We present a measurement of the top quark mass in the dilepton channel using a technique in which we form a posterior probability for the mass as a product of the per-event differential cross-section for leading order top quark pair production. The calculation of the differential cross section for processes which produce background events are used to reduce the impact of background events in the sample.
In 340 pb-1 of Run II data, we expect a statistical uncertainty of 9.4 GeV if Mtop=178.0 GeV/c2 (7.8 GeV/c2 if Mtop=165.0 GeV/c2) and a systematic uncertainty of 3.6 GeV/c2. We measure Mtop = 165.3 ± 6.3 (stat.) ± 3.6 (syst.) GeV/c2
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| Final posterior probability density as a function of top pole mass for the 33 dilepton candidate events in data. | ![]() |
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| Final posterior probability density as a function of top pole mass for the 33 dilepton candidate events in data with an overlaid gaussian fit. | ![]() |
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| Expected distribution of errors from MC (Mt=165 GeV/c2) and measured error in data. 17% of pseudo-experiments had an error lower than that measured in data. | ![]() |
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| Response for pseudo-experiments of signal and background events. | ![]() |
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| Residual, pull mean, and pull width for varying top mass MC samples before scaling of statistical error | ![]() |
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| Residual, pull mean, and pull width for varying top mass MC samples after scaling of statistical error | ![]() |
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| Table of systematic errors. | ![]() |
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| Evaluation of the ttbar probability (evaluated at Mtop=165 GeV/c2) for simulated events, scaled by expected contribution to the sample composition, and for observed events. | ![]() |
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| Evaluation of the Z+2 jet probability for simulated events, scaled by expected contribution to the sample composition, and for observed events. | ![]() |
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| Evaluation of the WW+2 jet probability for simulated events, scaled by expected contribution to the sample composition, and for observed events. | ![]() |
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| Evaluation of the W+3 jet probability for simulated events, scaled by expected contribution to the sample composition, and for observed events. | ![]() |
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| Projected statistical error for this method. | ![]() |
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