WO2021237869A1 - Parameter monitoring device and system for proton therapy - Google Patents

Parameter monitoring device and system for proton therapy Download PDF

Info

Publication number
WO2021237869A1
WO2021237869A1 PCT/CN2020/099492 CN2020099492W WO2021237869A1 WO 2021237869 A1 WO2021237869 A1 WO 2021237869A1 CN 2020099492 W CN2020099492 W CN 2020099492W WO 2021237869 A1 WO2021237869 A1 WO 2021237869A1
Authority
WO
WIPO (PCT)
Prior art keywords
proton
neural network
proton beam
recurrent neural
distribution
Prior art date
Application number
PCT/CN2020/099492
Other languages
French (fr)
Chinese (zh)
Inventor
彭浩
胡宗晟
张小可
Original Assignee
杭州珞珈质子科技有限公司
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by 杭州珞珈质子科技有限公司 filed Critical 杭州珞珈质子科技有限公司
Publication of WO2021237869A1 publication Critical patent/WO2021237869A1/en

Links

Images

Classifications

    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61NELECTROTHERAPY; MAGNETOTHERAPY; RADIATION THERAPY; ULTRASOUND THERAPY
    • A61N5/00Radiation therapy
    • A61N5/10X-ray therapy; Gamma-ray therapy; Particle-irradiation therapy
    • A61N5/1048Monitoring, verifying, controlling systems and methods
    • A61N5/1071Monitoring, verifying, controlling systems and methods for verifying the dose delivered by the treatment plan
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06NCOMPUTING ARRANGEMENTS BASED ON SPECIFIC COMPUTATIONAL MODELS
    • G06N3/00Computing arrangements based on biological models
    • G06N3/02Neural networks
    • G06N3/04Architecture, e.g. interconnection topology
    • G06N3/045Combinations of networks
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06NCOMPUTING ARRANGEMENTS BASED ON SPECIFIC COMPUTATIONAL MODELS
    • G06N3/00Computing arrangements based on biological models
    • G06N3/02Neural networks
    • G06N3/08Learning methods
    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61NELECTROTHERAPY; MAGNETOTHERAPY; RADIATION THERAPY; ULTRASOUND THERAPY
    • A61N5/00Radiation therapy
    • A61N5/10X-ray therapy; Gamma-ray therapy; Particle-irradiation therapy
    • A61N2005/1085X-ray therapy; Gamma-ray therapy; Particle-irradiation therapy characterised by the type of particles applied to the patient
    • A61N2005/1087Ions; Protons

