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Measurement of the Z boson cross-section in - Harvard University ...

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Chapter 4: Data Collection and Event Reconstruction 109<br />

ATLAS uses two methods for <strong>of</strong>fl<strong>in</strong>e beaml<strong>in</strong>e reconstruction: one based on pri-<br />

mary vertices, and <strong>the</strong> o<strong>the</strong>r on tracks. The vertex-based method estimates <strong>the</strong><br />

position and <strong>the</strong> Gaussian width <strong>of</strong> <strong>the</strong> beaml<strong>in</strong>e <strong>in</strong> all three coord<strong>in</strong>ates and deter-<br />

m<strong>in</strong>es <strong>the</strong> slope along <strong>the</strong> x and y coord<strong>in</strong>ates. Start<strong>in</strong>g with primary vertices from<br />

a suitably large number <strong>of</strong> bunch <strong>cross</strong><strong>in</strong>gs, <strong>the</strong> algorithm first performs a simple<br />

χ 2 m<strong>in</strong>imization to roughly estimate <strong>the</strong> position and slope <strong>of</strong> <strong>the</strong> beaml<strong>in</strong>e. Then<br />

it carries out a full parameter estimation us<strong>in</strong>g an unb<strong>in</strong>ned log-likelihood method,<br />

with specific selection criteria be<strong>in</strong>g applied to <strong>the</strong> positions and error matrices <strong>of</strong> <strong>the</strong><br />

primary vertices.<br />

The track-based method determ<strong>in</strong>es <strong>the</strong> position and slope <strong>of</strong> <strong>the</strong> beaml<strong>in</strong>e, but<br />

does not give width <strong>in</strong>formation. It starts with a suitably large number <strong>of</strong> tracks<br />

and performs a χ 2 m<strong>in</strong>imization [3]. Only tracks associated with primary vertices are<br />

used <strong>in</strong> <strong>the</strong> fit.<br />

Note that simplified versions <strong>of</strong> <strong>the</strong>se two algorithms can also run onl<strong>in</strong>e at Level-3<br />

for fast beaml<strong>in</strong>e reconstruction on short time scales (≈ few seconds) and feedback<br />

to <strong>the</strong> LHC.<br />

Electron reconstruction <strong>in</strong> <strong>the</strong> <strong>in</strong>ner detector<br />

Depend<strong>in</strong>g on <strong>the</strong> pseudorapidity, electrons lose between 20% and 50% <strong>of</strong> <strong>the</strong>ir<br />

energy <strong>in</strong> <strong>the</strong> form <strong>of</strong> bremsstrahlung before leav<strong>in</strong>g <strong>the</strong> SCT [17]. Energy loss leads to<br />

change <strong>in</strong> <strong>the</strong> track curvature <strong>of</strong> electrons, with <strong>the</strong> result that it becomes difficult to<br />

reconstruct <strong>the</strong> tracks and accurately measure track parameters. The measurements<br />

can be improved substantially, however, if <strong>the</strong> track fit takes possible bremsstrahlung<br />

losses <strong>in</strong>to account.

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