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2d ionization chamber array matrixxone  (IBA Dosimetry)

 
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    IBA Dosimetry 2d ionization chamber array matrixxone
    2d Ionization Chamber Array Matrixxone, supplied by IBA Dosimetry, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/product/2d+ionization+chamber+array/the+matrixx+evolution+2d+ionization+chamber+array/pmc12138570-65-15-20
    Average 90 stars, based on 1 article reviews
    2d ionization chamber array matrixxone - by Bioz Stars, 2026-10
    90/100 stars

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    Article Title: Characterization and use of a 2D-array of ion chambers for brachytherapy dosimetric quality assurance.
    Article Snippet: The two-dimensional (2D) ionization chamber array MatriXX Evolution is one of the 2D ionization chamber Received 08 April 2011 Accepted 13 September 2011 arrays developed by IBA Dosimetry (IBA Dosimetry, Germany) for megavoltage real-time absolute 2D dosimetry and verification of intensity-modulated radiation therapy (IMRT).. The purpose of this study was to (1) evaluate the performance of ion chamber array for submegavoltage range brachytherapy beam dose verification and quality assurance (QA) and (2) use the end-to-end dosimetric evaluation that mimics a patient treatment procedure and confirm the primary source strength calibration agrees in both the treatment planning system (TPS) and treatment delivery console computers.. The dose linearity and energy dependence of the 2D ion chamber array was studied using kilovoltage X-ray beams (100, 180 and 300 kVp).

    Article Title: The influence of a novel transmission detector on 6 MV x-ray beam characteristics.
    Article Snippet: The purpose of this work was to investigate the influence of a new transmission detector on 6 MV x-ray beam properties.. The device, COMPASS (IBA Dosimetry, Germany), contains 1600 plane parallel ionization chambers with a detector spacing of 6.5 mm and an active volume of 0.02 cm3.. Surface dose measurements were carried out using a Markus chamber and radiochromic film for a range of field sizes and source-to-surface distances (SSDs).



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    Image Search Results


    Signal amplitude from the CROSSmini detector with signal fitting and zoomed in views. Figures A, B and C, on the left, shows the signal amplitude from the CROSSmini detector of a spill duration for energy level 70.2, 150.2, and 228.7 MeV, respectively, with nominal beam current 8 MU/s. The red line represents the original signal from CROSSmini and the black line represents the piecewise fitting for the edges. On the right is the zoomed in view of the fitting. The piecewise fitting quantifies the risetime ( t rise ) and measured nominal beam current ( I 0 , measured ).

    Journal: International Journal of Particle Therapy

    Article Title: Phenomenological Study of Intra-Spill Break Spots in Dose-Driven Continuous Scanning Proton Therapy

    doi: 10.1016/j.ijpt.2026.101315

    Figure Lengend Snippet: Signal amplitude from the CROSSmini detector with signal fitting and zoomed in views. Figures A, B and C, on the left, shows the signal amplitude from the CROSSmini detector of a spill duration for energy level 70.2, 150.2, and 228.7 MeV, respectively, with nominal beam current 8 MU/s. The red line represents the original signal from CROSSmini and the black line represents the piecewise fitting for the edges. On the right is the zoomed in view of the fitting. The piecewise fitting quantifies the risetime ( t rise ) and measured nominal beam current ( I 0 , measured ).

    Article Snippet: The beam current was measured using a CROSSmini 2D strip ionization chamber detector array (Liverage Biomedical Inc, Taiwan) positioned at the isocenter plane.

    Techniques:

    Signal amplitude from the CROSSmini detector with signal fitting. shows the signal amplitude as a function of time measured by the CROSSmini detector and the piecewise fittings. Figures A, B, and C are measurements for energy level 70.2 MeV with nominal beam current 8, 14, and 20 MU/s, respectively. Figures D, E, and F are the measurements for energy level 228.7 MeV with nominal beam current 8, 14, and 20 MU/s, respectively.

    Journal: International Journal of Particle Therapy

    Article Title: Phenomenological Study of Intra-Spill Break Spots in Dose-Driven Continuous Scanning Proton Therapy

    doi: 10.1016/j.ijpt.2026.101315

    Figure Lengend Snippet: Signal amplitude from the CROSSmini detector with signal fitting. shows the signal amplitude as a function of time measured by the CROSSmini detector and the piecewise fittings. Figures A, B, and C are measurements for energy level 70.2 MeV with nominal beam current 8, 14, and 20 MU/s, respectively. Figures D, E, and F are the measurements for energy level 228.7 MeV with nominal beam current 8, 14, and 20 MU/s, respectively.

    Article Snippet: The beam current was measured using a CROSSmini 2D strip ionization chamber detector array (Liverage Biomedical Inc, Taiwan) positioned at the isocenter plane.

    Techniques:

    t rise comparison between analytical and measured. The blue and red plots represent the analytically derived t rise and CROSSmini measured t rise , respectively, across the various nominal beam current settings.

    Journal: International Journal of Particle Therapy

    Article Title: Phenomenological Study of Intra-Spill Break Spots in Dose-Driven Continuous Scanning Proton Therapy

    doi: 10.1016/j.ijpt.2026.101315

    Figure Lengend Snippet: t rise comparison between analytical and measured. The blue and red plots represent the analytically derived t rise and CROSSmini measured t rise , respectively, across the various nominal beam current settings.

    Article Snippet: The beam current was measured using a CROSSmini 2D strip ionization chamber detector array (Liverage Biomedical Inc, Taiwan) positioned at the isocenter plane.

    Techniques: Comparison, Derivative Assay

    (a) Measurement device combined with a 2D ionization chamber array and an accordion-type water phantom. (b) Typical results for PSQA. The upper and lower panels show the PC and HNC cases, respectively. The arrows on the dose distribution indicate the dose profile’s direction. (c) The gamma passing rate in the clinical cases.

    Journal: PLoS ONE

    Article Title: Commissioning a newly developed treatment planning system, VQA Plan, for fast-raster scanning of carbon-ion beams

    doi: 10.1371/journal.pone.0268087

    Figure Lengend Snippet: (a) Measurement device combined with a 2D ionization chamber array and an accordion-type water phantom. (b) Typical results for PSQA. The upper and lower panels show the PC and HNC cases, respectively. The arrows on the dose distribution indicate the dose profile’s direction. (c) The gamma passing rate in the clinical cases.

    Article Snippet: We performed the measurements using the PinPoint chamber and a commercial 2D ionization chamber array (OCTAVIUS Detector 1500 XDR, PTW-Freiburg GmbH, Freiburg, Germany) mounted on an accordion-type water phantom that enables the water-equivalent thickness to be changed easily [ ].

    Techniques: