activity at the tissue and organ levels has emerged as powerful novel approach during the last decade and has made a significant contribution to cardiovascular research. Exciting new developments in biophotonics suggest that the best is yet to come. The next decade is likely to yield (1) novel optical molecular probes for multiparametric optical sensing of various biological parameters, processes, molecules, proteins, and their functional states in real time with submillisecond resolution and (2) novel optical imaging modalities for 3D optical interrogation of molecular probes with precise anatomical localization of the signal origin with subcellular spatial resolution.


*    Acknowledgments
 
This work was supported by NIH R01 grants HL67322 and HL58808 (to I.R.E.) and HL57929, HL59614, HL69097, and HL70722 (to G.S.).


*    Footnotes
 
Original received February 2, 2004; revision received April 16, 2004; accepted April 20, 2004.


*    References
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowGeneral Principles
up arrowNew Molecular Probes for...
up arrowCalibration of Optical...
up arrowNeed for Optical Mapping
up arrowProgress in Imaging Technology:...
up arrowDesign of Optical Mapping...
up arrowMapping of Activation and...
up arrowMapping of Stimulation and...
up arrowMapping of the Impulse...
up arrowMapping of Atrial and...
up arrowMultiparametric Optical Mapping:...
up arrowMapping Transgenic Mouse Models
up arrowMapping Developing Myocardium
up arrowEmerging Optical Imaging...
up arrowConclusion
*References
 
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