134 research outputs found

    Maxwell-Bloch equation and Correlation function for penetrable Bose gas

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    We consider the quantum nonlinear Schr\"odinger equation in one space and one time dimension. We are interested in the non-free-fermionic case. We consider static temperature-dependent correlation functions. The determinant representation for correlation functions simplifies in the small mass limit of the Bose particle. In this limit we describe the correlation functions by the vacuum expectation value of a boson-valued solution for Maxwell-Bloch differential equation. We evaluate long-distance asymptotics of correlation functions in the small mass limit.Comment: LaTEX file, 20 pages, to appear J. Phys. A (1997

    Non-homogeneous systems of hydrodynamic type possessing Lax representations

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    We consider 1+1 - dimensional non-homogeneous systems of hydrodynamic type that possess Lax representations with movable singularities. We present a construction, which provides a wide class of examples of such systems with arbitrary number of components. In the two-component case a classification is given.Comment: 22 pages, latex, minor change

    A new design for a green calcium indicator with a smaller size and a reduced number of calcium-binding sites

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    Genetically encoded calcium indicators (GECIs) are mainly represented by two- or one-fluorophore-based sensors. One type of two-fluorophore-based sensor, carrying Opsanus troponin C (TnC) as the Ca2+-binding moiety, has two binding sites for calcium ions, providing a linear response to calcium ions. One-fluorophore-based sensors have four Ca2+-binding sites but are better suited for in vivo experiments. Herein, we describe a novel design for a one-fluorophore-based GECI with two Ca2+-binding sites. The engineered sensor, called NTnC, uses TnC as the Ca2+-binding moiety, inserted in the mNeonGreen fluorescent protein. Monomeric NTnC has higher brightness and pH-stability in vitro compared with the standard GECI GCaMP6s. In addition, NTnC shows an inverted fluorescence response to Ca2+. Using NTnC, we have visualized Ca2+ dynamics during spontaneous activity of neuronal cultures as confirmed by control NTnC and its mutant, in which the affinity to Ca2+ is eliminated. Using whole-cell patch clamp, we have demonstrated that NTnC dynamics in neurons are similar to those of GCaMP6s and allow robust detection of single action potentials. Finally, we have used NTnC to visualize Ca2+ neuronal activity in vivo in the V1 cortical area in awake and freely moving mice using two-photon microscopy or an nVista miniaturized microscope

    Π”ΠΈΡ„Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Π°Ρ экспрСссия ΠΌΠΈΠΊΡ€ΠΎΠ ΠΠš ΠΈ ΠΈΡ… Π³Π΅Π½ΠΎΠ²-мишСнСй ΠΏΡ€ΠΈ Ρ†Π΅Ρ€Π²ΠΈΠΊΠ°Π»ΡŒΠ½Ρ‹Ρ… ΠΈΠ½Ρ‚Ρ€Π°ΡΠΏΠΈΡ‚Π΅Π»ΠΈΠ°Π»ΡŒΠ½Ρ‹Ρ… нСоплазиях Ρ€Π°Π·Π½ΠΎΠΉ стСпСни тяТСсти

