24.12.2012 Views

References - Bogoliubov Laboratory of Theoretical Physics - JINR

References - Bogoliubov Laboratory of Theoretical Physics - JINR

References - Bogoliubov Laboratory of Theoretical Physics - JINR

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

(1.205 ± 0.0012) GeV/c, 10 10 p/s, 75% respectively. It was shown that the neutron longitudinal<br />

polarization reaches about 40% at the kinetic energies T ≥ 450 MeV. This beam<br />

was extensively used to fulfill the complete set <strong>of</strong> the np-elastic scattering experiments.<br />

Spin Transfer tensor in<br />

Inclusive Λ<br />

Figure 1: Depolarization DNN data as a function <strong>of</strong> pT .<br />

0 Production by<br />

Transversely Polarized Protons<br />

at 200 GeV/c<br />

This is the first and only example<br />

<strong>of</strong> non-zero Spin Transfer<br />

Mechanism, experimentally established<br />

at 200 GeV/c [5]. The<br />

depolarization tensor DNN =<br />

KN0;N0 (Wolfstein’s parameter)<br />

in the reaction p ↑ +p =Λ0 ↑<br />

+X has been measured with<br />

the transversely polarized protons<br />

at 200 GeV/c over a wide<br />

xF range and a moderate pT .<br />

DNN reaches positive values <strong>of</strong><br />

about 30% at high xF and pT ∼<br />

1.0 GeV/c (see Fig 2). This result proves the existence <strong>of</strong> the essential spin transfer mech-<br />

anism at sufficiently high energy.<br />

Figure 2: Longitudinal spin transfer <strong>of</strong> Λ and<br />

Λinμp collisions<br />

Longitudinal s pin transfer <strong>of</strong> Λ<br />

and Λ in DIS at COMPASS The Fig. 3<br />

presents the results <strong>of</strong> longitudinal spin<br />

transfer <strong>of</strong> Λ and ΛinDISatCOMPASS<br />

[6]. We would like to emphasize two features<br />

<strong>of</strong> these datas: 1) The spin transfer<br />

tensor DLL is not zero for Λ. This is in contrast<br />

to the generally accepted statement<br />

that the spin transfer is absent in the case<br />

when the final and initial baryons do not<br />

have any common quark. It means that<br />

there is another channel <strong>of</strong> transferring the<br />

polarization. As an example we may refer<br />

to pr<strong>of</strong>essor H.Artru, who indicated us that<br />

the polarized proton may emit the polarized<br />

gluon which fragments into polarized<br />

quark-antiquark pair. The polarized anti-<br />

quark may fragment into polarized antibaryon. Obviously the spin transfer in this chain<br />

should be small as it is seen from this slide. 2) It is surprizing that the spin transfer in<br />

the case <strong>of</strong> Λ- hyperon is zero. This is also in variance with the above general statement,<br />

since lambda and initial proton have common quarks. On the basis <strong>of</strong> these data we may<br />

expect that the spin transfer from the polarized proton to the final antiproton may be<br />

not zero also.<br />

186

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!