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References - Bogoliubov Laboratory of Theoretical Physics - JINR

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Intensity pr<strong>of</strong>ile (arb. units)<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

-6 -4 -2 0 2 4 6<br />

Polarization pr<strong>of</strong>ile<br />

0.1<br />

-6 -4 -2 0 2 4<br />

Polarization vs I/Imax<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

χ 2 / ndf 8.687 / 9<br />

Prob 0.4666<br />

Pmax 0.6208 ± 0.01836<br />

R 0.1108 ± 0.03984<br />

0.1<br />

0 0.2 0.4 0.6 0.8 1<br />

(a) (b)<br />

Figure 3: (a) Intensity (upper plot) and polarization (bottom plot) vs target position (arb. units),<br />

measured in one <strong>of</strong> the RHIC stores for 100 GeV beam; gaussian fits are shown. (b) Polarization vs<br />

intensity normalized to the intensity at beam center (I/Imax); fit <strong>of</strong> Eq. (6) to the data points is shown,<br />

with extracted parameters Pmax and R.<br />

4 Local Polarimeters<br />

Local polarimeters employed by PHENIX and STAR also make a vital contribution to<br />

the measurements and monitoring <strong>of</strong> the beam polarizations at RHIC. They are sensitive<br />

to beam transverse polarizations. Their main role is to set up and to monitor the spin<br />

direction at collision. For the physics measurements with longitudinally polarized beams<br />

they are to confirm the absence <strong>of</strong> the polarization in transverse plane. In addition, they<br />

also proved to be a precise tool to monitor beam polarization bunch by bunch and versus<br />

time.<br />

PHENIX local polarimetry is based on the analyzing power <strong>of</strong> the very forward neutron<br />

production discovered in the first polarized proton RHIC run <strong>of</strong> 2001-2002 [9]. Forward<br />

neutrons in PHENIX are measured by Zero-Degree Calorimeters (ZDC) with position<br />

sensitive Shower-Max Detectors which cover ±2.8 mrad <strong>of</strong> the forward and backward<br />

directions [10]. The analyzing power increases nearly linearity with center <strong>of</strong> mass energy<br />

<strong>of</strong> colliding beams in the fixed ZDC geometry, which may indicate on pT scaling <strong>of</strong> AN<br />

(Fig. 4a, [11]), taking into account the xF scaling <strong>of</strong> the forward neutron production cross<br />

section ( [11]).<br />

STAR local polarimetry is based on the sizable analyzing power <strong>of</strong> forward hadron<br />

production, first measured at √ s

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