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Physics World

The puzzles of daily life

Published Dec 1, 2012• 0 citations
Publisher

Abstract

We all know that everyday physical intuition is essentially useless for predicting the workings of the quantum-mechanical world.
DOI
10.1088/2058-7058/25/12/48

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Modern physical theories are deterministic in the sense that once we know the current state of the world, we can, in principle, predict all the future states. This was true for classical (pre-quantum) theories, this is true for modern quantum physics. On the other hand, we all know that we can make decision that change the state of the world -- even if, for most of us, a little bit. This intuitive idea of free will permeates all our life, all our activities -- and it seems to contradict the determinism of modern physics. It is therefore desirable to incorporate the idea of free will into physical theories. In this paper, we show that in quantum physics, free will leads to nonconservation of energy. This nonconservation is a microscopic purely quantum effect, but it needs to be taken into account in future free-will quantum theories.
As we are accustomed to everyday life, we may find quantum phenomena to be strange. If quantum phenomena were to happen often in our macroscopic world, we would react as if we had seen a ghost. A person to whom we were talking could move to another seat out of our sight in a moment, or his/her face could change. We might question if we are who we are. Fortunately experiencing quantum phenomena in everyday life is extremely hard. However, interestingly, quantum physics predicts that quantum phenomena can occur in the macroscopic world, regardless of our everyday experience. If that prediction is correct, why is experiencing quantum phenomena hard? Such a seemingly contradictory discussion was clearly raised by Schrodinger in his thought experiment, the so-called ‘Schrodinger cat paradox.’ Haroche’s group and Wineland’s group have independently performed experiments on the paradox. In this article, I discuss the historical background and the physical implications of the Schrodinger cat paradox.
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