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

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Chapter 3: Lum<strong>in</strong>osity <strong>Measurement</strong> at <strong>the</strong> LHC and <strong>in</strong> ATLAS 76<br />

directions. Several sets <strong>of</strong> scans have been performed <strong>in</strong> ATLAS dur<strong>in</strong>g <strong>the</strong> 2010<br />

data-tak<strong>in</strong>g [94], <strong>the</strong> results from one <strong>of</strong> which is shown <strong>in</strong> Figure 3.4. In this case,<br />

<strong>the</strong> rate <strong>of</strong> production <strong>of</strong> primary vertices was monitored <strong>in</strong> <strong>the</strong> ATLAS <strong>in</strong>ner detector<br />

as <strong>the</strong> beams were displaced aga<strong>in</strong>st each o<strong>the</strong>r. Each distribution was fitted with<br />

a double Gaussian with a common mean. The beam sizes thus determ<strong>in</strong>ed were<br />

47.3 ± 0.2 µm and 56.3 ± 0.3 µm respectively <strong>in</strong> <strong>the</strong> horizontal and vertical planes.<br />

We see that <strong>the</strong> accuracy from <strong>the</strong> fits is at <strong>the</strong> per mille level.<br />

3.2.3 Beam pr<strong>of</strong>ile measurement<br />

Several technologies are used at <strong>the</strong> LHC for measur<strong>in</strong>g beam pr<strong>of</strong>ile (bunch shape)<br />

<strong>in</strong> <strong>the</strong> transverse and longitud<strong>in</strong>al directions. We will briefly discuss three <strong>of</strong> <strong>the</strong>m:<br />

• sc<strong>in</strong>tillator and optical transition radiation monitors<br />

• wire scanners<br />

• synchrotron light monitors<br />

Sc<strong>in</strong>tillator and optical transition radiation (OTR) monitors: The basic<br />

concept here is to place a th<strong>in</strong> metal screen <strong>in</strong> <strong>the</strong> beam path. A sc<strong>in</strong>tillator screen<br />

is usually a doped alum<strong>in</strong>a foil, usable only for low-<strong>in</strong>tensity beams. Beam particles<br />

produce sc<strong>in</strong>tillation photons, which can be observed on a TV screen. An OTR<br />

monitor consists <strong>of</strong> a very th<strong>in</strong> titanium screen. Charged particles travers<strong>in</strong>g <strong>the</strong><br />

<strong>in</strong>terface between vacuum and <strong>the</strong> metal screen emit transition radiation photons.<br />

Two cones for backward OTR are produced around <strong>the</strong> angle <strong>of</strong> reflection, as well as

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