Muon g — 2 experiment at Brookhaven National Laboratory
A precise measurement of the anomalous g value, a + μ = ( g − 2)/2, for the positive muon has been made at the Brookhaven Alternating Gradient Synchrotron. The result a + μ = 11 659 202(14)(6) × 10 −10 (1.3 ppm) is in good agreement with previous measurements and has an error one third that of the c...
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Published in | Nuclear physics. Section B, Proceedings supplement Vol. 105; no. 1; pp. 156 - 159 |
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Main Authors | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format | Journal Article |
Language | English |
Published |
Elsevier B.V
01.02.2002
|
Online Access | Get full text |
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Summary: | A precise measurement of the anomalous
g value,
a
+
μ = (
g − 2)/2, for the positive muon has been made at the Brookhaven Alternating Gradient Synchrotron. The result
a
+
μ = 11 659 202(14)(6) × 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
μ(SM)= 11 659 159.6(6.7) × 10
−10 (0.57 ppm) and
a
μ(exp)−
a
μ(SM) = 42(16) × 10
−10 in which
a
μ(exp) is the world average experimental value. |
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ISSN: | 0920-5632 1873-3832 |
DOI: | 10.1016/S0920-5632(01)01972-7 |