Zobrazeno 1 - 4
of 4
pro vyhledávání: '"Munger, C. T."'
Publikováno v:
Phys.Rev.X 2 (2012) 041009
An improved measurement of the electron electric dipole moment (EDM) appears feasible using ground-state alkali atoms in an atomic fountain in which a strong electric field, which couples to a conceivable electron dipole moment (EDM), is applied perp
Externí odkaz:
http://arxiv.org/abs/1211.4057
Autor:
Barish, B C, Allen, M, Barklow, Timothy L, Bell, R, Brau, J E, Brown, K, Bunnell, K O, Burnett, T H, Cook, V, Cowan, R, Coward, D H, Eisenstein, B I, Faust, D, Fero, M J, Frey, R, Fryberger, D, Gan, K K, Gearhart, R A, Gladding, G E, Gómez-Cadenas, J J, Heusch, C A, Izen, J M, Jenkins, T, Johnson, R, Kirkby, Jasper, Lisin, A V, Lockman, W, Loew, G A, Meadows, B, Miller, R, Mir, R, Mockett, P M, Morton, P, Munger, C T, Nussbaum, M, Odian, A C, Paterson, J M, Perl, Martin Lewis, Ruth, Ronald D, Schindler, R, Seiden, A, Servranckx, R V, Sokoloff, M D, Saint-Lorant, S J, Stockdale, I E, Stroynowski, R, Thaler, J J, Thompson, K, Toki, W, Villa, F, Weidner, H, Weinstein, A, Yamamoto, R
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=od________65::41233dbe6d2f7b5b41c9f4aa8946c537
http://cds.cern.ch/record/210963
http://cds.cern.ch/record/210963
Autor:
Abrams, G. S., Adolphsen, C. E., Averill, D., Ballam, J., Barish, B. C., Barklow, T., Barnett, B. A., Bartelt, J., Bethke, S., Blockus, D., Bonvicini, G., Boyarski, A., Brabson, B., Breakstone, A., Brom, J. M., Bulos, F., Burchat, P. R., Burke, D. L., Cence, R. J., Chapman, J., Chmeissani, M., Cords, D., Coupal, D. P., Dauncey, P., DeStaebler, H. C., Dorfan, D. E., Dorfan, J. M., Drewer, D. C., Elia, R., Feldman, G. J., Fernandes, D., Field, R. C., Ford, W. T., Fordham, C., Frey, R., Fujino, D., Gan, K. K., Gero, E., Gidal, G., Glanzman, T., Goldhaber, G., Gomez Cadenas, J. J., Gratta, G., Grindhammer, G., Grosse-Wiesmann, P., Hanson, G., Harr, R., Harral, B., Harris, F. A., Hawkes, C. M., Hayes, K., Hearty, C., Heusch, C. A., Hildreth, M. D., Himel, T., Hinshaw, D. A., Hong, S. J., Hutchinson, D., Hylen, J., Innes, R., Jacobsen, R. G., Jaros, J. A., Jung, C. K., Kadyk, J. A., Kent, J., King, M., Klein, S. R., Koetke, D. S., Komamiya, S., Koska, W., Kowalski, L. A., Kozanecki, W., Kral, J. F., Kuhlen, M., Labarga, L., Lankford, A. J., Larsen, R. R., Le Diberder, F., Levi, M. E., Litke, A. M., Lou, X. C., Lüth, V., McKenna, J. A., Matthews, J. A. J., Mattison, T., Milliken, B. D., Moffeit, K. C., Munger, C. T., Murray, W. N., Nash, J., Ogren, H., O’Shaughnessy, K. F., Parker, S. I., Peck, C., Perl, M. L., Perrier, F., Petradza, M., Pitthan, R., Porter, F. C., Rankin, P., Riles, K., Rouse, F. R., Rust, D. R., Sadrozinski, H. F. W., Schaad, M. W., Schumm, B. A., Seiden, A., Smith, J. G., Snyder, A., Soderstrom, E., Stoker, D. P., Stroynowski, R., Swartz, M., Thun, R., Trilling, G. H., Van Kooten, R., Voruganti, P., Wagner, S. R., Watson, S., Weber, P., Weigend, A., Weir, A. J., Wicklund, E., Woods, M., Wu, D. Y., Yurko, M., Zaccardelli, C., von Zanthier, C., Weinstein, Alan J.
