PART 111. ABSORPTION AND SCATTERING OF B RADIATION1
T h e "coincident discharges" irl a 4x-counter have been esamined and found t o be due in t h e main t o gas and wall back-scattering. This can be resolved into two components-scattering near t o and
I N T R O D U C T I O NPrevious publications in this series (37, 38, 39) have described experimental work aimed a t improving the accuracy of absolute counting using a 49-counter. In this paper additional experimental data are presented, which enable identification t o be made of the agency giving rise t o the discharges occurring coiilcidently in both half-counters, and exami~lation t o be effected of some of the scattering and absorption processes involved in using a 49 steradian geometrical arrangement.The penetration of electronic radiation through matter is a complex phenomenon owing t o the variety of processes by which interaction may occur ( 5 ) .With an initially collimated beam of moiloenergetic electrons, interaction with a layer of material up t o a superficial density of a few hundred pgm./cm.2 occurs by means of a few scattering events per electron. This results in the beam spreading without too great an energy or intensity loss. With thicker layers, Inore scattering events per electron occur and a transition t o "multiple scattering" takes place. With still thiclier layers the electroils no longer have a preferred direction of motion and the process resembles diffusion. The number of electrons now emerging from the foil decreases with increasing foil thickness, i.e. absorptioil of the radiation occurs.The single scattering of electrons has been treated theoretically (2, 33) and the multiple scattering has beell treated in an approximate way (4).When the system is further complicated by an uncollimated /3 radiation with a coi~tinuous energy spectrum, a theoretical analysis is very difficult. Consequently the absorptioil and scattering of /3 radiation have only been described a ians. empirically, principally with counting geometries of less than 29 ster d'T h e absorption process, of interest both as a source of error in disintegrationrate measurements and as an energy determination method, has been the subject of a volumii~ous literature (6,17,19,20,21,27,29,41,42 For personal use only.