New Measurement of the Anomalous Magnetic Moment of the Positive Muon

The muon anomalous magnetic moment has been measured in a new experiment at Brookhaven. Polarized muons were stored in a superferric ring, and the angular frequency difference, {omega}{sub a} , between the spin precession and orbital frequencies was determined by measuring the time distribution of h...

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Veröffentlicht in:Physical Review Letters 1999-02, Vol.82 (8), p.1632-1635
Hauptverfasser: Carey, R. M., Earle, W., Efstathiadis, E., Hare, M. F., Hazen, E. S., Hughes, B. J., Krienen, F., Miller, J. P., Monich, V., Ouyang, J., Rind, O., Roberts, B. L., Sulak, L. R., Trofimov, A., Varner, G., Worstell, W. A., Benedict, E., Logashenko, I., Benante, J., Brown, H. N., Bunce, G., Cullen, J., Danby, G. T., Geller, J., Hseuh, H., Jackson, J. W., Jia, L., Kochis, S., Larsen, R., Lee, Y. Y., Mapes, M., Meng, W., Morse, W. M., Pai, C., Pearson, C., Polk, I., Prigl, R., Rankowitz, S., Sandberg, J., Semertzidis, Y. K., Shutt, R., Snydstrup, L., Soukas, A., Stillman, A., Tallerico, T., Tanaka, M., Toldo, F., von Lintig, D., Warburton, D., Woodle, K., Chertovskikh, A., Druzhinin, V. P., Fedotovich, G. V., Grigorev, D. N., Golubev, V. B., Khazin, B. I., Maksimov, A., Merzliakov, Yu, Ryskulov, N., Serednyakov, S., Shatunov, Yu. M., Solodov, E., Orlov, Y., Winn, D., Grossmann, A., Gerhaeuser, J., Jungmann, K., von Walter, P., zu Putlitz, G., Bunker, B., Deninger, W., Debevec, P. T., Hertzog, D. W., Jones, T. D., Polly, C., Sedykh, S., Urner, D., Haeberlen, U., Endo, K., Hirabayashi, H., Kurokawa, S., Yamamoto, A., Green, M. A., Cushman, P., Kindem, J., Duong, L., Giron, S., McNabb, R., Miller, D., Timmermans, C., Zimmerman, D., Mizumachi, Y., Iwasaki, M., Ahn, H. E., Deng, H., Dhawan, S. K., Disco, A., Farley, F. J. M., Fei, X., Grosse-Perdekamp, M.
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Sprache:eng
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Zusammenfassung:The muon anomalous magnetic moment has been measured in a new experiment at Brookhaven. Polarized muons were stored in a superferric ring, and the angular frequency difference, {omega}{sub a} , between the spin precession and orbital frequencies was determined by measuring the time distribution of high-energy decay positrons. The ratio R of {omega}{sub a} to the Larmor precession frequency of free protons, {omega}{sub p} , in the storage-ring magnetic field was measured. We find R=3.707thinsp220(48){times}10{sup {minus}3} . With {mu}{sub {mu}}/{mu}{sub p}=3.183thinsp 345thinsp47(47) this gives a{sub {mu}{sup +}}=1thinsp165thinsp 925(15){times}10{sup {minus}9} ({plus_minus}13 ppm ), in good agreement with the previous CERN measurements for {mu}{sup +} and {mu}{sup {minus}} and of approximately the same precision. {copyright} {ital 1999} {ital The American Physical Society}
ISSN:0031-9007
1079-7114
DOI:10.1103/PhysRevLett.82.1632