#### ${{\mathit \phi}{(1020)}}$ MASS

VALUE (MeV) EVTS DOCUMENT ID TECN  COMMENT
 $\bf{ 1019.461 \pm0.016}$ OUR AVERAGE
$1019.463$ $\pm0.061$ 2.3M 1
 2018
CMD3 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ , ${{\mathit K}_S^0}$ ${{\mathit K}_L^0}$
$1019.462$ $\pm0.042$ $\pm0.056$ 28k 2
 2014 H
BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}_L^0}$ ${{\mathit \gamma}}$
$1019.51$ $\pm0.02$ $\pm0.05$ 3
 2013 Q
BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \gamma}}$
$1019.30$ $\pm0.02$ $\pm0.10$ 105k
 2006
CMD2 $0.98 - 1.06$ ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$
$1019.52$ $\pm0.05$ $\pm0.05$ 17.4k
 2005
CMD2 0.60-1.38 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \gamma}}$
$1019.483$ $\pm0.011$ $\pm0.025$ 272k 4
 2004
CMD2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}_L^0}$ ${{\mathit K}_S^0}$
$1019.42$ $\pm0.05$ 1900k 5
 2001 E
SND ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ , ${{\mathit K}_{{S}}}{{\mathit K}_{{L}}}$ , ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$
$1019.40$ $\pm0.04$ $\pm0.05$ 23k
 2001 B
CMD2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \gamma}}$
$1019.36$ $\pm0.12$ 6
 2000 B
SND ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \gamma}}$
$1019.38$ $\pm0.07$ $\pm0.08$ 2200 7
 1999 F
CMD2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{}\geq{}2{{\mathit \gamma}}$
$1019.51$ $\pm0.07$ $\pm0.10$ 11169
 1998
CMD2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$
$1019.5$ $\pm0.4$
 1998
OMEG 450 ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit p}}{{\mathit p}}$2 ${{\mathit K}^{+}}$2 ${{\mathit K}^{-}}$
$1019.42$ $\pm0.06$ 55600
 1995
CMD2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ hadrons
$1019.7$ $\pm0.3$ 2012
 1986
MPSF 400 ${{\mathit p}}$ ${}^{}\mathrm {A}$ $\rightarrow$ 4 ${{\mathit K}}$ X
$1019.7$ $\pm0.1$ $\pm0.1$ 5079
 1985 D
ARG 10 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ X
$1019.3$ $\pm0.1$ 1500
 1982
AEMS 11.8 polar. ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}}{{\mathit K}}$
$1019.67$ $\pm0.17$ 25080 8
 1982
RVUE
$1019.52$ $\pm0.13$ 3681
 1978 C
OLYA ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ hadrons
• • We do not use the following data for averages, fits, limits, etc. • •
$1018.4$ $\pm0.5$ $\pm0.1$ 9
 2020
CBAR 0.9 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{0}}$
$1019.21$ $\pm0.04$ $\pm0.03$ 10
 2020
RVUE ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \pi}^{0}}{{\mathit \gamma}}$
$1019.54$ $\pm0.10$ $\pm0.51$ 11
 2019 H
LHCB ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit D}^{\pm}}{{\mathit X}}$
$1019.20$ $\pm0.02$ $\pm0.01$ 12
 2019
RVUE ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$
$1019.469$ $\pm0.061$ 1.7M
 2018
CMD3 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$
$1019.457$ $\pm0.061$ 610k
 2016
CMD3 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}_L^0}$
$1019.48$ $\pm0.01$
 2013 F
BABR ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$
$1019.441$ $\pm0.008$ $\pm0.080$ 542k 13
 2008
CMD2 1.02 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$
$1019.63$ $\pm0.07$ 12540 14
 2005 J
