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| author | Mitja Felicijan <mitja.felicijan@gmail.com> | 2024-06-19 22:13:49 +0200 |
|---|---|---|
| committer | Mitja Felicijan <mitja.felicijan@gmail.com> | 2024-06-19 22:13:49 +0200 |
| commit | c616d4e3c3a3abfcfeb5e9d96ddfbf7d3111603a (patch) | |
| tree | 236d658af6f97a56c20848f6f5994c135fca1316 /c-embed/test.txt | |
| download | probe-c616d4e3c3a3abfcfeb5e9d96ddfbf7d3111603a.tar.gz | |
Engage!
Diffstat (limited to 'c-embed/test.txt')
| -rw-r--r-- | c-embed/test.txt | 8 |
1 files changed, 8 insertions, 0 deletions
diff --git a/c-embed/test.txt b/c-embed/test.txt new file mode 100644 index 0000000..a3cac17 --- /dev/null +++ b/c-embed/test.txt @@ -0,0 +1,8 @@ +The first rule is typical of quantum physics. It results from the postulate of +unitary evolution. The second rule is a classical rule of the addition of +probabilities. It results from decoherence through observation. When +intermediate states are observed, the observed system is represented by a +mixture of states. The classical rule of addition of probabilities must then be +applied. Entanglement by observation thus explains Feynman's second rule. This +explains the Feynman Rules for calculating probabilities in quantum physics +(Feynman 1966). |
