73 research outputs found

    Matching Regge Theory to the OPE

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    The spectra of masses and decay constants for non-strange meson resonances in the energy range 0--2.5 GeV is analyzed. It is known from meson phenomenology that for given quantum numbers these spectra approximately follow linear trajectories with a universal slope. These facts can be understood in terms of an effective string description for QCD. For light meson states the trajectories deviate noticeably from the linear behavior. We investigate the possible corrections to the linear trajectories by matching two-point correlators of quark currents to the Operator Product Expansion (OPE). We find that the allowed modifications to the linear Regge behavior must decrease rapidly with the principal quantum number. After fitting the lightest states in each channel and certain low-energy constants the whole spectrum for meson masses and residues is obtained in a satisfactory agreement with phenomenology. We briefly speculate on possible implications for the QCD effective string.Comment: 24 pages, Latex, significant changes in discussion of fits, more refs adde

    On the nonlinear dynamics of topological solitons in DNA

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    Dynamics of topological solitons describing open states in the DNA double helix are studied in the frameworks of the model which takes into account asymmetry of the helix. It is shown that three types of topological solitons can occur in the DNA double chain. Interaction between the solitons, their interactions with the chain inhomogeneities and stability of the solitons with respect to thermal oscillations are investigated.Comment: 16 pages, 16 figure

    Studies of edge turbulence in the Uragan-3M torsatron

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    Spatial and temporal behavior of the edge fluctuations and their correlation with plasma density behavior inside the confinement region of the Uragan-3M torsatron are investigated. The key role of the radial electric field in turbulent transport suppression is shown.Đ”ĐŸŃĐ»Ń–ĐŽĐ¶Đ”ĐœĐŸ ĐŽĐžĐœĐ°ĐŒŃ–Đșу Ń„Đ»ŃƒĐșтуаціĐč ĐżĐŸĐ±Đ»ĐžĐ·Ńƒ ĐŒĐ”Đ¶Ń– ĐżĐ»Đ°Đ·ĐŒĐž та їх ĐșĐŸŃ€Đ”Đ»ŃŃ†Ń–Ń— Đ· ĐżĐŸĐČĐ”ĐŽŃ–ĐœĐșĐŸŃŽ Ń‰Ń–Đ»ŃŒĐœĐŸŃŃ‚Ń– ŃƒŃĐ”Ń€Đ”ĐŽĐžĐœŃ– ĐŸĐ±â€™Ń”ĐŒŃƒ ŃƒŃ‚Ń€ĐžĐŒĐ°ĐœĐœŃ Đ° Ń‚ĐŸŃ€ŃĐ°Ń‚Ń€ĐŸĐœŃ– ĐŁŃ€Đ°ĐłĐ°Đœ-3М. ĐżĐŸĐșĐ°Đ·Đ°ĐœĐ° ĐŸŃĐœĐŸĐČĐœĐ° Ń€ĐŸĐ»ŃŒ Ń€Đ°ĐŽŃ–Đ°Đ»ŃŒĐœĐŸĐłĐŸ ДлДĐșŃ‚Ń€ĐžŃ‡ĐœĐŸĐłĐŸ ĐżĐŸĐ»Ń ĐČ ĐżŃ€ĐžĐłĐœŃ–Ń‡Đ”ĐœŃ– Ń‚ŃƒŃ€Đ±ŃƒĐ»Đ”ĐœŃ‚ĐœĐŸĐłĐŸ ĐżĐŸŃ‚ĐŸĐșŃƒĐ˜ŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐ° ĐŽĐžĐœĐ°ĐŒĐžĐșĐ° Ń„Đ»ŃƒĐșтуацоĐč ĐČблОзО ĐłŃ€Đ°ĐœĐžŃ†Ń‹ ĐżĐ»Đ°Đ·ĐŒŃ‹ Đž ох ĐșĐŸŃ€Ń€Đ”Đ»ŃŃ†ĐžŃ с ĐżĐŸĐČĐ”ĐŽĐ”ĐœĐžĐ”ĐŒ ĐżĐ»ĐŸŃ‚ĐœĐŸŃŃ‚Đž ĐČĐœŃƒŃ‚Ń€Đž ĐŸĐ±ŃŠĐ”ĐŒĐ° ŃƒĐŽĐ”Ń€Đ¶Đ°ĐœĐžŃ ĐČ Ń‚ĐŸŃ€ŃĐ°Ń‚Ń€ĐŸĐœĐ” ĐŁŃ€Đ°ĐłĐ°Đœ-3М. ĐŸĐŸĐșĐ°Đ·Đ°ĐœĐ° ĐŸŃĐœĐŸĐČĐœĐ°Ń Ń€ĐŸĐ»ŃŒ раЮоĐșĐ°Đ»ŃŒĐœĐŸĐłĐŸ ŃĐ»Đ”ĐșтрОчДсĐșĐŸĐłĐŸ ĐżĐŸĐ»Ń ĐČ ĐżĐŸĐŽĐ°ĐČĐ»Đ”ĐœĐžĐž Ń‚ŃƒŃ€Đ±ŃƒĐ»Đ”ĐœŃ‚ĐœĐŸŃŃ‚Đž ĐżĐŸŃ‚ĐŸĐș

