Tag: Diagnostic Tools

  • Imaging (MCP)

    Imaging (MCP)

    Imaging (MCP) Throughout the ALPHA experiment, charged particles such as electrons, positrons and antiprotons are stored inside devices known as Penning traps. Micro-channel plates (MCPs) are used to image clouds of particles that are extracted from these traps, allowing us to measure and optimise their properties for antihydrogen production. Each MCP is formed from a

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  • Faraday Cup

    Faraday Cup

    Faraday Cup We use a Faraday cup to measure the total number of particles in our electron and positron plasmas. The plasmas are “dumped” onto the cup, thereby generating a voltage on the cup relative to the total charge of the plasma (and the capacitance of the cup). The signal is small, on the order

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  • Scintillator Panels

    Scintillator Panels

    Scintillator Panels Scintillators can be made from plastic, and are therefore a relatively inexpensive technology. We use flat panels of scintillating plastic to make simple detectors for general diagnostics of antiprotons and positron. Back to Diagnostic Tools

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  • ECR magnetometry

    ECR magnetometry

    ECR magnetometry The behavior of electrons in the ALPHA apparatus is very sensitive to magnetic fields. Electrons move in circular orbits with a period that depends on the strength of the magnetic field. For strong magnetic fields the motion is fast, for small fields, the electrons move more slowly. ALPHA has developed a magnetic field

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  • Temperature measurements

    Temperature measurements

    Temperature measurements The plasma temperature is an important property in antihydrogen experiments because we must achieve very low temperatures of positrons and antiprotons in order to effectively synthesize antihydrogen. The plasma temperature is related to the kinetic energy of the particles in the plasma. For a single particle, we can simply define the kinetic energy

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  • Annihilation Detectors

    Annihilation Detectors

    Annihilation Detectors Annihilation Process When an antiproton and a proton come into contact, they will annihilate into a range of subatomic particles. The antiproton and the protons are destroyed. Above shows a typical example of the annihilation process. However, the annihilation products can include different numbers or selections of pions, some are statistically more common

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