Definitions

  • the invention relates to the field of nuclear medicine imaging, in particular to a parameter monitoring device and system for proton therapy.
  • the current methods of treating tumors mainly include surgery, chemotherapy and radiotherapy, and more than 70% of tumor patients need to receive radiotherapy alone or combined with radiotherapy.
  • the ideal radiation therapy is to give a lethal dose to tumor cells while minimizing the radiation dose to the surrounding normal organs and tissues.
  • Proton therapy is such a cutting-edge radiotherapy technology for the precise treatment of cancer.
  • the radiation dose curve of the proton beam in tissues (such as humans, animals, etc.) first slowly rises, then gradually becomes faster, until the maximum dose deposition occurs at the Bragg peak, and then rapidly drops to zero.
  • the unique dose-depth characteristic of the proton beam enables the tumor tissue to receive the maximum radiation dose, and at the same time, it can avoid the normal organs behind the tumor tissue from being damaged by radiation and reduce the side effects of treatment.
  • the advantages of proton therapy are: 1) The dose at the end of the proton Bragg peak is three to four times higher than the dose at the entrance, and the dose after the Bragg peak is almost zero. This feature not only maximizes the dose at the tumor, but also Effectively protect the normal tissues before and after the tumor; 2) The energy of the proton beam can be adjusted to irradiate tumors of different depths, so that proton therapy can adapt to tumors of different depths and different sizes and shapes; 3) Proton transmission has better performance. The small scattering and background make the edge of the illumination field clear, so it can treat tumors close to sensitive organs.
  • the Bragg peak characteristic of the proton beam is the biggest advantage of proton therapy, but it is also because of the existence of the Bragg peak that the treatment effect is very sensitive to the range. Once the actual treatment range deviates from the treatment plan, it is easy to cause insufficient dose of tumor tissue or over-irradiation of normal tissue, which greatly increases the risk of tumor recurrence and complications of normal organs. Therefore, in the process of proton therapy, the monitoring of the dose of the proton beam in the tissue and the position of the Bragg peak is very important to the effect of proton therapy.
  • methods for monitoring the dose of proton therapy include prompt gamma measurement (for example, patent document CN 106291656A), acoustic wave monitoring and so on.
  • prompt gamma measurement for example, patent document CN 106291656A
  • acoustic wave monitoring and so on.
  • the prompt gamma method lacks a high-performance detector suitable for the gamma-ray energy spectrum region, and the detection efficiency of the detector is low; the sound signal in the acoustic wave method is very weak, and the signal-to-noise ratio is very low.
  • positron nuclides mainly carbon-11 and oxygen-15.
  • the PET system is used to image the activity of positron nuclides.
  • the present invention provides a parameter monitoring device and system for proton therapy, thereby realizing the monitoring and adjustment of the parameters of proton therapy.
  • a parameter monitoring device for proton therapy including:
  • a recurrent neural network module configured to provide a trained recurrent neural network model, the trained recurrent neural network model providing a non-linear relationship between the positron nuclide activity distribution of the proton beam and the dose distribution;
  • the PET acquisition module is configured to acquire a PET image of the activity distribution of positron nuclides produced by the reaction between protons and tissues from the positron annihilation tomography system;
  • a prediction module configured to input the PET image into the trained recurrent neural network model to predict the dose distribution and Bragg peak position of the proton beam;
  • the judgment module is configured to judge the positional relationship between the Bragg peak position and the target area according to the predicted dose distribution of the proton beam;
  • the adjustment module is configured to determine whether the beam output parameters of the proton beam need to be adjusted according to the judgment result of the judgment module.
  • the adjustment module is further configured to:
  • the judgment module judges that the predicted dose distribution of the proton beam and the Bragg peak position are within the target area, then the beam output parameters of the proton beam are not adjusted;
  • the judgment module judges that the predicted dose distribution of the proton beam and the Bragg peak position are outside the target area, readjust the beam output parameters of the proton beam.
  • the training samples of the recurrent neural network model during the training process at least include: stopping power, proton beam dose distribution, and positron nuclide activity distribution, wherein the stopping power passes the treatment
  • the CT value of the CT image of the subject is converted, and the dose distribution and the positron nuclide activity distribution are obtained through the tissue simulation constructed in the Monte Carlo system of the three-dimensional phantom of the subject.
  • the model is constructed based on the CT image of the subject.
  • the dose distribution and the positron nuclide activity distribution simulate different incident energies and/or different incident positions in a tissue constructed in a Monte Carlo system via a three-dimensional phantom of the subject to be treated The proton therapy process is obtained.
  • the stopping power is transformed according to the following steps:
  • the stopping power corresponding to each pixel is calculated according to the beam output parameter of the proton beam and the CT value of each pixel.
  • the training sample further includes the CT value of the path of the proton beam, in the training sample, the CT value of each pixel on the path of the proton beam, the CT value of the proton beam.
  • the stopping power and the distribution of positron nuclide activity corresponding to each pixel on the path are used as the input of the recurrent neural network model, and the dose distribution of the proton beam is used as the output of the recurrent neural network model to determine the Recursive neural network model for training.
  • the prediction result of the recurrent neural network model adopts the mean square error and/or the mean absolute error for quantitative evaluation.
  • the prediction result of the recurrent neural network model adopts the following steps to evaluate the generalization ability:
  • it further includes:
  • the CT acquisition module is configured to acquire the CT image of the treatment subject
  • the prediction module is further configured to input the CT image of the treatment subject acquired by the CT acquisition module and the stopping power obtained based on the conversion of the CT image of the treatment subject into the trained recurrent neural network model.
  • a parameter monitoring system for proton therapy including:
  • CT system configured to provide CT images of the subject
  • the Monte Carlo system is configured to construct a treatment object based on a three-dimensional phantom of the treatment object, and to obtain a dose distribution of a proton beam and a positron nuclide activity distribution by simulating, the three-dimensional phantom is constructed based on a CT image of the treatment object
  • a PET system configured to provide PET images of the activity distribution of positron nuclides produced by the reaction between protons and tissues
  • the parameter monitoring device for proton therapy as described above.
  • the invention adopts a trained recurrent neural network model, and predicts the corresponding dose distribution of PET image data collected in actual clinical practice by using the recurrent neural network model to realize the use of PET data to monitor the dose distribution and Bragg peak position in proton therapy.
  • the invention greatly improves the prediction accuracy of dose distribution and Bragg peak position through data collection, data processing and machine learning, and shortens the prediction time. Therefore, through the device and system provided by the present invention, it is ensured that the dose of proton beam irradiation to the tumor tissue during the proton therapy process is normal and the position is accurate, and the risk of tumor recurrence and normal organ complications is reduced, thereby ensuring the proton therapy for tumor patients The therapeutic effect.
  • Fig. 1 shows a block diagram of a parameter monitoring device for proton therapy according to an embodiment of the present invention.
  • Fig. 2 shows a schematic diagram of calculating stopping power according to an embodiment of the present invention.
  • Fig. 3 shows a schematic diagram of a recurrent neural network model according to an embodiment of the present invention.
  • Fig. 4 shows a block diagram of a parameter monitoring system for proton therapy according to an embodiment of the present invention.
  • Fig. 5 shows a schematic diagram of a recurrent neural network training process diagram according to an embodiment of the present invention.
  • Fig. 6 shows a schematic diagram of result prediction according to an embodiment of the present invention.
  • Fig. 7 shows a schematic diagram of a data acquisition system according to an embodiment of the present invention.
  • Fig. 8 shows a schematic diagram of a PET collection module according to an embodiment of the present invention.
  • Example embodiments will now be described more fully with reference to the accompanying drawings.
  • the example embodiments can be implemented in various forms, and should not be construed as being limited to the examples set forth herein; on the contrary, the provision of these embodiments makes the present invention more comprehensive and complete, and fully conveys the concept of the example embodiments To those skilled in the art.
  • the described features, structures or characteristics can be combined in one or more embodiments in any suitable way.
  • Fig. 1 shows a block diagram of a parameter monitoring device for proton therapy according to an embodiment of the present invention.
  • the parameter monitoring device 100 for proton therapy includes a recurrent neural network module 110, a PET acquisition module 120, a prediction module 130, a judgment module 140, and an adjustment module 150.
  • the recurrent neural network module 110 is configured to provide a trained recurrent neural network model that provides a non-linear relationship between the positron nuclide activity distribution of the proton beam and the dose distribution.
  • the recurrent neural network model may be a multi-input recurrent neural network model.
  • the training samples in the training process of the recurrent neural network model at least include stopping power (SP), the dose distribution of the proton beam, and the positron activity distribution.
  • the stopping power is obtained by transforming the CT value of the CT image of the subject.
  • the parameter monitoring device 100 for proton therapy may also include a CT acquisition module.
  • the CT acquisition module is configured to acquire a CT image of the treatment target (for example, a CT image of the patient's whole body) from a medical CT system.
  • CT images can be obtained from medical CT systems.
  • a three-dimensional phantom can be constructed based on the CT image of the subject to be treated, so as to determine the tumor focus area and the area of interest.
  • a medical CT system can be used to scan the whole body of the subject to obtain CT images, and the obtained multiple frames of CT images can be combined to construct a three-dimensional phantom, outline the location of the tumor lesion area, and appropriately expand the lesion area to obtain an interesting Region (Region of interest, ROI).
  • ROI interesting Region
  • the stopping power can be transformed according to the following steps: extract the CT value of each pixel on the path of the proton beam from the three-dimensional CT image composed of the CT image of the treatment subject; according to the beam parameters of the proton beam and the proton beam
  • the CT value on the passing path calculates the stopping power corresponding to each pixel on the path of the proton beam.
  • the stopping power can be calculated as follows:
  • the CT value of each pixel on the path of the proton beam is extracted from the three-dimensional CT image, combined with the incident energy of the proton beam, and the stopping power corresponding to each pixel on the path of the proton beam is calculated.
  • the formula is as follows:
  • the SP i is the i th pixel of the stopping power
  • constant k 51Mev fm 2
  • ⁇ i is the ratio of the speed of light and the particle velocity
  • m e is the electron mass
  • ⁇ e is the electron density per volume of the substance
  • I is the compound Average excitation energy
  • Is the shell correction item Is the polarization effect term
  • c is the speed of light
  • E is the energy remaining after the particle passes through the matter.
  • the electron density per volume ⁇ e of the substance and the average excitation energy I of the compound can be calculated according to the following formula:
  • N A is the Avogadro number
  • [rho] is the density of the material
  • i the Z is the atomic number of the element i
  • W i is the weight of element i weighting factor
  • the average excitation element i I i Yes where ⁇ , Z i and w i can be obtained by looking up the table of CT values.
  • the dose distribution and the positron nuclide activity distribution are obtained through a tissue simulation constructed in a Monte Carlo system with a three-dimensional phantom of the subject to be treated.
  • the tissues described in the embodiments of the present invention may include humans and/or animals.
  • the dose distribution and the positron nuclide activity distribution are obtained by simulating the proton treatment process of different incident energies and/or different incident positions in the tissue constructed in the Monte Carlo system through the three-dimensional phantom of the subject to be treated.
  • the parameters of the pencil beam source can be set in the Monte Carlo system, and the positron emission process can be simulated through the program to ensure sufficient beam flow and set the corresponding beam period.
  • the dose distribution information and the activity distribution information of positron emission are saved by the Monte Carlo tool.
  • the training sample further includes a CT value along the path of the proton beam.
  • the CT value of each pixel on the path of the proton beam, the stopping power corresponding to each pixel on the path of the proton beam, and the positron nuclide activity distribution are used as the recursive
  • the input of the neural network model, and the dose distribution is used as the output of the recurrent neural network model to train the recurrent neural network model to find the non-linear relationship between the positron nuclide activity distribution of the proton beam and the dose distribution .
  • the prediction result of the recurrent neural network model adopts mean square error (MSE) and/or mean absolute error (MAE) for quantitative evaluation.
  • MSE mean square error
  • MAE mean absolute error
  • the prediction result of the recurrent neural network model adopts the following steps to evaluate the generalization ability: the predicted dose distribution at different positions in the same picture is different from the evaluation and/or replacement of the Bragg peak position The estimated dose distribution and Bragg peak position were evaluated based on the PET activity image.
  • the PET acquisition module 120 is configured to acquire a PET image of the activity distribution of positron nuclides produced by the reaction between protons and tissues from the positron annihilation tomography system.
  • positron nuclides In clinical proton therapy, after entering the tissue, protons react with the tissue to produce positron nuclides.
  • the medical PET system is used to perform PET scanning on the target to obtain a PET reflecting the distribution of positron nuclides. Activity image.
  • the Monte Carlo system can also be used to simulate clinically treated subjects undergoing PET imaging after receiving proton therapy.
  • a corresponding hardware PET system can be set up through simulation software, positron nuclides are selected (carbon-11, oxygen-15), according to imaging needs, in order to obtain sufficient photon data statistics (projection information) , Select the corresponding Monte Carlo time to get enough counts.
  • the acquired projection is reconstructed, and the single-slice rebinning algorithm (Single-Slice Rebinning, SSRB) and the two-dimensional ordered subset maximum likelihood method (Ordered Subsets Expectation Maximization, OSEM) are used to image Iterative reconstruction to obtain the reconstructed PET activity image.
  • the attenuation correction of CT is completed, and the entire imaging field of the image is uniformized and corrected, and the corresponding PET image reflecting the activity distribution of positron nuclide is obtained.
  • the prediction module 130 is configured to input the PET image into the trained recurrent neural network model to predict the dose distribution and Bragg peak position of the proton beam.
  • the prediction module is further configured to input the CT image of the treatment subject acquired by the CT acquisition module and the stopping power obtained based on the conversion of the CT image of the treatment subject into the trained recurrent neural network model.
  • the determining module 140 is configured to determine the positional relationship between the Bragg peak position and the target area according to the predicted dose distribution of the proton beam.
  • the adjustment module 150 is configured to determine whether the beam output parameters of the proton beam need to be adjusted according to the judgment result of the judgment module 140.
  • the adjustment module 150 is further configured to:
  • the judgment module 140 judges that the predicted dose distribution of the proton beam and the Bragg peak position are within the target area, it judges that the proton beam radiotherapy is accurate, and continues to perform radiotherapy according to the existing proton beam emission parameters, and does not treat the proton beam.
  • the beam parameters of the beam are adjusted until the end of the treatment.
  • the present invention is not limited by this.
  • the judgment module 140 judges that the predicted dose distribution of the proton beam and the Bragg peak position are outside the target area, it judges that the proton beam radiotherapy is not accurate, and readjusts the beam parameters of the proton beam until the adjusted proton beam The dose distribution and Bragg peak position are consistent with the radiation treatment plan.
  • a trained recurrent neural network model is adopted, and the PET image data collected in the actual clinic is used to predict the corresponding dose distribution by using the recurrent neural network model to achieve The use of PET data in proton therapy to monitor dose distribution and Bragg peak position.
  • the invention greatly improves the prediction accuracy of dose distribution and Bragg peak position through data collection, data processing and machine learning, and shortens the prediction time.
  • the device and system provided by the present invention it is ensured that the dose of proton beam irradiation to the tumor tissue during the proton therapy process is normal and the position is accurate, and the risk of tumor recurrence and normal organ complications is reduced, thereby ensuring the proton therapy for tumor patients The therapeutic effect.
  • the monitoring method for dose and range verification in proton therapy based on the machine learning model of the present invention has a positive effect on the dose distribution, Broad applicability of Bragg peak position monitoring. It ensures that the dose of proton beam irradiation is normal and the position is accurate, and the risk of tumor recurrence and normal organ complications is reduced, thereby ensuring the therapeutic effect of proton therapy for tumor patients.
  • FIG. 1 only schematically shows the parameter monitoring device 100 for proton therapy provided by the present invention. Without violating the concept of the present invention, the splitting, merging, and adding of modules are all within the protection scope of the present invention.
  • the parameter monitoring device 100 for proton therapy provided by the present invention can be implemented by software, hardware, firmware, plug-ins and any combination between them, and the present invention is not limited to this.
  • Fig. 2 shows a schematic diagram of calculating stopping power according to an embodiment of the present invention.
  • the stopping power can be calculated according to the following method (see number 10 in Figure 2):
  • the stopping power corresponding to each pixel is calculated.
  • the stopping power calculation formula is as follows:
  • the SP i is the i-th pixel of the stopping power
  • constant k 51Mev fm 2
  • ⁇ i the speed of light
  • the ratio of particle velocity m e is the electron mass
  • ⁇ e the electron density per volume of the substance
  • I the compound Average excitation energy.
  • Is the shell correction item Is the polarization effect term
  • c the speed of light
  • E is the remaining kinetic energy of the particle after passing through the matter.
  • the electron density per volume of the substance ⁇ e is calculated as follows:
  • N A is the Avogadro number
  • [rho] is the density of the material
  • i the Z is the atomic number of the element i
  • W i is the weight of element i weighting factor.
  • the average excitation energy I of the compound is calculated as follows:
  • N A is the Avogadro number
  • [rho] is the density of the material
  • i the Z is the atomic number of the element i
  • W i is the weight of element i weighting factor
  • the average excitation element i I i can.
  • ⁇ , Z i , and w i are obtained through the CT value look-up table, where the look-up table is: the corresponding table of the CT value and the composition of different tissue elements.
  • Fig. 3 shows a schematic diagram of a recurrent neural network model according to an embodiment of the present invention.
  • Recurrent Neural Network is specialized in processing time series data. It converts a time series input into a time series output through a hidden layer state, and continuously trains and learns the mapping relationship between input and output through back propagation and gradient descent methods. .
  • the recurrent neural network model is composed of an input layer (x 0 ⁇ x n ), a hidden layer (h 0 ⁇ h n ), and an output layer (D 0 ⁇ D n ).
  • the input layer of the network is a multi-data input, consisting of the CT image of the treatment subject, the stopping power obtained based on the conversion of the CT image of the treatment subject, and the activity value obtained from the PET image, and then the CT value, Three arrays of SP value and positron nuclide distribution activity value are juxtaposed.
  • the output of the recurrent neural network model is the dose distribution, and the maximum position of the dose distribution is the Bragg peak. Further, the input data in the recurrent neural network model has a cascading relationship.
  • a network model is constructed through this embodiment to predict the proton beam dose distribution and Bragg peak position. After testing, the model has good prediction accuracy, anti-noise performance and generalization ability, and performs well in prediction based on PET images.
  • Fig. 4 shows a block diagram of a parameter monitoring system for proton therapy according to an embodiment of the present invention.
  • the parameter monitoring system for proton therapy includes a CT system 210, a Monte Carlo system 220, a PET system 230, and the parameter monitoring device 100 for proton therapy as shown in FIG. 1.
  • the CT system 210 is configured to provide CT images of the treatment subject. Furthermore, a three-dimensional phantom can be constructed to delineate the area of interest for the final proton therapy monitoring terminal.
  • the Monte Carlo system 220 is configured to construct the treatment object based on the three-dimensional phantom of the treatment object, and to obtain the dose distribution of the proton beam and the activity distribution of the positron nuclide by simulating to generate the training set required by the model.
  • the three-dimensional phantom is based on the The construction of CT images of the subject to be treated.
  • the PET system 230 is configured to provide a PET image of the activity distribution of positron nuclides produced by the reaction between protons and tissues.
  • the modules included in the parameter monitoring device 100 have been described above, and will not be repeated here.
  • the parameter monitoring device 100 can also perform a quantitative and qualitative evaluation of the predicted result, and follow up the adjustment of the proton beam.
  • Fig. 4 only schematically shows the parameter monitoring system of proton therapy provided by the present invention. Without violating the concept of the present invention, the splitting, merging, and adding of modules are all within the protection scope of the present invention.
  • the parameter monitoring system for proton therapy provided by the present invention can be implemented by software, hardware, firmware, plug-ins and any combination between them, and the present invention is not limited to this.
  • FIG. 5 shows a schematic diagram of a recurrent neural network training process diagram according to a specific embodiment of the present invention.
  • Figure 5 shows a data collection system, a data preprocessing system, a recurrent neural network RNN model system, and a model evaluation system.
  • the data collection system includes a data collection system, which mainly collects patient clinical data, including anatomical clinical information collected by the CT system, and clinical information collected by the PET system; the data collection system also includes a data simulation system, which is mainly based on CT images, Generate dose distribution diagram and activity distribution diagram in the Monte Carlo system. All the data obtained by the data collection system will be used for subsequent neural network model training and dose verification.
  • the data preprocessing module is used to convert CT data into stopping power, and to standardize the acquired data for better network training.
  • the shown recursive neural network model selects preprocessed data according to a predetermined batch and inputs it into the neural network model for training, uses the validation set data to evaluate the model, quantitatively analyzes the performance parameters of the model, and quantitatively evaluates the model error. Evaluate whether the plan goal is met, continuously adjust the model parameters until the goal plan is met, and save the model.
  • FIG. 6 shows a schematic diagram of result prediction according to an embodiment of the present invention.
  • Figure 6 shows the patient data module, which includes a data acquisition module and a data calculation module.
  • the data acquisition module mainly includes CT data acquisition and PET data acquisition.
  • the data calculation is mainly based on the collected CT data and calculates it as the corresponding stopping power (SP), then input the CT data collected by the CT system, the activity data collected by the PET and the calculated stopping power into the trained RNN model, and output the prediction results.
  • SP stopping power
  • FIG. 7 shows a schematic diagram of a data acquisition system according to an embodiment of the present invention.
  • FIG. 7 describes the data collection process and the method of obtaining data in a specific embodiment of the present invention.
  • Figure 7 shows an accelerator system that generates a proton beam and a commonly used clinical data acquisition system.
  • the accelerator system is mainly used to generate proton beams for proton therapy, and then the proton beams are shot into human tissues for tumor treatment.
  • the hardware data acquisition system in the acquisition system mainly includes a CT system and a PET system.
  • the CT system uses X-rays to image the structure of the tissue.
  • the X-rays of the CT system are generated in a high-vacuum X-ray tube.
  • the nuclear electric field acts to form radiation, which produces a continuous beam of X-rays.
  • X-ray scans human tissues, and forms X-ray projection data after tissue attenuation on the X-ray detector, and reconstructs the data to form CT image data.
  • the proton beam enters the human body, it will react with the nucleus in the human body to produce a positron decay nuclide.
  • the released positron annihilates two 511 keV photons in opposite directions. These annihilation photons are detected by the PET detector and then pass through another one.
  • a series of image reconstruction algorithms form a PET human body activity image.
  • FIG. 8 shows a schematic diagram of a PET collection module according to an embodiment of the present invention. It is known that the proton beam passing through the human body will react with the nucleus in the human body to produce positron decay nuclide, and the released positron annihilation produces two opposite 511keV photons, which are detected by the detector through positron annihilation imaging technology. (PET) Construct human activity images. It is necessary to image the positron-induced radionuclide activity signal so that the proton beam dose distribution can be found through the activity distribution. Therefore, it is necessary to build a PET system to collect data and complete the activity imaging.
  • PET positron annihilation imaging technology
  • FIG. 8 shows an In-Beam PET system built in a Monte Carlo system according to an embodiment of the present invention, which includes two detector array units 2. After the proton beam 1 enters the patient's body 3, it will excite photons to hit the detector. Through coincidence detection, the activity distribution map is reconstructed to form an activity distribution data set, which is used for data input of the neural network.
  • the invention adopts a trained recurrent neural network model, and predicts the corresponding dose distribution of PET image data collected in actual clinical practice by using the recurrent neural network model to realize the use of PET data to monitor the dose distribution and Bragg peak position in proton therapy.
  • the invention greatly improves the prediction accuracy of dose distribution and Bragg peak position through data collection, data processing and machine learning, and shortens the prediction time. Therefore, through the device and system provided by the present invention, it is ensured that the dose of proton beam irradiation to the tumor tissue during the proton therapy process is normal and the position is accurate, and the risk of tumor recurrence and normal organ complications is reduced, thereby ensuring the proton therapy for tumor patients The therapeutic effect.