    Transition to the improved confinement mode in torsatron U-3M in range of rare collision frequencies

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    Transition to the mode of improved plasma confinement in U-3M facility earlier was discussed in works [1-3]. In these studies discussed the various processes in the confinement volume and in the peripheral plasma that accompany the transition process. Study of plasma confinement and process of transition into the mode of improved confinement just at rare collisions between plasma particles is very important because future fusion reactor based on a toroidal magnetic trap will operate under plasma parameters with rare collision frequencies (“banana” mode). The peculiarity of experiments on torsatron U-3M is that they are conducted at small density ne ≀ 2×10^12 cm^-3 and, thereby, the frequency of collisions in the confinement area is in the "banana" mode [4]. And herewith, time of collisions is essentially smaller (up to several orders for electrons and up to the order for ions) than the lifetime of plasma particles. It ensures maxwellization of distribution function and possibility to compare the obtained results with data from other experiments. The objective of this work is to study the main regularity of transition into the mode of improved confinement. Also it is interesting to compare the results with data from other facilities

    First results of the renewed Uragan-2M torsatron

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    The results of experimental investigation on the vacuum magnetic surfaces in the l=2 torsatron with an additional toroidal field Uragan-2M at wide varying operation parameters are presented. Also the first results on the wall conditioning in the Uragan-2M with the ECR and RF discharges in atmosphere of hydrogen in steady-state mode at low magnetic field, plasma production and heating with RF power are described.