${{\mathit \phi}{(1020)}}$ MASS INSPIRE search

M004M
VALUE (MeV) EVTS DOCUMENT ID TECN  COMMENT
$\bf{ 1019.460 \pm0.016}$ OUR AVERAGE
$1019.444$ $\pm0.013$ $\pm0.060$
DRUZHININ
2025
SND ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}_L^0}$ ${{\mathit K}_S^0}$
$1019.463$ $\pm0.061$ 2.3M 1
KOZYREV
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
LEES
2014H
 BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}_L^0}$ ${{\mathit \gamma}}$
$1019.51$ $\pm0.02$ $\pm0.05$ 3
LEES
2013Q
 BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \gamma}}$
$1019.30$ $\pm0.02$ $\pm0.10$ 105k
AKHMETSHIN
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
AKHMETSHIN
2005
CMD2 0.60-1.38 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \gamma}}$
$1019.483$ $\pm0.011$ $\pm0.025$ 272k 4
AKHMETSHIN
2004
CMD2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}_L^0}$ ${{\mathit K}_S^0}$
$1019.42$ $\pm0.05$ 1900k 5
ACHASOV
2001E
 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
AKHMETSHIN
2001B
 CMD2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \gamma}}$
$1019.36$ $\pm0.12$ 6
ACHASOV
2000B
 SND ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \gamma}}$
$1019.38$ $\pm0.07$ $\pm0.08$ 2200 7
AKHMETSHIN
1999F
 CMD2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{}\geq{}2{{\mathit \gamma}}$
$1019.51$ $\pm0.07$ $\pm0.10$ 11169
AKHMETSHIN
1998
CMD2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$
$1019.5$ $\pm0.4$
BARBERIS
1998
OMEG 450 ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit p}}{{\mathit p}}$2 ${{\mathit K}^{+}}$2 ${{\mathit K}^{-}}$
$1019.42$ $\pm0.06$ 55600
AKHMETSHIN
1995
CMD2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ hadrons
$1019.7$ $\pm0.3$ 2012
DAVENPORT
1986
MPSF 400 ${{\mathit p}}$ ${}^{}\mathrm {A}$ $\rightarrow$ 4 ${{\mathit K}}$ X
$1019.7$ $\pm0.1$ $\pm0.1$ 5079
ALBRECHT
1985D
 ARG 10 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ X
$1019.3$ $\pm0.1$ 1500
ARENTON
1982
AEMS 11.8 polar. ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}}{{\mathit K}}$
$1019.67$ $\pm0.17$ 25080 8
PELLINEN
1982
RVUE
$1019.52$ $\pm0.13$ 3681
BUKIN
1978C
 OLYA ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ hadrons
• • • We do not use the following data for averages, fits, limits, etc. • • •
$1019.443$ $\pm0.010$ $\pm0.060$ 1.28M 9, 10
ACHASOV
2024
SND ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}_L^0}$ ${{\mathit K}_S^0}$
$1019.0330$ $\pm0.0084$ 11
DUBNICKA
2024
RVUE ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$ , ${{\mathit K}_S^0}$ ${{\mathit K}_L^0}$
$1019.761$ $\pm0.130$ 34M 12
IGNATOV
2024
CMD3 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$
$1018.4$ $\pm0.5$ $\pm0.1$ 13
ALBRECHT
2020
CBAR 0.9 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{0}}$
$1019.21$ $\pm0.04$ $\pm0.03$ 14
HOID
2020
RVUE ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \pi}^{0}}{{\mathit \gamma}}$
$1019.54$ $\pm0.10$ $\pm0.51$ 15
AAIJ
2019H
 LHCB ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit D}^{\pm}}{{\mathit X}}$
$1019.20$ $\pm0.02$ $\pm0.01$ 16
HOFERICHTER
2019
RVUE ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$
$1019.469$ $\pm0.061$ 1.7M
KOZYREV
2018
CMD3 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$
$1019.457$ $\pm0.061$ 610k
KOZYREV
2016
CMD3 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}_L^0}$
$1019.48$ $\pm0.01$
LEES
2013F
 BABR ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$
$1019.441$ $\pm0.008$ $\pm0.080$ 542k 17
AKHMETSHIN
2008
CMD2 1.02 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$
$1019.63$ $\pm0.07$ 12540 18
AUBERT,B
2005J
 BABR ${{\mathit D}^{0}}$ $\rightarrow$ ${{\overline{\mathit K}}^{0}}{{\mathit K}^{+}}{{\mathit K}^{-}}$
$1019.8$ $\pm0.7$
ARMSTRONG
1986
OMEG 85 ${{\mathit \pi}^{+}}$ /${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \pi}^{+}}$ /${{\mathit p}}$4 ${{\mathit K}}{{\mathit p}}$
$1020.1$ $\pm0.11$ 5526 18
ATKINSON
1986
OMEG 20$-$70 ${{\mathit \gamma}}{{\mathit p}}$
$1019.7$ $\pm1.0$
BEBEK
1986
CLEO ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(4S)}}$
