Höchstfrequenztechnik

First ADS analysis ofB−→D0K−decays in hadron collisions

“…In the GLW method [6,9] the CP asymmetry of B − → D CP± K − is studied, where D is D 0 or D 0 and CP± are the CP even and odd eigenstates of the D: D CP + → K + K − , π + π − and D CP− → K 0 s π 0 , K 0 s φ , K 0 s ω. We can define four observables:…”

“…According to the final state of the D, we have the following methods GLW (Gronau-London-Wyler) method [6,9], which uses CP eigenstates of D 0 , as D 0 [7,10], which uses the doubly Cabibbo suppressed mode D 0 → K + π − and GGSZ (or Dalitz) method [8,10], which uses three body decays of D 0 , as D 0 → K 0 s π + π − . All mentioned methods require no tagging or time-dependent measurements, and many of them only involve charged particles in the final state.…”

Monte-Carlo analysis of measurement uncertainties for on-wafer thru-reflect-line calibrations

“…Subsequently, these scattering parameters are used as input data for the TRL algorithm, as described e.g. in [7]. The TRL algorithm computes the error terms necessary for correcting the raw device-under-test (DUT) measurements.…”

“…We focus on the Thru-Reflect-Line (TRL) procedure introduced in [6], and described in greater detail e.g. in [7]. For the execution of this procedure as a second-tier calibration three calibration standards (Thru, Reflect and Line) must be contacted with the probe tips.…”

The Super Flavor Factory

“…The anticipated precision on ∆S for η ′ K 0 is ∼ 0.015 with a data sample of 50 ab −1 . In addition to relying on theoretical calculations of the SM pollution to these decays [39,40,41], it is possible to experimentally constrain the SM pollution using SU(3) symmetry [42]. This requires precision knowledge of the branching fractions of the B meson decays to the following pseudo-scalar pseudo-scalar (P P ) final states π 0 π 0 , π 0 η, π 0 η ′ , ηη, η ′ η, η ′ η ′ [43,44].…”