6
" I had ceased to be a writer of tolerably poor tales and essays, and had become a tolerably good Surveyor of the Customs. That was all. But, nevertheless, it is any thing but agreeable to be haunted by a suspicion that one's intellect is dwindling away; or exhaling, without your consciousness, like ether out of a phial; so that, at every glance, you find a smaller and less volatile residuum. Of the fact, there could be no doubt; and, examining myself and others, I was led to conclusions in reference to the effect of public office on the character, not very favorable to the mode of life in question. In some other form, perhaps, I may hereafter develop these effects. Suffice it here to say, that a Custom-House officer, of long continuance, can hardly be a very praiseworthy or respectable personage, for many reasons; one of them, the tenure by which he holds his situation, and another, the very nature of his business, which—though, I trust, an honest one—is of such a sort that he does not share in the united effort of mankind.
An effect—which I believe to be observable, more or less, in every individual who has occupied the position—is, that, while he leans on the mighty arm of the Republic, his own proper strength departs from him. He loses, in an extent proportioned to the weakness or force of his original nature, the capability of self-support. If he possess an unusual share of native energy, or the enervating magic of place do not operate too long upon him, his forfeited powers may be redeemable. The ejected officer—fortunate in the unkindly shove that sends him forth betimes, to struggle amid a struggling world—may return to himself, and become all that he has ever been. But this seldom happens. He usually keeps his ground just long enough for his own ruin, and is then thrust out, with sinews all unstrung, to totter along the difficult footpath of life as he best may. Conscious of his own infirmity,—that his tempered steel and elasticity are lost,—he for ever afterwards looks wistfully about him in quest of support external to himself. His pervading and continual hope—a hallucination, which, in the face of all discouragement, and making light of impossibilities, haunts him while he lives, and, I fancy, like the convulsive throes of the cholera, torments him for a brief space after death—is, that, finally, and in no long time, by some happy coincidence of circumstances, he shall be restored to office. This faith, more than any thing else, steals the pith and availability out of whatever enterprise he may dream of undertaking. Why should he toil and moil, and be at so much trouble to pick himself up out of the mud, when, in a little while hence, the strong arm of his Uncle will raise and support him? Why should he work for his living here, or go to dig gold in California, when he is so soon to be made happy, at monthly intervals, with a little pile of glittering coin out of his Uncle's pocket? It is sadly curious to observe how slight a taste of office suffices to infect a poor fellow with this singular disease. Uncle Sam's gold—meaning no disrespect to the worthy old gentleman—has, in this respect, a quality of enchantment like that of the Devil's wages. Whoever touches it should look well to himself, or he may find the bargain to go hard against him, involving, if not his soul, yet many of its better attributes; its sturdy force, its courage and constancy, its truth, its self-reliance, and all that gives the emphasis to manly character. "
― Nathaniel Hawthorne , The Scarlet Letter
9
" If we ascribe the ejection of the proton to a Compton recoil from a quantum of 52 x 106 electron volts, then the nitrogen recoil atom arising by a similar process should have an energy not greater than about 400,000 volts, should produce not more than about 10,000 ions, and have a range in the air at N.T.P. of about 1-3mm. Actually, some of the recoil atoms in nitrogen produce at least 30,000 ions. In collaboration with Dr. Feather, I have observed the recoil atoms in an expansion chamber, and their range, estimated visually, was sometimes as much as 3mm. at N.T.P.These results, and others I have obtained in the course of the work, are very difficult to explain on the assumption that the radiation from beryllium is a quantum radiation, if energy and momentum are to be conserved in the collisions. The difficulties disappear, however, if it be assumed that the radiation consists of particles of mass 1 and charge 0, or neutrons. The capture of the a-particle by the Be9 nucleus may be supposed to result in the formation of a C12 nucleus and the emission of the neutron. From the energy relations of this process the velocity of the neutron emitted in the forward direction may well be about 3 x 109 cm. per sec. The collisions of this neutron with the atoms through which it passes give rise to the recoil atoms, and the observed energies of the recoil atoms are in fair agreement with this view. Moreover, I have observed that the protons ejected from hydrogen by the radiation emitted in the opposite direction to that of the exciting a-particle appear to have a much smaller range than those ejected by the forward radiation.This again receives a simple explanation on the neutron hypothesis. "
