Book contents
- Frontmatter
- Contents
- List of illustrations
- Preface
- Part I Perspectives on the 1927 Solvay conference
- Part II Quantum foundations and the 1927 Solvay conference
- Part III The proceedings of the 1927 Solvay conference
- 13 The intensity of X-ray reflection
- 14 Disagreements between experiment and the electromagnetic theory of radiation
- 15 The new dynamics of quanta
- 16 Quantum mechanics
- 17 Wave mechanics
- 18 General discussion of the new ideas presented
- Appendix
- Bibliography
- Index
18 - General discussion of the new ideas presented
Published online by Cambridge University Press: 05 March 2013
- Frontmatter
- Contents
- List of illustrations
- Preface
- Part I Perspectives on the 1927 Solvay conference
- Part II Quantum foundations and the 1927 Solvay conference
- Part III The proceedings of the 1927 Solvay conference
- 13 The intensity of X-ray reflection
- 14 Disagreements between experiment and the electromagnetic theory of radiation
- 15 The new dynamics of quanta
- 16 Quantum mechanics
- 17 Wave mechanics
- 18 General discussion of the new ideas presented
- Appendix
- Bibliography
- Index
Summary
Causality, determinism, probability
Mr Lorentz. – I should like to draw attention to the difficulties one encounters in the old theories. We wish to make a representation of the phenomena, to form an image of them in our minds. Until now, we have always wanted to form these images by means of the ordinary notions of time and space. These notions are perhaps innate; in any case, they have developed from our personal experience, by our daily observations. For me, these notions are clear and I confess that I should be unable to imagine physics without these notions. The image that I wish to form of phenomena must be absolutely sharp and definite, and it seems to me that we can form such an image only in the framework of space and time.
For me, an electron is a corpuscle that, at a given instant, is present at a definite point in space, and if I had the idea that at a following moment the corpuscle is present somewhere else, I must think of its trajectory, which is a line in space. And if the electron encounters an atom and penetrates it, and after several incidents leaves the atom, I make up a theory in which the electron preserves its individuality; that is to say, I imagine a line following which the electron passes through the atom. Obviously, such a theory may be very difficult to develop, but a priori it does not seem to me impossible.
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- Chapter
- Information
- Quantum Theory at the CrossroadsReconsidering the 1927 Solvay Conference, pp. 432 - 470Publisher: Cambridge University PressPrint publication year: 2009