 
    
    
         
More detailed flavor analysis is possible with the asymmetry measurements 
for W productions, since the flavors participating in the reaction are 
almost fixed;
 , and
, and  . 
From parity violating asymmetries,
. 
From parity violating asymmetries,


the flavor decomposition of the anti-quark helicity distribution is possible.
We are going to identify the W production by 
observing Jacobian peak in the  spectrum of leptons. 
The decay electrons are detected in the EM calorimeter in Central Arm
and the decay muons are detected in North and South Muon Arms.
 spectrum of leptons. 
The decay electrons are detected in the EM calorimeter in Central Arm
and the decay muons are detected in North and South Muon Arms.
   
Figure 3: Correlation plot for energy of high- leptons and momentum 
fraction carried by incident quark. Left plot is for the muons detected in 
North and South Muon Arm, and right plot is for the electrons 
detected in Central Arm.
 leptons and momentum 
fraction carried by incident quark. Left plot is for the muons detected in 
North and South Muon Arm, and right plot is for the electrons 
detected in Central Arm.
The reconstruction of parton kinematics for W production is
difficult, since we can not measure the momentum carried by 
 . As shown in the left plot in Figure 3, however, 
there is a good correlation
between the muon energy and momentum fraction carried by the incident 
quark,
. As shown in the left plot in Figure 3, however, 
there is a good correlation
between the muon energy and momentum fraction carried by the incident 
quark,  . This correlation is due to the angular distribution of 
decay lepton in the W rest frame originated from the V-A nature of the 
weak process. 
In the limit of negligible
. This correlation is due to the angular distribution of 
decay lepton in the W rest frame originated from the V-A nature of the 
weak process. 
In the limit of negligible  of W,
 of W, 
Since  distribution follows
 distribution follows 
 ,
the first term in Equation. 10 dominates and a good correlation 
between
,
the first term in Equation. 10 dominates and a good correlation 
between  and
 and  is obtained. Once
 is obtained. Once  is determined
 is determined 
 can be deduced from Equation 9 in 
good approximation.
 can be deduced from Equation 9 in 
good approximation.
In the case of electrons detected in Central Arm, the sample are
biased in decay angle  due to the
 due to the 
 -coverage and both terms in Equation 10 equally 
contribute. Those are, however, useful in selecting existing models
on quark and anti-quark helicity distributions.
-coverage and both terms in Equation 10 equally 
contribute. Those are, however, useful in selecting existing models
on quark and anti-quark helicity distributions.
Using the muon sample which is divided into several energy bins thus x-bins, we have estimated the sensitivities of our measurements only with statistical error. Results are over-plotted on one of the model predictions for polarized structure functions [17] in Figure 4. Error bars indicate the expected statistical errors. Our measurement will be quite sensitive to both quark and anti-quark helicity distributions, though further studies are needed to minimize the background contributions.
   
Figure 4: Expected sensitivities for the flavor decomposed 
asymmetry in the structure functions imposed on the model predictions
by Bourrely and Soffer [17].
 
 
    
   