^_`a _ba^cc!cdA*c9% c9, ?% ! NLO 5 "#7 &<7 )9 :; * 4/04 )5 56 7 * 1 ,3+ ,$ ) #-.* 1,2%&'( )"#$ " 1 % % #$! ! " 2 ! " ) #%&$ '( 3 ! 4 %* %* ! 5 >? E .B$ C D @&/ &: ' A$ NLO >? #- :;< ='- =- 9 # $ -87 DGLAP #,-. / 0% #66. +) @A % 97 NLO9:% 9 :$ .% IJ" . #% G-% >? @&/ F! #- B! =- 9! +: + 9 ' % # $ .-7 M<-% #N O 9:% #"' :$ .% +7L - #% ; -% B< 9 9K- . #% @B ",7 BC -D :;< =- >J) #- :;< O $ = 9:$ .% ( R : .B$ 9:$ .% + < - EQ$ D - ' C* P$ :;< - 9 . #-O "' $ #$ R% EU7 -K-% # %'( %( B$ T .- -O S % #- Extracting the polarized parton distribution functions at NLO approximation ,using the laplace transforms F.Taghavi-Shahri 1,2; S. Atashbar Tehrani 1,3; A.Mirjalili 4; M. M. Yazdanpanah 5 1 School of Particles and Accelerators, Institute for Research in Fundamental Sciences (IPM),Tehran,Iran 2 Department of Physics, Ferdowsi University of Mashhad,, Mashhad, Iran 3 Department of Physics, Azad University, Yazd Branch, ran 4 Physics Department, Yazd University, Yazd, Iran 5 Faculty of Physics, Shahid Bahonar University of Kerman, Kerman,Iran Abstract We analytically solve the DGLAP evolution equations at the NLO approximation, using the Laplace transformation. Then we achieve to the polarized parton densities. For this propose we need to the Laplace transformation of the parton splitting functions at the related approximation. Extending the calculations to the NLO approximation requires the required recurrence relations in terms of the expanding parameters. Up to the desired accuracy, the iteration steps of the recurrence relations can be stopped. y accessing to the polarized parton densities, we can calculate the parton contributions to the nucleon spin. Following that we are able to compute the polarized proton structure functions in terms of the polarized parton densities. The results are in good agreement with the available experimental data and phenomenological models. PACS No. ( 13) 9* (DIS) J* YZ #"* %'( %77 - EQ$ EO $ #X-* P$ V-* V-* EQ$ 9 ='- - # O $ BO ' 967K ' P% 9A,-% 9:$ .% BO '% P$ EU7 -]-6" V-* E 9' B*) ' % O $ E E E W* #-X ( ' $ .B$ - 9K- -% ' ^__` _ba^cc!cdA*c9% c9, ?% 4S w D s (Q ) w ln Q 2 2 " %'( '-% 9 . B7 EQ$ EO $ -]-6" GG( x, Q 2 ) GFS (GPgqLO D s (Q 2 ) NLO GPgq )( x, Q 2 ) GG (GPggLO 4S D s (Q 2 ) NLO GPgg )( x, Q 2 ) 4S #,-. / 0% +) 9 * #% I& ; 9:$ .% #- ='- =- ef$ 'Q DGLAP - E ' C* P$ ( R 9:% E6% +: (3) 1 / 0% @&/ +: Q Ln h% h R ) x &: BN O E ' P #% S 9 Q F! ' k-! I& 9, ?% E #6:< * 9% . - EQ$ / 0% #66. +) 9 @&/ &: ' A$ :;< ='- =- P B$ NLO >? DGLAP .P* 9$ .% - :9* P* #% A$ @&/ Q ³ L[ GF ( w)GH (Q w)dw; s] 0 L[GF (Q ); s]L[GH (Q ); s] (4) #) / / 0% ((1)9, 0%) 9A,-% :( #% B$ @&/ +: Q w GFNS (Q ,W ) GFNS ( w,W )e (Q w) (GPqqLO (Q w) 0 wW D s (Q 2 ) NLO GPqq (Q w))dw 4S ³ (5) :B$ ' -N 9 @&/ F! / 9, 0% l-K W2 B$ GI NS (s ) GI NS ( s ) =- . GI NS W2 LO 1 4S (s) NLO W2 GI NS (s) W h% h :[1-6]B$ ' < ' 9N&O -; * I 1 W (Q0 , Q ) { 4S / 0% 2 2 Q2 ³D s (Q c 2 )d ln Q c 2 Q Ln Q0 2 1 x F! ' J #, +JA #/ 0% 9* DGLAP # @&/ +: ' d .P #% (Q ,W ) F! 9 ( x, Q 2 ) 9 W +JA / 0% U ' S 9 Q ' ='- =- >J) :K / 0% $ 9 % #, .B$ +) + < I 9 9* - #% +: - 9, 9 B"' @&/ @-0% +: ' BJ! * 9A,-% NLO >? .P* A$ eWGINS ( s )GF 0 NS ( s) GFNS ( s,W ) E FA ( x, Q 2 ) F! (6) ='- L&i 9* :;< - ='- / 9; 9* = -O *-* #!j V-* W ³ D s (W c) dW c . :- #% M0 9- / 0% ' A$ :;< -]-6" ='- DGLAP :( #% B$ 9- 0 =- E 9:$ .