Difference between revisions of "LB 170063 Nickel Information With Dead Time"
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||Rate (Hz) || <math> 1.009048 \times 10^6 \pm 1.2829 \times 10^4 </math> || <math>7.58401 \times 10^5 \pm 2.470 \times 10^3</math> ||<math> 4.15280 \times 10^5 \pm 1.248 \times 10^3 </math> || <math>1.84531 \times 10^5 \pm 8.58 \times 10^2 </math>||<math> 8.4720 \times 10^4 \pm 3.2115 \times 10^2</math> ||<math> 5.8017 \times 10^4 \pm 2.5233 \times 10^2 </math>|| <math> 3.5402 \times 10^4 \pm 1.9360 \times 10^2 </math> | ||Rate (Hz) || <math> 1.009048 \times 10^6 \pm 1.2829 \times 10^4 </math> || <math>7.58401 \times 10^5 \pm 2.470 \times 10^3</math> ||<math> 4.15280 \times 10^5 \pm 1.248 \times 10^3 </math> || <math>1.84531 \times 10^5 \pm 8.58 \times 10^2 </math>||<math> 8.4720 \times 10^4 \pm 3.2115 \times 10^2</math> ||<math> 5.8017 \times 10^4 \pm 2.5233 \times 10^2 </math>|| <math> 3.5402 \times 10^4 \pm 1.9360 \times 10^2 </math> | ||
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− | ||True Rate (Integral Method) (Hz) || <math>1.040020 \times 10^6 \pm 1.3222 \times 10^4 </math> ||<math> 7.81679 \times 10^5 \pm 2.5458 \times 10^3</math> ||<math> 4.29155 \times 10^5 \pm 1.290 \times 10^3 </math> || <math> 1.90175 \times 10^5 \pm 8.8425 \times 10^2 </math>||<math> 8.7072 \times 10^4 \pm 3.29 \times 10^2 </math> || <math> 5.9793 \times 10^4 \pm 2.59 \times 10^2 || <math> 3.6508 \times 10^4 \pm 2.00 \times 10^2 </math> | + | ||True Rate (Integral Method) (Hz) || <math>1.040020 \times 10^6 \pm 1.3222 \times 10^4 </math> ||<math> 7.81679 \times 10^5 \pm 2.5458 \times 10^3</math> ||<math> 4.29155 \times 10^5 \pm 1.290 \times 10^3 </math> || <math> 1.90175 \times 10^5 \pm 8.8425 \times 10^2 </math>||<math> 8.7072 \times 10^4 \pm 3.29 \times 10^2 </math> || <math> 5.9793 \times 10^4 \pm 2.59 \times 10^2 </math> || <math> 3.6508 \times 10^4 \pm 2.00 \times 10^2 </math> |
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Revision as of 19:07, 5 December 2017
Below is a table with thin windows, original windows, and expanded windows for the nickel on sample 170063. The thin window method can be found at LB Thesis Thin Window Analysis.