The Physical and Radiobiological Basis of the Local Effect Model:A Response to the Commentary by R. Katz

Abstract Scholz, M. and Kraft, G. The Physical and Radiobiological Basis of the Local Effect Model: A Response to the Commentary by R. Katz. Radiat. Res. 161, 612–620 (2004). The physical and biological basis of our model to calculate the biological effects of charged particles, termed the local effect model (LEM), has recently been questioned in a commentary by R. Katz. Major objections were related to the definition of the target size and the use of the term cross section. Here we show that the objections raised against our approach are unjustified and are largely based on serious misunderstandings of the conceptual basis of the local effect model. Furthermore, we show that the approach developed by Katz and coworkers itself suffers from exactly those deficiencies for which Katz criticizes our model. The essential conceptual differences between the two models are discussed by means of some illustrative examples, based on a comparison with experimental data. For these examples, the predictions of the local effect model are fully consistent with the experimental data. In contrast, e.g. for very heavy ions, there are significant discrepancies observed for the Katz approach. These discrepancies can be attributed to the inadequate definition of the target size in this model. Experimental data are thus clearly in favor of the definition of the target as used in the local effect model. Agreement with experimental data is achieved for protons within the Katz approach but at the cost of questionable approximations in combination with the violation of the fundamental physical principle of energy conservation.

[1]  M. Scholz,et al.  Computation of cell survival in heavy ion beams for therapy , 1997, Radiation and environmental biophysics.

[2]  M Goitein,et al.  Biophysical modelling of proton radiation effects based on amorphous track models , 2001, International journal of radiation biology.

[3]  J. Debus,et al.  Feasibility and toxicity of combined photon and carbon ion radiotherapy for locally advanced adenoid cystic carcinomas. , 2003, International journal of radiation oncology, biology, physics.

[4]  G. Taucher‐Scholz,et al.  A track structure model for simulation of strand breaks in plasmid DNA after heavy ion irradiation , 2003, Radiation and environmental biophysics.

[5]  W. John,et al.  Calculation of Heavy Ion Inactivation and Mutation Rates in Radial Dose Model of Track Structure , 1997 .

[6]  F. Cucinotta,et al.  RBE vs. dose for low doses of high-let radiations. , 1991, Health physics.

[7]  J. Debus,et al.  Acute radiation-induced toxicity of heavy ion radiotherapy delivered with intensity modulated pencil beam scanning in patients with base of skull tumors. , 2002, Radiotherapy and oncology : journal of the European Society for Therapeutic Radiology and Oncology.

[8]  D T Goodhead,et al.  Direct comparison between protons and alpha-particles of the same LET: I. Irradiation methods and inactivation of asynchronous V79, HeLa and C3H 10T1/2 cells. , 1992, International journal of radiation biology.

[9]  M. Scholz,et al.  Calculation of Heavy Ion Inactivation Probabilities Based on Track Structure, X Ray Sensitivity and Target Size , 1994 .

[10]  R. Katz The Parameter-Free Track Structure Model of Scholz and Kraft for Heavy-Ion Cross Sections , 2003, Radiation research.

[11]  E. Blakely,et al.  Heavy-ion effects on mammalian cells: inactivation measurements with different cell lines. , 1985, Radiation research. Supplement.

[12]  Robert Katz,et al.  Radial Distribution of Dose and Cross-Sections for the Inactivation of Dry Enzymes and Viruses , 1985 .

[13]  G. Taucher‐Scholz,et al.  Direct Evidence for the Spatial Correlation between Individual Particle Traversals and Localized CDKN1A (p21) Response Induced by High-LET Radiation , 2001, Radiation research.

[14]  F Ianzini,et al.  Inactivation and mutation induction in V79 cells by low energy protons: re-evaluation of the results at the LNL facility. , 1993, International journal of radiation biology.

[15]  M. Joiner,et al.  Renal damage in the mouse: the response to very small doses per fraction. , 1988, Radiation research.

[16]  R. Katz,et al.  Survey of cellular radiosensitivity parameters. , 1994, Radiation research.

[17]  M Scholz,et al.  Track structure and the calculation of biological effects of heavy charged particles. , 1996, Advances in space research : the official journal of the Committee on Space Research.

[18]  D. Dunn,et al.  Thindown in Radiobiology , 1985 .

[19]  B. Vojnovic,et al.  The irradiation of V79 mammalian cells by protons with energies below 2 MeV. Part I: Experimental arrangement and measurements of cell survival. , 1989, International journal of radiation biology.

[20]  M Scholz,et al.  Calculation of RBE for normal tissue complications based on charged particle track structure. , 1996, Bulletin du cancer. Radiotherapie : journal de la Societe francaise du cancer : organe de la societe francaise de radiotherapie oncologique.

[21]  S. C. Sharma,et al.  Inactivation of cells by heavy ion bombardment. , 1971, Radiation research.

[22]  S. C. Sharma,et al.  Response of cells to fast neutrons, stopped pions, and heavy ion beams , 1973 .

[23]  R. Katz,et al.  Tracks to therapy. , 1999, Radiation measurements.

[24]  R. Katz,et al.  Theory of RBE for heavy ion bombardment of dry enzymes and viruses. , 1967, Radiation research.

[25]  M. Joiner A comparison of the effects of p(62)-Be and d(16)-Be neutrons in the mouse kidney. , 1988, Radiotherapy and oncology : journal of the European Society for Therapeutic Radiology and Oncology.

[26]  John B. Shoven,et al.  I , Edinburgh Medical and Surgical Journal.

[27]  G. Taucher‐Scholz,et al.  Immediate Localized CDKN1A (p21) Radiation Response after Damage Produced by Heavy-Ion Tracks , 2000, Radiation research.