BABR ${{\mathit D}^{0}}$ $\rightarrow$ ${{\overline{\mathit K}}^{0}}{{\mathit K}^{+}}{{\mathit K}^{-}}$
$1019.8$ $\pm0.7$
 1986
OMEG 85 ${{\mathit \pi}^{+}}$ /${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \pi}^{+}}$ /${{\mathit p}}$4 ${{\mathit K}}{{\mathit p}}$
$1020.1$ $\pm0.11$ 5526 14
 1986
OMEG 20$-$70 ${{\mathit \gamma}}{{\mathit p}}$
$1019.7$ $\pm1.0$
 1986
CLEO ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$1019.411$ $\pm0.008$ 642k 15
 1986
SPEC 100$-$200 ${{\mathit \pi}^{\pm}}$ , ${{\overline{\mathit p}}}$ , ${{\mathit p}}$ , ${{\mathit K}^{\pm}}$ , on ${}^{}\mathrm {Be}$
$1020.9$ $\pm0.2$ 14
 1986
OMEG 13 ${{\mathit K}^{+}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit K}^{+}}{{\mathit p}}$
$1021.0$ $\pm0.2$ 14
 1983 B
OMEG 18.5 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit K}^{+}}{{\mathit \Lambda}}$
$1020.0$ $\pm0.5$ 14
 1983 B
OMEG 18.5 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit K}^{+}}{{\mathit \Lambda}}$
$1019.7$ $\pm0.3$ 14
 1983
GOLI 190 ${{\mathit \pi}^{-}}$ ${}^{}\mathrm {Be}$ $\rightarrow$ 2 ${{\mathit \mu}}$ X
$1019.8$ $\pm0.2$ $\pm0.5$ 766
 1981
OLYA 1$-$1.4 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$
$1019.4$ $\pm0.5$ 337
 1978 B
HBC 0.7$-$0.8 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}_L^0}$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$
$1020$ $\pm1$ 383 14
 1977
CNTR 10 ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \pi}^{-}}{{\mathit \phi}}{{\mathit p}}$
$1018.9$ $\pm0.6$ 800
 1977
ASPK 6 ${{\mathit \pi}^{\pm}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit N}}$
$1019.7$ $\pm0.5$ 454
 1976
HBC 2.18 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \Lambda}}{{\mathit K}}{{\overline{\mathit K}}}$
$1019.4$ $\pm0.8$ 984
 1974
CNTR 2 ${{\mathit \gamma}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit p}}{{\mathit K}^{+}}{{\mathit K}^{-}}$
$1020.3$ $\pm0.4$ 100
 1973
HBC 2.8$-$9.3 ${{\mathit \gamma}}{{\mathit p}}$
$1019.4$ $\pm0.7$
 1973 B
CNTR ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit n}}$
$1019.6$ $\pm0.5$ 120 16
 1972 B
HBC 3.9,4.6 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \Lambda}}{{\mathit K}^{+}}{{\mathit K}^{-}}$
$1019.9$ $\pm0.5$ 100 16
 1972 B
HBC 3.9,4.6 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit p}}{{\mathit K}^{+}}{{\mathit K}^{-}}$
$1020.4$ $\pm0.5$ 131
 1972
HBC 10 ${{\mathit K}^{+}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit p}}{{\mathit \phi}}$
$1019.9$ $\pm0.3$ 410
 1971
HBC 2.9 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \Sigma}}$ ${{\mathit \Lambda}}$ ${{\mathit K}}{{\overline{\mathit K}}}$
 1 Average of KOZYREV 2016 and KOZYREV 2018 values taking into account the correlated uncertainties. Supersedes individual KOZYREV 2016 and KOZYREV 2018 results.
 2 Using a vector meson dominance model with contribution from ${{\mathit \phi}{(1020)}}$ and higher mass excitations of ${{\mathit \rho}{(770)}}$ , ${{\mathit \omega}{(782)}}$ , and ${{\mathit \phi}{(1020)}}$ .
 3 Using a phenomenological model based on KUHN 1990 with a sum of Breit-Wigner resonances for ${{\mathit \rho}{(770)}}$ , ${{\mathit \omega}{(782)}}$ , ${{\mathit \phi}{(1020)}}$ and their higher mass excitations.
