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Int. J. Radiation Oncology Biol. Phys., Vol. 51, No. 1, pp. 213–214, 2001 Copyright © 2001 Elsevier Science Inc. Printed in the USA. All rights reserved 0360-3016/01/$–see front matter PII S0360-3016(01)01651-0 BIOLOGY CONTRIBUTION A SIMPLE ANALYTIC DERIVATION SUGGESTS THAT PROSTATE CANCER ␣/ RATIO IS LOW CHRISTOPHER R. KING, PH.D., M.D.,* AND JACK F. FOWLER, D.SC., PH.D.† *Department of Radiation Oncology, Stanford University School of Medicine, Stanford, CA; †Department of Human Oncology, University of Wisconsin Hospital, Madison, WI Prostate cancer, Radiotherapy, Radiobiology, ␣/ ratio. Since the publication of Brenner and Hall’s recent paper (1) suggesting that the ␣/ ratio for prostate cancer is 1.5 Gy, a debate has been propagated through the radiotherapy community (2–5). This surprisingly low value carries implications of more efficient (and perhaps less costly) regimens of external beam radiotherapy (i.e., hypofractionated schedules) and optimal forms of brachytherapy (i.e., high dose rate). Should it prove to be true, such a low ratio would negate the therapeutic advantage of conventional fractionation regimens and call out for clinical trials. There is certainly indirect evidence for a low ␣/ ratio. The very small proportion of proliferating cells (6, 7), the very long observed doubling times (8, 9), the slow response to irradiation, and the recent interim results of high-dose-rate brachytherapy of varying fractionation (10) are all are consistent with such a low value. The surprise is that this value is as low as, if not even lower than, normal tissue response to irradiation. Can one apply the linear-quadratic (LQ) equation to outcomes of a population of clinically localized prostate cancer after radiotherapy? The LQ equation, although purely phenomenological, has certainly proven to be of great use, both in the study of cultured tumor cells irradiated in vitro, in comparing regimens of different fractionation, and in the study of normal tissue response to radiation. Although issues of inter- and intratumor heterogeneity are not directly accounted for in the standard LQ formalism, these issues might not necessarily affect the ␣/ ratio when applied to changes in fraction size (4). Whereas the ␣ term, a direct measure of radiosensitivity, does depend upon heterogeneity (3) and is intimately tied to the number of clonogens, the ratio ␣/ might not. We present a simple analytical derivation of ␣/ that is a logical conclusion from the observation that, for clinically localized prostate cancer, external beam and permanent brachytherapy appear to achieve equivalent outcomes. This derivation makes no assumptions and does not attempt to fit models to specific clinical data. For fractionated external-beam irradiation to a total dose De, with dose per fraction d, the LQ survival fraction of clonogens can be written as follows: Reprint requests to: Christopher R. King, Ph.D., M.D., Department of Radiation Oncology, Stanford University School of Medicine, 300 Pasteur Drive, Stanford, CA 94305. Tel: (650) 723-1420; Fax: (650) 498-6922; E-mail: christopher@reyes. stanford.edu Received Dec 5, 2000. Accepted for publication Feb 15, 2001. S e ⫽ exp(⫺␣ D e关1 ⫹ d/共 ␣ /  兲兴) (1) For permanent low-dose-rate brachytherapy, the extension of the LQ equation from Dale (11) can be written as follows: S b ⫽ exp(⫺␣ D b关1 ⫹ GD b/共 ␣ /  兲兴) (2) where Db is the minimal peripheral dose to decay and G (sometimes called the “Lea-Catcheside” term) accounts for source decay and sublethal damage repair kinetics and is given by G ⫽ /共 ⫹ 兲, with the decay constant and the repair