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PhD thesis: Non-contextual inequalities and dimensionality
  Thesis defense

Friday 05 June 2015
from 14:00 to 18:00
at FB42
Speaker : Johan Ahrens (Stockholm University, Department of Physics)
Abstract : Abstract This PhD-thesis is based on the ve experiments I have performed during my time as a PhD-student. Three experiments are implementations of non-contextual inequalities and two are implementations of witness functions for classical- and quantum dimensions of sets of states. A dimension witness is an operator function that produce a value when applied to a set of states. This value has di erent upper bounds depending on the dimension of the set of states and also depending on if the states are classical or quantum. Therefore a dimension witness can only give a lower bound on the dimension of the set of states. The rst dimension witness is based on the CHSH-inequality and has the ability of discriminating between classical and quantum sets of states of two and three dimensions, it can also indicate if a set of states must be of dimension four or higher. The second dimension witness is based on a set theoretical representation of the possible combinations of states and measurements and grows with the dimension of the set of states you want to be able to identify, on the other hand there is a formula for expanding it to arbitrary dimension. Non-contextual hidden variable models is a family of hidden variable models which include local hidden variable models, so in a sence non-contextual inequal- ities are a generalisation of Bell-inequalities. The experiments presented in this thesis all use single particle quantum systems. The rst experiment is a violation of the KCBS-inequality, this is the sim- plest correlation inequality which is violated by quantum mechanics. The second experiment is a violation of the Wright-inequality which is the simplest inequality violated by quantum mechanics, it contains only projectors and not correlations. The nal experiment of the thesis is an implementation of a Hardy-like equal- ity for non-contextuality, this means that the operators in the KCBS-inequality have been rotated so that one term in the sum will be zero for all non-contextual hidden variable models and we get a contradiction since quantum mechanics gives a non-zero value for all terms. Keywords: Quantum information, quantum optics, non-contextuality, dimen- sion witness. Johan Ahrens

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