Abstract
It is now well known that many elements can be stimulated to produce characteristic X-rays. So far, the only successful method of obtaining the characteristic rays has been to place the element in the path of a beam of X-rays, whereupon it becomes a secondary radiator; and, if the exciting X-rays have the necessary penetrating power, the characteristic rays will make their appearance. Some years ago a remarkable paper by Kaye appeared, in which he showed that if an element, say, copper, were made the anticathode in an X-ray bulb, it could become a source of intense radiation characteristic of copper.
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