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Conventionally, inorganic materials such as selenium, cadmium sulfide and zinc oxide are used as organic photoconductive materials of photoconductive members to be used in image forming apparatus. However, the above-mentioned inorganic materials are not satisfactory with regard to environmental pollution and cost, and further their utilization limit is narrow.
On the other hand, many kinds of organic photoconductive materials have been proposed. In particular, the so-called “electrophotographic photoconductive materials” are extensively investigated. The electrophotographic photoconductive materials are widely used in an image forming apparatus such as a copying machine, a printer, a facsimile and a laser beam printer. In particular, the electrophotographic photoconductive material are widely used in a laser beam printer, because it is small-sized, lightweight, inexpensive, and maintenance is simple.
A photoconductive material to be used for the electrophotographic photoconductor is required to have the functions of maintaining the electric potential in a dark place and generating electric charges upon receipt of light. In particular, when the photoconductor is used for an electrophotographic process, after the electric charges are formed on the surface of the photoconductor, a latent electrostatic image is formed on the photoconductor and the latent electrostatic image is developed with a developer to form a visual image.
As the photoconductive material suitable for the above-mentioned uses, there is known a photoconductor using a perylene compound described in Japanese Laid-Open Patent Application 56-115566 and Japanese Laid-Open Patent Application 59-94346.
It has been desired to reduce the molecular weight of a perylene compound described in the above mentioned Japanese Laid-Open Patent Application 56-115566 and Japanese Laid-Open Patent Application 59-94346 in order to improve the performance of the photoconductor. The perylene compound is decomposed to be a low molecular weight compound when the perylene compound is allowed to stand in a high temperature atmosphere, whereby the performance of the photoconductor is deteriorated. Therefore, it is difficult to continuously use
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What does the flag N produces for the crossfilter dimension?
I’m implementing a similar to the map example found here. To use this implementation for my own application I want to add a flag, that produces a different dimension depending on the type of the input data.
In this example however I see that the flags I use to call the function (N, S, R) don’t produce the nice result, but instead produce the same dimension as the type parameter