 4 Update of AKHMETSHIN 1999D
 5 From the combined fit assuming that the total ${{\mathit \phi}{(1020)}}$ production cross section is saturated by those of ${{\mathit K}^{+}}{{\mathit K}^{-}}$ , ${{\mathit K}_{{S}}}{{\mathit K}_{{L}}}$ , ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ , and ${{\mathit \eta}}{{\mathit \gamma}}$ decays modes and using ACHASOV 2000B for the ${{\mathit \eta}}{{\mathit \gamma}}$ decay mode.
 6 Using a total width of $4.43$ $\pm0.05$ MeV. Systematic uncertainty included.
 7 Using a total width of $4.43$ $\pm0.05$ MeV.
 8 PELLINEN 1982 review includes AKERLOF 1977 , DAUM 1981 , BALDI 1977 , AYRES 1974 , DEGROOT 1974 .
 9 Width fixed at 4.2 MeV.
 10 The values were extracted from a dispersively improved Breit-Wigner parameterization and do not include vacuum polarization. Inclusion of vacuum polarization gives $1019.457$ $\pm0.020$ MeV.
 11 From the ${{\mathit D}^{\pm}}$ $\rightarrow$ ${{\mathit K}^{\pm}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ Dalitz plot fit with the Triple-M amplitude in the multimeson model of AOUDE 2018 .
 12 The values were extracted from a dispersively improved Breit-Wigner parameterization and do not include vacuum polarization.
 13 Strongly correlated with AKHMETSHIN 2004 .
 14 Systematic errors not evaluated.
 15 Weighted and scaled average of 12 measurements of DIJKSTRA 1986 .
 16 Mass errors enlarged by us to $\Gamma /\sqrt {\mathit N }$; see the note with the ${{\mathit K}^{*}{(892)}}$ mass.
References:
 ALBRECHT 2020
EPJ C80 453 Coupled channel analysis of ${\bar{p}p}\,\rightarrow \,\pi ^0\pi ^0\eta$, ${\pi ^0\eta \eta }$ and ${K^+K^-\pi ^0}$ at 900 MeV/c and of ${\pi \pi }$-scattering data
 HOID 2020
EPJ C80 988 Hadronic vacuum polarization and vector-meson resonance parameters from $e^+e^-\rightarrow \pi ^0\gamma$
 AAIJ 2019H
JHEP 1904 063 Dalitz plot analysis of the $D^+\to K^-K^+K^+$ decay
 HOFERICHTER 2019
JHEP 1908 137 Three-pion contribution to hadronic vacuum polarization
 KOZYREV 2018
PL B779 64 Study of the Process ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ in the Center-of-Mass Energy Range $1010 - 1060$ MeV with the CMD-3 Detector
 KOZYREV 2016
PL B760 314 Study of the Process ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}_L^0}$ in the Center-of-Mass Energy Range $1004 - 1060$ MeV with the CMD-3 Detector at the VEPP-2000 ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Collider
 LEES 2014H
PR D89 092002 Cross Sections for the Reactions ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}_L^0}$ , ${{\mathit K}_S^0}$ ${{\mathit K}_L^0}$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ , ${{\mathit K}_S^0}$ ${{\mathit K}_S^0}$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ , and ${{\mathit K}_S^0}$ ${{\mathit K}_S^0}$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ from Events with Initial-State Radiation
 LEES 2013Q
PR D88 032013 Precision Measurement of the ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$( ${{\mathit \gamma}}$) Cross Section with the Initial-State Radiation Method at BaBar
 LEES 2013F
PR D87 052010 Search for Direct $\mathit CP$ Violation in Singly Cabibbo-Suppressed ${{\mathit D}^{\pm}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{\pm}}$ Decays
