ANALITYCAL CALCULATION OF FWHM
AND COMPARISON WITH EXPERIMENTAL DATA
Copyright© 2013 Diego Cecchin - Davide Poggiali - Stefano De Marchi - Franco Bui
University Hospital of Padua - Nuclear Medicine Service
(Dir. Prof. Franco Bui)
Via Giustiniani 2 - 35128 - Padova - Italy
 
 
DATA (PROVIDED BY VENDOR) FOR ANALITYCAL CALCULATION
 L = Hole lenght (mm)
 c = Crystal Thickness (mm)
 D = Hole size (mm)
From:To: x = Source-Collimator distance (mm)
   [step (mm)]
 μ = linear att. coeff. of the coll. material at used energy
For a Lead Collimator (density ρ= 11.34 g/cm3)
At 150 KeV μ=1.910 cm2/g * 11.34 g/cm3=21.6594 cm-1 = 2.16594 mm-1
At 200 KeV μ=0.936 cm2/g * 11.34 g/cm3=10.61424 cm-1 = 1.061424 mm-1
At 300 KeV μ=0.373 cm2/g * 11.34 g/cm3=4.22982 cm-1 = 0.422982 mm-1
At 400 KeV μ=0.215 cm2/g * 11.34 g/cm3=2.4381 cm-1 = 0.24381 mm-1
At 500 KeV μ=0.150 cm2/g * 11.34 g/cm3=1.701 cm-1 = 0.1701 mm-1

 t = Septa Thickness (mm)
 K = Constant (0.26 for hexagonal holes; 0.28 for squared holes)
 Rint = Intrinsic Spatial Resolution (mm)

  Rcoll = D(Lcorr+x+c)/Lcorr

  Rsyst = √(Rcoll2 + Rint2) = FWHM

  Lcorr = L-2μ-1

  Max. septal penetration (%) = exp(-μ*w)*100
   where w=(Lt)/(2D+t)


  Collimator efficiency (in air) g = K2(D/Lcorr)2[D2/(D+t)2]


 
 
  DOWNLOAD Matlab/Octave code for FWHM calculation on static DICOM images
 
EXPERIMENTAL DATA
(if you want omit these values)
 X = EXPERIMENTAL DATA (mm) : Source-Collimator distance
 Y = EXPERIMENTAL DATA (mm) : FWHM
 SD = EXPERIMENTAL DATA (mm) : Standard deviation of FWHM
 


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