- #1
Heidi
- 418
- 40
Happy new year to all the forumers.
The Wigner's friend paradox appeared in the early years of quantum mechanics:
Wigner knows that his friend looked inside the box to see if the cat is dead or alive.
He has two cells in his mind to put what his friend saw.
As he ignores the result, he may assign a probability to each cell or he may see "friend + cat" as a quantum system and assigne amplitudes which have to be summed.
Then theorists invented a "cut". Macroscopic devices are classical and particles obey to quantum mechanics rules.
They also said that quantum systems evolve unitarily but that when measured by a
macroscopic device there are random non unitary projections.
We often read now that all systems are in a quantum state (or with a given density matrix)
There is also a purification theorem which allows to add degrees of freedom to get a greater pure state from a decohered one. What Bob and Alice see are given by partial trace on a pure state.
We are also used to assign amplitudes do Feynman diagrams not probabilities.
And when one tried to add probability to describe quantum experiments it gave
Bell inequalities.
So i wonder if the "Wigner's friend paradox" will not be as "the age of the twins paradox"
The Wigner's friend paradox appeared in the early years of quantum mechanics:
Wigner knows that his friend looked inside the box to see if the cat is dead or alive.
He has two cells in his mind to put what his friend saw.
As he ignores the result, he may assign a probability to each cell or he may see "friend + cat" as a quantum system and assigne amplitudes which have to be summed.
Then theorists invented a "cut". Macroscopic devices are classical and particles obey to quantum mechanics rules.
They also said that quantum systems evolve unitarily but that when measured by a
macroscopic device there are random non unitary projections.
We often read now that all systems are in a quantum state (or with a given density matrix)
There is also a purification theorem which allows to add degrees of freedom to get a greater pure state from a decohered one. What Bob and Alice see are given by partial trace on a pure state.
We are also used to assign amplitudes do Feynman diagrams not probabilities.
And when one tried to add probability to describe quantum experiments it gave
Bell inequalities.
So i wonder if the "Wigner's friend paradox" will not be as "the age of the twins paradox"