Constraining the magnitude of the chiral magnetic effect with event shape engineering in Pb-Pb collisions at root s(NN)=2.76 TeV

CNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICOFINEP - FINANCIADORA DE ESTUDOS E PROJETOSFAPESP - FUNDAÇÃO DE AMPARO À PESQUISA DO ESTADO DE SÃO PAULOIn ultrarelativistic heavy-ion collisions, the event-by-event variation of the elliptic flow v(2) reflects fluctuations in the shape of the initial state of the system. This allows to select events with the same centrality but different initial geometry. This selection technique, Event Shape Engineering, has been used in the analysis of charge-dependent two-and three-particle correlations in Pb-Pb collisions at root s(NN) = 2.76 TeV. The two-particle correlator < cos(phi(alpha) - phi(ss))gt;, calculated for different combinations of charges alpha and beta, is almost independent of v(2) (for a given centrality), while the three-particle correlator < cos(phi(alpha) + phi(beta) - 2 Psi(2))gt; scales almost linearly both with the event v(2) and charged-particle pseudorapidity density. The charge dependence of the three-particle correlator is often interpreted as evidence for the Chiral Magnetic Effect (CME), a parity violating effect of the strong interaction. However, its measured dependence on v(2) points to a large non-CME contribution to the correlator. Comparing the results with Monte Carlo calculations including a magnetic field due to the spectators, the upper limit of the CME signal contribution to the three-particle correlator in the 10-50% centrality interval is found to be 26-33% at 95% confidence level.777151162CNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICOFINEP - FINANCIADORA DE ESTUDOS E PROJETOSFAPESP - FUNDAÇÃO DE AMPARO À PESQUISA DO ESTADO DE SÃO PAULOCNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICOFINEP - FINANCIADORA DE ESTUDOS E PROJETOSFAPESP - FUNDAÇÃO DE AMPARO À PESQUISA DO ESTADO DE SÃO PAULOSem informaçãoSem informaçãoSem informaçãoAgências de fomento estrangeiras apoiaram essa pesquisa, mais informações acesse artig

Molecular Monitoring of RUNX1-RUNX1T1 Transcript Level in Acute Myeloblastic Leukemias on Treatment

Background. The current approach to treatment of acute myeloblastic leukemia (AML) includes the achievement of maximum tumor reduction and, therefore, eradication of a leukemic clone. The goal of the therapy is to achieve undetectable levels of the target gene, except an isolated molecular rearrangement of RUNX1-RUNX1T1. Aim. To estimate the dynamics of the RUNX1-RUNX1T1 level and relevant clinical manifestations during the monitoring of various stages of the program therapy and after its completion. Methods. The article presents a description of 10 cases of AML with isolated RUNX1-RUNX1T1 expression (n = 4) and the expression in combination with different molecular and cytogenetic abnormalities (n = 6). In addition, a long-term monitoring of the gene expression by quantitative determination of RUNX1-RUNX1T1 using a real-time PCR was presented. Results. The incidence of relapses in a group with a decreased RUNX1-RUNX1T1 expression level of >2 log is 75 % as compared to patients with a less significant reduction of the transcript level (with the relapse incidence equal to 0 %) (p = 0.05). The increase of the RUNX1-RUNX1T1 level against the background of bone marrow remission by more than 1 log coincided with a bone marrow relapse within 5–18 weeks. In addition, long-term persistence of a certain transcript level after the completion of a program therapy without relapse is possible. Conclusion. The study analyzed possible molecular background of different clinical outcomes of long-term persistence of the RUNX1-RUNX1T1 transcript that might lead to an individualized approach to AML patients

‘Photonic Hook’ based optomechanical nanoparticle manipulator

Abstract Specialized electromagnetic fields can be used for nanoparticle manipulation along a specific path, allowing enhanced transport and control over the particle’s motion. In this paper, we investigate the optical forces produced by a curved photonic jet, otherwise known as the “photonic hook”, created using an asymmetric cuboid. In our case, this cuboid is formed by appending a triangular prism to one side of a cube. A gold nanoparticle immersed in the cuboid’s transmitted field moves in a curved trajectory. This result could be used for moving nanoparticles around obstacles; hence we also consider the changes in the photonic hook’s forces when relatively large glass and gold obstacles are introduced at the region where the curved photonic jet is created. We show, that despite the obstacles, perturbing the field distribution, a particle can move around glass obstacles of a certain thickness. For larger glass slabs, the particle will be trapped stably near it. Moreover, we noticed that a partial obstruction of the photonic jet’s field using the gold obstacle results in a complete disruption of the particle’s trajectory