$1019.411$ $\pm0.008$ 642k 19
DIJKSTRA
1986
SPEC 100$-$200 ${{\mathit \pi}^{\pm}}$, ${{\overline{\mathit p}}}$, ${{\mathit p}}$, ${{\mathit K}^{\pm}}$, on ${}^{}\mathrm {Be}$
$1020.9$ $\pm0.2$ 18
FRAME
1986
OMEG 13 ${{\mathit K}^{+}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit K}^{+}}{{\mathit p}}$
$1021.0$ $\pm0.2$ 18
ARMSTRONG
1983B
 OMEG 18.5 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit K}^{+}}{{\mathit \Lambda}}$
$1020.0$ $\pm0.5$ 18
ARMSTRONG
1983B
 OMEG 18.5 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit K}^{+}}{{\mathit \Lambda}}$
$1019.7$ $\pm0.3$ 18
BARATE
1983
GOLI 190 ${{\mathit \pi}^{-}}$ ${}^{}\mathrm {Be}$ $\rightarrow$ 2 ${{\mathit \mu}}$ X
$1019.8$ $\pm0.2$ $\pm0.5$ 766
IVANOV
1981
OLYA 1$-$1.4 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$
$1019.4$ $\pm0.5$ 337
COOPER
1978B
 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 18
BALDI
1977
CNTR 10 ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \pi}^{-}}{{\mathit \phi}}{{\mathit p}}$
$1018.9$ $\pm0.6$ 800
COHEN
1977
ASPK 6 ${{\mathit \pi}^{\pm}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit N}}$
$1019.7$ $\pm0.5$ 454
KALBFLEISCH
1976
HBC 2.18 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \Lambda}}{{\mathit K}}{{\overline{\mathit K}}}$
$1019.4$ $\pm0.8$ 984
BESCH
1974
CNTR 2 ${{\mathit \gamma}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit p}}{{\mathit K}^{+}}{{\mathit K}^{-}}$
$1020.3$ $\pm0.4$ 100
BALLAM
1973
HBC 2.8$-$9.3 ${{\mathit \gamma}}{{\mathit p}}$
$1019.4$ $\pm0.7$
BINNIE
1973B
 CNTR ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit n}}$
$1019.6$ $\pm0.5$ 120 20
AGUILAR-BENIT..
1972B
 HBC 3.9,4.6 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \Lambda}}{{\mathit K}^{+}}{{\mathit K}^{-}}$
$1019.9$ $\pm0.5$ 100 20
AGUILAR-BENIT..
1972B
 HBC 3.9,4.6 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit p}}{{\mathit K}^{+}}{{\mathit K}^{-}}$
$1020.4$ $\pm0.5$ 131
COLLEY
1972
HBC 10 ${{\mathit K}^{+}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit p}}{{\mathit \phi}}$
$1019.9$ $\pm0.3$ 410
STOTTLEMYER
1971
HBC 2.9 ${{\mathit K}^{-}}$ ${{\mathit p}}$ ${{\mathit \Sigma}}$ ${{\mathit \Lambda}}$ ${{\mathit K}}$ ${{\overline{\mathit K}}}$
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  From a fit of the cross section in the energy region 1.000 $<$ $\sqrt {s }$ $<$ 1.100 GeV using a vector meson dominance model with contribution from ${{\mathit \phi}{(1020)}}$, ${{\mathit \rho}{(770)}}$, ${{\mathit \omega}{(782)}}$ and higher vector resonances.
10  Superseded by DRUZHININ 2025.
11  From the fit to data of CMD3, BABAR and BES3.
12  From a fit of the pion form factor in the energy range 0.32 $<$ $\sqrt {s }$ $<$ 1.2 GeV using the GOUNARIS 1968 parametrization with the complex phase of the ${{\mathit \rho}}−{{\mathit \omega}}$ interference leaving ${{\mathit \rho}{(1450)}}$, ${{\mathit \rho}{(1700)}}$ resonances as free parameters of the fit. Systematic errors not estimated.
13  Width fixed at 4.2 MeV.
14  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.
15  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.
16  The values were extracted from a dispersively improved Breit-Wigner parameterization and do not include vacuum polarization.
17  Strongly correlated with AKHMETSHIN 2004.
18  Systematic errors not evaluated.
19  Weighted and scaled average of 12 measurements of DIJKSTRA 1986.
20  Mass errors enlarged by us to $\Gamma /\sqrt {\mathit N }$; see the note with the ${{\mathit K}^{*}{(892)}}$ mass.
  References:
DRUZHININ 2025
PPN 56 405 Measurement of ?(1020) Parameters in the ${{e}^{ + }}{{e}^{ - }} \to {{K}_{S}}{{K}_{L}}$ Reaction
ACHASOV 2024
PR D110 072001 Measurement of the $e^+e^-\to K_SK_L$ cross section near the $\phi(1020)$ resonance with the SND detector
DUBNICKA 2024
PR D110 054019 What is the real value of the ratio R=??K+K-/KL0KS0?
IGNATOV 2024
PR D109 112002 Measurement of the $e^+e^-\to\pi^+\pi^-$ cross section from threshold to 1.2 GeV with the CMD-3 detector
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 ${\mathrm {GeV/}}\mathit c$