Effect of blood curve smearing on the accuracy of parameter estimates obtained for 82Rb/PET studies of blood-brain barrier permeability.

82Rb in conjunction with positron emission tomography (PET) has been used to estimate the blood to brain transport rate constant (K1) for Rb and the regional brain/tumour blood volume (Vb). Errors in K1 and Vb depend upon the accuracy of the measured arterial blood radioactivity and PET-monitored brain radioactivity. Arterial blood is usually sampled by placing a catheter in the radial artery and measuring the radioactivity in blood passing continuously in front of a detector or by counting discrete blood samples in a well scintillation detector. In either case, the passage of blood through catheter/pump tubing produces a smearing of the waveform as well as a delay in the arrival of radioactivity at the blood sampling site. The change in shape of the blood curve is significant for bolus-type injections and results in large errors in those model parameters which contribute substantially to the initial phase of the brain activity curve. We report here the results of computer simulations and an analysis of patient data which suggest that parameter estimation errors due to smearing and time shift may be large (greater than 50%) but that these errors can be minimised by the use of deconvolution techniques.

[1]  D A Rottenberg,et al.  Positron emission tomographic measurement of blood‐to‐brain and blood‐to‐tumor transport of 82Rb: The effect of dexamethasone and whole‐brain radiation therapy , 1985, Annals of neurology.

[2]  Iwao Kanno,et al.  Measurement of Cerebral Blood Flow Using Bolus Inhalation of C15O2 and Positron Emission Tomography: Description of the Method and its Comparison with the C15O2 Continuous Inhalation Method , 1984, Journal of cerebral blood flow and metabolism : official journal of the International Society of Cerebral Blood Flow and Metabolism.

[3]  L. Sokoloff,et al.  Quantitative measurement of regional circulation in the central nervous system by the use of radioactive inert gas. , 1958, Advances in biological and medical physics.

[4]  M. Mintun,et al.  Brain blood flow measured with intravenous H2(15)O. II. Implementation and validation. , 1983, Journal of nuclear medicine : official publication, Society of Nuclear Medicine.

[5]  M D Ginsberg,et al.  Emission tomographic measurement of local cerebral blood flow in humans by an in vivo autoradiographic strategy , 1984, Annals of neurology.

[6]  I. Kanno,et al.  Error Analysis of a Quantitative Cerebral Blood Flow Measurement Using H215O Autoradiography and Positron Emission Tomography, with Respect to the Dispersion of the Input Function , 1986, Journal of cerebral blood flow and metabolism : official journal of the International Society of Cerebral Blood Flow and Metabolism.

[7]  M. Reivich,et al.  Measurement of regional cerebral blood flow with antipyrine-14C in awake cats. , 1969, Journal of applied physiology.

[8]  R R Read,et al.  Catheter smearing correction using inverse filtering techniques. , 1972, IEEE transactions on bio-medical engineering.

[9]  M. Phelps,et al.  Effects of Temporal Sampling, Glucose Metabolic Rates, and Disruptions of the Blood—Brain Barrier on the FDG Model with and without a Vascular Compartment: Studies in Human Brain Tumors with PET , 1986, Journal of cerebral blood flow and metabolism : official journal of the International Society of Cerebral Blood Flow and Metabolism.

[10]  R. Hichwa,et al.  A Continuous Flow Input Function Detector for H2 15O Blood Flow Studies in Positron Emission Tomography , 1986, IEEE Transactions on Nuclear Science.

[11]  D A Rottenberg,et al.  Accuracy of PET RCBF measurements: effect of time shift between blood and brain radioactivity curves. , 1986, Physics in medicine and biology.

[12]  John A. Nelder,et al.  A Simplex Method for Function Minimization , 1965, Comput. J..