Saxsons Group

Medical Physicist's Notes · Delta4 Phantom+

One linac pulse is about 1 mGy. Delta4 resolves it at 50 nGy.

Modern radiotherapy is moving toward higher dose-per-pulse delivery — flattening-filter-free (FFF) beams, hypofractionated SBRT/SRS, and the emerging clinical interest in FLASH. The integrating detectors that work at conventional dose-per-pulse don't extrapolate cleanly to these regimes, for reasons that are well documented in the dosimetry literature. This page lays out the physics, the documented limits of conventional QA detectors, and what Delta4 Phantom+ does about it.

~1 mGy

typical dose per pulse

Conventional 6 MV linac, single dose pulse at iso. — the manufacturer figure.

50 nGy

Delta4 integration resolution

Per pulse — 1 part in 20,000 of a typical pulse. From the Manufacturer brochure.

≥40 Gy/s

FLASH instantaneous threshold

Pre-clinical sparing demonstrated above this rate — Vozenin 2019, Bourhis 2019.

The delivery this detector serves

A clinical linac delivers dose as a discrete train of bremsstrahlung pulses, each on the order of a few microseconds and depositing roughly 1 mGy at the isocentre under conventional 6 MV operation. Modern delivery techniques push that dose-per-pulse higher: FFF beams remove the flattening filter and raise the pulse intensity several-fold; SBRT and SRS use those higher rates to keep treatment times manageable at high prescription doses; and FLASH radiotherapy operates an order of magnitude higher again, at ≥40 Gy/s instantaneous, where pre-clinical normal-tissue sparing has been documented.

Sources: the manufacturer Delta4 Phantom+ brochure · Vozenin et al., Clin Cancer Res 25(1):35–42 (2019) · Bourhis et al., Radiother Oncol 139:18–22 (2019).

What the published literature says about high-dose-per-pulse measurement

None of the points below is rhetorical. Each is paraphrased from a peer-reviewed source and cited inline. The implication is consistent across them: the dosimetry chain that worked at 0.1–0.5 mGy per pulse does not extend without explicit correction to FFF, SBRT or UHDR delivery.

  1. 01

    Ion chambers under-respond at high dose-per-pulse

    General (Boag) recombination in vented ion chambers scales with the charge density produced by a single pulse. In flattening-filter-free (FFF) beams the dose-per-pulse is several-fold higher than conventional flattened beams, and the standard two-voltage Boag correction becomes inadequate — Wang & Rogers showed that the correction itself becomes dose-per-pulse dependent and recommends a polynomial recombination formalism specific to FFF.

    Wang LLW & Rogers DWO, J Appl Clin Med Phys 13(5):3758 (2012)

  2. 02

    Diodes show dose-per-pulse sensitivity drift

    Commercially available silicon diodes are not perfectly dose-per-pulse independent: characterised response can vary by a few percent across the dose-per-pulse range encountered when SSD or field size changes. The effect is small in flattened beams but becomes clinically relevant in FFF and short-SSD setups unless explicitly corrected.

    Saini AS & Zhu TC, Med Phys 31(4):914–24 (2004), PMID 15259635

  3. 03

    FLASH / UHDR beams break the assumptions of conventional detector models

    At ultra-high dose-rate (UHDR; ≥40 Gy/s instantaneous), Romano et al. document detector saturation and recombination effects across active dosimeters that are designed against conventional dose-per-pulse. The dosimetric chain that worked at 0.1–0.5 mGy per pulse does not extend without verification to the 1–10 mGy per pulse regime.

    Romano F et al., Med Phys 49(7):4912–4932 (2022), PMC9544810

  4. 04

    FLASH normal-tissue sparing depends on instantaneous, not mean, dose rate

    The pre-clinical advantage of FLASH (≥30–40 Gy/s) is documented in Vozenin 2019 in mini-pig and cat-cancer patients; Bourhis 2019 reports the first human FLASH case at 15 Gy in 90 ms. The biological effect is governed by the dose-rate during the pulse — not by the average treatment time — so any QA chain claiming FLASH coverage must resolve the pulse, not the integrated cumulative dose.

    Vozenin MC et al., Clin Cancer Res 25(1):35–42 (2019) · Bourhis J et al., Radiother Oncol 139:18–22 (2019)

What does a patient-QA detector look like when its time base matches the time base of the linac — and the correction chain is shorter, not longer, at higher dose rates?

Delta4 Phantom+ — three facts on the architecture

Each row pairs a documented dosimetric problem with the architectural decision in Delta4 that addresses it. Sources are inline so the mapping is auditable.

  • One pulse at a time — 50 nGy resolution

    The manufacturer product brochure specifies: "Delta4 integrates one dose pulse (typically 1 mGy) at a time with a resolution of 50 nGy." The detector array is read out per pulse, not by integrating a fixed time window — so the time base of the measurement matches the time base of the linac.

    Source: Manufacturer brochure — Delta4 Phantom+ wireless phantom.

  • 0.04 mm³ p-type silicon diodes — no recombination correction needed

    The 1,069 p-Si disc diodes (1 mm × 0.05 mm; active volume 0.04 mm³) are intrinsically dose-rate independent across the clinical photon range — silicon does not exhibit the Boag general-recombination loss that vented ion chambers do. The published detector stability is <0.1%/kGy, typically 0.04%/kGy at 6 MV.

    Source: the manufacturer Delta4 Phantom+ technical specification.

  • No add-on hardware for high dose-rate measurement

    High dose-rate verification on chamber-based or film-based chains typically requires dedicated UHDR-tolerant hardware (Romano 2022 reviews the available options — radiochromic film, alanine, plastic scintillator, calorimetry). The Delta4 array as shipped — without add-ons — operates on the same per-pulse read-out across conventional, FFF and UHDR delivery.

    Source: Romano F et al., Med Phys 49(7):4912–4932 (2022); the manufacturer Delta4 Phantom+ specification.

Scope of this page

The 50 nGy per-pulse integration spec is taken from the manufacturer Delta4 Phantom+ brochure. The implications for FFF, SBRT and FLASH dosimetry above are grounded in peer-reviewed dosimetry literature on dose-per-pulse dependence and UHDR detector behaviour — not in head-to-head Delta4 vs competitor measurements at UHDR, which to our knowledge have not been published. Treat this page as an architectural argument that can be checked against the cited physics, not as a UHDR commissioning comparison.

Sources cited on this page

  • the manufacturer. Delta4 Phantom+ — The wireless phantom. Product brochure. Quoted spec: "Delta4 integrates one dose pulse (typically 1 mGy) at a time with a resolution of 50 nGy." Product page ↗
  • Wang LLW, Rogers DWO. Ion recombination corrections of ionization chambers in flattening filter-free photon radiation. J Appl Clin Med Phys 13(5):3758 (2012). JACMP ↗
  • Saini AS, Zhu TC. Dose rate and SDD dependence of commercially available diode detectors. Med Phys 31(4):914–924 (2004). PMID 15259635. PubMed ↗
  • Romano F, Bailat C, Jorge PG, Lerch MLF, Darafsheh A. Ultra-high dose rate dosimetry: challenges and opportunities for FLASH radiation therapy. Med Phys 49(7):4912–4932 (2022). PMC9544810 ↗
  • Vozenin MC, et al. The advantage of FLASH radiotherapy confirmed in mini-pig and cat-cancer patients. Clin Cancer Res 25(1):35–42 (2019). AACR ↗
  • Bourhis J, et al. Treatment of a first patient with FLASH-radiotherapy. Radiother Oncol 139:18–22 (2019). PubMed ↗