ar X iv : 1 61 1 . 01 70 0 v 1 [ he p - ph ] 5 N ov 2 01 6 WW + jet at 14 and 100 TeV

ar X iv : 1 51 1 . 02 99 6 v 1 [ he p - th ] 1 0 N ov 2 01 5 When is an area law not an area law ?

Entanglement entropy is typically proportional to area, but sometimes it acquires an additional logarithmic pre-factor. We offer some intuitive explanations for these facts.

ar X iv : 1 61 1 . 00 87 9 v 1 [ m at h - ph ] 3 N ov 2 01 6 Stable laws for chaotic billiards with cusps at flat points ∗ PAUL

We consider billiards with a single cusp where the walls meeting at the vertex of the cusp have zero one-sided curvature, thus forming a flat point at the vertex. For Hölder continuous observables, we show that properly normalized Birkoff sums, with respect to the billiard map, converge in law to a totally skewed α-stable law.

ar X iv : 1 61 1 . 01 72 8 v 1 [ nu cl - e x ] 6 N ov 2 01 6 Jets and high - p T probes measured in the STAR experiment

Hard probes created through large momentum transfers are used to study the properties of QCD matter created in heavy-ion collisions, by comparing the measurements to those in p+p collisions. Jets, and the "quenching" or suppression of jets in the medium created in heavy-ion collisions, are studied through various different observables. We present the most recent measurements from √ sNN = 200 Ge...

ar X iv : h ep - e x / 97 11 01 6 v 1 2 1 N ov 1 99 7 Results on Λ 0 Production at HERMES

The production of Λ 0 's at the HERMES experiment is presented. Prospects for the future of Λ measurements at HERMES are discussed.

ar X iv : 1 11 1 . 37 97 v 1 [ qu an t - ph ] 1 6 N ov 2 01 1 Prony ’ s method and the connected – moments expansion