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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 />
<br />
Γ K 0 <br />
anything +Γ KK 0 <br />
Γ K 0<br />
anything +Γ KK 0<br />
anything anything /Γtotal /Γtotal /Γtotal /Γtotal<br />
Γ4/Γ<br />
VALUE EVTS DOCUMENT ID TECN COMMENT<br />
0.42 ±0.05 ±0.05 OUR AVERAGE<br />
0.455±0.050±0.032 COFFMAN 91 MRK3 e + e− 3.77 GeV<br />
0.29 ±0.11 13 SCHINDLER 81 MRK2 e + e− 3.771 GeV<br />
0.57 ±0.26 6 VUILLEMIN 78 MRK1 e + e− 3.772 GeV<br />
Γ K + anything Γ /Γtotal<br />
K + anything Γ /Γtotal<br />
K + anything Γ /Γtotal<br />
K + anything /Γtotal<br />
VALUE EVTS DOCUMENT ID TECN COMMENT<br />
0.034 +0.006<br />
−0.004<br />
OUR AVERAGE<br />
0.034+0.006<br />
−0.004<br />
OUR AVERAGE<br />
0.034+0.006<br />
−0.004<br />
OUR AVERAGE<br />
0.034+0.006<br />
−0.004<br />
OUR AVERAGE<br />
0.034 +0.007<br />
−0.005<br />
15 BARLAG 92C ACCM π− Cu 230 GeV<br />
0.028±0.009±0.004 COFFMAN 91 MRK3 e + e− 3.77 GeV<br />
0.03 +0.05<br />
−0.02<br />
AGUILAR-... 87E HYBR π p, pp 360, 400 GeV<br />
0.08 ±0.03 25 SCHINDLER 81 MRK2 e + e− 3.771 GeV<br />
15 BARLAG 92C computes the branching fraction using topological normalization.<br />
Γ5/Γ Γ5/Γ<br />
Semileptonic Semileptonic modes<br />
Γ K − ℓ + <br />
Γ νℓ /Γtotal Γ7/Γ<br />
K − ℓ + <br />
Γ νℓ /Γtotal Γ7/Γ<br />
K − ℓ + <br />
Γ νℓ /Γtotal Γ7/Γ<br />
K − ℓ + <br />
νℓ /Γtotal Γ7/Γ<br />
We average our K− e + νe and K− µ + ν µ branching fractions, after multiplying the<br />
latter by a phase-space factor of 1.03 to be able to use it with the K− e + νe fraction.<br />
Hence our ℓ + here is really an e + .<br />
VALUE DOCUMENT ID COMMENT<br />
0.0350±0.0017 OUR OUR AVERAGE Error includes scale factor of 1.3.<br />
0.0366±0.0018 PDG 98 Our Γ(K− e + 0.0333±0.0018 PDG 98<br />
νe )/Γtotal 1.03 × our Γ(K − µ + ν µ )/Γtotal Γ K − e + <br />
Γ νe /Γtotal Γ8/Γ<br />
K − e + <br />
Γ νe /Γtotal Γ8/Γ<br />
K − e + <br />
Γ νe /Γtotal Γ8/Γ<br />
K − e + <br />
νe /Γtotal Γ8/Γ<br />
VALUE EVTS DOCUMENT ID TECN COMMENT<br />
0.0366±0.0018 OUR OUR FIT<br />
0.034 0.034 ±0.005 ±0.005 ±0.004<br />
±0.004 55 ADLER 89 MRK3 e + e− 3.77 GeV<br />
Γ K − e + <br />
νe /Γ K − π + <br />
Γ K − e + <br />
νe /Γ K − π + <br />
Γ K − e + <br />
νe /Γ K − π + <br />
Γ K − e + <br />
νe /Γ K − π + <br />
Γ8/Γ19 Γ8/Γ19 Γ8/Γ19 Γ8/Γ19<br />
VALUE EVTS DOCUMENT ID TECN COMMENT<br />
0.95 ±0.04 ±0.04 OUR FIT<br />
0.95 ±0.04 ±0.04 OUR AVERAGE<br />
0.978±0.027±0.044 2510 16 BEAN 93C CLE2 e + e− ≈ Υ(4S)<br />
0.90 ±0.06 ±0.06<br />
0.91 ±0.07 ±0.11<br />
584<br />
250<br />
17 CRAWFORD<br />
18 ANJOS<br />
91B CLEO<br />
89F E691<br />
e + e− ≈ 10.5 GeV<br />
Photoproduction<br />
16 BEAN 93C uses K− µ + νµ as well as K− e + νe events and makes a small phase-space<br />
adjustment to the number of the µ + events to use them as e + events. A pole mass of<br />
2.00 ± 0.12 ± 0.18 GeV/c2 is obtained from the q2 dependence of the decay rate.<br />
17 CRAWFORD 91B uses K− e + νe and K− µ + ν µ candidates to measure a pole mass of<br />
2.1 +0.4<br />
−0.2 +0.3<br />
−0.2 GeV/c2 from the q2 dependence of the decay rate.<br />
18 ANJOS 89F measures a pole mass of 2.1<br />
+0.4<br />
−0.2 ± 0.2GeV/c2from the q2 dependence<br />
of the decay rate.<br />
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