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Reproduction of the blue mussel Mytilus galloprovincialis in wild populations follows seasonal changes of environmental factors such as food availability.The aim of this experiment was to analyse the effects of three conditioning diets on the maturation and development of M. galloprovincialis. We experimented three different algae-based treatments: two Non-Tetraselmis (NT) groups and one Tetraselmis (TS) group. Those in the NT groups received a mixture of Isochrysis galbana (clon T-Iso) and Chaetoceros sp. (1:1, based on cell volume). Those in the TS group received Isochrysis sp. (T-Iso), Chaetoceros sp., and Tetraselmis suecica (1:1:1, based on cell volume). Mussels in the NT-1, NT-2 and TS groups received, respectively, 1%, 2% and 2% of the mussels dry weight (MDW) based in algae dry weight (ADW) a day. After 2 months of conditioning, significant changes between wild mussels and the NT-1 group were not detected either in condition index (CI) value or in gonad stadia percentages. On the opposite, after conditioning CI values of mussels having received 2 % ration were higher than those of wild populations and NT-1 group, and ripe female percentage was higher in the TS group than in the NT-2 group. As a conclusion, this study demonstrates that for M. galloprovincialis conditioning, 1% of the MDW in ADW is not enough, and that a varied diet is more suitable.This work was supported by Interreg Project 0251_ECOAQUA_5_E, financed by the EDRF (European Regional Development Fund). www.juntadeandalucia.es/agriculturaypesca/ifapa/ecoaqua. La reproducción del mejillón Mytilus galloprovincialis en las poblaciones naturales sigue los cambios estacionales de factores ambientales como la disponibilidad de comida. El objetivo de este experimento fue analizar los efectos de tres dietas de acondicionamiento en la maduración y el desarrollo de M. galloprovincialis. Para ello, se experimentaron tres tratamientos diferentes a base de microalgas: dos grupos sin la microalga Tetraselmis suecica (NT) y un tercero con esta microalga (TS). Los mejillones de los grupos NT recibieron una mezcla de Isochrysis galbana (clon T-Iso) y Chaetoceros sp. (1:1, basado en el volumen celular). Los del grupo de TS recibido I. galbana (clon T-Iso), Chaetoceros sp., y T. suecica (1:1:1, basado en el volumen celular). Los ejemplares de los grupos NT-1, NT-2 y TS recibieron, respectivamente, 1%, 2% y 2% del peso seco de la masa corporal (PSM) basado en el peso seco del fitoplancton (PSF) al día. Después de 2 meses de acondicionamiento no se detectaron diferencias significativas en el valor del índice de condición (IC) ni en los porcentajes de estadios de madurez gonadal entre los mejillones del medio natural y el grupo NT-1. Sin embargo, después del acondicionamiento valores del IC de los mejillones que recibieron el 2% de ración fueron superiores a los de las poblaciones del medio natural y el grupo NT-1. Además, el porcentaje de hembras maduras fue mayor en el grupo TS que en el grupo NT-2. Como conclusión, este estudio demuestra que para el acondicionamiento de M. galloprovincialis un 1% de la PSM en PSF no es suficiente, y que una dieta variada es más adecuada.Este trabajo fue apoyado por el proyecto Interreg 0251_ECOAQUA_5_E , financiado por el FEDER (Fondo Europeo de Desarrollo Regional). www.juntadeandalucia.es / agriculturaypesca / IFAPA / ecoaqua. &nbsp

Relato de modificação da técnica criostático-histoquímica para a verificação da fluorescência das catecolaminas e da serotonina em secções de tecido nervoso central e periférico. São discutidas as vantagens desta modificação técnica em relação a outras propostas para a mesma finalidade.

Laser calibration facilities play a key role in the study and characterization of detectors like electromagnetic or hadronie calorimeters. They can be operated both during physics data taking and off run. Typically these facilities are based on a lasers source which deliver light to each detector element via a light distribution system. The laser control system typically manages the interface between the experiment and the laser source, allowing the generation of light pulses according to specific needs as detector calibration, study of detector performance in running conditions, evaluation of DAQ performance. Any specific implementation depends on hardware features. As an example light pulses could be generated according to a physics distribution as it appens in physics run or real data taking. In this case light pulses should be generated according to a pattern which follows a programmable function and changes on a statistical base event by event. In this work we present a laser control system for calibration of a calorimeter. It is a custom solution based on an hybrid platform hosting an FPGA and an ARM processor. We present the system architecture and the performances of a preliminary implementation.

In the Muon g-2 Experiment at Fermilab, a calibration apparatus based on a set of laser sources and a distribution system has been designed and implemented by the INFN group. The light pulses are read by specific photo-detectors, whose signals are digitized by custom electronics modules designed to match the experimental requirements. The data frames of each module are transmitted to a controller board that performs the event-building process and transfers the reconstructed data to the online farm. In this work we present the architecture and data flow of the acquisition system that depends on the laser calibration program defined inside the Laser Control board. Experimental results on the overall system performances, also including the software processes running both at controller and farm level will be described.

