| Literature DB >> 27510912 |
K Stingl1, K U Bartz-Schmidt1, A Braun2, F Gekeler1,3, U Greppmaier2, A Schatz1,3, A Stett4, T Strasser1, V Kitiratschky5, E Zrenner1,6.
Abstract
PURPOSE: The subretinal Alpha IMS visual implant is a CE-approved medical device for restoration of visual functions in blind patients with end-stage outer retina degeneration. We present a method to test the function of the implant objectively in vivo using standard electroretinographic equipment and to assess the devices' parameter range for an optimal perception.Entities:
Keywords: Artificial vision; Electrophysiology; Hereditary retinal diseases; Neuroprosthetics; Retinitis pigmentosa; Subretinal visual implant
Mesh:
Year: 2016 PMID: 27510912 PMCID: PMC5052310 DOI: 10.1007/s10633-016-9557-7
Source DB: PubMed Journal: Doc Ophthalmol ISSN: 0012-4486 Impact factor: 2.379
Fig. 1Subretinal alpha IMS implant (Retina Implant AG, Reutlingen, Germany). a The subdermal receiver coil behind the ear provides power and forwards control signals via a subdermal cable and a thin intraocular foil to the chip in the eye. b The external transmitter coil is magnetically kept in place above the subdermal coil behind the ear and provides power and signals via transdermal electric induction. c The chip is placed surgically beneath the fovea and contains 1500 pixels (independent microphotodiode-amplifier-electrode elements) on a 3 mm × 3 mm area. d Via a thin black cable, a small battery pack powers the primary external coil. Settings of contrast sensitivity and brightness can be adapted manually. (Figure modified from Stingl et al. [6]
Fig. 2Examples of in vivo CRIR recordings with 9 luminance steps showing a typical pulse shape with the sampling frequency of 5 kHz (black dots). The 1 ms anodic voltage pulse output from the implant electrodes results in a slowly rising current that shows an overshoot in the opposite direction after pulse offset and a subsequent return to the baseline. The full-field luminance levels for each particular step are indicated above each curve. With increasing luminance, the amplitude of the CRIR increases showing the dynamic range of the particular chip settings (here V gl = 20, V bias = 65). These amplitudes are then documented as a CRIR curve (as shown in Fig. 3)
Fig. 3CRIR as transfer characteristic curves in vivo in various combinations of the V gl/V bias settings that define the MPDA-amplifiers’ sensitivity and gain, respectively, from four patients measured at various time points during the 1-year follow-up visits. a patient C9, b patient C10, c patient C12 d patient C7. The inserted tables show values for V gl/V bias
Fig. 4a CRIR from patient C9, as taken from Fig. 4a, shows data measured during a single trial visit; b illustrates how changing the V gl value shifts the curve along the luminance range; c illustrates the change of minimum and maximum output when altering V bias. The values for V gl/V bias are shown in the upper left corner
Fig. 5Appearance, recording and characteristics of CRIRs. Left Output voltage (V chip), current (I chip) and charge per pulse (Q chip) of the MPDA. From the peak charge, the in vitro transfer curve as a function of illuminance is obtained. Middle Related to the current spread through the tissue, a voltage pulse at the cornea (V cornea) is observable. Right Voltage signal (V Filter) recorded with the ERG system. From the peak value of this filtered signal (CRIR), the in vivo transfer curve as a function of luminance is obtained. Details see text