Determination of the B¯→D*lν¯ decay width and |Vcb|
In the standard model, the charged current of the weak interaction is governed by a unitary quark mixing matrix that also leads to CP violation. Measurement of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements is essential to searches for new physics, either through the structure of the CKM matrix...
Ausführliche Beschreibung
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E-Artikel |
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| Erschienen: |
2003 |
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| Umfang: |
Online-Ressource 22 |
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| Reproduktion: |
APS Digital Backfile Archive 1893-2003 |
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| Übergeordnetes Werk: |
Enthalten in: Physical review / D - [S.l.] : Soc., 1970, 67(2003), 3 |
| Übergeordnetes Werk: |
volume:67 ; year:2003 ; number:3 ; extent:22 |
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| 520 | |a In the standard model, the charged current of the weak interaction is governed by a unitary quark mixing matrix that also leads to CP violation. Measurement of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements is essential to searches for new physics, either through the structure of the CKM matrix, or a departure from unitarity. We determine the CKM matrix element |Vcb| using a sample of 3×106 BB¯ events in the CLEO detector at the Cornell Electron Storage Ring. We determine the yield of reconstructed B0→D*+lν¯ and B-→D*0lν¯ decays as a function of w, the boost of the D* in the B rest frame, and from this we obtain the differential decay rate dΓ/dw. By extrapolating dΓ/dw to w=1, the kinematic end point at which the D* is at rest relative to the B, we extract the product |Vcb|F(1), where F(1) is the form factor at w=1. We find |Vcb|F(1)=0.0431±0.0013(stat)±0.0018(syst). We combine |Vcb|F(1) with theoretical results for F(1) to determine |Vcb|=0.0469±0.0014(stat)±0.0020(syst)±0.0018(theor). We also integrate the differential decay rate over w to obtain B(B0→D*+lν¯)=(6.09±0.19±0.40)% and B(B-→D*0lν¯)=(6.50±0.20±0.43)%. | ||
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| 700 | 1 | |a Adam, N. E. |4 oth | |
| 700 | 1 | |a Alexander, J. P. |4 oth | |
| 700 | 1 | |a Bebek, C. |4 oth | |
| 700 | 1 | |a Berger, B. E. |4 oth | |
| 700 | 1 | |a Berkelman, K. |4 oth | |
| 700 | 1 | |a Blanc, F. |4 oth | |
| 700 | 1 | |a Boisvert, V. |4 oth | |
| 700 | 1 | |a Cassel, D. G. |4 oth | |
| 700 | 1 | |a Drell, P. S. |4 oth | |
| 700 | 1 | |a Duboscq, J. E. |4 oth | |
| 700 | 1 | |a Ecklund, K. M. |4 oth | |
| 700 | 1 | |a Ehrlich, R. |4 oth | |
| 700 | 1 | |a Gibbons, L. |4 oth | |
| 700 | 1 | |a Gittelman, B. |4 oth | |
| 700 | 1 | |a Gray, S. W. |4 oth | |
| 700 | 1 | |a Hartill, D. L. |4 oth | |
| 700 | 1 | |a Heltsley, B. K. |4 oth | |
| 700 | 1 | |a Hsu, L. |4 oth | |
| 700 | 1 | |a Jones, C. D. |4 oth | |
| 700 | 1 | |a Kandaswamy, J. |4 oth | |
| 700 | 1 | |a Kreinick, D. L. |4 oth | |
| 700 | 1 | |a Magerkurth, A. |4 oth | |
| 700 | 1 | |a Mahlke-Krüger, H. |4 oth | |
| 700 | 1 | |a Meyer, T. O. |4 oth | |
| 700 | 1 | |a Mistry, N. B. |4 oth | |
| 700 | 1 | |a Nordberg, E. |4 oth | |
| 700 | 1 | |a Palmer, M. |4 oth | |
| 700 | 1 | |a Patterson, J. R. |4 oth | |
| 700 | 1 | |a Peterson, D. |4 oth | |
| 700 | 1 | |a Pivarski, J. |4 oth | |
| 700 | 1 | |a Riley, D. |4 oth | |
| 700 | 1 | |a Sadoff, A. J. |4 oth | |
| 700 | 1 | |a Schwarthoff, H. |4 oth | |
| 700 | 1 | |a Shepherd, M. R. |4 oth | |
| 700 | 1 | |a Thayer, J. G. |4 oth | |
| 700 | 1 | |a Urner, D. |4 oth | |
| 700 | 1 | |a Valant-Spaight, B. |4 oth | |
| 700 | 1 | |a Viehhauser, G. |4 oth | |
