会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 1. 发明公开
    • RIDGE FILTER AND METHOD FOR DESIGNING SAME IN A PBS TREATMENT SYSTEM
    • EP4183447A1
    • 2023-05-24
    • EP21208699.5
    • 2021-11-17
    • Ion Beam Applications
    • LABARBE, RudiHOTOIU, LucianPIN, Arnaud
    • A61N5/10G21K1/04
    • The present invention concerns a method for designing a ridge filter for a charged particle accelerator, for depositing with beams of accelerated particles (100.i) specific doses (Dij) into specific locations within a treatment volume (V) of tissue comprising tumoral cells (3t) by single layer pencil beam scanning (PBS), according to a predefined treatment plan (TP), the method comprising the following steps,
      • Defining an array of spots (Si) defining the bases of cylindrical subvolumes (Vi) defining the treatment volume (V); the subvolumes (Vi) are divided into N cells (Cij).
      • The ridge filter is designed comprising the same number of energy degrading units (11.i) as there are spots (Si). Each energy degrading unit (11.i) is formed by N cylindrical degrading subunits (11.ij) of lengths (Lij) and area (Aij).
      • The lengths (Lij) of each degrading subunit (11.ij) are calculated as Lij = Wij / Wu, and Wij = W0 ― dij, wherein
      ∘ Wij is the desired subunit water equivalent thickness (Wij),
      ∘ Wu is the subunit water equivalent thickness per unit length (Wu),
      ∘ W0 is the maximum beam range and
      ∘ dij is the desired position of the Bragg peak along the irradiation axis (X)..

      • The area (Aij) of each degrading subunit (11.ij) is obtained by determining the area boundary (Aij) of the integral at the numerator satisfying the following Equation (1). ω ij ∑ j ω ij = ∬ Aij F y z . dy . dz ∬ Abi F y z . dy . dz , wherein
      ∘ ω ij / ∑ j ω ij is the normalized beam weight,
      ∘ F(y,z) is the fluence of the beam,
      ∘ Abi is the base area (Abi) of the degrading unit (11.i).
    • 3. 发明公开
    • CHARGED PARTICLE TREATMENT PLANNING SYSTEM WITH PBS BEAMLETS SEQUENCE OPTIMIZED FOR HIGH DOSE DEPOSITION RATE
    • EP3932482A1
    • 2022-01-05
    • EP20194440.2
    • 2020-09-03
    • Ion Beam Applications S.A.
    • LABARBE, RudiHOTOIU, LucianPIN, Arnaud
    • A61N5/10
    • The present invention concerns a treatment planning system (TPS) for generating a plan for treatment by radiation with charged particles beams, preferably with proton beams, applied by pencil beam scanning (PBS) onto a target tissue (3t) comprising tumoral cells enclosed within a peripheral surface, wherein the TPS comprises,
      • a dose definition stage defining the doses to be deposited within the peripheral surface
      • a beam definition stage defining positions and dimensions of the beamlets of the PBS during the at least one high rate fraction, the beams definition stage comprising
      • a dose rate definition stage comprising at least one high rate fraction j, wherein specific volumes (Vs) comprising healthy cells are irradiated at a ultra-high dose deposition rate (HDR), wherein HDR = Dj / t ≥ 1 Gy / s, j, and
      • a beamlets scanning sequence stage defining a scanning sequence of irradiation of the beamlets.
      The beamlets scanning sequence stage aims at optimizing a time sequence of beamlets emission such that at the end of a fraction j, a dose is deposited onto at least a predefined fraction of each specific volume at a mean deposition rate (DRa) superior or equal to a predefined value (DRa0) of a mean ultra-high dose deposition rate boundary (DRa ≥ DRa0), wherein DRa is defined as, DRa = ∑Dj/Δt ≥ DRa0 ≥ 1 Gy / s, wherein ∑Dj is a sum of a percentile of at least 95%, preferably at least 98% of all the doses deposited by one or more beamlets onto a given volume and Δt is the time between the first and last doses deposited onto the given volume.
