${{\mathit D}_{{2}}^{*}{(2460)}}$0 MASS

INSPIRE   PDGID:
M119M
The fit includes ${{\mathit D}^{\pm}}$, ${{\mathit D}^{0}}$, ${{\mathit D}_{{s}}^{\pm}}$, ${{\mathit D}^{*\pm}}$, ${{\mathit D}^{*0}}$, ${{\mathit D}_{{s}}^{*\pm}}$, ${{\mathit D}_{{1}}{(2420)}^{0}}$, ${{\mathit D}_{{2}}^{*}{(2460)}^{0}}$, and ${{\mathit D}_{{s1}}{(2536)}^{\pm}}$ mass and mass difference measurements.
VALUE (MeV) EVTS DOCUMENT ID TECN  COMMENT
$\bf{ 2460.58 \pm0.34}$ OUR AVERAGE  Error includes scale factor of 2.5.  See the ideogram below.
$2463.7$ $\pm0.4$ $\pm0.7$ 28k 1
AAIJ
2016AH
LHCB ${{\mathit B}^{-}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{-}}$
$2464.0$ $\pm1.4$ $\pm0.5$ 2k 2
AAIJ
2015V
LHCB ${{\mathit B}^{-}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{-}}$
$2460.4$ $\pm0.4$ $\pm1.2$ 82k
AAIJ
2013CC
LHCB ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit D}^{*+}}{{\mathit \pi}^{-}}{{\mathit X}}$
$2460.4$ $\pm0.1$ $\pm0.1$ 675k
AAIJ
2013CC
LHCB ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}{{\mathit X}}$
$2462.5$ $\pm2.4$ ${}^{+1.3}_{-1.1}$ 2.3k 3
ABRAMOWICZ
2013
ZEUS ${{\mathit e}^{\pm}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit D}^{(*)+}}{{\mathit \pi}^{-}}{{\mathit X}}$
$2462.2$ $\pm0.1$ $\pm0.8$ 243k
DEL-AMO-SANCH..
2010P
BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}{{\mathit X}}$
$2460.4$ $\pm1.2$ $\pm2.2$ 3.4k
AUBERT
2009AB
BABR ${{\mathit B}^{-}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{-}}$
$2461.6$ $\pm2.1$ $\pm3.3$ 4
ABE
2004D
BELL ${{\mathit B}^{-}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{-}}$
$2464.5$ $\pm1.1$ $\pm1.9$ 5.8k 4
LINK
2004A
FOCS ${{\mathit \gamma}}$ A
$2465$ $\pm3$ $\pm3$ 486
AVERY
1994C
CLE2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}$ X
$2453$ $\pm3$ $\pm2$ 128
FRABETTI
1994B
E687 ${{\mathit \gamma}}$ ${}^{}\mathrm {Be}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}$ X
$2461$ $\pm3$ $\pm1$ 440
AVERY
1990
CLEO ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit D}^{*+}}{{\mathit \pi}^{-}}$ X
$2455$ $\pm3$ $\pm5$ 337
ALBRECHT
1989B
ARG ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}$ X
$2459$ $\pm3$ $\pm2$ 153
ANJOS
1989C
TPS ${{\mathit \gamma}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}$ X
• • We do not use the following data for averages, fits, limits, etc. • •
$2469.1$ $\pm3.7$ ${}^{+1.2}_{-1.3}$ 1.5k 5
CHEKANOV
2009
ZEUS ${{\mathit e}^{\pm}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit D}^{(*)+}}{{\mathit \pi}^{-}}{{\mathit X}}$
$2463.3$ $\pm0.6$ $\pm0.8$ 20k
ABULENCIA
2006A
CDF 1900 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}{{\mathit X}}$
$2461$ $\pm6$ 126 6
ABREU
1998M
DLPH ${{\mathit e}^{+}}{{\mathit e}^{-}}$
$2466$ $\pm7$ 1
ASRATYAN
1995
BEBC 53,40 ${{\mathit \nu}}$ ${{\overline{\mathit \nu}}}$ $\rightarrow$ ${{\mathit p}}{{\mathit X}}$ , ${{\mathit d}}{{\mathit X}}$
1  From the amplitude analysis in the model describing the ${{\mathit D}^{+}}{{\mathit \pi}^{-}}$ wave together with virtual contributions from the ${{\mathit D}^{*}{(2007)}^{0}}$ and ${{\mathit B}^{*0}}$ states, and components corresponding to the ${{\mathit D}_{{2}}^{*}{(2460)}^{0}}$, ${{\mathit D}_{{1}}^{*}{(2680)}^{0}}$, ${{\mathit D}_{{3}}^{*}{(2760)}^{0}}$, and ${{\mathit D}_{{2}}^{*}{(3000)}^{0}}$ resonances.