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(DE-627)NLEJ249939398 (DE-601)aps:0fcf5bd91536723f4b45e1eaa1bd1e605c1ba090 DE-627 ger DE-627 rakwb Determination of the B¯→D*lν¯ decay width and |Vcb| 2003 Online-Ressource 22 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In the standard model, the charged current of the weak interaction is governed by a unitary quark mixing matrix that also leads to CP violation. Measurement of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements is essential to searches for new physics, either through the structure of the CKM matrix, or a departure from unitarity. We determine the CKM matrix element |Vcb| using a sample of 3×106 BB¯ events in the CLEO detector at the Cornell Electron Storage Ring. We determine the yield of reconstructed B0→D*+lν¯ and B-→D*0lν¯ decays as a function of w, the boost of the D* in the B rest frame, and from this we obtain the differential decay rate dΓ/dw. By extrapolating dΓ/dw to w=1, the kinematic end point at which the D* is at rest relative to the B, we extract the product |Vcb|F(1), where F(1) is the form factor at w=1. We find |Vcb|F(1)=0.0431±0.0013(stat)±0.0018(syst). We combine |Vcb|F(1) with theoretical results for F(1) to determine |Vcb|=0.0469±0.0014(stat)±0.0020(syst)±0.0018(theor). We also integrate the differential decay rate over w to obtain B(B0→D*+lν¯)=(6.09±0.19±0.40)% and B(B-→D*0lν¯)=(6.50±0.20±0.43)%. APS Digital Backfile Archive 1893-2003 Adam, N. E. oth Alexander, J. P. oth Bebek, C. oth Berger, B. E. oth Berkelman, K. oth Blanc, F. oth Boisvert, V. oth Cassel, D. G. oth Drell, P. S. oth Duboscq, J. E. oth Ecklund, K. M. oth Ehrlich, R. oth Gibbons, L. oth Gittelman, B. oth Gray, S. W. oth Hartill, D. L. oth Heltsley, B. K. oth Hsu, L. oth Jones, C. D. oth Kandaswamy, J. oth Kreinick, D. L. oth Magerkurth, A. oth Mahlke-Krüger, H. oth Meyer, T. O. oth Mistry, N. B. oth Nordberg, E. oth Palmer, M. oth Patterson, J. R. oth Peterson, D. oth Pivarski, J. oth Riley, D. oth Sadoff, A. J. oth Schwarthoff, H. oth Shepherd, M. R. oth Thayer, J. G. oth Urner, D. oth Valant-Spaight, B. oth Viehhauser, G. oth Warburton, A. oth Weinberger, M. oth Enthalten in Physical review / D [S.l.] : Soc., 1970 67(2003), 3 Online-Ressource (DE-627)NLEJ248237861 (DE-600)1461167-3 1550-2368 nnns volume:67 year:2003 number:3 extent:22 https://www.tib.eu/de/suchen/id/aps%3A0fcf5bd91536723f4b45e1eaa1bd1e605c1ba090 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 67 2003 3 22 |
| spelling |
(DE-627)NLEJ249939398 (DE-601)aps:0fcf5bd91536723f4b45e1eaa1bd1e605c1ba090 DE-627 ger DE-627 rakwb Determination of the B¯→D*lν¯ decay width and |Vcb| 2003 Online-Ressource 22 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In the standard model, the charged current of the weak interaction is governed by a unitary quark mixing matrix that also leads to CP violation. Measurement of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements is essential to searches for new physics, either through the structure of the CKM matrix, or a departure from unitarity. We determine the CKM matrix element |Vcb| using a sample of 3×106 BB¯ events in the CLEO detector at the Cornell Electron Storage Ring. We determine the yield of reconstructed B0→D*+lν¯ and B-→D*0lν¯ decays as a function of w, the boost of the D* in the B rest frame, and from this we obtain the differential decay rate dΓ/dw. By extrapolating dΓ/dw to w=1, the kinematic end point at which the D* is at rest relative to the B, we extract the product |Vcb|F(1), where F(1) is the form factor at w=1. We find |Vcb|F(1)=0.0431±0.0013(stat)±0.0018(syst). We combine |Vcb|F(1) with theoretical results for F(1) to determine |Vcb|=0.0469±0.0014(stat)±0.0020(syst)±0.0018(theor). We also integrate