 AKHMETSHIN 2008
PL B669 217 Measurement of ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \phi}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ Cross Section with CMD-2 Detector at VEPP-2M Collider
 AKHMETSHIN 2006
PL B642 203 Study of ${{\mathit \phi}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ with CMD-2 Detector
 AKHMETSHIN 2005
PL B605 26 Study of the Processes ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \gamma}}$ , ${{\mathit \pi}^{0}}$ ${{\mathit \gamma}}$ $\rightarrow$ 3 ${{\mathit \gamma}}$ in the c.m. Energy Range $600 - 1380$ MeV at CMD-2
 AUBERT,B 2005J
PR D72 052008 Dalitz Plot Analysis of ${{\mathit D}^{0}}$ $\rightarrow$ ${{\overline{\mathit K}}^{0}}{{\mathit K}^{+}}{{\mathit K}^{-}}$
 AKHMETSHIN 2004
PL B578 285 Reanalysis of Hadronic Cross Section Measurements at CMD-2
 ACHASOV 2001E
PR D63 072002 Measurements of the Parameters of the ${{\mathit \phi}{(1020)}}$ Resonance through Studies of the Processes ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ , ${{\mathit K}_S^0}$ ${{\mathit K}_L^0}$ , and ${{\mathit \pi}^{+}}$ ${{\mathit \pi}^{-}}$ ${{\mathit \pi}^{0}}$
 AKHMETSHIN 2001B
PL B509 217 Study of the Process ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \gamma}}$ in Center-of-Mass Energy Range 600 to 1380 MeV at Center-of-Mass CMD-2
 ACHASOV 2000B
JETP 90 17 Measurement of the Relative Probability of ${{\mathit \phi}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \gamma}}$ Decay in the ${{\mathit \eta}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ Channel
 AKHMETSHIN 1999F
PL B460 242 Study of the Radiative Decay ${{\mathit \phi}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \gamma}}$ with CMD-2 Detector
 AKHMETSHIN 1998
PL B434 426 Study of Dynamics of ${{\mathit \phi}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$ Decay with CMD-2 Detector
 BARBERIS 1998
PL B432 436 A Study of the Centrally Produced ${{\mathit \phi}}$ ${{\mathit \phi}}$ System in ${{\mathit p}}$ ${{\mathit p}}$ Interactions at 450 ${\mathrm {GeV/}}\mathit c$
 AKHMETSHIN 1995
PL B364 199 Measurement of ${{\mathit \phi}}$ -Meson Parameters with CMD-2 Detector at VEPP-2M Collider
 ARMSTRONG 1986
PL 166B 245 Observation of Double ${{\mathit \phi}}$ Meson Production in the Central Region for the Reactions ${{\mathit \pi}^{+}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \pi}^{+}}$( ${{\mathit K}^{+}}{{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit K}^{-}}$) ${{\mathit p}}$ and ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit p}}$( ${{\mathit K}^{+}}{{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit K}^{-}}$) ${{\mathit p}}$ at 85 GeV
 ATKINSON 1986
ZPHY C30 521 Inclusive Photoproduction of ${{\mathit \phi}}$ , ${{\mathit K}^{*}{(890)}}$ and ${{\mathit K}^{*}{(1420)}}$ in the Photon Energy Range 20 to 70 GeV
 BEBEK 1986
PRL 56 1893 Decay ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \phi}}{{\overline{\mathit K}}^{0}}$
 DAVENPORT 1986
PR D33 2519 Observation of Double ${{\mathit \phi}}$ Meson Production in 400 ${\mathrm {GeV/}}\mathit c$ Proton Nucleon Interactions