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    Background. Currently, little is known about the specific microRNAs involved in the development of cervical intraepithelial neoplasia (CIN1, 2, 3) and the transition to cancer in situ (CIS). Our meta-analysis allowed us to isolate 8 microRNAs (hsa-miR-1246, hsa-miR- 145-5p, hsa-miR-196b-5p, hsa-miR-34a-5p, hsa-miR-20a-5p, hsa-miR-21-5p, hsa-miR-375-5p, hsa-miR-96-5p) with potential significance in the progression of precancerous diseases to cervical cancer. Objective: to analyze the expression features of hsa-miR-1246, hsa-miR-145-5p, hsa-miR-196b-5p, hsa-miR-34a-5p, hsa-miR-20a-5p, hsa-miR-21-5p, hsa-miR-375-5p, hsa-miR-96-5p and their target genes, as well as genes associated with them in common signaling pathways in the tissues of the cervix in patients with CIN1–3 and CIS. Materials and methods. To assess the expression level of microRNA and matrixRNA, the quantitative polymerase chain reaction in real time method was used. Data analysis was carried out in the Python programming language using the SciPy library. Search for target genes was performed using the TarPmiR algorithm and the overrepresentation of microRNAs in signaling pathways (Over-Representation Analysis) was analyzed. To identify genes associated with target genes in common signaling pathways, GIANT (Genome-scale Integrated Analysis of gene Networks in Tissues) and network integration with several associations algorithms were used. Results. For microRNAs miR-145, miR-196b, miR-34a, miR-20a, miR-21, miR-375 and miR-96 a decrease in expression was found in the subgroup of patients with CIS, while for 4 microRNAs (miR-145, miR-34a, miR-20a and miR-375), an increase in the expression level was found for CIN1, 2. The detected features of microRNA expression in subgroups of patients with CIN1–3 and CIS also affected the expression of their target genes (CDKN2A, MKI67, TOP2A and CD82), as well as the genes associated with them in common signaling pathways (PGK1, THBS4 (TSP4) and ECM1). Conclusion. Thus, the study revealed that each degree of CIN is characterized by its own specific molecular profile – the differential expression of microRNAs, their target genes and the genes associated with them in the general signaling pathways.Π’Π²Π΅Π΄Π΅Π½ΠΈΠ΅. Π’ настоящСС врСмя нСдостаточно извСстно ΠΎ спСцифичСских ΠΌΠΈΠΊΡ€ΠΎΠ ΠΠš (мкРНК), задСйствованных Π² Ρ€Π°Π·Π²ΠΈΡ‚ΠΈΠΈ Ρ†Π΅Ρ€Π²ΠΈΠΊΠ°Π»ΡŒΠ½ΠΎΠΉ ΠΈΠ½Ρ‚Ρ€Π°ΡΠΏΠΈΡ‚Π΅Π»ΠΈΠ°Π»ΡŒΠ½ΠΎΠΉ Π½Π΅ΠΎΠΏΠ»Π°Π·ΠΈΠΈ I, II, III стСпСнСй тяТСсти (CIN1, 2, 3) ΠΈ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π΅ ΠΊ ΠΊΠ°Ρ€Ρ†ΠΈΠ½ΠΎΠΌΠ΅ in situ (CIS). ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π½Ρ‹ΠΉ Π½Π°ΠΌΠΈ Ρ€Π°Π½Π΅Π΅ ΠΌΠ΅Ρ‚Π°Π°Π½Π°Π»ΠΈΠ· ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ» Π²Ρ‹Π΄Π΅Π»ΠΈΡ‚ΡŒ 8 мкРНК (hsa-miR-1246, hsa-miR-145-5p, hsa-miR-196b-5p, hsa-miR-34a-5p, hsa-miR-20a-5p, hsa-miR-21-5p, hsa-miR-375-5p, hsa-miR-96-5p), ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‰ΠΈΡ… ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½ΠΎΠΉ Π·Π½Π°Ρ‡ΠΈΠΌΠΎΡΡ‚ΡŒΡŽ Π² прогрСссировании ΠΏΡ€Π΅Π΄Ρ€Π°ΠΊΠΎΠ²Ρ‹Ρ… Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ Π² Ρ€Π°ΠΊ шСйки ΠΌΠ°Ρ‚ΠΊΠΈ. ЦСль исслСдования – Π°Π½Π°Π»ΠΈΠ· особСнностСй экспрСссии hsa-miR-1246, hsa-miR-145-5p, hsa-miR-196b-5p, hsa-miR-34a-5p, hsa-miR- 20a-5p, hsa-miR-21-5p, hsa-miR-375-5p, hsa-miR-96-5p ΠΈ ΠΈΡ… Π³Π΅Π½ΠΎΠ²-мишСнСй, Π° Ρ‚Π°ΠΊΠΆΠ΅ Π³Π΅Π½ΠΎΠ², ассоциированных с Π½ΠΈΠΌΠΈ Π² ΠΎΠ±Ρ‰ΠΈΡ… ΡΠΈΠ³Π½Π°Π»ΡŒΠ½Ρ‹Ρ… путях, Π² тканях шСйки ΠΌΠ°Ρ‚ΠΊΠΈ Ρƒ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠΊ с CIN1–3 ΠΈ CIS. ΠœΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Ρ‹ ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹. Для ΠΎΡ†Π΅Π½ΠΊΠΈ уровня экспрСссии мкРНК ΠΈ ΠΌΠ°Ρ‚Ρ€ΠΈΡ‡Π½ΠΎΠΉ РНК использовали ΠΌΠ΅Ρ‚ΠΎΠ΄ количСствСнной ΠΏΠΎΠ»ΠΈΠΌΠ΅Ρ€Π°Π·Π½ΠΎΠΉ Ρ†Π΅ΠΏΠ½ΠΎΠΉ Ρ€Π΅Π°ΠΊΡ†ΠΈΠΈ Π² Ρ€Π΅ΠΆΠΈΠΌΠ΅ Ρ€Π΅Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ. Анализ Π΄Π°Π½Π½Ρ‹Ρ… ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Π½Π° языкС программирования Python с использованиСм Π±ΠΈΠ±Π»ΠΈΠΎΡ‚Π΅ΠΊΠΈ SciPy. Поиск Π³Π΅Π½ΠΎΠ²-мишСнСй осущСствляли с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠ° TarPmiR ΠΈ Π°Π½Π°Π»ΠΈΠ·ΠΈΡ€ΠΎΠ²Π°Π»ΠΈ ΠΈΠ·Π±Ρ‹Ρ‚ΠΎΡ‡Π½ΡƒΡŽ ΠΏΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Π½ΠΎΡΡ‚ΡŒ мкРНК Π² ΡΠΈΠ³Π½Π°Π»ΡŒΠ½Ρ‹Ρ… путях (Over-Representation Analysis). Для выявлСния Π³Π΅Π½ΠΎΠ², ассоциированных с Π³Π΅Π½Π°ΠΌΠΈ-мишСнями Π² ΠΎΠ±Ρ‰ΠΈΡ… ΡΠΈΠ³Π½Π°Π»ΡŒΠ½Ρ‹Ρ… путях, использовали Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΡ‹ GIANT (Genome-scale Integrated Analysis of gene Networks in Tissues) ΠΈ «сСтСвая интСграция с нСсколькими ассоциациями». Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. Для мкРНК miR-145, miR-196b, miR-34a, miR-20a, miR-21, miR-375 ΠΈ miR-96 ΠΎΠ±Π½Π°Ρ€ΡƒΠΆΠ΅Π½ΠΎ сниТСниС экспрСссии Π² ΠΏΠΎΠ΄Π³Ρ€ΡƒΠΏΠΏΠ΅ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠΊ с CIS, ΠΏΡ€ΠΈ этом для 4 мкРНК (miR-145, miR-34a, miR-20a ΠΈ miR-375) выявлСно ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΠ΅ уровня экспрСссии ΠΏΡ€ΠΈ CIN1, 2. ΠžΠ±Π½Π°Ρ€ΡƒΠΆΠ΅Π½Π½Ρ‹Π΅ особСнности экспрСссии мкРНК Π² ΠΏΠΎΠ΄Π³Ρ€ΡƒΠΏΠΏΠ°Ρ… ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠΊ с CIN1–3 ΠΈ CIS Π±Ρ‹Π»ΠΈ ассоциированы с экспрСссиСй ΠΈΡ… Π³Π΅Π½ΠΎΠ²-мишСнСй (CDKN2A, MKI67, TOP2A ΠΈ CD82), Π° Ρ‚Π°ΠΊΠΆΠ΅ Π³Π΅Π½ΠΎΠ², связанных с Π½ΠΈΠΌΠΈ Π² ΠΎΠ±Ρ‰ΠΈΡ… ΡΠΈΠ³Π½Π°Π»ΡŒΠ½Ρ‹Ρ… путях (PGK1, THBS4 (TSP4) ΠΈ ECM1). Π—Π°ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ исслСдования ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΈ ΡƒΡΡ‚Π°Π½ΠΎΠ²ΠΈΡ‚ΡŒ, Ρ‡Ρ‚ΠΎ каТдая ΡΡ‚Π΅ΠΏΠ΅Π½ΡŒ CIN характСризуСтся особым молСкулярным ΠΏΡ€ΠΎΡ„ΠΈΠ»Π΅ΠΌ – Π΄ΠΈΡ„Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½ΠΎΠΉ экспрСссиСй мкРНК, ΠΈΡ… Π³Π΅Π½ΠΎΠ²-мишСнСй ΠΈ Π³Π΅Π½ΠΎΠ², ассоциированных с Π½ΠΈΠΌΠΈ Π² ΠΎΠ±Ρ‰ΠΈΡ… ΡΠΈΠ³Π½Π°Π»ΡŒΠ½Ρ‹Ρ… путях

