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Citation: J. Beringer et al. (Particle Data Group), PR D86, 010001 (2012) (URL: http://pdg.lbl.gov)
I (J P ) = 0(?? )
D ∗s2 (2573)
J P is natural, width and decay modes consistent with 2+ .
D ∗s2 (2573) MASS VALUE (MeV)
EVTS
DOCUMENT ID
2571.9± 0.8 OUR AVERAGE 2569.4± 1.6 ± 0.5 82 ± 17
AAIJ
2572.2± 0.3 ± 1.0 2574.5± 3.3 ± 1.6 + 1.7 ± 0.9 2573.2 − 217 1.6 • • • We do not use the following
AUBERT,BE ALBRECHT KUBOTA
TECN
COMMENT
11A LHCB Bs → D ∗ s2 (2573) µ ν X + − 06E BABR e e → D K X 96 ARG e+ e− → D0 K + X 94 CLE2 e + e − ∼ 10.5 GeV
data for averages, fits, limits, etc. • • • 1 EVDOKIMOV 04 SELX 600 Σ − A → D 0 K + X 2 HEISTER 02B ALEP e + e − → D 0 K + X
2570.0± 4.3 25 2568.6± 3.2 64 1 Not independent of the mass difference below. 2 Calculated using m = 1864.5 ± 0.5 MeV and the mass difference below. D0
mD∗
(2573)
(2573) s2
VALUE (MeV)
EVTS
− mD 0
DOCUMENT ID
TECN
COMMENT
704 ± 3 ± 1 64 HEISTER 02B ALEP e + e − → D 0 K + X • • • We do not use the following data for averages, fits, limits, etc. • • • 3 EVDOKIMOV 04 SELX 600 Σ − A → D 0 K + X 705.4± 4.3 25 3 Systematic errors not estimated.
D ∗s2 (2573) WIDTH VALUE (MeV)
EVTS
DOCUMENT ID
TECN
COMMENT
17 ± 4 OUR AVERAGE Error includes scale factor of 1.3. See the ideogram below. 12.1± 4.5 ± 1.6 82 ± 17 AAIJ 11A LHCB Bs → D ∗ (2573) µ ν X s2 27.1± 0.6 ± 5.6 AUBERT,BE 06E BABR e + e − → D K X 10.4± 8.3 ± 3.0 ALBRECHT 96 ARG e+ e− → D0 K + X 5 217 KUBOTA 94 CLE2 e + e − ∼ 10.5 GeV 16 + −4 ±3 • • • We do not use the following data for averages, fits, limits, etc. • • • 9 14 + −6
25
HTTP://PDG.LBL.GOV
4 EVDOKIMOV 04
Page 1
SELX
600 Σ − A → D 0 K + X
Created: 6/18/2012 15:09
Citation: J. Beringer et al. (Particle Data Group), PR D86, 010001 (2012) (URL: http://pdg.lbl.gov)
4 Systematic errors not estimated. WEIGHTED AVERAGE 17±4 (Error scaled by 1.3)
χ AAIJ AUBERT,BE ALBRECHT KUBOTA
1.0 3.3 0.5 0.0 4.9 (Confidence Level = 0.182)
-20
0
20
40
60
11A 06E 96 94
2
LHCB BABR ARG CLE2
80
D ∗s2 (2573) WIDTH (MeV)
D ∗s2 (2573)+ DECAY MODES − D∗ s2 (2573) modes are charge conjugates of the modes below.
Γ1 Γ2
Mode
Fraction (Γi /Γ)
D0 K + D ∗ (2007)0 K +
seen not seen
D ∗s2 (2573)+ BRANCHING RATIOS ¡ ¢ Γ D 0 K + /Γtotal VALUE