Landscapes

  • Engineering & Computer Science (AREA)
  • Health & Medical Sciences (AREA)
  • Theoretical Computer Science (AREA)
  • Biomedical Technology (AREA)
  • Physics & Mathematics (AREA)
  • General Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Computing Systems (AREA)
  • Software Systems (AREA)
  • Evolutionary Computation (AREA)
  • Computational Linguistics (AREA)
  • Molecular Biology (AREA)
  • Biophysics (AREA)
  • General Engineering & Computer Science (AREA)
  • General Physics & Mathematics (AREA)
  • Mathematical Physics (AREA)
  • Data Mining & Analysis (AREA)
  • Artificial Intelligence (AREA)
  • Pathology (AREA)
  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
  • Radiology & Medical Imaging (AREA)
  • Animal Behavior & Ethology (AREA)
  • Public Health (AREA)
  • Veterinary Medicine (AREA)
  • Nuclear Medicine (AREA)
  • Radiation-Therapy Devices (AREA)

Abstract

The present invention provides a parameter monitoring device and system for proton therapy. The device comprises: a recurrent neural network module, providing a trained recurrent neural network model, wherein the trained recurrent neural network model provides a nonlinear relationship between positron nuclide activity distribution and dose distribution of a proton beam; a PET obtaining module, obtaining, from a positron annihilation tomography system, a PET image of activity distribution of positron nuclides produced by a reaction between protons and tissues; a prediction module, inputting the PET image into the trained recurrent neural network model, and predicting the dose distribution and a Bragg peak position of the proton beam by means of the nonlinear relationship between the positron nuclide activity distribution and the dose distribution; a determination module, determining a positional relationship between the predicted dose distribution and Bragg peak position of the proton beam, and a target region; and an adjustment module, determining, according to a determination result of the determination module, whether a beam outlet parameter of the proton beam needs to be adjusted. The device and system provided in the present invention achieve the parameter monitoring and adjustment of proton therapy.