    • 4. 发明公开
    • VARIO-ENERGY ELECTRON ACCELERATOR
    • EP3661335A1
    • 2020-06-03
    • EP18208924.3
    • 2018-11-28
    • Ion Beam Applications
    • ABS, MichelBRISON, JeremyKLEEVEN, Willem
    • H05H13/10
    • The present invention concerns an electron accelerator comprising:
      (a) a resonant cavity (1) consisting of a hollow closed conductor symmetrical with respect to a mid-plane, Pm, normal to a central axis, Zc,
      (b) an electron source (20) adapted for radially injecting a beam of electrons (40) into the resonant cavity,
      (c) an RF system coupled to the resonant cavity and adapted for generating an electric field, E, in the resonant cavity,
      (d) N magnet units (30i), each one being centred on the mid-plane, Pm, and adapted for generating a magnetic field in a deflecting chamber (31) in fluid communication with the resonant cavity by a cavity outlet aperture and an cavity inlet aperture (31w), the magnetic field being adapted for, deflecting along a first deflecting trajectory of adding length, L+, an electron beam exiting the resonant cavity along a first radial trajectory to reintroduce it into the resonant cavity along a second radial trajectory different from the first radial trajectory,
      (e) an outlet (50) for extracting along an extraction path an accelerated electron beam of energy, W, from the resonant cavity towards a target (100),
      characterized in that, at least one of the N magnet units (30i) is adapted for modifying the corresponding first deflecting trajectory to a second deflecting trajectory of second length (L2) different from and preferably larger than the adding length (L+), thus allowing a variation of the energy, W, of the accelerated electron beam extracted from the outlet (50).
    • 9. 发明公开
    • METHOD AND SYSTEM FOR CONTROLLING ION BEAM PULSES EXTRACTION
    • 控制离子束脉冲提取的方法和系统
    • EP3307031A1
    • 2018-04-11
    • EP16192454.3
    • 2016-10-05
    • Ion Beam Applications S.A.
    • KRIER, GabrielHENROTIN, SébastienCLAEREBOUDT, Yves
    • H05H7/00H05H13/02
    • H05H13/02A61N5/1043A61N2005/1087H05H7/001H05H7/02H05H7/04H05H2007/008H05H2007/022H05H2007/025H05H2007/046H05H2277/10
    • A first aspect of present invention is related to a method for controlling the extraction of ion beam pulses produced by a synchrocyclotron according to an irradiation plan. The synchrocyclotron comprises electrodes configured to be placed in a magnetic field, wherein an alternating voltage is applied between the electrodes, and wherein the frequency of the alternating voltage is modulated in a cyclic manner. The method comprises the steps of starting an acceleration cycle of the synchrocyclotron (12), generating a reference signal (38) when the modulated frequency reaches a predefined value (42), communicating the time, at which the reference signal (38) is generated, to the one or more beam control elements (20, 22), assessing one or more status parameters of the one or more beam control elements (20, 22), wherein the assessment is synchronised with the generation of the reference signal (38), cancelling or proceeding with the extraction of the beam pulse depending on the results of the assessment. A second aspect of the present invention is related to an ion beam extraction system configured to perform the method according to the first aspect of the present invention.
    • 本发明的第一方面涉及一种用于根据照射计划来控制由同步回旋加速器产生的离子束脉冲的提取的方法。 同步回旋加速器包括被配置为放置在磁场中的电极,其中交流电压被施加在电极之间,并且其中交流电压的频率以循环的方式被调制。 该方法包括步骤:启动同步回旋加速器(12)的加速周期,当调制频率达到预定值(42)时产生参考信号(38),传送参考信号(38)产生的时间 向所述一个或多个射束控制元件(20,22)发送所述一个或多个射束控制元件(20,22)的一个或多个状态参数,其中所述评估与所述参考信号(38)的生成同步, ,根据评估结果取消或继续提取光束脉冲。 本发明的第二方面涉及配置成执行根据本发明的第一方面的方法的离子束提取系统。