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Dive into the research topics where Tsunetoyo Namba is active.

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Featured researches published by Tsunetoyo Namba.


Circulation Research | 2012

The Role of Fibroblasts in Complex Fractionated Electrograms During Persistent/Permanent Atrial Fibrillation Implications for Electrogram-Based Catheter Ablation

Takashi Ashihara; Ryo Haraguchi; Kazuo Nakazawa; Tsunetoyo Namba; Takanori Ikeda; Yuko Nakazawa; Tomoya Ozawa; Makoto Ito; Minoru Horie; Natalia A. Trayanova

Rationale: Electrogram-based catheter ablation, targeting complex fractionated atrial electrograms (CFAEs), is empirically known to be effective in halting persistent/permanent atrial fibrillation (AF). However, the mechanisms underlying CFAEs and electrogram-based ablation remain unclear. Objective: Because atrial fibrosis is associated with persistent/permanent AF, we hypothesized that electrotonic interactions between atrial myocytes and fibroblasts play an important role in CFAE genesis and electrogram-based catheter ablation. Methods and Results: We used a human atrial tissue model in heart failure and simulated propagation and spiral wave reentry with and without regionally proliferated fibroblasts. Coupling of fibroblasts to atrial myocytes resulted in shorter action potential duration, slower conduction velocity, and lower excitability. Consequently, heterogeneous fibroblast proliferation in the myocardial sheet resulted in frequent spiral wave breakups, and the bipolar electrograms recorded at the fibroblast proliferation area exhibited CFAEs. The simulations demonstrated that ablation targeting such fibroblast-derived CFAEs terminated AF, resulting from the ablation site transiently pinning the spiral wave and then pushing it out of the fibroblast proliferation area. CFAEs could not be attributed to collagen accumulation alone. Conclusions: Fibroblast proliferation in atria might be responsible for the genesis of CFAEs during persistent/permanent AF. Our findings could contribute to better understanding of the mechanisms underlying CFAE-targeted AF ablation.


Circulation | 2003

Widening of the Excitable Gap and Enlargement of the Core of Reentry During Atrial Fibrillation With a Pure Sodium Channel Blocker in Canine Atria

Ayaka Kawase; Takanori Ikeda; Kazuo Nakazawa; Takashi Ashihara; Tsunetoyo Namba; Tetsuya Kubota; Kaoru Sugi; Hironori Hirai

Background—This study aimed to assess the effects of pilsicainide, a pure sodium channel blocker, on electrophysiological action and wavefront dynamics during atrial fibrillation (AF). Methods and Results—In a newly developed model of isolated, perfused, and superfused canine atria (n=12), the right and left endocardia were mapped simultaneously by use of a computerized mapping system. AF was induced with 1 to 5 &mgr;mol/L acetylcholine. The antifibrillatory actions of pilsicainide on AF cycle length (AFCL), refractory period (RP), conduction velocity (CV), excitable gap (EG), and the core of the mother rotor were studied. The RP was defined as the shortest coupling interval that could capture the fibrillating atrium. The EG was estimated as the difference between the AFCL and RP. At baseline, multiple wavefronts were observed. After 2.5 &mgr;g/mL infusion of pilsicainide, all preparations showed irregular activity, and AF was terminated in 2 preparations. The AFCL and RP were prolonged, and CV was decreased significantly. The EG was widened (147%;P <0.01), and the core perimeter was increased (100%;P <0.01). Increasing the dosage either terminated AF (6 preparations) or converted to organized activity (ie, atypical atrial flutter) (4 preparations). On the maps, all “unorganized” AFs were terminated with the excitation of the core of the mother rotor by an outside wavefront, whereas in preparations with atrial flutter, pilsicainide did not terminate its activity. Conclusions—Widening of the EG by pilsicainide facilitates the excitation of the core of the mother rotor, leading to the termination of AF. In some experiments, pilsicainide converts AF to persistent atrial flutter.


Journal of Physiological Sciences | 2008

A procedural method for modeling the purkinje fibers of the heart.