Description

质子治疗的参数监测装置及系统Parameter monitoring device and system for proton therapy 技术领域Technical field
本发明涉及核医学影像领域,特别涉及一种质子治疗的参数监测装置及系统。The invention relates to the field of nuclear medicine imaging, in particular to a parameter monitoring device and system for proton therapy.
背景技术Background technique
目前治疗肿瘤(癌症)的手段主要包括手术、化学治疗和放射治疗,并且超过70%的肿瘤患者需要接受单独放疗或者与放疗结合的综合治疗。理想的放射治疗是给予肿瘤细胞致死剂量,同时最大限度地减小周围正常器官组织的照射剂量,质子治疗便是这样一种精确治疗癌症的尖端放疗技术。质子束在组织(如人体、动物等)内的照射剂量曲线先缓慢上升,随后逐渐变快,直到布拉格峰处产生最大的剂量沉积,之后快速下降并趋于零。质子束的独特的剂量-深度特性能使肿瘤组织接收到最大的照射剂量,同时能避免肿瘤组织后方的正常器官受到辐射伤害,降低治疗的副作用。The current methods of treating tumors (cancer) mainly include surgery, chemotherapy and radiotherapy, and more than 70% of tumor patients need to receive radiotherapy alone or combined with radiotherapy. The ideal radiation therapy is to give a lethal dose to tumor cells while minimizing the radiation dose to the surrounding normal organs and tissues. Proton therapy is such a cutting-edge radiotherapy technology for the precise treatment of cancer. The radiation dose curve of the proton beam in tissues (such as humans, animals, etc.) first slowly rises, then gradually becomes faster, until the maximum dose deposition occurs at the Bragg peak, and then rapidly drops to zero. The unique dose-depth characteristic of the proton beam enables the tumor tissue to receive the maximum radiation dose, and at the same time, it can avoid the normal organs behind the tumor tissue from being damaged by radiation and reduce the side effects of treatment.
质子治疗的优势在于:1)质子布拉格峰终点处的剂量比入口处的剂量高出三到四倍,在布拉格峰之后的剂量几乎为0,这种特点不仅能使肿瘤处剂量最大,还能有效保护肿瘤前后的正常组织;2)可以通过调整质子束的能量来照射不同深度的肿瘤,从而使质子治疗适应不同的深度位置处,不同大小和形状的肿瘤;3)质子传输时,具有较小的散射和本底,使得照射视野边缘清晰,因此可以治疗距离敏感器官近的肿瘤。The advantages of proton therapy are: 1) The dose at the end of the proton Bragg peak is three to four times higher than the dose at the entrance, and the dose after the Bragg peak is almost zero. This feature not only maximizes the dose at the tumor, but also Effectively protect the normal tissues before and after the tumor; 2) The energy of the proton beam can be adjusted to irradiate tumors of different depths, so that proton therapy can adapt to tumors of different depths and different sizes and shapes; 3) Proton transmission has better performance. The small scattering and background make the edge of the illumination field clear, so it can treat tumors close to sensitive organs.
质子束的布拉格峰特性是质子治疗的最大优势,但也正是由于布拉格峰的存在,使得治疗效果对射程十分敏感。一旦实际治疗过程中射程与治疗计划出现偏差,就很容易导致肿瘤组织的剂量不足或者正常组织过度照射,从而很大程度上增加了肿瘤复发和正常器官的并发症风险。所以,在质子治疗过程中,对质子束在组织中剂量和布拉格峰位置的监测,对质子治疗效果至关重要。The Bragg peak characteristic of the proton beam is the biggest advantage of proton therapy, but it is also because of the existence of the Bragg peak that the treatment effect is very sensitive to the range. Once the actual treatment range deviates from the treatment plan, it is easy to cause insufficient dose of tumor tissue or over-irradiation of normal tissue, which greatly increases the risk of tumor recurrence and complications of normal organs. Therefore, in the process of proton therapy, the monitoring of the dose of the proton beam in the tissue and the position of the Bragg peak is very important to the effect of proton therapy.
目前,对质子治疗剂量监测的方法有瞬发伽马测量法(例如专利文献CN 106291656A),声波监测法等。但这些方法都有其不足。例如,瞬发伽玛法缺少适用于该伽马射线能谱区域的高性能探测器,探测器探测效率低下;声波法中声音信号非常微弱,且信噪比很低。At present, methods for monitoring the dose of proton therapy include prompt gamma measurement (for example, patent document CN 106291656A), acoustic wave monitoring and so on. But these methods have their shortcomings. For example, the prompt gamma method lacks a high-performance detector suitable for the gamma-ray energy spectrum region, and the detection efficiency of the detector is low; the sound signal in the acoustic wave method is very weak, and the signal-to-noise ratio is very low.
在质子治疗中,质子会与组织发生核反应,产生正电子核素(主要是碳-11、氧-15),用PET系统对正电子核素进行活度成像。In proton therapy, protons will react with tissues to produce positron nuclides (mainly carbon-11 and oxygen-15). The PET system is used to image the activity of positron nuclides.
由此,如何通过计算机设备,采集核医学影像的数据,并通过对所采集的核医学影像的数据的处理,实现质子治疗的参数监测和调整。Therefore, how to collect nuclear medicine image data through computer equipment, and process the collected nuclear medicine image data to realize the parameter monitoring and adjustment of proton therapy.
发明内容Summary of the invention
本发明为了克服上述相关技术存在的缺陷,提供一种质子治疗的参数监测装置及系统,进而实现质子治疗的参数监测和调整。In order to overcome the defects of the above-mentioned related technologies, the present invention provides a parameter monitoring device and system for proton therapy, thereby realizing the monitoring and adjustment of the parameters of proton therapy.
根据本发明的一个方面,提供一种质子治疗的参数监测装置,包括:According to one aspect of the present invention, there is provided a parameter monitoring device for proton therapy, including:
递归神经网络模块,配置成提供经训练的递归神经网络模型,所述经训练的递归神经网络模型提供质子束的正电子核素活度分布与剂量分布的非线性关系;A recurrent neural network module, configured to provide a trained recurrent neural network model, the trained recurrent neural network model providing a non-linear relationship between the positron nuclide activity distribution of the proton beam and the dose distribution;
PET获取模块,配置成从正电子湮没断层扫描系统中获取质子与组织发生反应产生的正电子核素活度分布的PET图像;The PET acquisition module is configured to acquire a PET image of the activity distribution of positron nuclides produced by the reaction between protons and tissues from the positron annihilation tomography system;
预测模块,配置成将所述PET图像输入所述经训练的递归神经网络模型,预测质子束的剂量分布与布拉格峰位置;A prediction module, configured to input the PET image into the trained recurrent neural network model to predict the dose distribution and Bragg peak position of the proton beam;
判断模块,配置成根据所预测的质子束的剂量分布判断布拉格峰位置与目标区域的位置关系;The judgment module is configured to judge the positional relationship between the Bragg peak position and the target area according to the predicted dose distribution of the proton beam;
调整模块,配置成依据所述判断模块的判断结果确定质子束的出束参数是否需要调整。The adjustment module is configured to determine whether the beam output parameters of the proton beam need to be adjusted according to the judgment result of the judgment module.
在本发明的一些实施例中,所述调整模块还配置成:In some embodiments of the present invention, the adjustment module is further configured to:
若所述判断模块判断所预测的质子束的剂量分布与布拉格峰位置位于目标区域内,则不对所述质子束的出束参数进行调整;If the judgment module judges that the predicted dose distribution of the proton beam and the Bragg peak position are within the target area, then the beam output parameters of the proton beam are not adjusted;
若所述判断模块判断所预测的质子束的剂量分布与布拉格峰位置位于目标区域外,则重新调整所述质子束的出束参数。If the judgment module judges that the predicted dose distribution of the proton beam and the Bragg peak position are outside the target area, readjust the beam output parameters of the proton beam.
在本发明的一些实施例中,所述递归神经网络模型的在训练过程中的训练样本至少包括:阻止本领、质子束的剂量分布和正电子核素活度分布,其中,所述阻止本领通过治疗对象的CT图像的CT值转化获得,所述剂量分布和所述正电子核素活度分布经由治疗对象的三维体模在蒙特卡洛系统中构建的组织模拟获得,所述治疗对象的三维体模根据所述治疗对象的CT图像构建。In some embodiments of the present invention, the training samples of the recurrent neural network model during the training process at least include: stopping power, proton beam dose distribution, and positron nuclide activity distribution, wherein the stopping power passes the treatment The CT value of the CT image of the subject is converted, and the dose distribution and the positron nuclide activity distribution are obtained through the tissue simulation constructed in the Monte Carlo system of the three-dimensional phantom of the subject. The model is constructed based on the CT image of the subject.
在本发明的一些实施例中,所述剂量分布和所述正电子核素活度分布经由治疗对象的三维体模在蒙特卡洛系统中构建的组织中模拟不同入射能量和/或不同入射位置的质子治疗过程获得。In some embodiments of the present invention, the dose distribution and the positron nuclide activity distribution simulate different incident energies and/or different incident positions in a tissue constructed in a Monte Carlo system via a three-dimensional phantom of the subject to be treated The proton therapy process is obtained.
在本发明的一些实施例中,所述阻止本领根据如下步骤转化:In some embodiments of the present invention, the stopping power is transformed according to the following steps:
根据所述治疗对象的CT图像构成的三维CT图像中提取质子束经过路径上每个像素点的CT值;Extracting the CT value of each pixel on the path of the proton beam from the three-dimensional CT image formed by the CT image of the treatment subject;
根据所述质子束的出束参数以及所述每个像素点的CT值计算所述每个像素点对应的阻止本领。The stopping power corresponding to each pixel is calculated according to the beam output parameter of the proton beam and the CT value of each pixel.
在本发明的一些实施例中,所述训练样本还包括质子束经过路径上的CT值,在所述训练样本中,所述质子束经过路径上每个像素点的CT值、所述质子束经过路径上每个像素点对应的阻止本领、正电子核素活度分布被作为所述递归神经网络模型的输入,所述质子束的剂量分布被作为递归神经网络模型的输出,以对所述递归神经网络模型进行训练。In some embodiments of the present invention, the training sample further includes the CT value of the path of the proton beam, in the training sample, the CT value of each pixel on the path of the proton beam, the CT value of the proton beam The stopping power and the distribution of positron nuclide activity corresponding to each pixel on the path are used as the input of the recurrent neural network model, and the dose distribution of the proton beam is used as the output of the recurrent neural network model to determine the Recursive neural network model for training.
在本发明的一些实施例中,所述递归神经网络模型的预测结果采用均方误差和/或平均绝对误差进行定量评价。In some embodiments of the present invention, the prediction result of the recurrent neural network model adopts the mean square error and/or the mean absolute error for quantitative evaluation.
在本发明的一些实施例中,所述递归神经网络模型的预测结果采用通过如下步骤进行 泛化能力评价:In some embodiments of the present invention, the prediction result of the recurrent neural network model adopts the following steps to evaluate the generalization ability:
同一张图片中不同位置处预测的剂量分布与布拉格峰位置的评价和/或更换不同的PET活度图像进行的预测剂量分布与布拉格峰位置的评价。Evaluation of the predicted dose distribution and Bragg peak position at different positions in the same picture and/or the evaluation of the predicted dose distribution and Bragg peak position by replacing different PET activity images.
在本发明的一些实施例中,还包括:In some embodiments of the present invention, it further includes:
CT获取模块,配置成获取所述治疗对象的CT图像,The CT acquisition module is configured to acquire the CT image of the treatment subject,
其中,所述预测模块还配置成将所述CT获取模块获取的所述治疗对象的CT图像以及基于所述治疗对象的CT图像转换获得的阻止本领输入所述经训练的递归神经网络模型。Wherein, the prediction module is further configured to input the CT image of the treatment subject acquired by the CT acquisition module and the stopping power obtained based on the conversion of the CT image of the treatment subject into the trained recurrent neural network model.
根据本发明的又一方面,还提供一种质子治疗的参数监测系统,包括:According to another aspect of the present invention, there is also provided a parameter monitoring system for proton therapy, including:
CT系统,配置成提供治疗对象的CT图像;CT system, configured to provide CT images of the subject;
蒙特卡洛系统,配置成基于治疗对象的三维体模构建治疗对象,并模拟获得质子束的剂量分布和正电子核素活度分布,所述三维体模根据所述治疗对象的CT图像构建The Monte Carlo system is configured to construct a treatment object based on a three-dimensional phantom of the treatment object, and to obtain a dose distribution of a proton beam and a positron nuclide activity distribution by simulating, the three-dimensional phantom is constructed based on a CT image of the treatment object
PET系统,配置成提供质子与组织发生反应产生的正电子核素活度分布的PET图像;以及A PET system configured to provide PET images of the activity distribution of positron nuclides produced by the reaction between protons and tissues; and
如上所述的质子治疗的参数监测装置。The parameter monitoring device for proton therapy as described above.
相比现有技术,本发明的优势在于:Compared with the prior art, the advantages of the present invention are:
