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1.
J Neural Eng ; 16(3): 036007, 2019 06.
Article in English | MEDLINE | ID: mdl-30818288

ABSTRACT

OBJECTIVE: Microstimulation to the cortical tissue applied with penetrating electrodes delivers current that spreads concentrically around the electrode tip and is known to evoke focal visual sensations, i.e. phosphenes. However, to date, there is no direct evidence depicting the spatiotemporal properties of neuronal activity induced immediately after microstimulation and how such activity drives the subsequent local cortical circuits. APPROACH: In the present study, we imaged the spatiotemporal distribution of action potentials (APs) directly induced by microstimulation and the subsequent trans-synaptic signal propagation using a voltage-sensitive dye (VSD) and a calcium-sensitive dye (CaSD) in slice preparations of the mouse primary visual cortex. MAIN RESULTS: The directly induced APs were confined to the close vicinity of the electrode tip, and the effective distance of excitation was proportional to the square root of the current intensity. The excitation around the electrode tip in layer IV mainly propagated to layer II/III to further induce the subsequent focal activation in downstream local cortical circuits. The extent of activation in the downstream circuits was restrained by competitive interactions between excitatory and inhibitory signals. Namely, the spread of the excitation to lateral neighbor neurons along the layer II/III was confined by the delayed inhibition that also spread laterally at a faster rate. SIGNIFICANCE: These observations indicate that dynamic interactions between excitatory and inhibitory signals play a critical role in the focal activation of a cortical circuit in response to intracortical microstimulation and, therefore, in evoking a localized phosphene.


Subject(s)
Action Potentials/physiology , Electrodes, Implanted , Nerve Net/physiology , Neurons/physiology , Visual Cortex/physiology , Animals , Electric Stimulation/methods , Female , Male , Mice , Mice, Inbred C57BL , Microelectrodes , Nerve Net/cytology , Organ Culture Techniques , Phosphenes/physiology , Visual Cortex/cytology
2.
Langmuir ; 24(18): 10402-6, 2008 Sep 16.
Article in English | MEDLINE | ID: mdl-18702474

ABSTRACT

Low-density tin dioxide (SnO2) is required for radiating monochromatic extreme ultraviolet (EUV) light with low debris and high conversion efficiency from a laser. In this paper, tin dioxide nanoparticle hollow microcapsules were successfully fabricated by a layer-by-layer template technique. The obtained capsules have a rougher surface (30 nm in rms) compared to the freshly prepared polyelectrolyte capsules. Based on the X-ray diffraction (XRD) results, the tin dioxide nanoparticles well maintained their size after they were assembled on the capsules' surfaces. In order to remove the polymer template, a heat treatment was introduced, and after the heat treatment the capsule sizes shrank about 71% (the average size was from 4.9 to 3.5 mum), and the obtained capsules maintained their round shape after water evaporation. The narrowest bandwidth at the 13.5 nm emission in the EUV region was observed when the capsules were irradiated by a CO2 laser with an intensity of 2.9 x 10(10) W/cm (2).


Subject(s)
Carbon Dioxide/chemistry , Tin Compounds/chemistry , Tin/chemistry , Adsorption , Electrolytes , Hot Temperature , Lasers , Microscopy, Atomic Force , Microscopy, Electron, Scanning , Microspheres , Models, Statistical , Nanoparticles/chemistry , Surface Properties , Ultraviolet Rays , X-Ray Diffraction
3.
Phys Rev Lett ; 95(23): 235004, 2005 Dec 02.
Article in English | MEDLINE | ID: mdl-16384313

ABSTRACT

Opacity effects on extreme ultraviolet (EUV) emission from laser-produced tin (Sn) plasma have been experimentally investigated. An absorption spectrum of a uniform Sn plasma generated by thermal x rays has been measured in the EUV range (9-19 nm wavelength) for the first time. Experimental results indicate that control of the optical depth of the laser-produced Sn plasma is essential for obtaining high conversion to 13.5 nm-wavelength EUV radiation; 1.8% of the conversion efficiency was attained with the use of 2.2 ns laser pulses.

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