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. 2011 Feb 1;38(2):1089–1102. doi: 10.1118/1.3539602

Table 2.

The RMSD and the COV calculated against the recorded spectra measured by all of the comparators of the DXMCT-1. The numbers in brackets below the tube current values are the mean counts per keV between 30 and 150 keV.

  Scheme Tube current (μA)
    25 [30.9] 50 [63.9] 75 [97.4] 100 [119.6] 200 [192.9] 300 [234.7] 400 [261.6] 500 [277.5]
  NPa, NModel(E)b 10.8 7.8 11.1 12.3 53.0 73.9 85.3 87.5  
RMSD NPa, aR×S0(E)c 6.6 17.3 30.8 37.2 62.7 80.5 104.4 128.8
[counts] Pd, NModel(E)b 3.7 1.7 5.8 4.5 10.0 17.1 41.3 71.8
  Pd, aR×S0(E)c 3.9 7.5 11.6 16.5 49.7 95.2 130.5 153.3
  NPa, NModel(E)b 32.7 11.7 11.6 10.2 27.3 31.3 32.4 31.3
COV NPa, aR×S0(E)c 20.2 25.9 32.1 30.7 32.3 34.1 39.6 46.0
[%] Pd, NModel(E)b 11.3 2.6 6.0 3.7 5.2 7.2 15.7 25.7
  Pd, aR×S0(E)c 12.0 11.3 12.1 13.6 25.6 40.3 49.5 54.8
a

Nonparalyzable detection model.

b

Estimated by pulse pileup model, Eq. 6.

c

PDF of incident spectrum S0(E) scaled by aR.

d

Paralyzable detection model.