ĐŸŃ€Đ”ĐŽŃŃ‚Đ°ĐČĐ»Đ”ĐœĐŸ Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Đž Đ”ĐșŃĐżĐ”Ń€ĐžĐŒĐ”ĐœŃ‚Đ°Đ»ŃŒĐœĐŸĐłĐŸ ĐŽĐŸŃĐ»Ń–ĐŽĐ¶Đ”ĐœĐœŃ ĐČĐ°ĐșŃƒŃƒĐŒĐœĐžŃ… ĐŒĐ°ĐłĐœŃ–Ń‚ĐœĐžŃ… ĐżĐŸĐČĐ”Ń€Ń…ĐŸĐœŃŒ ĐČ l=2 Ń‚ĐŸŃ€ŃĐ°Ń‚Ń€ĐŸĐœŃ– Đ· ĐŽĐŸĐŽĐ°Ń‚ĐșĐŸĐČĐžĐŒ ĐŒĐ°ĐłĐœŃ–Ń‚ĐœĐžĐŒ ĐżĐŸĐ»Đ”ĐŒ ĐŁŃ€Đ°ĐłĐ°Đœ-2М ĐŽĐ»Ń ŃˆĐžŃ€ĐŸĐșĐŸŃ— Đ·ĐŒŃ–ĐœĐž ĐŸĐżĐ”Ń€Đ°Ń†Ń–ĐčĐœĐžŃ… ĐżĐ°Ń€Đ°ĐŒĐ”Ń‚Ń€Ń–ĐČ. йаĐșĐŸĐ¶ ĐŸĐżĐžŃĐ°ĐœŃ– ĐżĐ”Ń€ŃˆŃ– Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Đž ĐżŃ–ĐŽĐłĐŸŃ‚ĐŸĐČĐșĐž ĐżĐ”Ń€ŃˆĐŸŃ— ŃŃ‚Ń–ĐœĐșĐž ĐČ ĐŁŃ€Đ°ĐłĐ°ĐœŃ–-2М Đ·Đ° ĐŽĐŸĐżĐŸĐŒĐŸĐłĐŸŃŽ ЕЩР і ВЧ Ń€ĐŸĐ·Ń€ŃĐŽŃ–ĐČ ĐČ Đ°Ń‚ĐŒĐŸŃŃ„Đ”Ń€Ń– ĐČĐŸĐŽĐœŃŽ ĐČ ŃŃ‚Đ°Ń†Ń–ĐŸĐœĐ°Ń€ĐœĐŸĐŒŃƒ Ń€Đ”Đ¶ĐžĐŒŃ– про ĐœĐžĐ·ŃŒĐșĐŸĐŒŃƒ ĐŒĐ°ĐłĐœŃ–Ń‚ĐœĐŸĐŒŃƒ ĐżĐŸĐ»Ń–, стĐČĐŸŃ€Đ”ĐœĐœŃ і ĐœĐ°ĐłŃ€Ń–ĐČу ĐżĐ»Đ°Đ·ĐŒĐž ВЧ ĐżĐŸŃ‚ŃƒĐ¶ĐœŃ–ŃŃ‚ŃŽ.ĐŸŃ€Đ”ĐŽŃŃ‚Đ°ĐČĐ»Đ”ĐœŃ‹ Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Ń‹ эĐșŃĐżĐ”Ń€ĐžĐŒĐ”ĐœŃ‚Đ°Đ»ŃŒĐœĐŸĐłĐŸ ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžŃ ĐČĐ°ĐșŃƒŃƒĐŒĐœŃ‹Ń… ĐŒĐ°ĐłĐœĐžŃ‚ĐœŃ‹Ń… ĐżĐŸĐČĐ”Ń€Ń…ĐœĐŸŃŃ‚Đ”Đč ĐČ l=2 Ń‚ĐŸŃ€ŃĐ°Ń‚Ń€ĐŸĐœĐ” с ĐŽĐŸĐżĐŸĐ»ĐœĐžŃ‚Đ”Đ»ŃŒĐœŃ‹ĐŒ ĐŒĐ°ĐłĐœĐžŃ‚ĐœŃ‹ĐŒ ĐżĐŸĐ»Đ”ĐŒ ĐŁŃ€Đ°ĐłĐ°Đœ-2М ĐŽĐ»Ń ŃˆĐžŃ€ĐŸĐșĐŸĐłĐŸ ĐžĐ·ĐŒĐ”ĐœĐ”ĐœĐžŃ ĐŸĐżĐ”Ń€Đ°Ń†ĐžĐŸĐœĐœŃ‹Ń… ĐżĐ°Ń€Đ°ĐŒĐ”Ń‚Ń€ĐŸĐČ. йаĐșжД ĐŸĐżĐžŃĐ°ĐœŃ‹ пДрĐČŃ‹Đ” Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Ń‹ ĐżĐŸĐŽĐłĐŸŃ‚ĐŸĐČĐșĐž пДрĐČĐŸĐč ŃŃ‚Đ”ĐœĐșĐž ĐČ ĐŁŃ€Đ°ĐłĐ°ĐœĐ”-2М про ĐżĐŸĐŒĐŸŃ‰Đž Đ­ĐŠĐ  Đž ВЧ Ń€Đ°Đ·Ń€ŃĐŽĐŸĐČ ĐČ Đ°Ń‚ĐŒĐŸŃŃ„Đ”Ń€Đ” ĐČĐŸĐŽĐŸŃ€ĐŸĐŽĐ° ĐČ ŃŃ‚Đ°Ń†ĐžĐŸĐœĐ°Ń€ĐœĐŸĐŒ Ń€Đ”Đ¶ĐžĐŒĐ” про ĐœĐžĐ·ĐșĐŸĐŒ ĐŒĐ°ĐłĐœĐžŃ‚ĐœĐŸĐŒ ĐżĐŸĐ»Đ”, ŃĐŸĐ·ĐŽĐ°ĐœĐžŃ Đž ĐœĐ°ĐłŃ€Đ”ĐČĐ° ĐżĐ»Đ°Đ·ĐŒŃ‹ ВЧ- ĐŒĐŸŃ‰ĐœĐŸŃŃ‚ŃŒŃŽ

    Measurement of prompt D0^{0} and D‟\overline{D}0^{0} meson azimuthal anisotropy and search for strong electric fields in PbPb collisions at root SNN\sqrt{S_{NN}} = 5.02 TeV

