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Bell inequality violations under reasonable and under weak hypotheses

机译:在合理和弱假设下违反贝尔不平等

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摘要

Given a sequence of pairs of spin-one half particles in the singlet state,assume that Alice measures the normalized projections along some vector of thespins of one vector per pair along that vector while Bob measures thenormalized projections along some vector of the spins of the other member ofeach pair. Then Quantum Mechanics, or QM, lets one evaluate the correlation ofthe projections along these two vectors as minus the cosinus of the anglebetween said vectors; we assume that all vectors are chosen in a fixed plane.Assuming Classical Microscopic Realism, or CMR, there exist also normalizedprojection pairs of the spins of the pairs of particles along some other pairof vectors. Assuming QM and MR, we also have that the correlations of theprojections along the other vectors as minus the cosinus of the angle betweenthe extra vectors. Assuming Locality,i.e., the impossibility of any effect ofan event on another event when said events are spatially separated, beside QMand MR, the theory of Bell lets one deduce various violations of someinequalities at some choices of quadruplets of the vectors that have beenchosen. Our main result is the existence of quadruplets where at least one ofthe said inequalities is violated if one only assumes QM, MR and some very mildfurther hypotheses. These weak hypotheses only concern the behavior ofcorrelations that we use near special quadruplets. We thus get versions ofBell's theorem that are strictly stronger than the original one and inparticular do not assume Locality.
机译:给定一系列成对的单峰状态的自旋半粒子对,假设Alice沿着该向量测量一对向量中每个向量的自旋的某个向量的归​​一化投影,而Bob沿着另一个向量的自旋的某个向量测量归一化的投影每对成员。然后,量子力学(QM)让我们评估沿着这两个向量的投影的相关性,以减去所述向量之间的夹角余弦。我们假设所有向量都是在固定平面上选择的。假设经典微观现实主义(CMR),沿着另一些向量对还存在粒子对自旋的归一化投影对。假设QM和MR,我们还具有沿着其他矢量的投影的相关性,即减去额外矢量之间的角度的余弦值。假设局部性,即当事件在空间上分离时,事件对另一事件的任何影响都是不可能的,除了QM和MR之外,贝尔理论还允许人们推论选择了矢量的四联体的某些选择时对某些不等式的各种违反。我们的主要结果是存在四元组,如果仅假设QM,MR和一些非常温和的假设,则至少会违反上述不等式之一。这些弱假设仅涉及我们在特殊四联体附近使用的相关行为。因此,我们得到的贝尔定理的版本严格地强于原始定理,尤其是不假定局部性。

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