Physical mechanism of normal-tissue sparing at ultra-high dose rate · revision history

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Accepted · first revision · record

Title
Physical mechanism of normal-tissue sparing at ultra-high dose rate
Plain
Healthy tissue survives better when the dose arrives in a flash rather than slowly. The task is to find the physical or chemical process responsible.
Precise
Identify the mechanism by which mean dose rates above roughly $4000\ \mathrm{rad}/\mathrm{s}$ ($1\ \mathrm{rad} = 100\ \mathrm{erg}/\mathrm{g}$), delivered in under $200\ \mathrm{ms}$, raise normal-tissue tolerance at fixed total dose (typically $1000\ \text{to}\ 3000\ \mathrm{rad}$ single fraction) without a matching rise in tumour tolerance. Candidate classes: transient radiolytic oxygen depletion, inter-track radical-radical recombination altering peroxidation yields, differential iron and labile metal pools, immune and vascular responses. An answer is a quantitative model reproducing the measured sparing as a function of dose, dose rate, pulse structure and tissue oxygen tension.
Settled by
A model whose parameters are fixed by independent chemical and physiological measurements and that predicts, without refitting, the sparing measured across electron, proton and photon FLASH experiments in several tissues.
Kind
phenomenon
Answer type
mechanism
References
(empty)
Literature status
open
Status note
As of 2025 oxygen depletion alone is widely judged insufficient and no consensus mechanism exists.
Posed since
2014