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    The strong Coulomb field created in ultrarelativistic heavy ion collisions is expected to produce a rapiditydependent difference (Av2) in the second Fourier coefficient of the azimuthal distribution (elliptic flow, v2) between D0 (uc) and D0 (uc) mesons. Motivated by the search for evidence of this field, the CMS detector at the LHC is used to perform the first measurement of Av2. The rapidity-averaged value is found to be (Av2) = 0.001 ? 0.001 (stat)? 0.003 (syst) in PbPb collisions at ?sNN = 5.02 TeV. In addition, the influence of the collision geometry is explored by measuring the D0 and D0mesons v2 and triangular flow coefficient (v3) as functions of rapidity, transverse momentum (pT), and event centrality (a measure of the overlap of the two Pb nuclei). A clear centrality dependence of prompt D0 meson v2 values is observed, while the v3 is largely independent of centrality. These trends are consistent with expectations of flow driven by the initial-state geometry. ? 2021 The Author. Published by Elsevier B.V. This is an open access article under the CC BY licens

    Measurement of the CP-violating phase ϕs_{s} in the B0^{0}s_{s}→J/ψ φ(1020) →ΌâșΌ⁻KâșK⁻ channel in proton-proton collisions at √s = 13 TeV

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    Observation of electroweak production of Wγ with two jets in proton-proton collisions at √s = 13 TeV

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    A first observation is presented for the electroweak production of a W boson, a photon, and two jets in proton-proton collisions. The W boson decays are selected by requiring one identified electron or muon and an imbalance in transverse momentum. The two jets are required to have a high dijet mass and a large separation in pseudorapidity. The measurement is based on data collected with the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb−1^{-1}. The observed (expected) significance for this process is 4.9 (4.6) standard deviations. After combining with previously reported CMS results at 8 TeV, the observed (expected) significance is 5.3 (4.8) standard deviations. The cross section for the electroweak Wγjj_{γjj} production in a restricted fiducial region is measured as 20.4 +/- 4.5 fb and the total cross section for Wγ_{γ} production in association with 2 jets in the same fiducial region is 108 +/- 16 fb. All results are in good agreement with recent theoretical predictions. Constraints are placed on anomalous quartic gauge couplings in terms of dimension-8 effective field theory operators

    Measurement of the azimuthal anisotropy of Y(1S) and Y(2S) mesons in PbPb collisions at √S^{S}NN = 5.02 TeV

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    The second-order Fourier coefficients (υ2_{2}) characterizing the azimuthal distributions of ΄(1S) and ΄(2S) mesons produced in PbPb collisions at sNN\sqrt{s_{NN}} = 5.02 TeV are studied. The ΄mesons are reconstructed in their dimuon decay channel, as measured by the CMS detector. The collected data set corresponds to an integrated luminosity of 1.7 nb−1^{-1}. The scalar product method is used to extract the υ2_{2} coefficients of the azimuthal distributions. Results are reported for the rapidity range |y| < 2.4, in the transverse momentum interval 0 < pT_{T} < 50 GeV/c, and in three centrality ranges of 10–30%, 30–50% and 50–90%. In contrast to the J/ψ mesons, the measured υ2_{2} values for the ΄ mesons are found to be consistent with zero

    Performance of the CMS Level-1 trigger in proton-proton collisions at √s = 13 TeV

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    At the start of Run 2 in 2015, the LHC delivered proton-proton collisions at a center-of-mass energy of 13\TeV. During Run 2 (years 2015–2018) the LHC eventually reached a luminosity of 2.1× 1034^{34} cm−2^{-2}s−1^{-1}, almost three times that reached during Run 1 (2009–2013) and a factor of two larger than the LHC design value, leading to events with up to a mean of about 50 simultaneous inelastic proton-proton collisions per bunch crossing (pileup). The CMS Level-1 trigger was upgraded prior to 2016 to improve the selection of physics events in the challenging conditions posed by the second run of the LHC. This paper describes the performance of the CMS Level-1 trigger upgrade during the data taking period of 2016–2018. The upgraded trigger implements pattern recognition and boosted decision tree regression techniques for muon reconstruction, includes pileup subtraction for jets and energy sums, and incorporates pileup-dependent isolation requirements for electrons and tau leptons. In addition, the new trigger calculates high-level quantities such as the invariant mass of pairs of reconstructed particles. The upgrade reduces the trigger rate from background processes and improves the trigger efficiency for a wide variety of physics signals
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