the differential decay rate over w to obtain B(B0→D*+lν¯)=(6.09±0.19±0.40)% and B(B-→D*0lν¯)=(6.50±0.20±0.43)%. APS Digital Backfile Archive 1893-2003 Adam, N. E. oth Alexander, J. P. oth Bebek, C. oth Berger, B. E. oth Berkelman, K. oth Blanc, F. oth Boisvert, V. oth Cassel, D. G. oth Drell, P. S. oth Duboscq, J. E. oth Ecklund, K. M. oth Ehrlich, R. oth Gibbons, L. oth Gittelman, B. oth Gray, S. W. oth Hartill, D. L. oth Heltsley, B. K. oth Hsu, L. oth Jones, C. D. oth Kandaswamy, J. oth Kreinick, D. L. oth Magerkurth, A. oth Mahlke-Krüger, H. oth Meyer, T. O. oth Mistry, N. B. oth Nordberg, E. oth Palmer, M. oth Patterson, J. R. oth Peterson, D. oth Pivarski, J. oth Riley, D. oth Sadoff, A. J. oth Schwarthoff, H. oth Shepherd, M. R. oth Thayer, J. G. oth Urner, D. oth Valant-Spaight, B. oth Viehhauser, G. oth Warburton, A. oth Weinberger, M. oth Enthalten in Physical review / D [S.l.] : Soc., 1970 67(2003), 3 Online-Ressource (DE-627)NLEJ248237861 (DE-600)1461167-3 1550-2368 nnns volume:67 year:2003 number:3 extent:22 https://www.tib.eu/de/suchen/id/aps%3A0fcf5bd91536723f4b45e1eaa1bd1e605c1ba090 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 67 2003 3 22 |
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(DE-627)NLEJ249939398 (DE-601)aps:0fcf5bd91536723f4b45e1eaa1bd1e605c1ba090 DE-627 ger DE-627 rakwb Determination of the B¯→D*lν¯ decay width and |Vcb| 2003 Online-Ressource 22 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In the standard model, the charged current of the weak interaction is governed by a unitary quark mixing matrix that also leads to CP violation. Measurement of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements is essential to searches for new physics, either through the structure of the CKM matrix, or a departure from unitarity. We determine the CKM matrix element |Vcb| using a sample of 3×106 BB¯ events in the CLEO detector at the Cornell Electron Storage Ring. We determine the yield of reconstructed B0→D*+lν¯ and B-→D*0lν¯ decays as a function of w, the boost of the D* in the B rest frame, and from this we obtain the differential decay rate dΓ/dw. By extrapolating dΓ/dw to w=1, the kinematic end point at which the D* is at rest relative to the B, we extract the product |Vcb|F(1), where F(1) is the form factor at w=1. We find |Vcb|F(1)=0.0431±0.0013(stat)±0.0018(syst). We combine |Vcb|F(1) with theoretical results for F(1) to determine |Vcb|=0.0469±0.0014(stat)±0.0020(syst)±0.0018(theor). We also integrate the differential decay rate over w to obtain B(B0→D*+lν¯)=(6.09±0.19±0.40)% and B(B-→D*0lν¯)=(6.50±0.20±0.43)%. APS Digital Backfile Archive 1893-2003 Adam, N. E. oth Alexander, J. P. oth Bebek, C. oth Berger, B. E. oth Berkelman, K. oth Blanc, F. oth Boisvert, V. oth Cassel, D. G. oth Drell, P. S. oth Duboscq, J. E. oth Ecklund, K. M. oth Ehrlich, R. oth Gibbons, L. oth Gittelman, B. oth Gray, S. W. oth Hartill, D. L. oth Heltsley, B. K. oth Hsu, L. oth Jones, C. D. oth Kandaswamy, J. oth Kreinick, D. L. oth Magerkurth, A. oth Mahlke-Krüger, H. oth Meyer, T. O. oth Mistry, N. B. oth Nordberg, E. oth Palmer, M. oth Patterson, J. R. oth Peterson, D. oth Pivarski, J. oth Riley, D. oth Sadoff, A. J. oth Schwarthoff, H. oth Shepherd, M. R. oth Thayer, J. G. oth Urner, D. oth Valant-Spaight, B. oth Viehhauser, G. oth Warburton, A. oth Weinberger, M. oth Enthalten in Physical review / D [S.l.] : Soc., 1970 67(2003), 3 Online-Ressource (DE-627)NLEJ248237861 (DE-600)1461167-3 1550-2368 nnns volume:67 year:2003 number:3 extent:22 https://www.tib.eu/de/suchen/id/aps%3A0fcf5bd91536723f4b45e1eaa1bd1e605c1ba090 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 67 2003 3 22 |
