ND experiment
Physics
At the beginning of 80s the leading cross sections of the electron -positron annihilation in the final states with charged particles were measured in the energy range 2E=0.5-1.4 GeV. Processes with the neutral particles in the final state were less studied. To investigate the radiative decays of the
ρ
0
{\displaystyle \rho ^{0}}
,
ω
{\displaystyle \omega }
, and
ϕ
{\displaystyle \phi }
mesons and other processes involving photons ,
π
0
{\displaystyle \pi ^{0}}
, and
η
{\displaystyle \eta }
mesons the ND
was constructed. Its distinguishing features are defined by the specially designed electromagnetic calorimeter based on NaI (Tl) scintillation counters .
List of published analyses
e
+
e
−
→
ρ
,
ω
,
ϕ
→
π
0
γ
,
η
γ
{\displaystyle e^{+}e^{-}\to \rho ,\omega ,\phi \to \pi ^{0}\gamma ,\eta \gamma }
ϕ
→
η
′
γ
{\displaystyle \phi \to \eta ^{\prime }\gamma }
Rare decays of the
ρ
0
{\displaystyle \rho ^{0}}
,
ω
{\displaystyle \omega }
, and
ϕ
{\displaystyle \phi }
mesons
ω
,
ϕ
→
π
0
e
+
e
−
{\displaystyle \omega ,\phi \to \pi ^{0}e^{+}e^{-}}
ϕ
→
π
+
π
−
{\displaystyle \phi \to \pi ^{+}\pi ^{-}}
ρ
→
π
+
π
−
π
0
{\displaystyle \rho \to \pi ^{+}\pi ^{-}\pi ^{0}}
ω
,
ϕ
→
π
0
π
0
γ
{\displaystyle \omega ,\phi \to \pi ^{0}\pi ^{0}\gamma }
ϕ
→
π
0
η
γ
{\displaystyle \phi \to \pi ^{0}\eta \gamma }
light scalars
a
0
(
980
)
{\displaystyle a_{0}(980)}
and
f
0
(
975
)
{\displaystyle f_{0}(975)}
in
ϕ
{\displaystyle \phi }
-meson radiative decays
e
+
e
−
→
ω
π
0
{\displaystyle e^{+}e^{-}\to \omega \pi ^{0}}
e
+
e
−
→
π
+
π
−
π
0
,
π
+
π
−
η
{\displaystyle e^{+}e^{-}\to \pi ^{+}\pi ^{-}\pi ^{0},~~\pi ^{+}\pi ^{-}\eta }
e
+
e
−
→
π
+
π
−
π
+
π
−
,
π
+
π
−
π
0
π
0
{\displaystyle e^{+}e^{-}\to \pi ^{+}\pi ^{-}\pi ^{+}\pi ^{-},~~\pi ^{+}\pi ^{-}\pi ^{0}\pi ^{0}}
e
+
e
−
→
γ
γ
γ
γ
{\displaystyle e^{+}e^{-}\to \gamma \gamma \gamma \gamma }
e
+
e
−
→
e
+
e
−
γ
γ
{\displaystyle e^{+}e^{-}\to e^{+}e^{-}\gamma \gamma }
e
+
e
−
→
e
+
e
−
e
+
e
−
{\displaystyle e^{+}e^{-}\to e^{+}e^{-}e^{+}e^{-}}
e
+
e
−
→
e
+
e
−
γ
{\displaystyle e^{+}e^{-}\to e^{+}e^{-}\gamma }
(virtual Compton scattering )
Analyses of other processes
Measurement of the ω-meson parameters
Upper limits on electron width of scalar and tensor mesons
f
0
(
975
)
{\displaystyle f_{0}(975)}
,
f
2
(
1270
)
{\displaystyle f_{2}(1270)}
,
f
0
(
1300
)
{\displaystyle f_{0}(1300)}
,
a
0
(
980
)
{\displaystyle a_{0}(980)}
, and
a
2
(
1320
)
{\displaystyle a_{2}(1320)}
ϕ
→
π
+
π
−
π
0
,
K
S
0
K
L
0
{\displaystyle \phi \to \pi ^{+}\pi ^{-}\pi ^{0},~~K_{S}^{0}K_{L}^{0}}
Search for
e
+
e
−
→
π
0
π
0
γ
{\displaystyle e^{+}e^{-}\to \pi ^{0}\pi ^{0}\gamma }
K
S
0
→
γ
γ
{\displaystyle K_{S}^{0}\to \gamma \gamma }
e
+
e
−
→
C
(
1480
)
→
ϕ
π
0
{\displaystyle e^{+}e^{-}\to C(1480)\to \phi \pi ^{0}}
Detector
Neutral Detector r-φ view.
Neutral Detector r-θ view; 1-vacuum chamber of the storage ring, 2-cylindrical proportional chambers, 3-plastic scintillation counters, 4-NaI(Tl) counters, 5-flat proportional chambers, 6-iron absorber, 7-anticoincidence counters.
