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Simulation on the Response of the STAR HFT Pixel Detector Alex Cimaroli 07/23/09
Simulation on the Response of the STAR HFT Pixel Detector Alex Cimaroli 07/23/09

... Quarks come in six varieties: up, down, strange, charm, bottom, and top. Gluons bind quarks into mesons (2 quarks) and baryons (3 quarks) – this is called “confinement”. ...
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... the electrode, which places the electrode at a much higher potential than the surrounding glass. There now exists a strong electric field within the glass dome. The electric field is strong enough to ionize some of the inert gas particles, leaving a neutral mixture of electrons and ions. This ionize ...
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Kovchegov2 - Institute for Nuclear Theory
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Understanding Nothing - University of Southampton
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... Every so often quantum effects create a quark anti-quark pair. The attractive force is so strong that binding energy >> mass energy The vacuum has lower energy if it fills itself with quark antiquark pairs! ...
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1.1 Principles of nuclear fusion

... In order to achieve fusion, the reacting nuclei have to get very close to each other to activate the strong nuclear force. However, there is a large electrostatic repulsion between them as they come together because the protons in nuclei are positively charged. There is several possibilities how to ...
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An Introduction to the Standard Model of Particle Physics

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Search for Heavy, Long-Lived Neutral Particles that Decay to

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... divided into smaller parts by physical means, yet that they have structure, was shared by prominent scientists well into the nineteenth century AD. The Roman poet Lucretius (98–55 BC) was an eloquent exponent of the theory that atoms, infinite in number but limited in their varieties, are, along wit ...
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... Theory describe the data within the measured uncertainties. Other centralities show similar IAA(pt) within current uncertainties which contradict the picture of volume and surface emission. ...
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... example, one can use it to gain some information about the number of elementary building blocks of matter-quarks and leptons. The present picture of particle physics is that mesons and baryons are two or three quark composites, respectively. Quarks and leptons are arranged in "generations." The firs ...
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... becomes substrate of subsequent reactions. A second band, Figure 1, results from a latter drop of temperature allowing particles in which electroweak interaction became manifest and the deconfined energy supports the creation of new particles. As the distances between pions became greater than 1 Fer ...
The ATLAS Detector - University of Birmingham
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... the paths, momentum and energy of the We’re used to living in 3 dimensions but could it be particles thrown out of proton collisions, possible for there to be more? allowing them to be individually identified. Evidence for the existence of extra dimensions could be the extreme At 46m long with a 25m ...
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... their rest-mass (mc2) energies. • At the very high densities, collisions between particles were very frequent, keeping all `species' of particles very close to thermal equilibrium (same amount of mass energy per particle) • A few seconds after the Big Bang, the main particle species present were pro ...
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... But: sometimes, surface terms are important Instantons: classical Euclidean solutions of QCD which map color SU(2) onto the sphere S3; in Minkowski space, describe quantum tunneling between ...
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Strangeness production



Strangeness production is a signature and a diagnostic tool of quark–gluon plasma (or QGP) formation and properties. Unlike up and down quarks, from which everyday matter is made, strange quarks are formed in pair-production processes in collisions between constituents of the plasma. The dominant mechanism of production involves gluons only present when matter has become a quark–gluon plasma. When quark–gluon plasma disassembles into hadrons in a breakup process, the high availability of strange antiquarks helps to produce antimatter containing multiple strange quarks, which is otherwise rarely made. Similar considerations are at present made for the heavier charm flavor, which is made at the beginning of the collision process in the first interactions and is only abundant in the high-energy environments of CERN's Large Hadron Collider.
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