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Double spin asymmetries for hadron production in semi-inclusive DIS

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The Fifth Conference “ Nuclear Science and Its Application”, 14-17 October 2008

DOUBLE SPIN ASYMMETRIES FOR HADRON PRODUCTION IN SEMI-

INCLUSIVE DIS

S.K.ABDULLAYEV, M.SH.GOJAYEV

Baku State University, Azerbaijan, [email protected]

High energy experiment with polarized beams and targets has opened a new wmdow for

(2)

The Fifth Conference “ Nuclear Science and Its Application”, 14-17 October 2008

revealing QCD dynamics and hadron structures. In this we study the hadron production in polarized semi-inclusive deep inelastic scattering (DIS) off nucleon:

t { X ) + N(hN) = > f +h + X, (1) v n(vtl) + N(hN) = > v il(v]l) + h + X, (2)

+ + Af,(3) p +(A,) + N(hN) =>v^(yil) + h + X , (4) where ! is the lepton spirality, hN is the longitudinal polarization of nucleon-target.The cross-section for the production of a hadron h in the current fragmentation region are given by

e 2) “ ^ ( z , q

2)

dxdydz qih^} ay ¥ (

5)

where f N{hs)(x9 Q2) is the distribution function of polarized quarks in the polarized nucleon, ^ f (hq)

D hq(z, Q1) is the fragmentation function of the quark into the detected hadron h , do/dy is the

elementary cross-section, x, y and z are the usual DIS variables.

Insteadofthe usual asymmetry A hN = ( N ^ - N ^ ) / ( N hn + N ^ ) one has to measure so called

“difference asymmetry” A%~k which is expressed in term of the respective counting rate as = [ ( < - < ) ~ ( < - < ) ] / [ ( < - * £ ) + ( < - < ) ] , (6) where N^ ^ are the number of events for parallel (antiparallel) orientations of here lepton and target nuclear spins for hadrons of type

h

registered.

We consider separately the different processes and derive explicit expressions for the double spin asymmetries in term of elementary dynamics, spirality amplitudes, quark distribution and fragmentation functions. For example, in the processes (1) expressions for the difference asymmetries look like:

= m 4 _jr

- f ( y )

4A»V - Adv 4uv - d v Aw„ A,K +-K~

= f ( y )

4Adv - Auv

4d„

— w„ = a

k

/ - k~

= /(y )A » v ± -4 4 ;

...

f ( y)

- 1 (1

y)

,

(

7

)

uv + d v 1 + (1 + y)

Asymmetries (7) contain only valence quark polarized densities, and to be free any fragmentation functions.

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