Based on goals of the physics program the ND consist of
Electromagnetic calorimeter
168 rectangular NaI (Tl) scintillation counters
total mass of NaI (Tl) is 2.6 t
solid angle coverage is 65% of 4π sr
minimum thickness is 32 cm or 12 radiation length
energy resolution for photons is σ/E = 4% / √ E
Charged particle coordinate system
3 layers of coaxial cylindrical 2-d wire proportional chambers in the center of the detector
solid angle coverage is 80% of 4π sr
angular resolution is 0.5° in the azimuthal and 1.5° in the polar direction
surrounded by the 5-mm thick plastic scintillation counter for trigger
Flat (shower) coordinate 2-d wire proportional chambers
2 layers of flat 2-d wire proportional chambers.
angular resolution is 2° in the azimuthal and 3.5° in the polar direction for 0.5 GeV photons
Iron absorber & anti-coincidence counters
The electromagnetic calorimeter is covered by the 10-cm thick iron absorber and plastic scintillation anti-coincidence counters.
Results
Data collected with the ND experiment corresponds to the integrated luminosity 19 pb−1 .
Results of the experiments with ND are presented in Ref.,
and are included in the PDG Review.
References
1 2 3
Dolinsky, S. I.; et al. (1991). "Summary of experiments with the neutral detector at the e+ e− storage ring VEPP-2M". Physics Reports . 202 (3): 99– 170. Bibcode :1991PhR...202...99D . doi :10.1016/0370-1573(91)90127-8 .
↑
Golubev, V. B.; et al. (1984). "The neutral detector at VEPP-2M". Nuclear Instruments and Methods in Physics Research Section A . 227 (3): 467– 469. Bibcode :1984NIMPA.227..467G . doi :10.1016/0168-9002(84)90202-X .
1 2
Dolinsky, S. I.; et al. (1984). "Radiative decays of ρ and ω mesons". Zeitschrift für Physik C . 42 (4): 511– 518. doi :10.1007/BF01557655 . S2CID 122486080 .
↑
Druzhinin, V. P.; et al. (1984). "Measurement of Φ-meson radiative decays at the storage ring VEPP-2M with the neutral detector". Physics Letters B . 144 (1– 2): 136– 140. Bibcode :1984PhLB..144..136D . doi :10.1016/0370-2693(84)90192-8 .
1 2 3
Druzhinin, V. P.; et al. (1987). "Search for rare radiative decays of Φ-meson at VEPP-2M". Zeitschrift für Physik C . 37 (1): 1– 5. Bibcode :1987ZPhyC..37....1D . doi :10.1007/BF01442062 . S2CID 120341644 .
↑ S.I. Dolinsky et al. , Sov. J. Nucl. Phys. 48 (1988) 277.
↑ V. B. Golubev et al. , Sov. J. Nucl. Phys. 44 (1986) 409.
↑ V. B. Vasserman et al. , Sov. J. Mod. Phys. 48 (1988) 480.
↑ V. M. Aulchcnko et al. , Preprini INP 87-90 (Novosibirsk, 1987).
↑
Dolinsky, S. I.; et al. (1986). "The reaction e+ e− → ωπ0 in the cm energy range from 1.0 to 1.4 GeV". Phys. Lett. B . 174 (4): 453– 457. Bibcode :1986PhLB..174..453D . doi :10.1016/0370-2693(86)91036-1 .
↑ A. D. Bukin et al. , Sov. J. Nucl. Phys. 50 (1989) 621.
↑
Druzhinin, V. P.; et al. (1986). "Investigation of the reaction e+ e− → ηπ+ π− in the energy range up to 1.4 GeV". Phys. Lett. B . 174 (1): 115– 117. Bibcode :1986PhLB..174..115D . doi :10.1016/0370-2693(86)91140-8 .
↑ V. M. Aulchenko et al. , Preprint INP 86-106 (Novosibirsk, 1987).
↑ V. P. Druzhinin et al. , Preprint INP 85-98 (Novosibirsk, 1985).
↑ V. M. Aulchcnko et al. , Preprint INP 86-173 (Novosibirsk, 1986).
↑ V. B. Golubev et al. , Sov. J. Nucl. Phys. 41(1985) 752.
↑
Aulchenko, V. M.; et al. (1987). "The width of the ω-meson". Phys. Lett. B . 186 (3– 4): 432– 434. Bibcode :1987PhLB..186..432A . doi :10.1016/0370-2693(87)90322-4 .
↑ P. V. Vorobyov et al. , Sov. J. Nucl. Phys. 48 (1988) 436.
↑ V. P. Druzhinin et al. , Preprint INP 85-97 (Novosibirsk, 1985).
↑ V. B. Golubev et al. , Sov. J. Nucl. Phys. 45 (1987) 622.
↑ I. B. Vasserman et al. , JETP Lett. 43(1986) 588.
↑ V. M. Aulchenkoet al. , JETP Lett. 45 (1987) 145.
↑ The Review of Particle Physics ,
K. Nakamura et al. (Particle Data Group), J. Phys. G 37, 075021 (2010)