Method of making photoconductive coating
AssigneeCoulter Systems Corporation
InventorManfred R. Kuehnle
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AssigneeCoulter Systems Corporation
InventorManfred R. Kuehnle
Estimating the term…
A method of making a photoconductive coating of the type which comprises a crystalline layer of wholly inorganic material on a suitable substrate for use as an electrophotographic member, said method including the steps of depositing the coating in a vacuum chamber by sputtering with R.F. energy in such a manner that the deposit is crystalline, with the individual crystals oriented substantially vertically, the size of the crystals being uniform and hexagonal in configuration and of the order of 700 to 800 Angstroms in diameter and with a barrier layer coating on the surface that is of extreme resistivity, each crystal acting independently as an independent field domain, the crystal length normal to the substrate being the same as the coating thickness and the deposit evidencing single crystal configuration in response to diffraction pattern measurements. Background gas, including minute measured quantities of oxygen, being introduced during the sputtering and permitted to react with the surface of the sputtered coating.
In a method of depositing a wholly inorganic dielectric photoconductive coating onto a substrate in which there is a pressure vessel having therein target means comprising at least one target of the material to be deposited, a supply of substrate, an anode in the vessel, means for leading the substrate to pass over and in engagement with the anode during the sputtering process, an external source of radio frequency energy having electrical couplings to the anode, target means and shielding arranged in the vicinity of the anode and target means, a supply of background gas including an inert ionizable gas and a second gas having at least one constituent for preventing disassociation of the compound during sputtering, means for establishing and maintaining a stable condition of sputtering plasma in the vessel between the target means and the anode, the steps of:
In a method of depositing a wholly inorganic dielectric photconductive coating onto a substrate in which there is a provided a pressure vessel having therein target means comprising at least one target of the material to be deposited, there is provided a supply of substrate, there is an anode disposed in the vessel, means are provided for leading the substrate to pass over and in engagement with the anode during the sputtering process, there is an external source of radio frequency energy having electrical couplings to the anode, target means and to shielding arranged in the vicinity of the anode and target means, there is provided a supply of background gas including an inert ionizable gas and a second gas having at least one constituent for preventing disassociation of the compound during sputtering, there are provided means for establishing and maintaining a stable condition of sputtering plasma in the vessel between the target means and the anode, the steps of:
A method of making an electrophotographic member formed of a photoconductive coating on a substrate, the photoconductive coating being formed of a wholly inorganic dielectric compound which is microcrystalline of hexagonal, orderly, closely packed, highly uniform crystals having a crystal diameter less than 0.1 micron and a height equal to the thickness of the coating, the crystals all being arranged substantially vertically oriented relative to the plane of the substrate, the coating capable of accepting a charge of electrons at speeds of nanoseconds as well as at substantially slower speeds, such charge providing surface potential of the order of 10 volts per thousand Angstroms coating thickness, having a dark decay characteristic of surface potential versus time that drops off immediately after charging at a generally logarithmic rate, but with the rate of decay decreasing with time such that there remains substantially more than ten percent of the original maximum surface potential after several minutes with an absolute value sufficient to tone an image with an excellent grey scale, said member capable of being selectively discharged after being charged, by means of said radiation in any increment of area capable of being distinguished as finely as electronically from an immediately adjacent increment, said discharge occurring proportionally to the degree of radiation intensity to which said increment is subjected, the member being capable of total discharge, the increment assuming immediately after said discharge a decay characteristic of surface potential versus time which maintains proportionality of the said characteristics of all other increments of said member for a substantial period of time during which said increment can continue to be distinguished from all others, said method comprising the steps of
Dependencies are inferred from the claim text.