Abstract: 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.

Abstract: A computer implemented method for optimizing tolerance values of operating parameters of a particle accelerating system allowing a plurality of beamlets of particles accelerated along an irradiation axis, to deposit doses by pencil beam scanning into a structure of interest of a patient according to a treatment plan. The method calculates the dose (rate) volume histograms for a statistically representative number N of values randomly selected within a defined confidence level in preselected tentative statistical distributions of the operating parameters and compares the obtained calculated dose (rate) volume histogram with an acceptable band of variation of a target dose (rate) volume histogram. Once a tentative statistical distribution yields N calculated dose (rate) volume histograms which all fall within the acceptable band of variation, it is set as the final statistical distribution, and the particle accelerating system can be programmed with the final statistical distribution.

Abstract: A particle therapy system that is adapted to irradiate a target volume (1) with charged particles in compliance with a desired 3-D dose distribution. Such a desired 3-D dose distribution is achieved while delivering a plurality of particle energy distributions at the output of an energy-shaping device (10) crossed by an incident mono-energetic charged particle beam (6). The energy-shaping device comprises a plurality of groups (12, 22) of energy-shaping elements (11, 21), each of them comprising an individual layer of fluid or solid material (13), which thickness is adapted individually by a control unit (14). The use of configurable layers of fluids or solid materials makes the energy-shaping device reusable for treating different patients.

Abstract: A treatment device includes a pulsed particles accelerator and a processor for controlling the latter to deliver a treatment plan by deposition at HDR of charged particles into a flash volume (Vht) by PBS. To shorten the time for depositing a target dose (Dti) into the cells spanned by the flash spots (Si) of the flash volume (Vht), the flash spots are combined into k sets of n flash spots (Si). After depositing a jth pulse dose (Dij) into the cells spanned by a ith flash spot (Si) the beam commutes from the ith flash spot (Si) to a next (i+1)th flash spot according to a flash scanning subsequence to deposit a jth dose into the cells spanned by each of the subsequent flash spots of the flash scanning subsequence, until returning to the ith flash spot to deposit a (j+1)th dose (Di(j+1)), and so on When all the cells spanned by all the flash spots of a set have received their corresponding target dose, the beam moves to a next set of combined flash spots and repeats the foregoing pulse deposition steps.

Abstract: A treatment planning system for generating a plan for treatment by radiation with charged particles beams applied by pencil beam scanning onto a target tissue comprising tumoral cells is provided. The treatment planning system performs 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 including a dose rate definition stage comprising at least one high rate fraction, and a beamlets scanning sequence stage defining a scanning sequence of irradiation of the beamlets. The beamlets scanning sequence stage optimizes 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 superior or equal to a predefined value.

Abstract: A treatment planning system for generating a plan for treatment with charged particles beams, of a target tissue including tumoral cells enclosed within a peripheral surface, which is surrounded by healthy cells the plan including N fractions of irradiation including irradiation of volumes including tumoral cells and healthy cells at a conventional dose deposition rate, irradiation of volumes including tumoral cells and healthy cells at an ultra-high dose deposition rate, wherein an equivalent healthy fraction dose does not exceed a maximum equivalent healthy fraction dose for preserving the healthy cells after each fraction, and a total equivalent healthy dose delivered to and cumulated in a volume of a healthy tissue at the end of N fractions does not exceed a maximum equivalent healthy dose for preserving the healthy cells at the end of the N fractions.

Abstract: A treatment planning system for generating a plan for treatment by radiation with charged particles beams applied by pencil beam scanning onto a target tissue comprising tumoral cells is provided. The treatment planning system performs 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 including a dose rate definition stage comprising at least one high rate fraction, and a beamlets scanning sequence stage defining a scanning sequence of irradiation of the beamlets. The beamlets scanning sequence stage optimizes 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 superior or equal to a predefined value.