% . G : #! =- @&/ +: :L - #/-i i f 9* 9!" -N NLO >? .B$ -O ( ( ' G-% s F! 9, ='- =- EJ B, ) E :;< ='- =- - #% @&/ @-0% +: ' A$ .( B$ #!j *-* 4S w D s (Q ) w ln Q 2 2 GFNS ( x, Q 2 ) GFNS (GPqqLO D s (Q 2 ) NLO GPqq )( x, Q 2 ) 4S 4S w 2 D s (Q ) w ln Q 2 2 G FS ( x , Q ) (1) LO G FS (G Pqq 2 G5D A > H D s (Q ) 4S NLO 2 LO )( x , Q ) G G (G Pqg NLO 2 )( x , Q ) G Pqq 2 D s (Q ) 4S G Pqg 2 ^___ _ba^cc!cdA*c9% c9, ?% I ' A$ - #% (11) (10) / 0% ' #- :;< ='- =- 9A,-% 9:$ .% / p .B! #f$ GG ( s,U ) GFS ( s,U ) @&/ +: ' A$ 9 ' :;< -]-6" =- 9:$ .% E P U 9 W ' S 9 Q ' # @&/ I ' A$ *S% . #% @&/ F! (iteration) I ' A$ 9 ' -K E! F! I -O 96 BJ #66. s +) 0% 9 .- -O #/-i J NLO >? :$ .% .P NLO GM g #-r6" Wf B! =- 9! +: + Y0% NLO GT g C'/ 9* #% # l-K 9 # B$ .J +7L 9 B:J DGLAP / 0% a(W ) D s (W ) 4S UGFS ( s, U ) Gf S0 ( s) +) ' %( B$ - O $ = I' ' ( Gg 0 ( s ) :;< ='- =- .B$ A$ #D #66. NLO GI S GI S ( s )GFS ( s, U ) LO ( s ) L[a(W )Gf S ( s, W );U ] GT S ( s )GG ( s, U ) LO NLO GT S ( s ) L[a(W )Gg ( s,W );U ] (7) B t % 9- s F! 9, @ ?% >J) 9* - O $ = #6* I' ' ' -% E -K-% #D B$ 9- ='- =- :B$ %( B$ O $ = Gq( s, Q02 ) N qK q (1 c q ³ f 0 e svGq ( x e v , Q02 )dv s aq s a q bq 1 ) B( s a q , bq 1) . #% 6 = B q {u v , d v , q, g} / 9; 9* M0 :- -O 9- (S,U) F! % 4A Gf S0 ( s) )9, @ ?% #- ='- =- E! a0 a1e b1W UGG( s,U ) Gg 0 (s) NLO GI g LO GT g GI g ( s )GG ( s, U ) LO ( s ) L[a(W )Gg ( s,W );U ] ( s )GF ( s, U ) NLO GT g ( s ) L[a(W )Gf ( s,W );U ] (8) A$ @&/ &: 9:$ .% ' 9; ' A$ -O $ 9, 0% E (8) (7) p :9-; #!j V-* :;< ='- =- T 1 + + .B$ ( NLO >? -]-6" #66. +) ' %( B$ - :;< O $ = 2 9J ?% 3 + .B$ ( #D ( 9J ?% .B$ C D #$ R% = E 1 L[a(W )Gf ( s,W );U ] ¦ a Gf (s,U b ) j j j 0 1 L[a(W )Gg ( s,W );U ] ¦ a Gg (s,U b ); b j j 0 0 j 0 (9) >? DGLAP / 0% ' 9, 0% B :P U s F! NLO (U GI S )GFS ( s,U ) GT S ( s )GG( s,U ) Gf S0 (s) a1 (GI SNLO ( s )Gf ( s, U b1 ) GT SNLO ( s )Gg ( s, U b1 )) (10) GT g ( s )GF ( s,U ) (U GI g ( s ))GG(s,U ) Gg 0 (s) a1 (GI gNLO ( s )Gf (s,U b1 ) GT gNLO ( s )Gg (s,U b1 )) (11) ^__^ _ba^cc!cdA*c9% c9, ?% P$ P < #- :;< ='- =- 9:$ .% ' d R u% .P - EQ$ - ' C* : P Q 2 4GeV 2 'u v (Q 2 4GeV 2 ) 'd v (Q 2 4GeV 2 ) 1 ³ Gu ( x, Q )dx ³ Gd ( x, Q )dx ³ Gd ( x, Q )dx ³ Gd ( x, Q )dx v 0 ' q (Q 2 4GeV 2 ) 'g (Q 2 4GeV 2 ) 1 0 1 0 2 0.928 2 0.342 v 0 1 2 0.0661 2 3.393 v v " p$- %( B$ T #-O v ; T E .[8-13] # %'( -r " D %I =- ef$ #66. +) E, 9, ?% E #66. +) ' %( B$ #- :;< ='- =- :1 + NLO >? DGLAP / 0% ' A$ #- :;< ='- T .B$ " 9] NLO >? @&/ &: v!- :;< O $ =- #- :;< ='- =- -K-% #$ ,% #D #-O J . ,67 [1] M. M. Block, L. Durand, P. Ha, and D.W. McKay, Eur.Phys. J. C 69, 425 (2010). [2] M. M. Block, L. Durand, P. Ha, and D.W. McKay, Phys.Rev. D 84, 094010 (2011). [3] M. M. Block, L. Durand, P. Ha, and D.W. McKay, Phys.Rev. D 83, v0cv054009 (2011). 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