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Review of <strong>Particle</strong> Physics: C. Caso et al. (<strong>Particle</strong> <strong>Data</strong> <strong>Group</strong>), European Physical Journal C3, 1 (1998)<br />
Γ K − π + Γ /Γtotal<br />
K − π + Γ /Γtotal<br />
K − π + Γ /Γtotal<br />
K − π + /Γtotal<br />
Hadronic modes modes with a a aa K K or or KKKK KKKK K K<br />
Γ19/Γ Γ19/Γ<br />
VALUE<br />
0.0385±0.0009 OUR OUR FIT<br />
EVTS DOCUMENT ID TECN COMMENT<br />
0.0388±0.0009 OUR OUR AVERAGE<br />
0.0381±0.0015±0.0016<br />
0.0390±0.0009±0.0012 5392<br />
31 ARTUSO<br />
31 BARATE<br />
98 CLE2<br />
97C ALEP<br />
e + e− ≈ Υ(4S)<br />
From Z decays<br />
0.045 ±0.006 ±0.004 32 ALBRECHT 94 ARG e + e− ≈ Υ(4S)<br />
0.0341±0.0012±0.0028<br />
0.0395±0.0008±0.0017<br />
1173 31 ALBRECHT<br />
4208<br />
94F ARG e + e− ≈ Υ(4S)<br />
31,33 AKERIB 93 CLE2 e + e− 0.0362±0.0034±0.0044 31 DECAMP 91J ALEP<br />
≈ Υ(4S)<br />
From Z decays<br />
0.045 ±0.008 ±0.005<br />
0.042 ±0.004 ±0.004<br />
56<br />
930<br />
31 ABACHI<br />
ADLER<br />
88 HRS<br />
88C MRK3<br />
e + e− 29 GeV<br />
e + e− 3.77 GeV<br />
0.041 ±0.006 263 34 SCHINDLER 81 MRK2 e + e− 3.771 GeV<br />
0.043 ±0.010 130 35 PERUZZI 77 MRK1 e + e− 3.77 GeV<br />
31 ABACHI 88, DECAMP 91J, AKERIB 93, ALBRECHT 94F, BARATE 97C, and AR-<br />
TUSO 98 use D∗ (2010) + → <strong>D0</strong> π + decays. The π + is both slow and of low pT with<br />
respect to the event thrust axis or nearest jet (≈ D∗+ direction). The excess number<br />
of such π + ’s over background gives the number of D∗ (2010) + → <strong>D0</strong> π + events, and<br />
the fraction with <strong>D0</strong> → K− π + gives the <strong>D0</strong> → K− π + branching fraction.<br />
32 ALBRECHT 94 uses <strong>D0</strong> mesons from B0 → D∗+ ℓ− νℓ decays. This is a different set<br />
of events than used by ALBRECHT 94F.<br />
33 This AKERIB 93 value includes radiative corrections; without them the value is 0.0391 ±<br />
0.0008 ± 0.0017.<br />
34 SCHINDLER 81 (MARK-2) measures σ(e + e− → ψ(3770)) × branching fraction to be<br />
0.24 ± 0.02 nb. We use the MARK-3 (ADLER 88C) valueofσ=5.8±0.5±0.6nb. 35 PERUZZI 77 (MARK-1) measures σ(e + e− → ψ(3770)) × branching fraction to be<br />
0.25 ± 0.05 nb. We use the MARK-3 (ADLER 88C) valueofσ=5.8±0.5±0.6nb. Γ K 0 π0 /Γ K − π +<br />
Γ K 0 π0 /Γ K − π +<br />
Γ K 0 π0 /Γ K − π +<br />
Γ K 0 π0 /Γ K − π +<br />
VALUE EVTS DOCUMENT ID TECN COMMENT<br />
0.55±0.06 OUR FIT FIT Error includes scale factor of 1.1.<br />
1.36±0.23±0.22 119 ANJOS 92B E691 γ Be 80–240 GeV<br />
Γ K 0 π0 /Γ K 0 π + π− Γ K 0 π0 /Γ K 0 π + π− Γ K 0 π0 /Γ K 0 π + π− Γ K 0 π0 /Γ K 0 π + π− Γ20/Γ19 Γ20/Γ19 Γ20/Γ19 Γ20/Γ19<br />
Γ20/Γ21 Γ20/Γ21 Γ20/Γ21 Γ20/Γ21<br />
VALUE<br />
0.390±0.031 0.390±0.031 OUR FIT<br />
EVTS DOCUMENT ID TECN COMMENT<br />
0.378±0.033 0.378±0.033 OUR AVERAGE<br />
0.44 ±0.02 ±0.05 1942 PROCARIO 93B CLE2 e + e− 10.36–10.7 GeV<br />
0.34 ±0.04 ±0.02 92 36 ALBRECHT 92P ARG e + e− ≈ 10 GeV<br />
0.36 ±0.04 ±0.08 104 KINOSHITA 91 CLEO e + e− ∼ 10.7 GeV<br />
36 This value is calculated from numbers in Table 1 of ALBRECHT 92P.<br />
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