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81.
K. Hertzog 《Fresenius' Journal of Analytical Chemistry》1960,172(6):437
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K. Hertzog 《Fresenius' Journal of Analytical Chemistry》1960,172(5):388
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K. Hertzog 《Fresenius' Journal of Analytical Chemistry》1959,171(4):285
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K. Hertzog 《Fresenius' Journal of Analytical Chemistry》1959,167(5):387
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K. Hertzog 《Fresenius' Journal of Analytical Chemistry》1960,176(2):128
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K. Hertzog 《Fresenius' Journal of Analytical Chemistry》1960,175(5):385
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Brown HN Bunce G Carey RM Cushman P Danby GT Debevec PT Deile M Deng H Deninger W Dhawan SK Druzhinin VP Duong L Efstathiadis E Farley FJ Fedotovich GV Giron S Gray F Grigoriev D Grosse-Perdekamp M Grossmann A Hare MF Hertzog DW Hughes VW Iwasaki M Jungmann K Kawall D Kawamura M Khazin BI Kindem J Krienen F Kronkvist I Larsen R Lee YY Logashenko I McNabb R Meng W Mi J Miller JP Morse WM Nikas D Onderwater CJ Orlov Y Ozben CS Paley JM Polly C Pretz J Prigl R zu Putlitz G Redin SI Rind O 《Physical review letters》2001,86(11):2227-2231
A precise measurement of the anomalous g value, a(mu) = (g-2)/2, for the positive muon has been made at the Brookhaven Alternating Gradient Synchrotron. The result a(mu+) = 11 659 202(14) (6) x 10(-10) (1.3 ppm) is in good agreement with previous measurements and has an error one third that of the combined previous data. The current theoretical value from the standard model is a(mu)(SM) = 11 659 159.6(6.7) x 10(-10) (0.57 ppm) and a(mu)(exp) - a(mu)(SM) = 43(16) x 10(-10) in which a(mu)(exp) is the world average experimental value. 相似文献