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| 001 | 131500 | ||
| 005 | 20240228145604.0 | ||
| 024 | 7 | _ | |a 10.1088/1361-6560/aa8989 |2 doi |
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| 037 | _ | _ | |a DKFZ-2017-06167 |
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| 100 | 1 | _ | |a Debus, Charlotte |0 P:(DE-He78)c0d7724ccc0d258281c66fd40653c978 |b 0 |e First author |u dkfz |
| 245 | _ | _ | |a Impact of fitting algorithms on errors of parameter estimates in dynamic contrast-enhanced MRI. |
| 260 | _ | _ | |a Bristol |c 2017 |b IOP Publ. |
| 336 | 7 | _ | |a article |2 DRIVER |
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| 520 | _ | _ | |a Parameter estimation in dynamic contrast-enhanced MRI (DCE MRI) is usually performed by non-linear least square (NLLS) fitting of a pharmacokinetic model to a measured concentration-time curve. The two-compartment exchange model (2CXM) describes the compartments plasma and interstitial volume and their exchange in terms of plasma flow and capillary permeability. The model function can be defined by either a system of two coupled differential equations or a closed-form analytical solution. The aim of this study was to compare these two representations in terms of accuracy, robustness and computation speed, depending on parameter combination and temporal sampling. The impact on parameter estimation errors was investigated by fitting the 2CXM to simulated concentration-time curves. Parameter combinations representing five tissue types were used, together with two arterial input functions, a measured and a theoretical population based one, to generate 4D concentration images at three different temporal resolutions. Images were fitted by NLLS techniques, where the sum of squared residuals was calculated by either numeric integration with the Runge-Kutta method or convolution. Furthermore two example cases, a prostate carcinoma and a glioblastoma multiforme patient, were analyzed in order to investigate the validity of our findings in real patient data. The convolution approach yields improved results in precision and robustness of determined parameters. Precision and stability are limited in curves with low blood flow. The model parameter v e shows great instability and little reliability in all cases. Decreased temporal resolution results in significant errors for the differential equation approach in several curve types. The convolution excelled in computational speed by three orders of magnitude. Uncertainties in parameter estimation at low temporal resolution cannot be compensated by usage of the differential equations. Fitting with the convolution approach is superior in computational time, with better stability and accuracy at the same time. |
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| 700 | 1 | _ | |a Floca, R. |0 P:(DE-He78)f0ab09cfecf353f363bab4cc983de95d |b 1 |u dkfz |
| 700 | 1 | _ | |a Nörenberg, D. |b 2 |
| 700 | 1 | _ | |a Abdollahi, A. |0 P:(DE-He78)360c5bc2b71a849e35aca747c041dda7 |b 3 |u dkfz |
| 700 | 1 | _ | |a Ingrisch, M. |b 4 |
| 773 | _ | _ | |a 10.1088/1361-6560/aa8989 |g Vol. 62, no. 24, p. 9322 - 9340 |0 PERI:(DE-600)1473501-5 |n 24 |p 9322 - 9340 |t Physics in medicine and biology |v 62 |y 2017 |x 1361-6560 |
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