A count rate from a decaying source is measured in four equal time windows

PHYSICS · Multi-part · Fermi University Physics · Scientific Practice & Experimental Methods · Uncertainty in measurement · Data analysis and model fitting in the laboratory

Mathematical Methods for Physics, Ch Estimation, fitting and hypothesis testing

Problem

A count rate from a decaying source is measured in four equal time windows, giving counts CjC_j at times tjt_j: C=800C=800 at t=0 st=0\,\mathrm{s}, C=340C=340 at t=15 st=15\,\mathrm{s}, C=120C=120 at t=30 st=30\,\mathrm{s}, C=44C=44 at t=45 st=45\,\mathrm{s}. Someone argues: “To get the half-life I fit ln⁡C\ln C against tt. I used an ordinary, unweighted least-squares fit, because weighting the points seemed complicated and least squares just minimises the sum of squared residuals regardless. This gave a slope b=−0.0650 s−1±0.0019 s−1b=-0.0650\,\mathrm{s}^{-1}\pm0.0019\,\mathrm{s}^{-1} (one sigma), so the half-life is ln⁡2/0.0650=10.7±0.3 s\ln2/0.0650=10.7\pm0.3\,\mathrm{s}.” ((a)) Identify the error in choosing an unweighted fit for these data, and state what the weight wjw_j of each point should be instead, with numerical values. ((b)) Redo the fit with those weights, and quote the slope and the half-life, each with its uncertainty. ((c)) Find the minimised χ2\chi^2 of the weighted fit and its number of degrees of freedom, and say whether Poisson errors account for the scatter of the four points.

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