本发明采用经训练的递归神经网络模型,将实际临床中采集得到的PET图像数据通过用递归神经网络模型预测对应的剂量分布,实现了质子治疗中运用PET数据监测剂量分布与布拉格峰位置。本发明通过数据采集、数据处理及机器学习大大地提高了剂量分布与布拉格峰位置的预测精度,缩短了预测的时间。由此,通过本发明提供的装置和系统,保证质子治疗过程中对肿瘤组织进行质子束照射的剂量正常、位置准确,降低肿瘤复发和正常器官并发症的风险,从而保证对肿瘤患者进行质子治疗的治疗效果。The invention adopts a trained recurrent neural network model, and predicts the corresponding dose distribution of PET image data collected in actual clinical practice by using the recurrent neural network model to realize the use of PET data to monitor the dose distribution and Bragg peak position in proton therapy. The invention greatly improves the prediction accuracy of dose distribution and Bragg peak position through data collection, data processing and machine learning, and shortens the prediction time. Therefore, through the device and system provided by the present invention, it is ensured that the dose of proton beam irradiation to the tumor tissue during the proton therapy process is normal and the position is accurate, and the risk of tumor recurrence and normal organ complications is reduced, thereby ensuring the proton therapy for tumor patients The therapeutic effect.
附图说明Description of the drawings
通过参照附图详细描述其示例实施方式,本发明的上述和其它特征及优点将变得更加明显。The above-mentioned and other features and advantages of the present invention will become more apparent by describing in detail the exemplary embodiments thereof with reference to the accompanying drawings.
图1示出了根据本发明实施例的质子治疗的参数监测装置的模块图。Fig. 1 shows a block diagram of a parameter monitoring device for proton therapy according to an embodiment of the present invention.
图2示出了根据本发明实施例的计算阻止本领的示意图。Fig. 2 shows a schematic diagram of calculating stopping power according to an embodiment of the present invention.
图3示出了根据本发明实施例的递归神经网络模型的示意图。Fig. 3 shows a schematic diagram of a recurrent neural network model according to an embodiment of the present invention.
图4示出了根据本发明实施例的质子治疗的参数监测系统的模块图。Fig. 4 shows a block diagram of a parameter monitoring system for proton therapy according to an embodiment of the present invention.
图5示出了根据本发明实施例的递归神经网络训练过程图的示意图。Fig. 5 shows a schematic diagram of a recurrent neural network training process diagram according to an embodiment of the present invention.
图6示出了根据本发明实施例的结果预测的示意图。Fig. 6 shows a schematic diagram of result prediction according to an embodiment of the present invention.
图7示出了根据本发明实施例的数据采集系统的示意图。Fig. 7 shows a schematic diagram of a data acquisition system according to an embodiment of the present invention.
图8示出了根据本发明实施例的PET采集模块的示意图。Fig. 8 shows a schematic diagram of a PET collection module according to an embodiment of the present invention.
具体实施方式Detailed ways
现在将参考附图更全面地描述示例实施方式。然而,示例实施方式能够以多种形式实施,且不应被理解为限于在此阐述的范例;相反,提供这些实施方式使得本发明将更加全面和完整,并将示例实施方式的构思全面地传达给本领域的技术人员。所描述的特征、结构或特性可以以任何合适的方式结合在一个或更多实施方式中。Example embodiments will now be described more fully with reference to the accompanying drawings. However, the example embodiments can be implemented in various forms, and should not be construed as being limited to the examples set forth herein; on the contrary, the provision of these embodiments makes the present invention more comprehensive and complete, and fully conveys the concept of the example embodiments To those skilled in the art. The described features, structures or characteristics can be combined in one or more embodiments in any suitable way.
此外,附图仅为本发明的示意性图解,并非一定是按比例绘制。图中相同的附图标记表示相同或类似的部分,因而将省略对它们的重复描述。附图中所示的一些方框图是功能实体,不一定必须与物理或逻辑上独立的实体相对应。可以采用软件形式来实现这些功能实体,或在一个或多个硬件模块或集成电路中实现这些功能实体,或在不同网络和/或处理器装置和/或微控制器装置中实现这些功能实体。In addition, the drawings are only schematic illustrations of the present invention and are not necessarily drawn to scale. The same reference numerals in the figures denote the same or similar parts, and thus their repeated description will be omitted. Some of the block diagrams shown in the drawings are functional entities and do not necessarily correspond to physically or logically independent entities. These functional entities may be implemented in the form of software, or implemented in one or more hardware modules or integrated circuits, or implemented in different networks and/or processor devices and/or microcontroller devices.
附图中所示的流程图仅是示例性说明,不是必须包括所有的步骤。例如,有的步骤还可以分解,而有的步骤可以合并或部分合并,因此,实际执行的顺序有可能根据实际情况改变。The flowchart shown in the drawings is only an exemplary description, and does not necessarily include all the steps. For example, some steps can be decomposed, and some steps can be combined or partially combined. Therefore, the actual execution order may be changed according to actual conditions.
图1示出了根据本发明实施例的质子治疗的参数监测装置的模块图。Fig. 1 shows a block diagram of a parameter monitoring device for proton therapy according to an embodiment of the present invention.
质子治疗的参数监测装置100包括递归神经网络模块110、PET获取模块120、预测模块130、判断模块140以及调整模块150。The parameter monitoring device 100 for proton therapy includes a recurrent neural network module 110, a PET acquisition module 120, a prediction module 130, a judgment module 140, and an adjustment module 150.
递归神经网络模块110配置成提供经训练的递归神经网络模型,所述经训练的递归神经网络模型提供质子束的正电子核素活度分布与剂量分布的非线性关系。具体而言,所述递归神经网络模型可以是多输入递归神经网络模型。The recurrent neural network module 110 is configured to provide a trained recurrent neural network model that provides a non-linear relationship between the positron nuclide activity distribution of the proton beam and the dose distribution. Specifically, the recurrent neural network model may be a multi-input recurrent neural network model.
在本发明的一些实施例中,所述递归神经网络模型的在训练过程中的训练样本至少包括:阻止本领(stopping power,SP)、质子束的剂量分布和正电子核素活度分布。In some embodiments of the present invention, the training samples in the training process of the recurrent neural network model at least include stopping power (SP), the dose distribution of the proton beam, and the positron activity distribution.
所述阻止本领通过治疗对象的CT图像的CT值转化获得。The stopping power is obtained by transforming the CT value of the CT image of the subject.
具体而言,质子治疗的参数监测装置100还可以包括CT获取模块。CT获取模块配置成从医用CT系统获取所述治疗对象的CT图像(例如患者的全身的CT图像)。CT图像可以从医用CT系统中获取。可以根据治疗对象的CT图像构建三维体模,从而确定肿瘤病灶区域和感兴趣区。具体而言,可以采用医用CT系统扫描治疗对象全身获得CT图像,将获得的多帧CT图像结合起来,构建成一个三维体模,勾画出肿瘤病灶区域位置,适当扩大病灶区域,得到一个感兴趣区(Region of interest,ROI)。Specifically, the parameter monitoring device 100 for proton therapy may also include a CT acquisition module. The CT acquisition module is configured to acquire a CT image of the treatment target (for example, a CT image of the patient's whole body) from a medical CT system. CT images can be obtained from medical CT systems. A three-dimensional phantom can be constructed based on the CT image of the subject to be treated, so as to determine the tumor focus area and the area of interest. Specifically, a medical CT system can be used to scan the whole body of the subject to obtain CT images, and the obtained multiple frames of CT images can be combined to construct a three-dimensional phantom, outline the location of the tumor lesion area, and appropriately expand the lesion area to obtain an interesting Region (Region of interest, ROI).
所述阻止本领可以根据如下步骤转化:根据所述治疗对象的CT图像构成的三维CT图像中提取质子束经过路径上每个像素点的CT值;根据所述质子束的出束参数以及质子束经过路径上的CT值计算所述质子束经过路径上每个像素点对应的阻止本领。The stopping power can be transformed according to the following steps: extract the CT value of each pixel on the path of the proton beam from the three-dimensional CT image composed of the CT image of the treatment subject; according to the beam parameters of the proton beam and the proton beam The CT value on the passing path calculates the stopping power corresponding to each pixel on the path of the proton beam.
阻止本领可以按如下方式计算:The stopping power can be calculated as follows:
根据质子束的入射位置,从三维CT图像中提取质子束经过路径上的每个像素点CT值,结合质子束入射能量,计算出质子束经过路径上每个像素点对应的阻止本领, 具体计算公式如下:According to the incident position of the proton beam, the CT value of each pixel on the path of the proton beam is extracted from the three-dimensional CT image, combined with the incident energy of the proton beam, and the stopping power corresponding to each pixel on the path of the proton beam is calculated. The formula is as follows:
Figure PCTCN2020099492-appb-000001
Figure PCTCN2020099492-appb-000001
其中,SP i是第i个像素点的阻止本领,常数k=51Mev fm 2,β i是光速与粒子速度的比值,m e是电子质量,ρ e是物质每体积的电子密度,I是化合物的平均激发能,
Figure PCTCN2020099492-appb-000002
是壳修正项,
Figure PCTCN2020099492-appb-000003
是极化效应项,c是光速,E是粒子穿过物质后剩余的能量。
Wherein, the SP i is the i th pixel of the stopping power, constant k = 51Mev fm 2, β i is the ratio of the speed of light and the particle velocity, m e is the electron mass, ρ e is the electron density per volume of the substance, I is the compound Average excitation energy,
Figure PCTCN2020099492-appb-000002
Is the shell correction item,
Figure PCTCN2020099492-appb-000003
Is the polarization effect term, c is the speed of light, and E is the energy remaining after the particle passes through the matter.
其中,物质每体积的电子密度ρ e,化合物的平均激发能I可以按公式如下公式计算: Among them, the electron density per volume ρ e of the substance and the average excitation energy I of the compound can be calculated according to the following formula:
Figure PCTCN2020099492-appb-000004
Figure PCTCN2020099492-appb-000004
Figure PCTCN2020099492-appb-000005
Figure PCTCN2020099492-appb-000005
其中,N A是阿伏伽德罗常数,ρ是物质密度,Z i是元素i的原子序数,A i元素i的质量数,w i是元素i的权重因子,I i元素i的平均激发能,其中,ρ,Z i,w i可以通过CT值查表得到的。 Wherein, N A is the Avogadro number, [rho] is the density of the material, i the Z is the atomic number of the element i, A i mass number of element i, W i is the weight of element i weighting factor, the average excitation element i I i Yes, where ρ, Z i and w i can be obtained by looking up the table of CT values.
所述剂量分布和所述正电子核素活度分布经由治疗对象的三维体模在蒙特卡洛系统中构建的组织模拟获得。具体而言,本发明各实施例所描述的组织可以包括人体和/或动物。具体而言,所述剂量分布和所述正电子核素活度分布经由治疗对象的三维体模在蒙特卡洛系统中构建的组织中模拟不同入射能量和/或不同入射位置的质子治疗过程获得。例如,可以在蒙特卡洛系统中设定笔形束源的参数,通过程序模拟正电子发射过程,保证充足的束流量,设定相应的射束周期。通过蒙特卡洛工具保存剂量分布信息和正电子发射的活度分布信息。The dose distribution and the positron nuclide activity distribution are obtained through a tissue simulation constructed in a Monte Carlo system with a three-dimensional phantom of the subject to be treated. Specifically, the tissues described in the embodiments of the present invention may include humans and/or animals. Specifically, the dose distribution and the positron nuclide activity distribution are obtained by simulating the proton treatment process of different incident energies and/or different incident positions in the tissue constructed in the Monte Carlo system through the three-dimensional phantom of the subject to be treated. . For example, the parameters of the pencil beam source can be set in the Monte Carlo system, and the positron emission process can be simulated through the program to ensure sufficient beam flow and set the corresponding beam period. The dose distribution information and the activity distribution information of positron emission are saved by the Monte Carlo tool.
在本发明的一些实施例中,所述训练样本还包括所述质子束经过路径上的CT值。所述训练样本中,所述质子束经过路径上每个像素点的CT值、所述质子束经过路径上每个像素点对应的阻止本领、所述正电子核素活度分布作为所述递归神经网络模型的输入,所述剂量分布作为所述递归神经网络模型的输出,以对所述递归神经网络模型进行训练,以找到质子束的正电子核素活度分布与剂量分布的非线性关系。In some embodiments of the present invention, the training sample further includes a CT value along the path of the proton beam. In the training sample, the CT value of each pixel on the path of the proton beam, the stopping power corresponding to each pixel on the path of the proton beam, and the positron nuclide activity distribution are used as the recursive The input of the neural network model, and the dose distribution is used as the output of the recurrent neural network model to train the recurrent neural network model to find the non-linear relationship between the positron nuclide activity distribution of the proton beam and the dose distribution .
在本发明的一些实施例中,所述递归神经网络模型的预测结果采用均方误差(MSE)和/或平均绝对误差(MAE)进行定量评价。In some embodiments of the present invention, the prediction result of the recurrent neural network model adopts mean square error (MSE) and/or mean absolute error (MAE) for quantitative evaluation.
在本发明的一些实施例中,所述递归神经网络模型的预测结果采用通过如下步骤进行泛化能力评价:同一张图片中不同位置处预测的剂量分布与布拉格峰位置的评价和/或更换不同的PET活度图像进行的预测剂量分布与布拉格峰位置的评价。In some embodiments of the present invention, the prediction result of the recurrent neural network model adopts the following steps to evaluate the generalization ability: the predicted dose distribution at different positions in the same picture is different from the evaluation and/or replacement of the Bragg peak position The estimated dose distribution and Bragg peak position were evaluated based on the PET activity image.