Takashi Ijiri; Takashi Ashihara; Takeshi Yamaguchi; Kenshi Takayama; Takeo Igarashi; Tatsuo Shimada; Tsunetoyo Namba; Kazuo Nakazawa

The Purkinje fibers are located in the ventricular walls of the heart, just beneath the endocardium and conduct excitation from the right and left bundle branches to the ventricular myocardium. Recently, anatomists succeeded in photographing the Purkinje fibers of a sheep, which clearly showed the mesh structure of the Purkinje fibers. In this study, we present a technique for modeling the mesh structure of Purkinje fibers semiautomatically using an extended L-system. The L-system is a formal grammar that defines the growth of a fractal structure by generating rules (or rewriting rules) and an initial structure. It was originally formulated to describe the growth of plant cells, and has subsequently been applied for various purposes in computer graphics such as modeling plants, buildings, streets, and ornaments. For our purpose, we extended the growth process of the L-system as follows: 1) each growing branch keeps away from existing branches as much as possible to create a uniform distribution, and 2) when branches collide, we connect the colliding branches to construct a closed mesh structure. We designed a generating rule based on observations of the photograph of Purkinje fibers and manually specified three terminal positions on a three-dimensional (3D) heart model: those of the right bundle branch, the anterior fascicle, and the left posterior fascicle of the left branch. Then, we grew fibers starting from each of the three positions based on the specified generating rule. We achieved to generate 3D models of Purkinje fibers of which physical appearances closely resembled the real photograph. The generation takes a few seconds. Variations of the Purkinje fibers could be constructed easily by modifying the generating rules and parameters.


Journal of Cardiovascular Electrophysiology | 2001

Breakthrough waves during ventricular fibrillation depend on the degree of rotational anisotropy and the boundary conditions: a simulation study.

Takashi Ashihara; Tsunetoyo Namba; Takanori Ikeda; Makoto Ito; Masahiko Kinoshita; Kazuo Nakazawa

Breakthroughs in VF Depend on Rotational Anisotropy. Introduction: The left ventricle (LV) and right ventricle (RV) are characterized by specific fiber orientation known as “rotational anisotropy.” However, it remains unclear whether the LV and RV are different with regard to the effect of rotational anisotropy on the dynamics of scroll waves during ventricular fibrillation (VF). To resolve this issue, we used a computation‐based model to study scroll wave behavior.


Journal of Cardiovascular Electrophysiology | 2003

Vortex cordis as a mechanism of postshock activation: Arrhythmia induction study Using a bidomain model

Takashi Ashihara; Tsunetoyo Namba; Takenori Yao; Tomoya Ozawa; Ayaka Kawase; Takanori Ikeda; Kazuo Nakazawa; Makoto Ito

Introduction: The ventricular apex has a helical arrangement of myocardial fibers called the “vortex cordis.” Experimental studies have demonstrated that the first postshock activation originates from the ventricular apex, regardless of the electrical shock outcome; however, the related underlying mechanism is unclear. We hypothesized that the vortex cordis contributes to the initiation of postshock activation. To clarify this issue, we numerically studied the transmembrane potential distribution produced by various electrical shocks.


Journal of Cardiovascular Electrophysiology | 2004

Spiral Wave Control by a Localized Stimulus: A Bidomain Model Study

Takashi Ashihara; Tsunetoyo Namba; Makoto Ito; Takanori Ikeda; Kazuo Nakazawa; Natalia A. Trayanova

Introduction: It has been reported that electrical stimulation can control spiral wave (SW) reentry. However, previous research does not account for the effects of stimulus‐induced virtual electrode polarization (VEP) and the ensuing cathode‐break (CB) excitation. The aim of the present study was to examine the interaction of VEP with SW reentry in a bidomain model of electrical stimulation and thus provide insight into the mechanistic basis of SW control.


Journal of Cardiovascular Electrophysiology | 2001

Electroporation in a Model of Cardiac Defibrillation

Takashi Ashihara; Takenori Yao; Tsunetoyo Namba; Makoto Ito; Takanori Ikeda; Ayaka Kawase; Sunao Toda; Toru Suzuki; Masashi Inagaki; Masaru Sugimachi; Masahiko Kinoshita; Kazuo Nakazawa

Electroporation in a Model of Cardiac Defibrillation. Introduction: It is known that highstrength shock disrupts the lipid matrix of the myocardial cell membrane and forms reversible aqueous pores across the membrane. This process is known as “electroporation.” However, it remains unclear whether electroporation contributes to the mechanism of ventricular defibrillation. The aim of this computer simulation study was to examine the possible role of electroporation in the success of defibrillation shock.


