1995
DOI: 10.1063/1.48862
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Mo̸ller polarimetry at SLAC

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Cited by 3 publications
(3 citation statements)
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“…x dy y g(y;Q 2 )P qg (x=y) (70) The splitting function P qq (z) is dened exactly as P qq (z) for the unpolarized case [Eq. (57)], P qq (z) = 4 3 1 + z 2 1 z + (71) while the probability for a quark to lose a gluon which carries the fraction z of the original momentum is slightly dierent from Eq.…”
Section: Polarized Casementioning
confidence: 99%
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“…x dy y g(y;Q 2 )P qg (x=y) (70) The splitting function P qq (z) is dened exactly as P qq (z) for the unpolarized case [Eq. (57)], P qq (z) = 4 3 1 + z 2 1 z + (71) while the probability for a quark to lose a gluon which carries the fraction z of the original momentum is slightly dierent from Eq.…”
Section: Polarized Casementioning
confidence: 99%
“…The ferromagnetic (49% Fe, 49% Co, 2% Va b y w eight) foils of dierent thickness (20 to 154 m) were located in the alcove of End Station A [68] [69]. Helmholtz coils created a homogeneous 0.01 T magnetic eld polarizing about two of the 3d electrons (M-shell), which resulted in an 8% overall electron polarization [70]. The foil polarization was measured with a relative error of 0.017 [69].…”
Section: Mller Polarimetermentioning
confidence: 99%
“…The ferromagnetic (49% Fe, 49% Co, 2% Va b y w eight) foils of dierent thickness (20 to 154 m) were located in the alcove of End Station A [68] [69]. Helmholtz coils created a homogeneous 0.01 T magnetic eld polarizing about two of the 3d electrons (M-shell), which resulted in an 8% overall electron polarization [70]. The foil polarization was measured with a relative error of 0.017 [69].…”
Section: Mller Polarimetermentioning
confidence: 99%