The Muon g –2 experiment at Fermilab (E989) plans to measure the muon anomalous magnetic moment to a precision of 140 parts per billion (ppb), which corresponds to a total uncertainty of 1 . 6 × 1 0 − 10 . To achieve this level of precision the experiment must detect more than 1 . 8 × 1 0 11 decay positrons by using the 24 calorimeters distributed around the muon storage ring. Each calorimeter consists of 54 Pb F 2 crystals read out by SiPMs. The response of each of the 1296 channels must be calibrated and monitored to keep uncertainties due to gain fluctuations at the sub-per mil level in the time interval corresponding to one beam fill ( 700 μ s ) and at the sub-percent level on longer time scales. These requirements are much more demanding than those needed by most high energy physics experiments. This paper presents a novel laser-based calibration system that distributes light to all calorimeter cells, while allowing one to correct for laser intensity fluctuations and to monitor the distribution chain stability at unprecedented levels of accuracy. Results on the system performance during the first few months of stored muon operation in 2018 are also presented.

The new Muon g-2 experiment at Fermilab (E989) will measure the muon anomaly a μ = (g μ -2)/2 to an uncertainty of 16 x 10−11 (0.14 ppm). The experiment is running with a positive muon beam. The decay positrons are detected by 24 electromagnetic calorimeters placed on the inner radius of the magnetic storage ring. As the gain fluctuation of each calorimeter channel must be corrected to a few parts in 104, a state-of-art laser calibration system has been realized which provides short laser pulses to the calorimeters. The monitoring of these light signals is done by specific photo-detectors read by a specialized Monitoring Electronics, which is organized in devoted crates and performs the full data acquisition of the calibration signals starting from pre-amplification, then digitization and finally transfer of the information. Here we describe few key elements of the whole system, namely the single readout channel of the Monitoring Board.

In this paper we simulate the emission by charged particles in complex structures with help of Geant4. We take into account Cherenkov radiation, transition radiation, bremsstrahlung, pair production and other accompanying processes. As an application we investigate the full size electromagnetic calorimeter for the muon g-2 experiment at Fermilab. A calorimeter module (24 are expected in the experiment) consists of a Delrin front panel for installation of the laser calibration system, 54 PbF2 Cherenkov crystals wrapped by the black Millipore paper, and silicon photo-multiplier sensors. We report here on a simulation of radiation from positrons passing through the calorimeter system. We carry out the simulation using Geant4 toolkit, which provides a complete set of tools for all areas of detector simulation: geometry, tracking, detector response, run, event and track management, and visualization. We consider Cherenkov photons expansion when a positron moves down through the calorimeter at the arbitrary angle of incidence. Both spectral and angular distributions of Cherenkov optical photons in different parts of the calorimeter system have been evaluated as well as the transition radiation and pre-shower distributions from the panel and from the Al vacuum chamber of the storage ring. (The paper is in progress)., Comment: The 7th International Conference "Channeling 2016 - Charged & Neutral Particles Channeling Phenomena"/ in progress

The anomalous muon dipole magnetic moment can be measured (and calculated) with great precision thus providing insight on the Standard Model and new physics. Currently an experiment is under construction at Fermilab (U.S.A.) which is expected to measure the anomalous muon dipole magnetic moment with unprecedented precision. One of the improvements with respect to the previous experiments is expected to come from the laser calibration system which has been designed and constructed by the Italian part of the collaboration (INFN). Furthermore, an emphasis of this paper will be on the calibration system that is in the final stages of construction as well as the experiment which is expected to start data taking this year.

We report the test of many of the key elements of the laser-based calibration system for muon g - 2 experiment E989 at Fermilab. The test was performed at the Laboratori Nazionali di Frascati's Beam Test Facility using a 450 MeV electron beam impinging on a small subset of the final g - 2 lead-fluoride crystal calorimeter system. The calibration system was configured as planned for the E989 experiment and uses the same type of laser and most of the final optical elements. We show results regarding the calorimeter's response calibration, the maximum equivalent electron energy which can be provided by the laser and the stability of the calibration system components., Comment: Submitted to Nuclear Instrument and Methods A

The Muon g - 2 Experiment at Fermilab is expected to start data taking in 2017. It will measure the muon anomalous magnetic moment, a mu = (g mu - 2)/2 to an unprecedented precision: the goal is 0.14 parts per million (ppm). The new experiment will require upgrades of detectors, electronics and data acquisition equipment to handle the much higher data volumes and slightly higher instantaneous rates. In particular, it will require a continuous monitoring and state- of- art calibration of the detectors, whose response may vary on both the millisecond and hour long timescale. The calibration system is composed of six laser sources and a light distribution system will provide short light pulses directly into each crystal (54) of the 24 calorimeters which measure energy and arrival time of the decay positrons. A Laser Control board will manage the interface between the experiment and the laser source, allowing the generation of light pulses according to specific needs including detector calibration, study of detector performance in running conditions, evaluation of DAQ performance. Here we present and discuss the main features of the Laser Control board.