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Chapter 3: Lum<strong>in</strong>osity <strong>Measurement</strong> at <strong>the</strong> LHC and <strong>in</strong> ATLAS 75<br />

3.2.2 Beam size measurement us<strong>in</strong>g Van der Meer scans<br />

An accurate method <strong>of</strong> measur<strong>in</strong>g <strong>the</strong> transverse beam size is to displace <strong>the</strong><br />

beams aga<strong>in</strong>st each o<strong>the</strong>r and monitor <strong>the</strong> relative lum<strong>in</strong>osity as a function <strong>of</strong> <strong>the</strong><br />

beam separation (Figure 3.4). Known as separation scans or Van der Meer scans,<br />

this method can also be used to m<strong>in</strong>imize <strong>the</strong> beam separation <strong>in</strong> order to maximize<br />

<strong>in</strong>stantaneous lum<strong>in</strong>osity.<br />

]<br />

−2<br />

p)<br />

11<br />

[Hz (10<br />

2<br />

/ N<br />

1<br />

Rate(PV|MBTS_1) / N<br />

12000<br />

10000<br />

8000<br />

6000<br />

4000<br />

2000<br />

ATLAS prelim<strong>in</strong>ary<br />

RMS: 50.0 µ m<br />

Σx:<br />

(47.3 ± 0.2) µ m<br />

0<br />

−300 −200 −100 0 100 200 300<br />

Δ x [ µ m]<br />

]<br />

−2<br />

p)<br />

11<br />

[Hz (10<br />

2<br />

/ N<br />

1<br />

Rate(PV|MBTS_1) / N<br />

12000<br />

10000<br />

8000<br />

6000<br />

4000<br />

2000<br />

ATLAS prelim<strong>in</strong>ary<br />

RMS: 60.6 µ m<br />

Σy:<br />

(56.3 ± 0.3) µ m<br />

0<br />

−300 −200 −100 0 100 200 300<br />

Δ y [ µ m]<br />

Figure 3.4: Variation <strong>in</strong> <strong>the</strong> rate <strong>of</strong> primary vertices seen <strong>in</strong> <strong>the</strong> ATLAS <strong>in</strong>ner detector<br />

as <strong>the</strong> two beams are displaced relative to each o<strong>the</strong>r <strong>in</strong> <strong>the</strong> horizontal plane (left)<br />

and <strong>in</strong> <strong>the</strong> vertical plane (right). The beam size <strong>in</strong> each direction obta<strong>in</strong>ed from <strong>the</strong><br />

double Gaussian fit is shown.<br />

The lum<strong>in</strong>osity reduction due to <strong>of</strong>fset beams is given by formula 3.10:<br />

W = exp(− d2<br />

4σ2 ) (3.15)<br />

i<br />

where d is <strong>the</strong> beam separation along <strong>the</strong> ith axis, and i = x, y. A fit <strong>of</strong> <strong>the</strong> observed<br />

variation <strong>in</strong> lum<strong>in</strong>osity, as shown <strong>in</strong> Figure 3.4 [58], to <strong>the</strong> above expression gives<br />

<strong>the</strong> beam size. The scans are performed separately <strong>in</strong> <strong>the</strong> horizontal and vertical

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