02255nas a2200169 4500008004100000022001400041245007100055210006700126260001200193300001400205490000700219520174400226653002001970100002601990700002102016856004802037 2003 eng d a1090-058600aEEG-based communication and control: speed-accuracy relationships.0 aEEGbased communication and control speedaccuracy relationships c09/2003 a217–2310 v283 aPeople can learn to control mu (8-12 Hz) or beta (18-25 Hz) rhythm amplitude in the EEG recorded over sensorimotor cortex and use it to move a cursor to a target on a video screen. In our current EEG-based brain-computer interface (BCI) system, cursor movement is a linear function of mu or beta rhythm amplitude. In order to maximize the participant's control over the direction of cursor movement, the intercept in this equation is kept equal to the mean amplitude of recent performance. Selection of the optimal slope, or gain, which determines the magnitude of the individual cursor movements, is a more difficult problem. This study examined the relationship between gain and accuracy in a 1-dimensional EEG-based cursor movement task in which individuals select among 2 or more choices by holding the cursor at the desired choice for a fixed period of time (i.e., the dwell time). With 4 targets arranged in a vertical column on the screen, large gains favored the end targets whereas smaller gains favored the central targets. In addition, manipulating gain and dwell time within participants produces results that are in agreement with simulations based on a simple theoretical model of performance. Optimal performance occurs when correct selection of targets is uniform across position. Thus, it is desirable to remove any trend in the function relating accuracy to target position. We evaluated a controller that is designed to minimize the linear and quadratic trends in the accuracy with which participants hit the 4 targets. These results indicate that gain should be adjusted to the individual participants, and suggest that continual online gain adaptation could increase the speed and accuracy of EEG-based cursor control.10aVideo Recording1 aMcFarland, Dennis, J.1 aWolpaw, Jonathan uhttp://www.ncbi.nlm.nih.gov/pubmed/1296445303960nas a2200325 4500008004100000022001400041245011500055210006900170260001200239300001200251490000700263520302600270653001203296653002403308653001803332653002403350653001203374653001303386653002803399653001703427653002903444653002003473100001703493700001303510700001703523700001403540700001903554700001403573856004703587 1998 eng d a0009-732200aQuantification of effects of global ischemia on dynamics of ventricular fibrillation in isolated rabbit heart.0 aQuantification of effects of global ischemia on dynamics of vent c10/1998 a1688-960 v983 a

BACKGROUND: 

Ventricular fibrillation (VF) leads to global ischemia of the heart. After 1 to 2 minutes of onset, the VF rate decreases and appears more organized. The objectives of this study were to determine the effects of no-flow global ischemia on nonlinear wave dynamics and establish the mechanism of ischemia-induced slowing of the VF rate.

METHODS AND RESULTS: 

Activation patterns of VF in the Langendorff-perfused rabbit heart were studied with the use of 2 protocols: (1) 15 minutes of no-flow global ischemia followed by reperfusion (n=7) and (2) decreased excitability induced by perfusion with 5 micromol/L of tetrodotoxin (TTX) followed by washout (n=3). Video imaging ( approximately 7500 pixels per frame; 240 frames per second) with a voltage-sensitive dye, ECG, and signal processing (fast Fourier transform) were used for analysis. The dominant frequency of VF decreased from 13.5+/-1.3 during control to 9.3+/-1.4 Hz at 5 minutes of global ischemia (P<0.02). The dominant frequency decreased from 13.9+/-1.1 during control to 7.0+/-0.3 Hz at 2 minutes of TTX infusion (P<0.001). The rotation period of rotors on the epicardial surface (n=27) strongly correlated with the inverse dominant frequency of the corresponding episode of VF (R2=0. 93). The core area, measured for 27 transiently appearing rotors, was 5.3+/-0.7 mm2 during control. A remarkable increase in core area was observed both during global ischemia (13.6+/-1.7 mm2; P<0.001) and TTX perfusion (16.8+/-3.6 mm2; P<0.001). Density of wave fronts decreased during both global ischemia (P<0.002) and TTX perfusion (P<0.002) compared with control.

CONCLUSIONS: 

This study suggests that rotating spiral waves are most likely the underlying mechanism of VF and contribute to its frequency content. Ischemia-induced decrease in the VF rate results from an increase in the rotation period of spiral waves that occurs secondary to an increase in their core area. Remarkably, similar findings in the TTX protocol suggest that reduced excitability during ischemia is an important underlying mechanism for the changes seen.

10aAnimals10aElectrocardiography10aLinear Models10aMyocardial Ischemia10aRabbits10aRotation10aSodium Channel Blockers10aTetrodotoxin10aVentricular Fibrillation10aVideo Recording1 aMandapati, R1 aAsano, Y1 aBaxter, Bill1 aGray, R A1 aDavidenko, J M1 aJalife, J uhttp://www.ncbi.nlm.nih.gov/pubmed/977833603382nas a2200349 4500008004100000022001400041245008900055210006900144260001200213300001100225490000700236520236800243653002202611653001502633653001202648653003502660653001602695653002402711653002602735653002102761653004002782653002702822653001002849653002502859653002002884100001702904700001902921700001402940700001702954700001402971856004702985 1997 eng d a0090-696400aTechnical features of a CCD video camera system to record cardiac fluorescence data.0 aTechnical features of a CCD video camera system to record cardia c07/1997 a713-250 v253 a

A charge-coupled device (CCD) camera was used to acquire movies of transmembrane activity from thin slices of sheep ventricular epicardial muscle stained with a voltage-sensitive dye. Compared with photodiodes, CCDs have high spatial resolution, but low temporal resolution. Spatial resolution in our system ranged from 0.04 to 0.14 mm/pixel; the acquisition rate was 60, 120, or 240 frames/sec. Propagating waves were readily visualized after subtraction of a background image. The optical signal had an amplitude of 1 to 6 gray levels, with signal-to-noise ratios between 1.5 and 4.4. Because CCD cameras integrate light over the frame interval, moving objects, including propagating waves, are blurred in the resulting movies. A computer model of such an integrating imaging system was developed to study the effects of blur, noise, filtering, and quantization on the ability to measure conduction velocity and action potential duration (APD). The model indicated that blurring, filtering, and quantization do not affect the ability to localize wave fronts in the optical data (i.e., no systematic error in determining spatial position), but noise does increase the uncertainty of the measurements. The model also showed that the low frame rates of the CCD camera introduced a systematic error in the calculation of APD: for cutoff levels > 50%, the APD was erroneously long. Both noise and quantization increased the uncertainty in the APD measurements. The optical measures of conduction velocity were not significantly different from those measured simultaneously with microelectrodes. Optical APDs, however, were longer than the electrically recorded APDs. This APD error could be reduced by using the 50% cutoff level and the fastest frame rate possible.

10aAction Potentials10aAlgorithms10aAnimals10aBody Surface Potential Mapping10aCalibration10aComputer Simulation10aElectric Conductivity10aFluorescent Dyes10aImage Processing, Computer-Assisted10aModels, Cardiovascular10aSheep10aVentricular Function10aVideo Recording1 aBaxter, Bill1 aDavidenko, J M1 aLoew, L M1 aWuskell, J P1 aJalife, J uhttp://www.ncbi.nlm.nih.gov/pubmed/9236983