scholarly journals On the excitation of characteristic X-rays from light elements

In an attempt to fill up the gap between the shortest ultra-violet light waves hitherto produced and the longest X-ray waves known, Hughes recently made a study of the characteristic X-rays emitted by carbon and by boron when bombarded by electrons. In this investigation the energy of the bombarding electrons was increased by steps, and the critical values were determined that were necessary and just sufficient to cause the bombarded element to emit its characteristic radiations with measurable intensities. These characteristic radiations were detected, and their intensities measured, by their photo-electric action on an insulated electrode of nickel or of silver. The method followed by Hughes in recording his results was to plot curves with the values of the accelerating potentials of the electrons as abscissæ and the measures of the photo-electric effect divided by the corresponding electronic currents as ordinates. At certain critical accelerating voltages it was found that these curves showed marked and abrupt kinks or changes of curvature, and these changes were taken to connote the beginning of the emission by the bombarded element of its characteristic radiations.

Hertz’s observation that ultra-violet light can facilitate the passage of an electric spark led to the discovery of other photo-electric actions. In the earliest experiments on the photo-electric effect of metals it was noticed that the action was diminished by exposure to light. Thus Hallwachs, who found that a metal becomes positively electrified under the influence of ultra-violet light, states that “old surfaces no longer show the phenomenon. The radiation itself lowers the potential to which the plates can be electrified, so that with any succeeding experiment made with the same surface the potential obtained is lower, while the rise to it takes place more rapidly, and the decrease is greater than when for the same interval of time between the experiments the plate was not illuminated.” This diminution of the photo-electric action is spoken of as the "fatigue" of metals under the influence of light. It has received attention from many physicists, of whom Buisson and Ladenburg may be specially referred to.


Development ◽  
1958 ◽  
Vol 6 (4) ◽  
pp. 634-637
Author(s):  
G. G. Selman

For several years in this laboratory, ultra-violet light has been used to produce haploid amphibian embryos, sometimes to provide haploid nuclei for transplantation experiments, as in Pantelouris & Jacob (1958). The ultra-violet method gives a high proportion of haploids, is very simple and speedy to carry out and involves the use of only inexpensive apparatus. Our method and results are described here to help others choose between this and alternative methods such as the use of toluidine blue by Briggs (1952), or X-rays by Lehman (1955) and Rugh (1939). Other methods are reviewed in Fankhauser (1937) and Drebinger (1951). Eggs were taken from the oviducts of newt females and were placed close together in groups on cellophane squares to which they adhered by their jelly coats so that their animal surfaces were uppermost. The cellophane squares of unfertilized eggs were then placed in Petri dishes in air kept moist with a piece of damp filter paper at one side.


1971 ◽  
Vol 5 (3) ◽  
pp. 258-281 ◽  
Author(s):  
Roger H. Stuewer

The modern corpuscular theory of radiation was born in 1905 when Einstein advanced his light quantum hypothesis; and the steps by which Einstein's hypothesis, after years of profound scepticism, was finally and fully vindicated by Arthur Compton's 1922 scattering experiments constitutes one of the most stimulating chapters in the history of recent physics. To begin to appreciate the complexity of this chapter, however, it is only necessary to emphasize an elementary but very significant point, namely, that while Einstein based his arguments for quanta largely on the behaviour of high-frequency black body radiation or ultra-violet light, Compton experimented with X-rays. A modern physicist accustomed to picturing ultra-violet light and X-radiation as simply two adjacent regions in the electromagnetic spectrum might regard this distinction as hair-splitting. But who in 1905 was sure that X-rays and γ-rays are far more closely related to ultra-violet light than to α-particles, for example ? This only became evident after years of painstaking research, so that moving without elaboration from Einstein's hypothesis to Compton's experiments automatically eliminates from consideration an important segment of history—a segment in which a major role was played by William Henry Bragg.


Methods are described whereby the frequency of mutations induced in Drosophila spermatozoa by ultra-violet light may be brought to approximately 5%. Among the means used to increase the mutation rate was the selection of those individuals in which, as shown by their earlier death, the radiation had penetrated more effectively. It has been shown by the use of a combination of filters that the region in which the mutation-inducing effect of ultra-violet light begins lies between 320 and 300 mμ, as expected for nucleic acid absorption. Further results, with an improved genetic technique whereby the production of gene mutations and gross rearrangements could be studied in the same individual, have confirmed our earlier conclusion that, as compared with X-rays of the same gene-mutational strength, ultra-violet rays are ineffective in causing gross structural changes of chromosomes. Preliminary evidence was obtained that ultra-violet rays are similarly ineffective in the production of minute structural changes, and that (in Drosophila ) they also fail to produce, by 'simple breakage', chromosome fragments that are capable of surviving ('terminal deficiencies'). It may be concluded that activation of the nucleic acid by ultra-violet is ineffective in producing breakage of the chromosome, although it is effective in producing gene mutations. The gene mutations produced by ultra-violet must occur secondarily, as a consequence of transfer of energy from the nucleic acid, resulting in turn in a change of the distinctive gene material, which is probably of protein nature. It is therefore illegitimate to calculate the size or number of genes from the frequency with which gene mutations are produced by a given dose of radiation. The gene-mutational change apparently differs in some essential way from the change involved in demonstrable minute rearrangements, but the minute rearrangements appear to be essentially similar to the gross rearrangements, involving a similar kind of thoroughgoing breakage of the chromonema. The effect of ultra-violet in discriminating between gene mutations on the one hand and both minute and gross rearrangements on the other hand, lends some support to the conception that the 'genes' represent definite segments of the chromonema, and that the connexions between the parts of these segments are different in kind from the connexions between the segments themselves. A possible means of attack on the mutation theory of cancer, derived from the above conclusions regarding the mechanism of action of ultra-violet light, is pointed out.


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