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ND experiment
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ND experiment : ウィキペディア英語版
ND experiment
Neutral Detector (ND) is a detector for particle physics experiments created by the team of physicists in the
Budker Institute of Nuclear Physics, Novosibirsk, Russia.
Experiments with the ND were conducted from 1982 to 1987 at the e+e storage ring VEPP-2M in the energy range 2E=0.5-1.4 GeV.
== 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 \rho^0, \omega, and \phi mesons and other processes involving photons, \pi^0, and \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 〔

* Radiative decays
: e^+e^- \to \rho, \omega, \phi \to \pi^0 \gamma, \eta \gamma
〕〔

: \phi \to \eta^\prime \gamma

* Rare decays of the \rho^0, \omega, and \phi mesons
: \omega, \phi \to \pi^0 e^+e^- 〔S.I. Dolinsky ''et al.'', Sov. J. Nucl. Phys. 48 (1988) 277.〕
: \phi \to \pi^+ \pi^- 〔V. B. Golubev ''et al.'', Sov. J. Nucl. Phys. 44 (1986) 409.〕
* Search for rare decays
: \rho \to \pi^+ \pi^- \pi^0 〔V. B. Vasserman ''et al.'', Sov. J. Mod. Phys. 48 (1988) 480.〕
: \omega, \phi \to \pi^0 \pi^0 \gamma 〔〔
: \phi \to \pi^0 \eta \gamma 〔V. M. Aulchcnko ''et al.'', Preprini INP 87-90 (Novosibirsk, 1987).〕
: light scalars a_0(980) and f_0(975) in \phi-meson radiative decays 〔
* Non-resonant electron-positron annihilation into hadrons
: e^+e^- \to \omega \pi^0

: e^+e^- \to \pi^+ \pi^- \pi^0 ,~~ \pi^+ \pi^- \eta 〔A. D. Bukin ''et al.'', Sov. J. Nucl. Phys. 50 (1989) 621.〕〔

: e^+e^- \to \pi^+ \pi^- \pi^+ \pi^-,~~ \pi^+ \pi^- \pi^0 \pi^0 〔V. M. Aulchenko ''et al.'', Preprint INP 86-106 (Novosibirsk, 1987).〕
* Test of QED processes 〔V. P. Druzhinin ''et al.'', Preprint INP 85-98 (Novosibirsk, 1985).〕〔V. M. Aulchcnko ''et al.'', Preprint INP 86-173 (Novosibirsk, 1986).〕
: e^+e^- \to \gamma \gamma \gamma \gamma
: e^+e^- \to e^+e^- \gamma \gamma
: e^+e^- \to e^+e^- e^+e^-
: e^+e^- \to e^+e^- \gamma (virtual Compton scattering) 〔V. B. Golubev ''et al.'', Sov. J. Nucl. Phys. 41(1985) 752.〕
* Analyses of other processes
*
*Measurement of the ω-meson parameters 〔

*
*Upper limits on electron width of scalar and tensor mesons f_0(975), f_2(1270), f_0(1300), a_0(980), and a_2(1320) 〔P. V. Vorobyov ''et al.'', Sov. J. Nucl. Phys. 48 (1988) 436.〕
*
* \phi \to \pi^+ \pi^- \pi^0,~~ K^0_S K^0_L 〔V. P. Druzhinin ''et al.'', Preprint INP 85-97 (Novosibirsk, 1985).〕
*
*Search for
*
*
* e^+e^- \to \pi^0 \pi^0 \gamma 〔V. B. Golubev ''et al.'', Sov. J. Nucl. Phys. 45 (1987) 622.〕
*
*
* K^0_S \to \gamma \gamma 〔I. B. Vasserman ''et al.'', JETP Lett. 43(1986) 588.〕
*
*
* e^+e^- \to C(1480) \to \phi \pi^0 〔V. M. Aulchenko''et al.'', JETP Lett. 45 (1987) 145.〕

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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