PET获取模块120配置成从正电子湮没断层扫描系统中获取质子与组织发生反应产生的正电子核素活度分布的PET图像。The PET acquisition module 120 is configured to acquire a PET image of the activity distribution of positron nuclides produced by the reaction between protons and tissues from the positron annihilation tomography system.
具体而言,临床中,在质子治疗时,质子在进入组织后,与组织发生反应,产生正电子核素,用医用PET系统,对治疗对象进行PET扫描,得到反映正电子核素分布的PET活度图像。Specifically, in clinical proton therapy, after entering the tissue, protons react with the tissue to produce positron nuclides. The medical PET system is used to perform PET scanning on the target to obtain a PET reflecting the distribution of positron nuclides. Activity image.
具体而言,还可以利用蒙特卡洛系统模拟临床上治疗对象在接受质子治疗后进行PET成像。具体而言,可以通过模拟软件,设定一个相应的硬件PET系统,正电子核素选用(碳-11、氧-15),根据成像的需求,为了获得充足的光子数据统计信息(投影信息),选取相应的蒙卡时间,得到足够的计数。在充分取得投影信息后,对取得的投影进行重建,用单片重组算法(Single-Slice Rebinning,SSRB),和二维的有序子集最大似然法(Ordered Subsets Expectation Maximization,OSEM)进行图像迭代重建,得到重建的PET活度图像。完成CT的衰减校正,对图像整个成像视野进行均匀化校正,得到对应的反映正电子核素活度分布的PET图像。Specifically, the Monte Carlo system can also be used to simulate clinically treated subjects undergoing PET imaging after receiving proton therapy. Specifically, a corresponding hardware PET system can be set up through simulation software, positron nuclides are selected (carbon-11, oxygen-15), according to imaging needs, in order to obtain sufficient photon data statistics (projection information) , Select the corresponding Monte Carlo time to get enough counts. After sufficient projection information is obtained, the acquired projection is reconstructed, and the single-slice rebinning algorithm (Single-Slice Rebinning, SSRB) and the two-dimensional ordered subset maximum likelihood method (Ordered Subsets Expectation Maximization, OSEM) are used to image Iterative reconstruction to obtain the reconstructed PET activity image. The attenuation correction of CT is completed, and the entire imaging field of the image is uniformized and corrected, and the corresponding PET image reflecting the activity distribution of positron nuclide is obtained.
预测模块130配置成将所述PET图像输入所述经训练的递归神经网络模型,预测质子束的剂量分布与布拉格峰位置。The prediction module 130 is configured to input the PET image into the trained recurrent neural network model to predict the dose distribution and Bragg peak position of the proton beam.
所述预测模块还用于将所述CT获取模块获取的所述治疗对象的CT图像以及基于所述治疗对象的CT图像转换获得的阻止本领输入所述经训练的递归神经网络模型。The prediction module is further configured to input the CT image of the treatment subject acquired by the CT acquisition module and the stopping power obtained based on the conversion of the CT image of the treatment subject into the trained recurrent neural network model.
判断模块140配置成根据所预测的质子束的剂量分布判断布拉格峰位置与目标区域的位置关系。The determining module 140 is configured to determine the positional relationship between the Bragg peak position and the target area according to the predicted dose distribution of the proton beam.
调整模块150配置成依据所述判断模块140的判断结果确定质子束的出束参数是否需要调整。The adjustment module 150 is configured to determine whether the beam output parameters of the proton beam need to be adjusted according to the judgment result of the judgment module 140.
具体而言,如果质子束剂量分布没有落在肿瘤病灶区域内,而是偏离肿瘤病灶区域,那么可能是在进行质子束照射时,照射的位置发生了偏离,需要调整质子束治疗头的照射位置;如果质子束剂量分布没有落在肿瘤病灶区域内,而是蔓延出了肿瘤病灶区域,那么说明在进行质子束照射时,质子束能量偏大,需要调整质子束的剂量。由此,所述调整模块150还配置成:Specifically, if the proton beam dose distribution does not fall within the tumor lesion area, but deviates from the tumor lesion area, then the irradiation position may be deviated when the proton beam is irradiated, and the irradiation position of the proton beam treatment head needs to be adjusted ; If the proton beam dose distribution does not fall within the tumor focus area, but spreads out of the tumor focus area, it means that the proton beam energy is too large when the proton beam is irradiated, and the dose of the proton beam needs to be adjusted. Therefore, the adjustment module 150 is further configured to:
若所述判断模块140判断所预测的质子束的剂量分布与布拉格峰位置位于目标区域内,则判断质子束放射治疗准确,继续按照现有的质子束出束参数进行放射治疗,不对所述质子束的出束参数进行调整,直到治疗结束。本发明并非以此为限制。If the judgment module 140 judges that the predicted dose distribution of the proton beam and the Bragg peak position are within the target area, it judges that the proton beam radiotherapy is accurate, and continues to perform radiotherapy according to the existing proton beam emission parameters, and does not treat the proton beam. The beam parameters of the beam are adjusted until the end of the treatment. The present invention is not limited by this.
若所述判断模块140判断所预测的质子束的剂量分布与布拉格峰位置位于目标区域外,则判断质子束放射治疗不准确,重新调整所述质子束的出束参数,直到调整后的质子束剂量分布与布拉格峰位置与放射治疗计划一致。If the judgment module 140 judges that the predicted dose distribution of the proton beam and the Bragg peak position are outside the target area, it judges that the proton beam radiotherapy is not accurate, and readjusts the beam parameters of the proton beam until the adjusted proton beam The dose distribution and Bragg peak position are consistent with the radiation treatment plan.
在本发明的示例性实施方式的质子治疗的参数监测装置100中,采用经训练的递归神经网络模型,将实际临床中采集得到的PET图像数据通过用递归神经网络模型预测对应的剂量分布,实现了质子治疗中运用PET数据监测剂量分布与布拉格峰位置。本发明通过数据采集、数据处理及机器学习大大地提高了剂量分布与布拉格峰位置的预测精度,缩短了预测的时间。由此,通过本发明提供的装置和系统,保证质子治疗 过程中对肿瘤组织进行质子束照射的剂量正常、位置准确,降低肿瘤复发和正常器官并发症的风险,从而保证对肿瘤患者进行质子治疗的治疗效果。In the parameter monitoring device 100 for proton therapy according to the exemplary embodiment of the present invention, a trained recurrent neural network model is adopted, and the PET image data collected in the actual clinic is used to predict the corresponding dose distribution by using the recurrent neural network model to achieve The use of PET data in proton therapy to monitor dose distribution and Bragg peak position. The invention greatly improves the prediction accuracy of dose distribution and Bragg peak position through data collection, data processing and machine learning, and shortens the prediction time. Therefore, through the device and system provided by the present invention, it is ensured that the dose of proton beam irradiation to the tumor tissue during the proton therapy process is normal and the position is accurate, and the risk of tumor recurrence and normal organ complications is reduced, thereby ensuring the proton therapy for tumor patients The therapeutic effect.
在本发明的示例性实施方式的质子治疗的参数监测装置100中,如实地验证了本发明的基于机器学习模型的质子治疗中的剂量与范围验证的监控方法在质子治疗过程中对剂量分布、布拉格峰位置监测的广泛适用性。保证了质子束照射的剂量正常、位置准确,降低肿瘤复发和正常器官并发症的风险,从而保证对肿瘤患者进行质子治疗的治疗效果。In the parameter monitoring device 100 for proton therapy according to the exemplary embodiment of the present invention, it is verified that the monitoring method for dose and range verification in proton therapy based on the machine learning model of the present invention has a positive effect on the dose distribution, Broad applicability of Bragg peak position monitoring. It ensures that the dose of proton beam irradiation is normal and the position is accurate, and the risk of tumor recurrence and normal organ complications is reduced, thereby ensuring the therapeutic effect of proton therapy for tumor patients.
图1仅仅是示意性的示出本发明提供的质子治疗的参数监测装置100,在不违背本发明构思的前提下,模块的拆分、合并、增加都在本发明的保护范围之内。本发明提供的质子治疗的参数监测装置100可以由软件、硬件、固件、插件及他们之间的任意组合来实现,本发明并非以此为限。FIG. 1 only schematically shows the parameter monitoring device 100 for proton therapy provided by the present invention. Without violating the concept of the present invention, the splitting, merging, and adding of modules are all within the protection scope of the present invention. The parameter monitoring device 100 for proton therapy provided by the present invention can be implemented by software, hardware, firmware, plug-ins and any combination between them, and the present invention is not limited to this.
图2示出了根据本发明实施例的计算阻止本领的示意图。阻止本领可以根据如下方式(见图2标号10)计算:Fig. 2 shows a schematic diagram of calculating stopping power according to an embodiment of the present invention. The stopping power can be calculated according to the following method (see number 10 in Figure 2):
首先,根据CT图像中每个像素的CT值,计算出每个像素点对应的阻止本领,其中阻止本领的计算公式如下:First, according to the CT value of each pixel in the CT image, the stopping power corresponding to each pixel is calculated. The stopping power calculation formula is as follows:
Figure PCTCN2020099492-appb-000006
Figure PCTCN2020099492-appb-000006
其中,SP i是第i个像素的阻止本领,常数k=51Mev fm 2,β i是光速与粒子速度的比值,m e是电子质量,ρ e是物质每体积的电子密度,I是化合物的平均激发能。
Figure PCTCN2020099492-appb-000007
是壳修正项,
Figure PCTCN2020099492-appb-000008
是极化效应项,c是光速,E是粒子穿过物质后剩余的动能。
Wherein, the SP i is the i-th pixel of the stopping power, constant k = 51Mev fm 2, β i is the speed of light, the ratio of particle velocity, m e is the electron mass, ρ e is the electron density per volume of the substance, I is the compound Average excitation energy.
Figure PCTCN2020099492-appb-000007
Is the shell correction item,
Figure PCTCN2020099492-appb-000008
Is the polarization effect term, c is the speed of light, and E is the remaining kinetic energy of the particle after passing through the matter.
其中,物质每体积的电子密度ρ e,其计算公式如下: Among them, the electron density per volume of the substance ρ e is calculated as follows:
Figure PCTCN2020099492-appb-000009
Figure PCTCN2020099492-appb-000009
N A是阿伏伽德罗常数,ρ是物质密度,Z i是元素i的原子序数,A i元素i的质量数,w i是元素i的权重因子。 N A is the Avogadro number, [rho] is the density of the material, i the Z is the atomic number of the element i, the mass number of the element i A i, W i is the weight of element i weighting factor.
其中,化合物的平均激发能I,其计算公式如下:Among them, the average excitation energy I of the compound is calculated as follows:
Figure PCTCN2020099492-appb-000010
Figure PCTCN2020099492-appb-000010
其中,N A是阿伏伽德罗常数,ρ是物质密度,Z i是元素i的原子序数,A i元素i的质量数,w i是元素i的权重因子,I i元素i的平均激发能。其中,ρ,Z i,w i是通过CT值查表得到的,其中查找表为:CT值与不同组织元素组成对应表。 Wherein, N A is the Avogadro number, [rho] is the density of the material, i the Z is the atomic number of the element i, A i mass number of element i, W i is the weight of element i weighting factor, the average excitation element i I i can. Among them, ρ, Z i , and w i are obtained through the CT value look-up table, where the look-up table is: the corresponding table of the CT value and the composition of different tissue elements.
由于随着质子不断地穿过组织,粒子的能量在逐渐递减,质子在所穿过的路径上不断的沉积少部分能量,直到在质子束末端将能量全部释放,形成布拉格峰,见图2标号20。图2中bethe theory即文中的SP计算公式(Bethe—Block公式)。As the protons continue to pass through the tissue, the energy of the particles is gradually decreasing, and the protons continue to deposit a small amount of energy on the path they pass, until all the energy is released at the end of the proton beam, forming a Bragg peak, as shown in Figure 2. 20. The bethe theory in Figure 2 is the SP calculation formula (Bethe-Block formula) in the text.
通过本实施例能够准确计算质子在所经过的像素位置所沉积的能量,为模型的训练提供准确的训练样本;将其用作为神经网络的一个输入,为机器学习模型提供一个先验,降低学习难度,提升模型的预测精度、抗噪性能及泛化能力。Through this embodiment, it is possible to accurately calculate the energy deposited by the proton at the pixel position passed by, and provide accurate training samples for the training of the model; use it as an input to the neural network to provide a priori for the machine learning model, reducing learning Difficulty, to improve the prediction accuracy, anti-noise performance and generalization ability of the model.
图3示出了根据本发明实施例的递归神经网络模型的示意图。Fig. 3 shows a schematic diagram of a recurrent neural network model according to an embodiment of the present invention.
