ar X iv : 1 70 9 . 02 78 9 v 1 [ qu an t - ph ] 8 S ep 2 01 7 Magic State Distillation at Intermediate Size

ar X iv : 1 70 8 . 02 82 2 v 1 [ qu an t - ph ] 9 A ug 2 01 7 General implementation of arbitrary nonlinear quadrature phase gates

Petr Marek, ∗ Radim Filip, Hisashi Ogawa, Atsushi Sakaguchi, Shuntaro Takeda, Jun-ichi Yoshikawa, 3 and Akira Furusawa † Department of Optics, Palacký University, 17. listopadu 1192/12, 77146 Olomouc, Czech Republic Department of Applied Physics, School of Engineering, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan Quantum-Phase Electronics Center, School of Engineering,...

ar X iv : q - a lg / 9 70 90 01 v 1 1 S ep 1 99 7 Bilinear identity for q - hypergeometric integrals

ar X iv : 0 90 9 . 02 95 v 2 [ qu an t - ph ] 8 S ep 2 00 9 1 Quantum weak values are not unique What do they actually measure ?

Precise definitions of “weak [quantum] measurements” and “weak value” [of a quantum observable] are offered, which seem to capture the meaning of the often vague ways that these terms are used in the literature. Simple finite dimensional examples are given showing that weak values are not unique. They therefore cannot correspond to any physical attribute of the system being “weakly” measured, c...

ar X iv : h ep - e x / 01 12 02 6 v 1 1 9 D ec 2 00 1 Results on CP Violation from Belle

I describe the recent measurement of the CP violating parameter sin 2φ 1 = (0.99 ± 0.14 ± 0.05) from the Belle experiment at KEK.

ar X iv : 0 90 9 . 02 95 v 1 [ qu an t - ph ] 2 S ep 2 00 9 1 Quantum weak values are not unique What do they actually measure ?

Precise definitions of “weak [quantum] measurements” and “weak value” [of a quantum observable] are offered, which seem to capture the meaning of the often vague ways that these terms are used in the literature. Simple finite dimensional examples are given showing that weak values are not unique. They therefore cannot correspond to any physical attribute of the system being “weakly” measured, c...