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02, and the behavior of θg(x) in this region is determined almost by the functional form in the assumption. To constraint θG more precisely, the data points in the small Bjorken x region are necessary. 2 Uncertainty in Functional Form of g(x) ALL ( pT ) in pp collisions gives an integral with respect to Bjorken x such like ˆ 1 , x2 , pT /z)D(z) d x1 d x2 dz θ f i (x1 )θ f j (x2 )θσ(x . g. heavy quark and direct γ production, which has sensitivity on different Bjorken x region and sign of θg(x) from the current measurements.

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Phys. C. 0079 (2013) D. , Phys. Rev. D 71, 094018 (2005) T. 3820 (2007) T. , JHEP 0605, 026 (2006) A. , Phys. Rev. 1 Manual. pdf (1994) E. , Phys. Rev. D 82, 114018 (2010) 62. 63. 64. 65. 66. 67. 68. 69. 70. 71. 72. 73. 74. 75. 76. 77. 78. 79. 80. 81. 82. Chapter 2 Experimental Setup Abstract This analysis is based on the data which were taken at Relativistic Heavy Ion Collider (RHIC) with the PHENIX detector at Brookhaven National Laboratory (BNL) in the United√States during the 2009 run. In this run, longitudinally polarized p + p collisions at s = 200 GeV were performed for 10 weeks (April 19–June 29).

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[Article] Resistance of tomato seedlings to early blight by Barksdale, T. H.


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