20 research outputs found
Light Scalar Mesons from Phi to Psi
The following topics are considered. 1) Confinement, chiral dynamics, and
light scalar mesons. 2) Chiral shielding of the . 3) The
meson radiative decays about nature of light scalar resonances. 4) The
decays about nature of light scalar resonances. 5) The
and decays about nature of
light scalar resonances. 6) New round in , the Belle
data. Arguments in favor of the four-quark model of the and
mesons are given.Comment: 7 pages, 7 figures. Talk presented by N.N. Achasov at the
International Workshop "e+e- Collisions from Phi to Psi", February 27--March
2, 2006, BINP, Novosibirsk, Russian Federatio
First-order formalism for dark energy and dust
This work deals with first-order formalism for dark energy and dust in
standard cosmology, for models described by real scalar field in the presence
of dust in spatially flat space. The field dynamics may be standard or
tachyonic, and we show how the equations of motion can be solved by first-order
differential equations. We investigate a model to illustrate how the dustlike
matter may affect the cosmic evolution using this framework.Comment: 5 pages, 1 figure; title changed, new author included, discussions
extended, references added, version to appear in EPJ
First experimental results obtained using the highpower free electron laser at the siberian center for photochemical research
The first lasing near the wavelength of 140 ”m was achieved in April 2003 using a high-power free electron laser (FEL) constructed at the Siberian Center for Photochemical Research. In this paper we briefly describe the design of the FEL driven by an acceleratorârecuperator. Characteristics of the electron beam and terahertz laser radiation, obtained in the first experiments, are also presented in the paper.ĐŁ ХОбŃŃŃŃĐșĐŸĐŒŃ ŃĐ”ĐœŃŃŃ ŃĐŸŃĐŸŃ
ŃĐŒŃŃĐœĐžŃ
ĐŽĐŸŃĐ»ŃĐŽĐ¶Đ”ĐœŃ ĐœĐ°ĐČĐ”ŃĐœŃ 2003 ŃĐŸĐșŃ ĐŸŃŃĐžĐŒĐ°ĐœĐ° ĐłĐ”ĐœĐ”ŃĐ°ŃŃŃ ĐČОпŃĐŸĐŒŃĐœŃĐČĐ°ĐœĐœŃ Đ· ĐŽĐŸĐČĐ¶ĐžĐœĐŸŃ Ń
ĐČĐžĐ»Ń 140 ĐŒĐșĐŒ ĐœĐ° ĐżĐŸŃŃĐ¶ĐœĐŸĐŒŃ Đ»Đ°Đ·Đ”ŃŃ ĐœĐ° ĐČŃĐ»ŃĐœĐžŃ
ДлДĐșŃŃĐŸĐœĐ°Ń
(ĐĐĐ). ĐŁ ŃĐŸĐ±ĐŸŃŃ ĐșĐŸŃĐŸŃĐșĐŸ ĐŸĐżĐžŃĐ°ĐœĐ° ĐșĐŸĐœŃŃŃŃĐșŃŃŃ ĐĐĐ ĐœĐ° Đ±Đ°Đ·Ń ĐżŃĐžŃĐșĐŸŃŃĐČĐ°ŃĐ° ŃĐ”ĐșŃпДŃĐ°ŃĐŸŃĐ° Ń ĐżŃДЎŃŃĐ°ĐČĐ»Đ”ĐœŃ ŃДзŃĐ»ŃŃĐ°ŃĐž ĐČĐžĐŒŃŃŃĐČĐ°ĐœĐœŃ ĐŽĐ”ŃĐșĐžŃ
паŃĐ°ĐŒĐ”ŃŃŃĐČ Đ”Đ»Đ”ĐșŃŃĐŸĐœĐœĐŸĐłĐŸ ĐżŃŃĐșĐ° Ń ŃĐ”ŃагДŃŃĐŸĐČĐŸĐłĐŸ ĐČОпŃĐŸĐŒŃĐœŃĐČĐ°ĐœĐœŃ.РХОбОŃŃĐșĐŸĐŒ ŃĐ”ĐœŃŃĐ” ŃĐŸŃĐŸŃ
ĐžĐŒĐžŃĐ”ŃĐșĐžŃ
ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐč ĐČĐ”ŃĐœĐŸĐč 2003 ĐłĐŸĐŽĐ° ĐżĐŸĐ»ŃŃĐ”ĐœĐ° ĐłĐ”ĐœĐ”ŃĐ°ŃĐžŃ ĐžĐ·Đ»ŃŃĐ”ĐœĐžŃ Ń ĐŽĐ»ĐžĐœĐŸĐč ĐČĐŸĐ»ĐœŃ 140 ĐŒĐșĐŒ ĐœĐ° ĐŒĐŸŃĐœĐŸĐŒ лазДŃĐ” ĐœĐ° ŃĐČĐŸĐ±ĐŸĐŽĐœŃŃ
ŃлДĐșŃŃĐŸĐœĐ°Ń
(ĐĐĄĐ). Đ ŃĐ°Đ±ĐŸŃĐ” ĐșŃĐ°ŃĐșĐŸ ĐŸĐżĐžŃĐ°ĐœĐ° ĐșĐŸĐœŃŃŃŃĐșŃĐžŃ ĐĐĄĐ ĐœĐ° базД ŃŃĐșĐŸŃĐžŃĐ”Đ»Ń ŃĐ”ĐșŃпДŃĐ°ŃĐŸŃĐ° Đž ĐżŃДЎŃŃĐ°ĐČĐ»Đ”ĐœŃ ŃДзŃĐ»ŃŃĐ°ŃŃ ĐžĐ·ĐŒĐ”ŃĐ”ĐœĐžŃ ĐœĐ”ĐșĐŸŃĐŸŃŃŃ
паŃĐ°ĐŒĐ”ŃŃĐŸĐČ ŃлДĐșŃŃĐŸĐœĐœĐŸĐłĐŸ ĐżŃŃĐșĐ° Đž ŃĐ”ŃагДŃŃĐŸĐČĐŸĐłĐŸ ОзлŃŃĐ”ĐœĐžŃ
Observation of J/Ï-pair production in pp collisions at âs=7 TeV
The production of J/Ï pairs in protonâproton collisions at a centre-of-mass energy of 7 TeV has been observed using an integrated luminosity of 37.5 pbâ1 collected with the LHCb detector. The production cross-section for pairs with both J/Ï in the rapidity range 2 < yJ/Ï < 4.5 and transverse momentum pJ/Ï T <10 GeV/c is ÏJ/ÏJ/Ï =5.1±1.0±1.1 nb, where the ïŹrst uncertainty is statistical and the second systematic