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(DE-627)NLEJ249939398 (DE-601)aps:0fcf5bd91536723f4b45e1eaa1bd1e605c1ba090 DE-627 ger DE-627 rakwb Determination of the B¯→D*lν¯ decay width and |Vcb| 2003 Online-Ressource 22 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In the standard model, the charged current of the weak interaction is governed by a unitary quark mixing matrix that also leads to CP violation. Measurement of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements is essential to searches for new physics, either through the structure of the CKM matrix, or a departure from unitarity. We determine the CKM matrix element |Vcb| using a sample of 3×106 BB¯ events in the CLEO detector at the Cornell Electron Storage Ring. We determine the yield of reconstructed B0→D*+lν¯ and B-→D*0lν¯ decays as a function of w, the boost of the D* in the B rest frame, and from this we obtain the differential decay rate dΓ/dw. By extrapolating dΓ/dw to w=1, the kinematic end point at which the D* is at rest relative to the B, we extract the product |Vcb|F(1), where F(1) is the form factor at w=1. We find |Vcb|F(1)=0.0431±0.0013(stat)±0.0018(syst). We combine |Vcb|F(1) with theoretical results for F(1) to determine |Vcb|=0.0469±0.0014(stat)±0.0020(syst)±0.0018(theor). We also integrate the differential decay rate over w to obtain B(B0→D*+lν¯)=(6.09±0.19±0.40)% and B(B-→D*0lν¯)=(6.50±0.20±0.43)%. APS Digital Backfile Archive 1893-2003 Adam, N. E. oth Alexander, J. P. oth Bebek, C. oth Berger, B. E. oth Berkelman, K. oth Blanc, F. oth Boisvert, V. oth Cassel, D. G. oth Drell, P. S. oth Duboscq, J. E. oth Ecklund, K. M. oth Ehrlich, R. oth Gibbons, L. oth Gittelman, B. oth Gray, S. W. oth Hartill, D. L. oth Heltsley, B. K. oth Hsu, L. oth Jones, C. D. oth Kandaswamy, J. oth Kreinick, D. L. oth Magerkurth, A. oth Mahlke-Krüger, H. oth Meyer, T. O. oth Mistry, N. B. oth Nordberg, E. oth Palmer, M. oth Patterson, J. R. oth Peterson, D. oth Pivarski, J. oth Riley, D. oth Sadoff, A. J. oth Schwarthoff, H. oth Shepherd, M. R. oth Thayer, J. G. oth Urner, D. oth Valant-Spaight, B. oth Viehhauser, G. oth Warburton, A. oth Weinberger, M. oth Enthalten in Physical review / D [S.l.] : Soc., 1970 67(2003), 3 Online-Ressource (DE-627)NLEJ248237861 (DE-600)1461167-3 1550-2368 nnns volume:67 year:2003 number:3 extent:22 https://www.tib.eu/de/suchen/id/aps%3A0fcf5bd91536723f4b45e1eaa1bd1e605c1ba090 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 67 2003 3 22 |
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(DE-627)NLEJ249939398 (DE-601)aps:0fcf5bd91536723f4b45e1eaa1bd1e605c1ba090 DE-627 ger DE-627 rakwb Determination of the B¯→D*lν¯ decay width and |Vcb| 2003 Online-Ressource 22 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In the standard model, the charged current of the weak interaction is governed by a unitary quark mixing matrix that also leads to CP violation. Measurement of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements is essential to searches for new physics, either through the structure of the CKM matrix, or a departure from unitarity. We determine the CKM matrix element |Vcb| using a sample of 3×106 BB¯ events in the CLEO detector at the Cornell Electron Storage Ring. We determine the yield of reconstructed B0→D*+lν¯ and B-→D*0lν¯ decays as a function of w, the boost of the D* in the B rest frame, and from this we obtain the differential decay rate dΓ/dw. By extrapolating dΓ/dw to w=1, the kinematic end point at which the D* is at rest relative to the B, we extract the product |Vcb|F(1), where F(1) is the form factor at w=1. We find |Vcb|F(1)=0.0431±0.0013(stat)±0.0018(syst). We combine |Vcb|F(1) with theoretical results for F(1) to determine |Vcb|=0.0469±0.0014(stat)±0.0020(syst)±0.0018(theor). We also integrate the