递归神经网络(RNN)是专门处理时间序列数据的,它将一个时序的输入通过隐层状态转化为一个时序的输出,通过反向传播和梯度下降法不断训练学习输入与输出之间的映射关系。递归神经网络模型由输入层(x 0~x n)、隐含层(h 0~h n)、输出层组成(D 0~D n)。其中,网络的输入层为多数据输入,由所述治疗对象的CT图像、基于所述治疗对象的CT图像转换获得的阻止本领以及所述PET图像获得的活度值组成,再将CT值,SP值,正电子核素分布活度值三个数组并列组成。递归神经网络模型的输出为剂量分布,剂量分布的最大值位置即为布拉格峰。进一步地,递归神经网络模型中输入数据之间具有级联关系。 Recurrent Neural Network (RNN) is specialized in processing time series data. It converts a time series input into a time series output through a hidden layer state, and continuously trains and learns the mapping relationship between input and output through back propagation and gradient descent methods. . The recurrent neural network model is composed of an input layer (x 0 ~x n ), a hidden layer (h 0 ~h n ), and an output layer (D 0 ~D n ). Wherein, the input layer of the network is a multi-data input, consisting of the CT image of the treatment subject, the stopping power obtained based on the conversion of the CT image of the treatment subject, and the activity value obtained from the PET image, and then the CT value, Three arrays of SP value and positron nuclide distribution activity value are juxtaposed. The output of the recurrent neural network model is the dose distribution, and the maximum position of the dose distribution is the Bragg peak. Further, the input data in the recurrent neural network model has a cascading relationship.
通过本实施例构建网络模型,预测质子束剂量分布和布拉格峰位置,经过测试,该模型具有良好的预测精度,抗噪性能及泛化能力,并且在基于PET图像的预测上表现良好。A network model is constructed through this embodiment to predict the proton beam dose distribution and Bragg peak position. After testing, the model has good prediction accuracy, anti-noise performance and generalization ability, and performs well in prediction based on PET images.
图4示出了根据本发明实施例的质子治疗的参数监测系统的模块图。质子治疗的参数监测系统包括CT系统210、蒙特卡洛系统220、PET系统230以及如图1所示的质子治疗的参数监测装置100。Fig. 4 shows a block diagram of a parameter monitoring system for proton therapy according to an embodiment of the present invention. The parameter monitoring system for proton therapy includes a CT system 210, a Monte Carlo system 220, a PET system 230, and the parameter monitoring device 100 for proton therapy as shown in FIG. 1.
CT系统210配置成提供治疗对象的CT图像。进而可构建三维体模,勾画感兴趣区,用于最终质子治疗监测终端。蒙特卡洛系统220配置成基于治疗对象的三维体模构建治疗对象,并模拟获得质子束的剂量分布和正电子核素活度分布,以生成模型所需要的训练集,所述三维体模根据所述治疗对象的CT图像构建。PET系统230配置成提供质子与组织发生反应产生的正电子核素活度分布的PET图像。参数监测装置100所包括的模块已在上文描述,在此不予赘述。参数监测装置100还可以对预测的结果进行定量定性的评价,对于质子束的调整进行跟进追踪。The CT system 210 is configured to provide CT images of the treatment subject. Furthermore, a three-dimensional phantom can be constructed to delineate the area of interest for the final proton therapy monitoring terminal. The Monte Carlo system 220 is configured to construct the treatment object based on the three-dimensional phantom of the treatment object, and to obtain the dose distribution of the proton beam and the activity distribution of the positron nuclide by simulating to generate the training set required by the model. The three-dimensional phantom is based on the The construction of CT images of the subject to be treated. The PET system 230 is configured to provide a PET image of the activity distribution of positron nuclides produced by the reaction between protons and tissues. The modules included in the parameter monitoring device 100 have been described above, and will not be repeated here. The parameter monitoring device 100 can also perform a quantitative and qualitative evaluation of the predicted result, and follow up the adjustment of the proton beam.
图4仅仅是示意性的示出本发明提供的质子治疗的参数监测系统,在不违背本发明构思的前提下,模块的拆分、合并、增加都在本发明的保护范围之内。本发明提供的质子治疗的参数监测系统可以由软件、硬件、固件、插件及他们之间的任意组合来实现,本发明并非以此为限。Fig. 4 only schematically shows the parameter monitoring system of proton therapy provided by the present invention. Without violating the concept of the present invention, the splitting, merging, and adding of modules are all within the protection scope of the present invention. The parameter monitoring system for proton therapy provided by the present invention can be implemented by software, hardware, firmware, plug-ins and any combination between them, and the present invention is not limited to this.
下面参见图5,图5示出了根据本发明一个具体实施例的递归神经网络训练过程图的示意图。图5示出了数据收集系统、数据预处理系统、递归神经网络RNN模型系统、模型评估系统。其中数据收集系统包含数据采集系统,主要采集病人的临床数 据,包括CT系统采集的解剖学临床信息,也包括PET系统采集的临床信息;数据收集系统还包括数据模拟系统,主要是基于CT图像,在蒙特卡洛系统中生成剂量分布图与活度分布图。数据收集系统获得的所有的数据都将用于后面的神经网络模型的训练与剂量的验证。Next, referring to Fig. 5, Fig. 5 shows a schematic diagram of a recurrent neural network training process diagram according to a specific embodiment of the present invention. Figure 5 shows a data collection system, a data preprocessing system, a recurrent neural network RNN model system, and a model evaluation system. The data collection system includes a data collection system, which mainly collects patient clinical data, including anatomical clinical information collected by the CT system, and clinical information collected by the PET system; the data collection system also includes a data simulation system, which is mainly based on CT images, Generate dose distribution diagram and activity distribution diagram in the Monte Carlo system. All the data obtained by the data collection system will be used for subsequent neural network model training and dose verification.
数据预处理模块用于将CT数据转化为阻止本领,以及将取得的数据标准化以用于更好的网络训练。示出的递归神经网络模型,根据既定的批量选取经过预处理的数据输入到神经网络模型中进行训练,用验证集数据对模型进行评估,定量的分析模型的各性能参数,定量评价模型误差,对是否满足计划目标进行评价,不断调整模型参数直到满足目标计划,保存模型。The data preprocessing module is used to convert CT data into stopping power, and to standardize the acquired data for better network training. The shown recursive neural network model selects preprocessed data according to a predetermined batch and inputs it into the neural network model for training, uses the validation set data to evaluate the model, quantitatively analyzes the performance parameters of the model, and quantitatively evaluates the model error. Evaluate whether the plan goal is met, continuously adjust the model parameters until the goal plan is met, and save the model.
下面参见图6,图6示出了根据本发明实施例的结果预测的示意图。图6示出了病人数据模块,包含数据采集模块与数据计算模块,其中数据采集模块主要包含CT数据采集与PET数据采集,数据计算主要是基于采集到的CT数据将其计算为对应的阻止本领(SP),然后将CT系统采集的CT数据,PET采集的活度数据及计算得到的阻止本领输入到训练好的RNN模型中,输出预测结果。Next, referring to FIG. 6, FIG. 6 shows a schematic diagram of result prediction according to an embodiment of the present invention. Figure 6 shows the patient data module, which includes a data acquisition module and a data calculation module. The data acquisition module mainly includes CT data acquisition and PET data acquisition. The data calculation is mainly based on the collected CT data and calculates it as the corresponding stopping power (SP), then input the CT data collected by the CT system, the activity data collected by the PET and the calculated stopping power into the trained RNN model, and output the prediction results.
下面参见图7,图7示出了根据本发明实施例的数据采集系统的示意图。图7描述了本发明一具体实施例的数据采集过程以及数据得到的方法途径。图7示出了产生质子束的加速器系统与常用的临床数据采集系统。其中主要通过加速器系统产生用于质子治疗的质子束,然后将质子束打到人体组织内,用于肿瘤的治疗。而采集系统中的硬件数据采集系统主要包含CT系统与PET系统。其中CT系统是通过X射线对组织进行结构成像,其中,CT系统的X射线是在高度真空的X射线管中产生的,是高能高速的电子撞击阳极靶面,运动突然受到阻止,高速电子与核电场作用形成辐射,产生一束连续X线。X射线扫描人体组织,在X射线探测器上形成经过组织衰减的X射线投影数据,对数据进行重建就形成CT图像数据。而质子束进入人体后,会与人体内原子核反应产生正电子衰变核素,释放出的正电子湮灭产生的两个方向相反的511keV光子,这些湮灭光子被PET探测器探测到后,再经过一系列的图像重建算法就形成PET人体活度图像。Next, referring to Fig. 7, Fig. 7 shows a schematic diagram of a data acquisition system according to an embodiment of the present invention. FIG. 7 describes the data collection process and the method of obtaining data in a specific embodiment of the present invention. Figure 7 shows an accelerator system that generates a proton beam and a commonly used clinical data acquisition system. Among them, the accelerator system is mainly used to generate proton beams for proton therapy, and then the proton beams are shot into human tissues for tumor treatment. The hardware data acquisition system in the acquisition system mainly includes a CT system and a PET system. Among them, the CT system uses X-rays to image the structure of the tissue. Among them, the X-rays of the CT system are generated in a high-vacuum X-ray tube. The nuclear electric field acts to form radiation, which produces a continuous beam of X-rays. X-ray scans human tissues, and forms X-ray projection data after tissue attenuation on the X-ray detector, and reconstructs the data to form CT image data. After the proton beam enters the human body, it will react with the nucleus in the human body to produce a positron decay nuclide. The released positron annihilates two 511 keV photons in opposite directions. These annihilation photons are detected by the PET detector and then pass through another one. A series of image reconstruction algorithms form a PET human body activity image.
下面参见图8,图8示出了根据本发明实施例的PET采集模块的示意图。已知质子束流穿过人体,会与人体内原子核反应产生正电子衰变核素,释放出的正电子湮灭产生的两个方向相反的511keV的光子,被探测器探测,通过正电子湮没成像技术(PET)构建人体活度图像。需要对正电子诱导的核素活度信号进行成像,以便能够通过活度分布找到质子束剂量分布,因此需要搭建PET系统采集数据,完成活度成像。图8示出本发明实施例的在蒙特卡洛系统中搭建的一个In-Beam PET系统,包含两个探测器阵列单元2。质子束1入射病人体3后,会激发光子打在探测器上,通过符合探测,重构活度分布图,形成活度分布数据集,用于神经网络的数据输入。Next, referring to FIG. 8, FIG. 8 shows a schematic diagram of a PET collection module according to an embodiment of the present invention. It is known that the proton beam passing through the human body will react with the nucleus in the human body to produce positron decay nuclide, and the released positron annihilation produces two opposite 511keV photons, which are detected by the detector through positron annihilation imaging technology. (PET) Construct human activity images. It is necessary to image the positron-induced radionuclide activity signal so that the proton beam dose distribution can be found through the activity distribution. Therefore, it is necessary to build a PET system to collect data and complete the activity imaging. FIG. 8 shows an In-Beam PET system built in a Monte Carlo system according to an embodiment of the present invention, which includes two detector array units 2. After the proton beam 1 enters the patient's body 3, it will excite photons to hit the detector. Through coincidence detection, the activity distribution map is reconstructed to form an activity distribution data set, which is used for data input of the neural network.
以上仅仅是本发明的多个具体实现方式,各具体实现可以单独或组合来实现,本 发明并非以此为限制。The above are only multiple specific implementations of the present invention, and each specific implementation can be implemented individually or in combination, and the present invention is not limited thereto.
相比现有技术,本发明的优势在于:Compared with the prior art, the advantages of the present invention are:
本发明采用经训练的递归神经网络模型,将实际临床中采集得到的PET图像数据通过用递归神经网络模型预测对应的剂量分布,实现了质子治疗中运用PET数据监测剂量分布与布拉格峰位置。本发明通过数据采集、数据处理及机器学习大大地提高了剂量分布与布拉格峰位置的预测精度,缩短了预测的时间。由此,通过本发明提供的装置和系统,保证质子治疗过程中对肿瘤组织进行质子束照射的剂量正常、位置准确,降低肿瘤复发和正常器官并发症的风险,从而保证对肿瘤患者进行质子治疗的治疗效果。The invention adopts a trained recurrent neural network model, and predicts the corresponding dose distribution of PET image data collected in actual clinical practice by using the recurrent neural network model to realize the use of PET data to monitor the dose distribution and Bragg peak position in proton therapy. The invention greatly improves the prediction accuracy of dose distribution and Bragg peak position through data collection, data processing and machine learning, and shortens the prediction time. Therefore, through the device and system provided by the present invention, it is ensured that the dose of proton beam irradiation to the tumor tissue during the proton therapy process is normal and the position is accurate, and the risk of tumor recurrence and normal organ complications is reduced, thereby ensuring the proton therapy for tumor patients The therapeutic effect.
本领域技术人员在考虑说明书及实践这里公开的发明后,将容易想到本发明的其它实施方案。本申请旨在涵盖本发明的任何变型、用途或者适应性变化,这些变型、用途或者适应性变化遵循本发明的一般性原理并包括本发明未公开的本技术领域中的公知常识或惯用技术手段。说明书和实施例仅被视为示例性的,本发明的真正范围和精神由所附的权利要求指出。Those skilled in the art will easily think of other embodiments of the present invention after considering the specification and practicing the invention disclosed herein. This application is intended to cover any variations, uses, or adaptive changes of the present invention. These variations, uses, or adaptive changes follow the general principles of the present invention and include common knowledge or conventional technical means in the technical field that are not disclosed by the present invention. . The description and the embodiments are to be regarded as exemplary only, and the true scope and spirit of the present invention are pointed out by the appended claims.

