an observation of large CP-violation in the neutral B meson system[7] measurement of the branching fraction of inclusive B → X s γ {\displaystyle B\to X_{s}\gamma } decays[8] observation of the b → s l + l − {\displaystyle b\to sl^{+}l^{-}} transition with B → K l + l − {\displaystyle B\to Kl^{+}l^{-}} [9] and B → K ∗ l + l − {\displaystyle B\to K^{*}l^{+}l^{-}} [10] measurement of ϕ 3 {\displaystyle \phi _{3}} using the B → D K , D → K S π + π − {\displaystyle B\to DK,D\to K_{S}\pi ^{+}\pi ^{-}} Dalitz plot[5] measurement of the CKM quark mixing matrix elements | V u b | {\displaystyle |V_{ub}|} and | V c b | {\displaystyle |V_{cb}|} [1] observation of direct CP-violation in B 0 → π + π − {\displaystyle B^{0}\to \pi ^{+}\pi ^{-}} [11] and B 0 → K − π + {\displaystyle B^{0}\to K^{-}\pi ^{+}} [12] observation of b → d {\displaystyle b\to d} transitions[13] evidence for B → τ ν {\displaystyle B\to \tau \nu } [14] observations of a number of new particles including the X(3872)[15]