differential decay rate over w to obtain B(B0→D*+lν¯)=(6.09±0.19±0.40)% and B(B-→D*0lν¯)=(6.50±0.20±0.43)%. APS Digital Backfile Archive 1893-2003 Adam, N. E. oth Alexander, J. P. oth Bebek, C. oth Berger, B. E. oth Berkelman, K. oth Blanc, F. oth Boisvert, V. oth Cassel, D. G. oth Drell, P. S. oth Duboscq, J. E. oth Ecklund, K. M. oth Ehrlich, R. oth Gibbons, L. oth Gittelman, B. oth Gray, S. W. oth Hartill, D. L. oth Heltsley, B. K. oth Hsu, L. oth Jones, C. D. oth Kandaswamy, J. oth Kreinick, D. L. oth Magerkurth, A. oth Mahlke-Krüger, H. oth Meyer, T. O. oth Mistry, N. B. oth Nordberg, E. oth Palmer, M. oth Patterson, J. R. oth Peterson, D. oth Pivarski, J. oth Riley, D. oth Sadoff, A. J. oth Schwarthoff, H. oth Shepherd, M. R. oth Thayer, J. G. oth Urner, D. oth Valant-Spaight, B. oth Viehhauser, G. oth Warburton, A. oth Weinberger, M. oth Enthalten in Physical review / D [S.l.] : Soc., 1970 67(2003), 3 Online-Ressource (DE-627)NLEJ248237861 (DE-600)1461167-3 1550-2368 nnns volume:67 year:2003 number:3 extent:22 https://www.tib.eu/de/suchen/id/aps%3A0fcf5bd91536723f4b45e1eaa1bd1e605c1ba090 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 67 2003 3 22 |
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Adam, N. E. @@oth@@ Alexander, J. P. @@oth@@ Bebek, C. @@oth@@ Berger, B. E. @@oth@@ Berkelman, K. @@oth@@ Blanc, F. @@oth@@ Boisvert, V. @@oth@@ Cassel, D. G. @@oth@@ Drell, P. S. @@oth@@ Duboscq, J. E. @@oth@@ Ecklund, K. M. @@oth@@ Ehrlich, R. @@oth@@ Gibbons, L. @@oth@@ Gittelman, B. @@oth@@ Gray, S. W. @@oth@@ Hartill, D. L. @@oth@@ Heltsley, B. K. @@oth@@ Hsu, L. @@oth@@ Jones, C. D. @@oth@@ Kandaswamy, J. @@oth@@ Kreinick, D. L. @@oth@@ Magerkurth, A. @@oth@@ Mahlke-Krüger, H. @@oth@@ Meyer, T. O. @@oth@@ Mistry, N. B. @@oth@@ Nordberg, E. @@oth@@ Palmer, M. @@oth@@ Patterson, J. R. @@oth@@ Peterson, D. @@oth@@ Pivarski, J. @@oth@@ Riley, D. @@oth@@ Sadoff, A. J. @@oth@@ Schwarthoff, H. @@oth@@ Shepherd, M. R. @@oth@@ Thayer, J. G. @@oth@@ Urner, D. @@oth@@ Valant-Spaight, B. @@oth@@ Viehhauser, G. @@oth@@ Warburton, A. @@oth@@ Weinberger, M. @@oth@@ |
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Determination of the B¯→D*lν¯ decay width and |Vcb| |
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Determination of the B¯→D*lν¯ decay width and |Vcb| |
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Determination of the B¯→D*lν¯ decay width and |Vcb| |
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determination of the b¯→d*lν¯ decay width and |vcb| |
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Determination of the B¯→D*lν¯ decay width and |Vcb| |
| abstract |
In the standard model, the charged current of the weak interaction is governed by a unitary quark mixing matrix that also leads to CP violation. Measurement of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements is essential to searches for new physics, either through the structure of the CKM matrix, or a departure from unitarity. We determine the CKM matrix element |Vcb| using a sample of 3×106 BB¯ events in the CLEO detector at the Cornell Electron Storage Ring. We determine the yield of reconstructed B0→D*+lν¯ and B-→D*0lν¯ decays as a function of w, the boost of the D* in the B rest frame, and from this we obtain the differential decay rate dΓ/dw. By extrapolating dΓ/dw to w=1, the kinematic end point at which the D* is at rest relative to the B, we extract the product |Vcb|F(1), where F(1) is the form factor at w=1. We find |Vcb|F(1)=0.0431±0.0013(stat)±0.0018(syst). We combine |Vcb|F(1) with theoretical results for F(1) to determine |Vcb|=0.0469±0.0014(stat)±0.0020(syst)±0.0018(theor). We also integrate the differential decay rate over w to obtain B(B0→D*+lν¯)=(6.09±0.19±0.40)% and B(B-→D*0lν¯)=(6.50±0.20±0.43)%. |
