Inclusive decays B → DX and B → D X

We report new measurements of the differential and total branching ratios for inclusive B decay to D{sup 0}, D{sup +}, and D{sup *+} and the first measurement of the same quantities for inclusive B decay to D{sup *0}. Here B is the mixture of B{sub d} and B{sub u} from {Upsilon}(4S) decay. Furthermo...

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Veröffentlicht in:Physical Review, D D, 1997-10, Vol.56 (7), p.3783-3802
Hauptverfasser: Gibbons, L., Johnson, S. D., Kwon, Y., Roberts, S., Thorndike, E. H., Jessop, C. P., Lingel, K., Marsiske, H., Perl, M. L., Schaffner, S. F., Ugolini, D., Wang, R., Zhou, X., Coan, T. E., Fadeyev, V., Korolkov, I., Maravin, Y., Narsky, I., Shelkov, V., Staeck, J., Stroynowski, R., Volobouev, I., Ye, J., Artuso, M., Efimov, A., Frasconi, F., Gao, M., Goldberg, M., He, D., Kopp, S., Horwitz, N., Moneti, G. C., Mountain, R., Mukhin, Y., Schuh, S., Skwarnicki, T., Stone, S., Thulasidas, M., Viehhauser, G., Xing, X., Bartelt, J., Csorna, S. E., Jain, V., Marka, S., Freyberger, A., Godang, R., Kinoshita, K., Lai, I. C., Pomianowski, P., Schrenk, S., Bonvicini, G., Cinabro, D., Greene, R., Perera, L. P., Barish, B., Chadha, M., Chan, S., Eigen, G., Miller, J. S., O'Grady, C., Schmidtler, M., Urheim, J., Weinstein, A. J., Würthwein, F., Asner, D. M., Bliss, D. W., Brower, W. S., Masek, G., Paar, H. P., Sharma, V., Gronberg, J., Kutschke, R., Lange, D. J., Menary, S., Morrison, R. J., Nelson, H. N., Nelson, T. K., Qiao, C., Richman, J. D., Roberts, D., Ryd, A., Witherell, M. S., Balest, R., Behrens, B. H., Cho, K., Ford, W. T., Park, H., Rankin, P., Roy, J., Smith, J. G., Alexander, J. P., Bebek, C., Berger, B. E., Berkelman, K., Bloom, K., Cassel, D. G., Cho, H. A., Coffman, D. M., Crowcroft, D. S., Dickson, M.
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Sprache:eng
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Zusammenfassung:We report new measurements of the differential and total branching ratios for inclusive B decay to D{sup 0}, D{sup +}, and D{sup *+} and the first measurement of the same quantities for inclusive B decay to D{sup *0}. Here B is the mixture of B{sub d} and B{sub u} from {Upsilon}(4S) decay. Furthermore, since more than one charm particle (or antiparticle) of the same kind can be produced in B decay, here {open_quotes}inclusive B branching ratio{close_quotes} is used to mean the average number of charm particles and their antiparticles of a certain species produced in B decay. We obtain the following results (the first error is statistical, the second systematic of this analysis, the third propagated from other measurements): B(B{r_arrow}D{sup 0}X)=(0.636{plus_minus}0.014{plus_minus}0.019{plus_minus}0.0 8), B(B{r_arrow}D{sup +}X)=(0.235{plus_minus}0.009{plus_minus}0.009{plus_minus}0.024), B(B{r_arrow}D{sup *0}X) =(0.247{plus_minus}0.012{plus_minus}0.018{plus_minus}0.018), B(B{r_arrow}D{sup *+}X)=(0.239{plus_minus}0.011{plus_minus}0.014{plus_minus}0. 09). The following ratio of branching ratios is not affected by most of the systematic errors: B(B{r_arrow}D{sup *0}X)/ B(B{r_arrow}D{sup *+}X)=(1.03{plus_minus}0.07{plus_minus}0.09{plus_minus}0.08). We also report the first measurement of the momentum-dependent D{sup *0} polarization and a new measurement of the D{sup *+} polarization in inclusive B decay. Using these measurements and other CLEO results and making some additional assumptions, we calculate the average number of c and {bar c} quarks produced in B decay to be {l_angle}n{sub c}{r_angle}=1.10{plus_minus}0.05. {copyright} {ital 1997} {ital The American Physical Society}
ISSN:0556-2821
1089-4918
DOI:10.1103/PhysRevD.56.3783