1927
DOI: 10.1017/s0305004100013815
|View full text |Cite
|
Sign up to set email alerts
|

The Amount of Energy Emitted in the γ-Ray Form by Radium E

Abstract: The β-ray type of disintegration is accompanied in general by two forms of radiation, the β-rays and the γ-rays. Radium E is noteworthy in that it gives a large amount of γ-radiation that it can only be detected by careful measurements. Yet, since it differs in this way from β-ray elements such as radium B and radium C, it is important for theoretical discussion that we should obtain as much knowledge as possible about this small amount of γ-radiation.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

0
4
0

Year Published

1959
1959
2023
2023

Publication Types

Select...
4
4

Relationship

0
8

Authors

Journals

citations
Cited by 33 publications
(4 citation statements)
references
References 4 publications
0
4
0
Order By: Relevance
“…The IB process has a probability per electron emission of approximately α, the fine-structure constant (Struzynski and Pollock [16], Evans [8] ). The existence of this case has been observed by Aston [17]. When the probability is taken into account, the shape of the IB distribution remains the same.…”
Section: Monte Carlo Simulationmentioning
confidence: 57%
“…The IB process has a probability per electron emission of approximately α, the fine-structure constant (Struzynski and Pollock [16], Evans [8] ). The existence of this case has been observed by Aston [17]. When the probability is taken into account, the shape of the IB distribution remains the same.…”
Section: Monte Carlo Simulationmentioning
confidence: 57%
“…This mechanism was first reported by Aston (1927). Subsequently, many theories have been developed to study this process in which the radiation arises from the emission of a b-particle and its energy loss as it leaves the nucleus.…”
Section: Introductionmentioning
confidence: 97%
“…IB is a low intensity, continuous electromagnetic radiation that is emitted within the transforming atom due to change in nuclear charge by orbital electron capture or beta particle emission, whereas EB is a continuous electromagnetic radiation existing due to the deflection of charged particles (in general) in the Coulomb field of the nucleus of a medium (stopping material), and this EB process occurs in thick target materials [10]. For the first time, Aston [11] observed the emission of IB radiation during beta decay. The quantum theory for IB, without considering the Coulomb effects for allowed beta transitions, was developed by Knipp and Uhlenbeck [12] and Bloch [13].…”
Section: Introduction mentioning
confidence: 99%