    Transverse-momentum-dependent Multiplicities of Charged Hadrons in Muon-Deuteron Deep Inelastic Scattering

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    A semi-inclusive measurement of charged hadron multiplicities in deep inelastic muon scattering off an isoscalar target was performed using data collected by the COMPASS Collaboration at CERN. The following kinematic domain is covered by the data: photon virtuality Q2>1Q^{2}>1 (GeV/cc)2^2, invariant mass of the hadronic system W>5W > 5 GeV/c2c^2, Bjorken scaling variable in the range 0.003<x<0.40.003 < x < 0.4, fraction of the virtual photon energy carried by the hadron in the range 0.2<z<0.80.2 < z < 0.8, square of the hadron transverse momentum with respect to the virtual photon direction in the range 0.02 (GeV/c)2<PhT2<3c)^2 < P_{\rm{hT}}^{2} < 3 (GeV/cc)2^2. The multiplicities are presented as a function of PhT2P_{\rm{hT}}^{2} in three-dimensional bins of xx, Q2Q^2, zz and compared to previous semi-inclusive measurements. We explore the small-PhT2P_{\rm{hT}}^{2} region, i.e. PhT2<1P_{\rm{hT}}^{2} < 1 (GeV/cc)2^2, where hadron transverse momenta are expected to arise from non-perturbative effects, and also the domain of larger PhT2P_{\rm{hT}}^{2}, where contributions from higher-order perturbative QCD are expected to dominate. The multiplicities are fitted using a single-exponential function at small PhT2P_{\rm{hT}}^{2} to study the dependence of the average transverse momentum ⟨PhT2⟩\langle P_{\rm{hT}}^{2}\rangle on xx, Q2Q^2 and zz. The power-law behaviour of the multiplicities at large PhT2P_{\rm{hT}}^{2} is investigated using various functional forms. The fits describe the data reasonably well over the full measured range.Comment: 28 pages, 20 figure

    Search for Axionlike and Scalar Particles with the NA64 Experiment

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    We carried out a model-independent search for light scalar (s) and pseudoscalar axionlike (a) particles that couple to two photons by using the high-energy CERN SPS H4 electron beam. The new particles, if they exist, could be produced through the Primakoff effect in interactions of hard bremsstrahlung photons generated by 100 GeV electrons in the NA64 active dump with virtual photons provided by the nuclei of the dump. The a(s) would penetrate the downstream HCAL module, serving as shielding, and would be observed either through their a(s)β†’Ξ³Ξ³a(s)\to\gamma \gamma decay in the rest of the HCAL detector or as events with large missing energy if the a(s) decays downstream of the HCAL. This method allows for the probing the a(s) parameter space, including those from generic axion models, inaccessible to previous experiments. No evidence of such processes has been found from the analysis of the data corresponding to 2.84Γ—10112.84\times10^{11} electrons on target allowing to set new limits on the a(s)Ξ³Ξ³a(s)\gamma\gamma-coupling strength for a(s) masses below 55 MeV.Comment: This publication is dedicated to the memory of our colleague Danila Tlisov. 7 pages, 5 figures, revised version accepted for publication in Phys. Rev. Let

    Constraints on New Physics in the Electron g-2 from a Search for Invisible Decays of a Scalar, Pseudoscalar, Vector, and Axial Vector

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    We performed a search for a new generic XX boson, which could be a scalar (SS), pseudoscalar (PP), vector (VV) or an axial vector (AA) particle produced in the 100 GeV electron scattering off nuclei, eβˆ’Zβ†’eβˆ’ZXe^- Z \to e^- Z X, followed by its invisible decay in the NA64 experiment at CERN. No evidence for such process was found in the full NA64 data set of 2.84Γ—10112.84\times 10^{11} electrons on target. We place new bounds on the S,P,V,AS, P, V, A coupling strengths to electrons, and set constraints on their contributions to the electron anomalous magnetic moment aea_e, βˆ£Ξ”aXβˆ£β‰²10βˆ’15βˆ’10βˆ’13|\Delta a_{X}| \lesssim 10^{-15} - 10^{-13} for the XX mass region mX≲1m_X\lesssim 1 GeV. These results are an order of magnitude more sensitive compared to the current accuracy on aea_e from the electron gβˆ’2g-2 experiments and recent high-precision determination of the fine structure constant.Comment: 6 pages, 4 figure

    Hunting down the X17 boson at the CERN SPS

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    Recently, the ATOMKI experiment has reported new evidence for the excess of e+eβˆ’e^+ e^- events with a mass ∼\sim17 MeV in the nuclear transitions of 4^4He, that they previously observed in measurements with 8^8Be. These observations could be explained by the existence of a new vector X17X17 boson. So far, the search for the decay X17β†’e+eβˆ’X17 \rightarrow e^+ e^- with the NA64 experiment at the CERN SPS gave negative results. Here, we present a new technique that could be implemented in NA64 aiming to improve the sensitivity and to cover the remaining X17X17 parameter space. If a signal-like event is detected, an unambiguous observation is achieved by reconstructing the invariant mass of the X17X17 decay with the proposed method. To reach this goal an optimization of the X17X17 production target, as well as an efficient and accurate reconstruction of two close decay tracks, is required. A dedicated analysis of the available experimental data making use of the trackers information is presented. This method provides independent confirmation of the NA64 published results [Phys. Rev. D101, 071101 (2020)], validating the tracking procedure. The detailed Monte Carlo study of the proposed setup and the background estimate shows that the goal of the proposed search is feasible
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