2  From the amplitude analysis in the model describing the ${{\mathit D}^{+}}{{\mathit \pi}^{-}}$ wave together with virtual contributions from the ${{\mathit D}^{*}{(2007)}^{0}}$ and ${{\mathit B}^{*0}}$ states, nonresonant spin-0 and spin-1 components as well as the ${{\mathit D}_{{0}}^{*}{(2400)}^{0}}$, ${{\mathit D}_{{2}}^{*}{(2460)}^{0}}$ and ${{\mathit D}_{{1}}^{*}{(2760)}^{0}}$ resonances.
3  From the combined fit of the ${{\mathit M}}$( ${{\mathit D}^{+}}{{\mathit \pi}^{-}}$ ) and ${{\mathit M}}$( ${{\mathit D}^{*+}}{{\mathit \pi}^{-}}$ ) distributions. and A$_{{{\mathit D}_{{2}}}}$ fixed to the theoretical prediction of $-1$.
4  Fit includes the contribution from ${{\mathit D}_{{0}}^{*}{(2400)}^{0}}$.
5  Calculated using the mass difference $\mathit m({{\mathit D}_{{2}}^{*0}}$) $−$ $\mathit m({{\mathit D}^{*+}})_{PDG}$ reported below and $\mathit m({{\mathit D}^{*+}})_{PDG}$ = $2010.27$ $\pm0.17$ MeV. The 0.17 MeV uncertainty of the PDG mass value should be added to the experimental uncertainty of ${}^{+1.2}_{-1.3}$ MeV.
6  No systematic error given.

           ${{\mathit D}_{{2}}^{*}{(2460)}^{0}}$ mass (MeV)
References:
AAIJ 2016AH
PR D94 072001 Amplitude analysis of ${{\mathit B}^{-}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{-}}$ Decays
AAIJ 2015V
PR D91 092002 First Observation and Amplitude Analysis of the ${{\mathit B}^{-}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{-}}$ Decay
Also
PR D93 119901 (errat.) Erratum to AAIJ 2015V: First Observation and Amplitude Analysis of the ${{\mathit B}^{-}}$ $\rightarrow$ ${{\mathit D}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{-}}$ Decay
AAIJ 2013CC
JHEP 1309 145 Study of ${{\mathit D}_{{J}}}$ Meson Decays to ${{\mathit D}^{+}}{{\mathit \pi}^{-}}$, ${{\mathit D}^{0}}{{\mathit \pi}^{+}}$ and ${{\mathit D}^{*+}}{{\mathit \pi}^{-}}$ Final States in ${{\mathit p}}{{\mathit p}}$ Collisions
ABRAMOWICZ 2013
NP B866 229 Production of the Excited Charm Mesons ${{\mathit D}_{{1}}}$ and ${{\mathit D}_{{2}}^{*}}$ at HERA
DEL-AMO-SANCHEZ 2010P
PR D82 111101 Observation of New Resonances Decaying to ${{\mathit D}}{{\mathit \pi}}$ and ${{\mathit D}^{*}}{{\mathit \pi}}$ in Inclusive ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Collisions near $\sqrt {s }$ = 10.58 GeV
AUBERT 2009AB
PR D79 112004 Dalitz Plot Analysis of
CHEKANOV 2009
EPJ C60 25 Production of Excited Charm and Charm-Strange Mesons at HERA
ABULENCIA 2006A
PR D73 051104 Measurement of Mass and Width of the Excited Charmed Meson States ${{\mathit D}_{{1}}^{0}}$ and ${{\mathit D}_{{2}}^{*0}}$ at CDF
ABE 2004D
PR D69 112002 Study of ${{\mathit B}^{-}}$ $\rightarrow$ ${{\mathit D}^{**0}}{{\mathit \pi}^{-}}$ ( ${{\mathit D}^{**0}}$ $\rightarrow$ ${{\mathit D}}{}^{(*)+}$ ${{\mathit \pi}^{-}}$ ) Decays
LINK 2004A
PL B586 11 Measurement of Masses and Widths of Excited Charm Mesons ${{\mathit D}_{{2}}^{*}}$ and Evidence for Broad States
ABREU 1998M
PL B426 231 First Evidence for a Charm Radial Excitation, ${{\mathit D}^{*'}}$
ASRATYAN 1995
ZPHY C68 43 Study of ${{\mathit D}^{*+}}$ and Search for ${{\mathit D}^{**0}}$ Production by Neutrinos in BEBC
AVERY 1994C
PL B331 236 Production and Decay of ${{\mathit D}_{{1}}{(2420)}^{0}}$ and ${{\mathit D}_{{2}}^{*}{(2460)}^{0}}$
FRABETTI 1994B
PRL 72 324 Measurement of the Masses and Widths of $\mathit L$ = 1 Charm Mesons
AVERY 1990
PR D41 774 P-wave Charmed Mesons in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Annihilation
ALBRECHT 1989B
PL B221 422 Observation of ${{\mathit D}^{*}{(2459)}^{0}}$ in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Annihilation
ANJOS 1989C
PRL 62 1717 Observation of Excited Charmed Mesons