| Literature DB >> 29692701 |
Micha E Spira1, Nava Shmoel1, Shun-Ho M Huang1, Hadas Erez1.
Abstract
Multielectrode arrays (MEA) are used extensively for basic and applied electrophysiological research of neuronal- and cardiomyocyte-networks. Whereas immense progress has been made in realizing sophisticated MEA platforms of thousands of addressable, high-density, small diameter, low impedance sensors, the quality of the interfaces formed between excitable cells and classical planar sensor has not improved. As a consequence in vitro and in vivo MEA are "blind" to the rich and important "landscape" of sub-threshold synaptic potentials generated by individual neurons. Disregarding this essential fraction of network signaling repertoire has become the standard and almost the "scientific ideology" of MEA users. To overcome the inherent limitations of substrate integrated planar MEA platforms that only record extracellular field potentials, a number of laboratories have developed in vitro MEA for intracellular recordings. Most of these novel devices use vertical nano-rods or nano-wires that penetrate the plasma membrane of cultured cells and record the electrophysiological signaling in a manner similar to sharp intracellular microelectrodes. In parallel, our laboratory began to develop a bioinspired approach in-which cell biological energy resources are harnessed to self-force a cell into intimate contact with extracellular gold mushroom-shaped microelectrodes to record attenuated synaptic- and action-potentials with characteristic features of intracellular recordings. Here we describe some of the experiments that helped evolve the approach and elaborate on the biophysical principles that make it possible to record intracellular potentials by an array of extracellular electrode. We illustrate the qualities and limitations of the method and discuss prospects for further improvement of this technology.Entities:
Keywords: Aplysia; action-potential; cardiomyocytes; electrophysiology; hippocampus; multielectrode-array; skeletal- myotubes; synaptic-potentials
Year: 2018 PMID: 29692701 PMCID: PMC5902558 DOI: 10.3389/fnins.2018.00212
Source DB: PubMed Journal: Front Neurosci ISSN: 1662-453X Impact factor: 4.677
Figure 1(Ai) Schematic drawing of a cell (green) residing on a planar sensing electrode (yellow) and the space between them (white). (Aii) An analog electrical circuit of the cell-electrode interface. In the model, the cell's surface area is subdivided into a non-junctional membrane (njm, red) that faces the grounded culture medium, and a junctional membrane (jm, blue) that faces the electrode. Each of these membrane compartments is represented by a resistor and capacitor in parallel Rnjm, Cnjm, Rjm, and Cjm, respectively. The cleft between the cell and the sensor is represented by a resistor (the seal resistance-Rs). The electrode is represented by a resistor and capacitor (Re, Ce, respectively). The electrical coupling coefficient (CC) between a cell and a recording device is defined as the ratio between the voltage recorded by the device (electrode-amplifier) and the voltage generated across the plasma membrane of an excitable cell (Velect/Vcell). The square pulse in between the ground jm and njm is a voltage calibration pulse (Bi,Bii) schematic illustrations of downward displacement of a cell to increase the seal resistance (mp-a fire polished pipette to exert the pressure, μe-intracellular recording electrode). (Biii) Concomitant alterations in the extracellularly recorded FPs (upper traces- black) and intracellular APs (lower traces- red) during the displacement of the neuron's cell body toward the planar electrode. From left to right, initially the increased FPs amplitude is not associated with changes in the intracellular AP amplitude. Thereafter (4th trace), the extracellular FP recorded by the planar electrode transformed to intracellular recordings of an AP. This is associated by reduction in the AP amplitude recorded by the μE. Release of the mechanical pressure led to the reversal of the process (traces 6 and 7). (Biv) Super positioning of the intracellular recorded APs with the sharp electrode and the extracellular planar electrode (multiplied by 8). Note that although the amplitudes of the two APs are different the shapes of the APs are similar (Biii,Biv modified with permission from Cohen et al., 2008). (C) A scanning electron microscope image of a gMμE. (D) a latex bead engulfed by a cultured Aplysia neuron. (E) An electron microscope image of a thin section showing a gMμE (black) tightly engulfed by a cultured PC12 cell.
Figure 2(Ai) Differences in the levels of the seal resistance formed between a single Aplysia neuron residing on 8 gMμEs (insert) leads to differences in the IN-CELL recorded APs amplitudes. A cultured Aplysia neuron was intracellularly stimulated to fire 3 consecutive APs (red trace). Simultaneous recordings of these APs by 8 gMμE (blue traces) revealed differences in the IN-CELL recorded amplitudes. (Aii) Synaptic- and action-potentials recorded by an extracellular gMμE. Stimulation of a presynaptic neuron by an intracellular sharp electrode (red) lead to the generation of excitatory post synaptic potentials (blue) recorded by a gMμE. Note the summation of the EPSPs to reach firing threshold (Ai,Aii modified with permission from Hai et al., 2010a). (B) Spontaneous activity recorded by a gMμEs from a cultured hippocampal neuron. (Bi) Control spontaneous APs firing recorded by a gMμE, (Bii) 10 min after the application of 10 μm GABAzin the firing pattern was changed. (Biii) Enlargements of the records in (Bi). (Biv) Enlargement of the right box in (Biii,Bv) enlargement of the left box in (Biii). The low amplitude long duration potentials in (Biii) (left box) have the features of excitatory post synaptic potentials. The fast spikelets indicated by * could be either dendritic spikes or the firing of electrically coupled neurons. As the dynamics and amplitudes of the potentials shown in (Bv) are not altered by GABAzin it is unlikely that they reflect barrage of FPs generated by remote neurons. (C) Comparison of intracellular recorded potentials to IN-CELL recordings from cultured myotubes obtained by gMμE electroporation. (Ci,Cii) Depict simultaneous extracellular FPs recordings by a gMμE (Ci) and intracellular recordings by a sharp electrode (Cii). The recordings (Ci,Cii) revealed identical firing patterns and similar qualitative alterations in the amplitudes of the recorded action potentials. (Ciii) Electroporation of the myotube changed the recording mode by the gMμE from extracellular to the IN-CELL. Note that although the IN-CELL recorded amplitude of the APs is about an order of magnitude lower than that of the intracellular electrode APs, the shape of the recorded potentials are identical. Also, note that both the gMμE (Ciii) and the intracellular sharp electrode (Civ) recorded subthreshold potentials in between the APs (C modified with permission from Rabieh et al., 2016). (D) IN-CELL recordings from cultured human cardiomyocytes. Three seconds before electroporation 4. Thirty-three and sixty-three seconds after electroporation.