| abstractGer |
In the standard model, the charged current of the weak interaction is governed by a unitary quark mixing matrix that also leads to CP violation. Measurement of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements is essential to searches for new physics, either through the structure of the CKM matrix, or a departure from unitarity. We determine the CKM matrix element |Vcb| using a sample of 3×106 BB¯ events in the CLEO detector at the Cornell Electron Storage Ring. We determine the yield of reconstructed B0→D*+lν¯ and B-→D*0lν¯ decays as a function of w, the boost of the D* in the B rest frame, and from this we obtain the differential decay rate dΓ/dw. By extrapolating dΓ/dw to w=1, the kinematic end point at which the D* is at rest relative to the B, we extract the product |Vcb|F(1), where F(1) is the form factor at w=1. We find |Vcb|F(1)=0.0431±0.0013(stat)±0.0018(syst). We combine |Vcb|F(1) with theoretical results for F(1) to determine |Vcb|=0.0469±0.0014(stat)±0.0020(syst)±0.0018(theor). We also integrate the differential decay rate over w to obtain B(B0→D*+lν¯)=(6.09±0.19±0.40)% and B(B-→D*0lν¯)=(6.50±0.20±0.43)%. |
| abstract_unstemmed |
In the standard model, the charged current of the weak interaction is governed by a unitary quark mixing matrix that also leads to CP violation. Measurement of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements is essential to searches for new physics, either through the structure of the CKM matrix, or a departure from unitarity. We determine the CKM matrix element |Vcb| using a sample of 3×106 BB¯ events in the CLEO detector at the Cornell Electron Storage Ring. We determine the yield of reconstructed B0→D*+lν¯ and B-→D*0lν¯ decays as a function of w, the boost of the D* in the B rest frame, and from this we obtain the differential decay rate dΓ/dw. By extrapolating dΓ/dw to w=1, the kinematic end point at which the D* is at rest relative to the B, we extract the product |Vcb|F(1), where F(1) is the form factor at w=1. We find |Vcb|F(1)=0.0431±0.0013(stat)±0.0018(syst). We combine |Vcb|F(1) with theoretical results for F(1) to determine |Vcb|=0.0469±0.0014(stat)±0.0020(syst)±0.0018(theor). We also integrate the differential decay rate over w to obtain B(B0→D*+lν¯)=(6.09±0.19±0.40)% and B(B-→D*0lν¯)=(6.50±0.20±0.43)%. |
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Determination of the B¯→D*lν¯ decay width and |Vcb| |
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Adam, N. E. Alexander, J. P. Bebek, C. Berger, B. E. Berkelman, K. Blanc, F. Boisvert, V. Cassel, D. G. Drell, P. S. Duboscq, J. E. Ecklund, K. M. Ehrlich, R. Gibbons, L. Gittelman, B. Gray, S. W. Hartill, D. L. Heltsley, B. K. Hsu, L. Jones, C. D. Kandaswamy, J. Kreinick, D. L. Magerkurth, A. Mahlke-Krüger, H. Meyer, T. O. Mistry, N. B. Nordberg, E. Palmer, M. Patterson, J. R. Peterson, D. Pivarski, J. Riley, D. Sadoff, A. J. Schwarthoff, H. Shepherd, M. R. Thayer, J. G. Urner, D. Valant-Spaight, B. Viehhauser, G. Warburton, A. Weinberger, M. |
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Adam, N. E. Alexander, J. P. Bebek, C. Berger, B. E. Berkelman, K. Blanc, F. Boisvert, V. Cassel, D. G. Drell, P. S. Duboscq, J. E. Ecklund, K. M. Ehrlich, R. Gibbons, L. Gittelman, B. Gray, S. W. Hartill, D. L. Heltsley, B. K. Hsu, L. Jones, C. D. Kandaswamy, J. Kreinick, D. L. Magerkurth, A. Mahlke-Krüger, H. Meyer, T. O. Mistry, N. B. Nordberg, E. Palmer, M. Patterson, J. R. Peterson, D. Pivarski, J. Riley, D. Sadoff, A. J. Schwarthoff, H. Shepherd, M. R. Thayer, J. G. Urner, D. Valant-Spaight, B. Viehhauser, G. Warburton, A. Weinberger, M. |
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