We have measured the mass of the Z boson to be 91.14±0.12 GeV/c^2, and its width to be 2.42-0.35+0.45 GeV. If we constrain the visible width to its standard-model value, we find the partial width to invisible decay modes to be 0.46±0.10 GeV, corres
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=od________38::ab49d40085f79f24eb07b9af7543e4b1
https://resolver.caltech.edu/CaltechAUTHORS:ABRprl89c
https://resolver.caltech.edu/CaltechAUTHORS:ABRprl89c
Autor:
Abrams, G. S., Adolphsen, C. E., Aleksan, R., Alexander, J. P., Allen, M. A., Atwood, W. B., Averill, D., Ballam, J., Bambade, P., Barish, B. C., Barklow, T., Barnett, B. A., Bartelt, J., Bethke, S., Blockus, D., de Boer, W., Bonvicini, G., Boyarski, A., Brabson, B., Breakstone, A., Breidenbach, M., Brom, J. M., Brown, J. L., Brown, K. L., Bulos, F., Burchat, P. R., Burke, D. L., Cence, R. J., Chapman, J., Chmeissani, M., Clendenin, J., Cords, D., Coupal, D. P., Dauncey, P., Dean, N. R., DeStaebler, H. C., Dorfan, D. E., Dorfan, J. M., Drell, P. S., Drewer, D. C., Dydak, F., Ecklund, S., Elia, R., Erickson, R. A., Fay, J., Feldman, G. J., Fernandes, D., Field, R. C., Fieguth, T. H., Fischer, G. E., Ford, W. T., Fordham, C., Frey, R., Fujino, D., Gan, K. K., Gatto, C., Gero, E., Gidal, G., Glanzman, T., Goldhaber, G., Gomez Cadenas, J. J., Gratta, G., Grindhammer, G., Grosse-Wiesmann, P., Hanson, G., Harr, R., Harral, B., Harris, F. A., Hawkes, C. M., Hayes, K., Hearty, C., Herrup, D., Heusch, C. A., Hildreth, M. D., Himel, T., Hinshaw, D. A., Holmgren, S. O., Hong, S. J., Hutchinson, D., Hutton, A., Hylen, J., Innes, W. R., Jacobsen, R. G., Jaffre, M., Jaros, J. A., Jobe, R. K., Jung, C. K., Kadyk, J. A., Karlen, D., Kent, J., King, M., Klein, S. R., Koetke, D. S., Komamiya, S., Koska, W., Kowalski, L. A., Kozanecki, W., Kral, J. F., Kuhlen, M., Kulikov, A. V., Labarga, L., Lankford, A. J., Larsen, R. R., Le Diberder, F., Levi, M. E., Litke, A. M., Lohse, T., Lüth, V., Lynch, G. R., McKenna, J. A., Matthews, J. A. J., Mattison, T., Milliken, B. D., Moffeit, K. C., Munger, C. T., Murray, J. J., Murray, W. N., Nash, J., Ogren, H., Ong, R. A., O’Shaughnessy, K. F., Parker, S. I., Peck, C., Perl, M. L., Perrier, F., Petersen, A., Petradza, M., Phinney, N., Pitthan, R., Porter, F. C., Rankin, P., Rees, J. R., Richman, J. D., Riles, K., Rivkin, L., Ross, M. C., Rouse, F. R., Rust, D. R., Sadrozinski, H. F. W., Schaad, M. W., Schalk, T. L., Schumm, B. A., Schwarz, A. S., Seeman, J. T., Seiden, A., Sheppard, J. C., Smith, J. G., Snyder, A., Soderstrom, E., Stiening, R., Stoker, D. P., Stroynowski, R., Swartz, M., Thun, R., Toge, N., Trilling, G. H., Van Kooten, R., Voruganti, P., Wagner, S. R., Watson, S., Weber, P., Weigend, A., Weir, A. J., White, S. L., Wicklund, E., Wolf, R. C., Wood, D. R., Woods, M., Wormser, G., Wright, R., Wu, D. Y., Yurko, M., Zaccardelli, C., von Zanthier, C., Weinstein, A. J.
We have measured the mass of the Z boson to be 91.11±0.23 GeV/c^2, and its width to be 1.61-0.43+0.60 GeV. If we constrain the visible width to its standard-model value, we find the partial width to invisible decay modes to be 0.62±0.23 GeV, corres
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=od________38::a89cd14221c1edc839ed944be513059e
https://resolver.caltech.edu/CaltechAUTHORS:ABRprl89a
https://resolver.caltech.edu/CaltechAUTHORS:ABRprl89a