Europace | 2010

Abnormal restitution property of action potential duration and conduction delay in Brugada syndrome: both repolarization and depolarization abnormalities

Nobuhiro Nishii; Satoshi Nagase; Hiroshi Morita; Kengo Kusano; Tsunetoyo Namba; Daiji Miura; Kohei Miyaji; Shigeki Hiramatsu; Takeshi Tada; Masato Murakami; Atsuyuki Watanabe; Kimikazu Banba; Yoshiaki Sakai; Kazufumi Nakamura; Takefumi Oka; Tohru Ohe

AIMS This study sought to examine the action potential duration restitution (APDR) property and conduction delay in Brugada syndrome (BrS) patients. A steeply sloped APDR curve and conduction delay are known to be important determinants for the occurrence of ventricular fibrillation (VF). METHODS AND RESULTS Endocardial monophasic action potential was obtained from 39 BrS patients and 9 control subjects using the contact electrode method. Maximum slopes of the APDR curve were obtained at both the right ventricular outflow tract (RVOT) and the right ventricular apex (RVA). The onset of activation delay (OAD) after premature stimulation was examined as a marker of conduction delay. Maximum slope of the APDR curve in BrS patients was significantly steeper than that in control subjects at both the RVOT and the RVA (0.77 +/- 0.21 vs. 058 +/- 0.14 at RVOT, P = 0.009; 0.98 +/- 0.23 vs. 0.62 +/- 0.16 at RVA, P = 0.001). The dispersion of maximum slope of the APDR curve between the RVOT and the RVA was also larger in BrS patients than in control subjects. The OAD was significantly longer in BrS patients than in control subjects from the RVOT to RVA and from the RVA to RVOT (from RVOT to RVA: 256 +/- 12 vs. 243 +/- 7 ms, P = 0.003; from RVA to RVOT: 252 +/- 11 vs. 241 +/- 9 ms, P = 0.01). CONCLUSIONS Abnormal APDR properties and conduction delay were observed in BrS patients. Both repolarization and depolarization abnormalities are thought to be related to the development of VF in BrS patients.


Archive | 2000

Computational Analysis and Visualization of Spiral Wave Reentry in a Virtual Heart Model

Kazuo Nakazawa; Tohru Suzuki; Takashi Ashihara; Masashi Inagaki; Tsunetoyo Namba; Takanori Ikeda; Ryoji Suzuki

It has been suggested that spiral wave reentry is the principal mechanism of functional tachyarrhythmias. In this study, we present images of the dynamics of tachyarrhythmic excitation propagation based on spiral wave reentry obtained in a virtual heart model. For this purpose, we employed high-performance computation techniques using a supercomputer and visualizing techniques using color computer graphics. In this heart model, the myocardial units were represented by two types of non-linear ordinary differential equations. The myocardial units were connected to each other into simple shaped two-or three-dimensional media corresponding to the heart walls and also into a human ventricular-shaped medium. The dynamics of excitation propagation were visualized intelligibly through various improvements in the visualizing techniques employed in the implementation of the three-dimensional graphics. Our results suggested that it is possible for lethal arrhythmia, commonly called ventricular fibrillation, to occur even in hearts without any conduction abnormalities or repolarization heterogeneity, e.g., infarction or ischemia, and cause sudden death.


Circulation | 2004

Mechanisms of Myocardial Capture and Temporal Excitable Gap During Spiral Wave Reentry in a Bidomain Model

Takashi Ashihara; Tsunetoyo Namba; Takanori Ikeda; Makoto Ito; Kazuo Nakazawa; Natalia A. Trayanova

Background—Recent studies have demonstrated that regional capture during cardiac fibrillation is associated with an elevated capture threshold. It is typically assumed that the temporal excitable gap (capture window) during fibrillation reflects the size of the spatial excitable gap (excitable tissue between fibrillation waves). Because capture threshold is high, virtual electrode polarization is expected to be involved in the process. However, little is known about the underlying mechanisms of myocardial capture during fibrillation. Methods and Results—To clarify these issues, we conducted altogether 3168 simulations of single spiral wave capture in a bidomain sheet. Unipolar stimuli of strengths 4, 8, 16, and 24 mA and 2-ms duration were delivered at 99 locations in the sheet. We found that cathode-break rather than cathode-make excitation was the dominant mechanism of myocardial capture. When the stimulation site was located diagonally with respect to the core (upper left or lower right if the spiral wave rotates counterclockwise), the cathode-break excitation easily invaded the spatial excitable gap and resulted in a successful capture as a result of the formation of virtual anodes in the direction of the myocardial fibers. Thus, the spatial distribution of the temporal excitable gap did not reflect the spatial excitable gap. Conclusions—The areas exhibiting wide temporal excitable gaps were areas in which the cathode-break excitation wave fronts easily invaded the spatial excitable gap via the virtual anodes. This study provides mechanistic insight into myocardial capture.

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Takashi Ashihara

Shiga University of Medical Science

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Takenori Yao

Shiga University of Medical Science

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Makoto Ito

Shiga University of Medical Science

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Masahiko Kinoshita

Shiga University of Medical Science

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