constant. Values of 59.7 days for the half-life of 125 I and typically 1–2 hours for repair half-life result in G⬇10⫺3. Thus Eq. 2 may be simplified to: S b ⫽ exp(⫺␣ D b) (3) Because external beam and permanent brachytherapy are indeed nearly equivalent therapies, Se ⫽ Sb. Simple algebraic manipulation of Eqs. 1 and 3 yields: ␣ /  ⫽ d/共D b/D e ⫺ 1兲 (4) For standard values (i.e., d ⫽ 1.8 –2 Gy, De ⫽ 70 –74 Gy, and Db ⫽ 145 Gy [TG-43]), this yields: ␣/⬇2 Gy. If one wishes to include source decay and repair kinetics, then Eq. 4 becomes: ␣ /  ⫽ 共d ⫺ GD b2/D e兲/共D b/D e ⫺ 1兲 (5) For typical values this yields: ␣/ ⬃ 1.8 Gy. 213 214 I. J. Radiation Oncology ● Biology ● Physics It is interesting that this derivation is not dependent upon ␣ or estimates of clonogen number, or specific clinical outcome data. It simply follows from the LQ equations and the clinical observation that external beam and permanent brachytherapy achieve similar outcomes with current regimens. Because clinical outcomes for 125I or 103Pd are equivalent (12), similar values are expected if 103Pd data are used (i.e., half-life of 17 days and prescribed dose of 124 Gy Volume 51, Number 1, 2001 [NIST-99]). These values are ␣/ ⬃ 2.8 (or ⬃ 2 if decay and repair are included, as in Eq. 5). The values obtained here are consistent with those of Brenner and Hall (1) and Fowler et al. (5), who fit the LQ model to clinical series and continue to provide interesting insights into the clinical radiobiology of prostate cancer. They also provoke thought that perhaps prostate cancer might be optimally treated with hypofractionated regimens. REFERENCES 1. Brenner DJ, and Hall EJ. Fractionation and protraction for radiotherapy of prostate carcinoma. Int J Radiat Oncol Biol Phys 1999;43:1095–1101. 2. Duschesne GM, Peters LJ. What is the ␣/ ratio for prostate cancer? Rationale for hypofractionated high-dose-rate brachytherapy. Int J Radiat Oncol Biol Phys 1999;44:747–748 (editorial). 3. King CR, and Mayo CS. Is the prostate ␣/ Ŕatio of 1.5 from Brenner and Hall a modeling artifact? Int J Radiat Oncol Biol Phys 2000;47:536 –538 (letter). 4. Brenner DJ, Hall EJ. Low ␣/ values for prostate cancer appear to be independent of modeling details. Int J Radiat Oncol Biol Phys 2000;47:538 –539 (letter). 5. Fowler JF, Chappell R, Ritter MA. Is ␣/ for prostate really low? Int J Radiat Oncol Biol Phys 2001;50:1021–1031. 6. Haustermans KMG, Hofland I, Van Poppel H, Oyen R, Van der Voorde W, Begg AC, and Fowler JF. Cell kinetic measurements in prostate cancer. Int J Radiat Oncol Biol Phys 1997;37:1067–1070. 7. Haustermans KMG, and Fowler JF. A comment on prolifer- 8. 9. 10. 11. 12. ation rates in human prostate cancer. Int J Radiat Oncol Biol Phys 2000;48:303 (letter). Lee WR, Hanks GE, Corn BW, Schultheiss TE. Observations of pretreatment prostate-specific antigen doubling time in 107 patients referred for definitive radiotherapy. Int J Radiat Oncol Biol Phys 1995;31:21–24. Schmid HP. Tumour markers in patients on deferred treatment: Prostate specific antigen doubling times. Cancer Surv 1995;23:157–167. Martinez AA, Kestin LL, Stromberg JS, et al. Interim report of image-guided conformal high-dose-rate brachytherapy for patients with unfavorable prostate cancer: The William Beaumont phase II dose-escalation trial. Int J Radiat Oncol Biol Phys 2000;47:343–352. Dale RG. The application of the linear-quadratic dose-effect equation to fractionated and protracted radiotherapy. Br J Radiol 1985;58:515–528. Cha CM, Potters L, Ashley R, Freeman K, Wang X-H, Waldbaum R, and Leibel S. Isotope selection for patients undergoing prostate brachytherapy. Int J Radiat Oncol Biol Phys 1999;45:391–395.