 DIJKSTRA 1986
ZPHY C31 375 High Statistics Inclusive ${{\mathit \phi}}$ Meson Production at SPS Energy
 FRAME 1986
NP B276 667 A Spin Parity Analysis of the ${{\mathit \phi}}$ ${{\mathit K}^{+}}$ System Produced in the Reaction ${{\mathit K}^{+}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit K}^{+}}{{\mathit p}}$ , ${{\mathit \phi}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ at 13 ${\mathrm {GeV/}}\mathit c$
 ALBRECHT 1985D
PL 153B 343 Production and Decay of the ${{\mathit D}_{{s}}}$ Meson in ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ Annihilation at 10 GeV Centre of Mass Energy
 ARMSTRONG 1983B
NP B224 193 Search for New (${\mathit {\mathit s}}{\mathit {\overline{\mathit s}}}$) States in the ${{\mathit K}^{-}}$ Induced ${{\mathit K}^{+}}$ ${{\mathit K}^{-}}$ System
 BARATE 1983
PL 121B 449 Search for Beauty Mesons
 ARENTON 1982
PR D25 2241 ${{\mathit \phi}}$ Meson Production in the Reaction ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit p}}{{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit p}}$ at 11.75 ${\mathrm {GeV/}}\mathit c$
 PELLINEN 1982
PS 25 599 A Precision Determination of the ${{\mathit \phi}}$ Meson Mass
 IVANOV 1981
PL 107B 297 Measurement of the Charged Kaon Formfactor in the Energy Range 1.0 to 1.4 GeV
 Also
Private Comm. Private Communication
 BUKIN 1978C
SJNP 27 516 The ${{\mathit \phi}}$ Meson: Precision Measurement of its Mass, Observation of the ${{\mathit \omega}}$ ${{\mathit \phi}}$ Interference
 COOPER 1978B
NP B146 1 ${{\mathit \phi}}$ and ${{\mathit \omega}}$ Meson Production in ${{\overline{\mathit p}}}$ ${{\mathit p}}$ Annihilations at $0.70 - 0.76$ ${\mathrm {GeV/}}\mathit c$ and the OZI Rule
 BALDI 1977
PL 68B 381 Comparison of ${{\mathit \phi}}$ Production by ${{\mathit \pi}}$ , ${{\mathit K}}$ and ${{\mathit p}}$ Incident on Protons at 10 GeV
 COHEN 1977
PRL 38 269 ${{\mathit \phi}}$ Meson Production in the Reactions ${{\mathit \pi}^{\pm}}$ ${{\mathit n}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit K}^{+}}{{\mathit n}}$ at 6 ${\mathrm {GeV/}}\mathit c$
 KALBFLEISCH 1976
PR D13 22 The Decay ${{\mathit \phi}{(1020)}}$ $\rightarrow$ ${{\mathit \rho}{(770)}}{{\mathit \pi}}$
 BESCH 1974
NP B70 257 Photoproduction of ${{\mathit \phi}}$ Mesons on Protons at 2.0 GeV
 BALLAM 1973
PR D7 3150 Vector Meson Production by Polarized Photons at 2.8, 4.7, and 9.3 GeV
 BINNIE 1973B
PR D8 2789 Study of Narrow Mesons near their Thresholds
 AGUILAR-BENITEZ 1972B
PR D6 29 Study of Nonstrange Mesons Produced in ${{\mathit K}^{-}}$ ${{\mathit p}}$ Interactions at 3.9 and 4.6 ${\mathrm {GeV/}}\mathit c$
 COLLEY 1972
NP B50 1 Properties of the ${{\mathit \phi}}$ and ${{\mathit f}_{{2'}}{(1525)}}$ Produced in the Channel ${{\mathit K}^{+}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit p}}{{\mathit K}}{{\overline{\mathit K}}}$ at 10 ${\mathrm {GeV/}}\mathit c$
 STOTTLEMYER 1971
Thesis ORO 2504 170 An Analysis of the ${{\mathit Y}}{{\mathit K}}{{\overline{\mathit K}}^{0}}$ and ${{\mathit \Xi}^{0}}{{\mathit K}^{+}}{{\mathit \pi}^{-}}$ Three Body Final States from ${{\mathit K}^{-}}{{\mathit p}}$ Interactions at 2.9 ${\mathrm {GeV/}}\mathit c$