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References - Bogoliubov Laboratory of Theoretical Physics - JINR

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the polarimetry at the energies between 0.88 and 2.0 GeV [1]. These data are necessary<br />

to provide good precision <strong>of</strong> the beam polarization measurement for DSS project [2] at<br />

the LHEP-<strong>JINR</strong>.<br />

The experimental data on the deuteron analyzing<br />

powers for large phase space were obtained at 130 MeV<br />

at KVI [3]. Ay, Ayy and Axx analyzing powers in dpbreakup<br />

will be investigated at Internal Target Station<br />

at 200-500 MeV. The predictions for tensor analyzing<br />

power Ayy and differential cross section in the selected dpbreakup<br />

configurations at 400 MeV are shown in Fig.1.<br />

The light shaded band contains the theoretical predictions<br />

based on CD-Bonn, AV18, Nijm I, II and Nijm<br />

93. The darker band represents predictions when these<br />

NN forces are combined with the TM 3NF. The solid<br />

line is for AV18+Urbana IX and the dashed line for CD<br />

Bonn+TM. One can see large sensitivity <strong>of</strong> these observables<br />

to the model <strong>of</strong> 3NF.<br />

The details <strong>of</strong> the experiment on the measurements<br />

<strong>of</strong> analyzing powers in dp-elastic scattering at Nuclotron<br />

can be found in ref. [4]. The polarization <strong>of</strong> the deuteron<br />

beam was measured at 270 MeV, where high-precision<br />

Figure 1: The tensor analyzing<br />

power Ayy and differential cross section<br />

in selected breakup configurations<br />

at 400 MeV. The curves are<br />

explained in the text.<br />

data on the analyzing powers from dp-elastic scattering from RIKEN exist [5]. Two<br />

particles from the dp-elastic scattering were clearly distinguished by their time-<strong>of</strong>-flight<br />

differences from the target and their energy losses in the plastic scintillators. Values on<br />

the vector and tensor polarizations <strong>of</strong> the deuteron beam were obtained. These values<br />

are in good agreement with the results obtained by low energy polarimeter based on<br />

3 He(d, p(0 ◦ )) 4 He reactions [6].<br />

A 0.8<br />

y Td=880<br />

MeV<br />

0.6<br />

0.4<br />

0.2<br />

-0<br />

-0.2<br />

-0.4<br />

-0.6<br />

0 20 40 60 80 100 120 140 160 180<br />

Θcm,<br />

deg<br />

A 0.8<br />

y Td=880<br />

MeV<br />

0.6<br />

0.4<br />

0.2<br />

-0<br />

-0.2<br />

-0.4<br />

-0.6<br />

0 20 40 60 80 100 120 140 160 180<br />

Θcm,<br />

deg<br />

Axx<br />

1<br />

0.5<br />

0<br />

-0.5<br />

-1<br />

Td=880<br />

MeV<br />

-1.5<br />

0 20 40 60 80 100 120 140 160 180<br />

Θcm,<br />

deg<br />

(a) (b) (c)<br />

Figure 2: (a) Vector Ay and (b) tensor Ayy, (c) Axx analyzing powers for the dp- elastic scattering at<br />

880 MeV. The curves are described in the text.<br />

The true numbers <strong>of</strong> the dp- elastic events at 880 MeV were obtained by imposing <strong>of</strong><br />

the cut on two-dimensional plot <strong>of</strong> ADC signals from deuterons and protons detectors.<br />

Additionally, the graphical cuts were applied on the time-<strong>of</strong>-flight difference between<br />

deuterons and protons from the target. The contribution <strong>of</strong> the carbon dependent on the<br />

scattering angle was subtracted.<br />

The experimental data obtained at 880 MeV are compared with the theoretical predictions<br />

in Fig.2. Solid curves correspond to Faddeev calculation using the CD-Bonn<br />

NN potential. One can see that the Faddeev calculations reproduce the behavior <strong>of</strong> all<br />

the analyzing powers. Dotted curves correspond to the calculations in optical potential<br />

289

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