Claims (10)

  1. 一种质子治疗的参数监测装置,其特征在于,包括:A parameter monitoring device for proton therapy, which is characterized in that it comprises:
    递归神经网络模块,配置成提供经训练的递归神经网络模型,所述经训练的递归神经网络模型提供质子束的正电子核素活度分布与剂量分布的非线性关系;A recurrent neural network module, configured to provide a trained recurrent neural network model, the trained recurrent neural network model providing a non-linear relationship between the positron nuclide activity distribution of the proton beam and the dose distribution;
    PET获取模块,配置成从正电子湮没断层扫描系统中获取质子与组织发生反应产生的正电子核素活度分布的PET图像;The PET acquisition module is configured to acquire a PET image of the activity distribution of positron nuclides produced by the reaction between protons and tissues from the positron annihilation tomography system;
    预测模块,配置成将所述PET图像输入所述经训练的递归神经网络模型,通过所述经训练的递归神经网络模型提供的质子束的正电子核素活度分布与剂量分布的非线性关系,预测质子束的剂量分布与布拉格峰位置;A prediction module configured to input the PET image into the trained recurrent neural network model, and the non-linear relationship between the positron nuclide activity distribution of the proton beam and the dose distribution provided by the trained recurrent neural network model , To predict the dose distribution of the proton beam and the position of the Bragg peak;
    判断模块,配置成根据所述预测的质子束的剂量分布判断布拉格峰位置与目标区域的位置关系;A judging module, configured to judge the positional relationship between the Bragg peak position and the target area according to the predicted dose distribution of the proton beam;
    调整模块,配置成依据所述判断模块判断的结果确定质子束的出束参数是否需要调整。The adjustment module is configured to determine whether the beam output parameters of the proton beam need to be adjusted according to the judgment result of the judgment module.
  2. 如权利要求1所述的质子治疗的参数监测装置,其特征在于,所述调整模块还配置成:The parameter monitoring device for proton therapy according to claim 1, wherein the adjustment module is further configured to:
    若所述判断模块判断所预测的质子束的剂量分布与布拉格峰位置位于目标区域内,则不对所述质子束的出束参数进行调整;If the judgment module judges that the predicted dose distribution of the proton beam and the Bragg peak position are within the target area, then the beam output parameters of the proton beam are not adjusted;
    若所述判断模块判断所预测的质子束的剂量分布与布拉格峰位置位于目标区域外,则重新调整所述质子束的出束参数。If the judgment module judges that the predicted dose distribution of the proton beam and the Bragg peak position are outside the target area, readjust the beam output parameters of the proton beam.
  3. 如权利要求1所述的质子治疗的参数监测装置,其特征在于,所述递归神经网络模型在训练过程中的训练样本至少包括:阻止本领、质子束的剂量分布和正电子核素活度分布,其中,所述阻止本领通过治疗对象的CT图像的CT值转化获得,所述剂量分布和所述正电子核素活度分布经由治疗对象的三维体模在蒙特卡洛系统中构建的组织模拟获得,所述治疗对象的三维体模根据所述治疗对象的CT图像构建。The parameter monitoring device for proton therapy according to claim 1, wherein the training samples of the recurrent neural network model during the training process at least include: stopping power, proton beam dose distribution and positron nuclide activity distribution, Wherein, the stopping power is obtained by transforming the CT value of the CT image of the treatment subject, and the dose distribution and the positron nuclide activity distribution are obtained by the tissue simulation constructed in the Monte Carlo system through the three-dimensional phantom of the treatment subject , The three-dimensional phantom of the treatment target is constructed according to the CT image of the treatment target.
  4. 根据权利要求3所述的质子治疗的参数监测装置,其特征在于,所述剂量分布和所述正电子核素活度分布经由治疗对象的三维体模在蒙特卡洛系统中构建的组织中模拟不同入射能量和/或不同入射位置的质子治疗过程获得。The parameter monitoring device for proton therapy according to claim 3, wherein the dose distribution and the positron nuclide activity distribution are simulated in a tissue constructed in a Monte Carlo system via a three-dimensional phantom of the subject to be treated. Different incident energy and/or different incident positions are obtained during proton therapy.
  5. 根据权利要求3所述的质子治疗的参数监测装置,其特征在于,所述阻止本领根据如下步骤转化:The parameter monitoring device for proton therapy according to claim 3, wherein the stopping power is transformed according to the following steps:
    根据所述治疗对象的CT图像构成的三维CT图像中提取质子束经过路径上每个像素点的CT值;Extracting the CT value of each pixel on the path of the proton beam from the three-dimensional CT image formed by the CT image of the treatment subject;
    根据所述质子束的出束参数以及所述每个像素点的CT值计算所述每个像素点对应的阻止本领。The stopping power corresponding to each pixel is calculated according to the beam output parameter of the proton beam and the CT value of each pixel.
  6. 根据权利要求3所述的质子治疗的参数监测装置,其特征在于,所述训练样本还包括质子束经过路径上的CT值,在所述训练样本中,所述质子束经过路径上每个像素点 的CT值、所述质子束经过路径上每个像素点对应的阻止本领、正电子核素活度分布被作为所述递归神经网络模型的输入,所述质子束的剂量分布被作为递归神经网络模型的输出,以对所述递归神经网络模型进行训练。The parameter monitoring device for proton therapy according to claim 3, wherein the training sample further includes CT values on the path of the proton beam, and in the training sample, the proton beam passes through each pixel on the path. The CT value of a point, the stopping power corresponding to each pixel on the path of the proton beam, and the distribution of positron nuclide activity are used as the input of the recurrent neural network model, and the dose distribution of the proton beam is used as the recursive nerve The output of the network model is used to train the recurrent neural network model.
  7. 根据权利要求1所述的质子治疗的参数监测装置,其特征在于,所述递归神经网络模型的预测结果采用均方误差和/或平均绝对误差进行定量评价。The parameter monitoring device for proton therapy according to claim 1, wherein the prediction result of the recurrent neural network model is quantitatively evaluated by means of mean square error and/or mean absolute error.
  8. 根据权利要求1所述的质子治疗的参数监测装置,其特征在于,所述递归神经网络模型的预测结果采用通过如下步骤进行泛化能力评价:The parameter monitoring device for proton therapy according to claim 1, wherein the prediction result of the recurrent neural network model adopts the following steps to evaluate the generalization ability:
    同一张图片中不同位置处预测的剂量分布与布拉格峰位置的评价和/或更换不同的PET活度图像进行的预测剂量分布与布拉格峰位置的评价。Evaluation of the predicted dose distribution and Bragg peak position at different positions in the same picture and/or the evaluation of the predicted dose distribution and Bragg peak position by replacing different PET activity images.
  9. 根据权利要求1所述的质子治疗的参数监测装置,其特征在于,还包括:The parameter monitoring device for proton therapy according to claim 1, further comprising:
    CT获取模块,配置成获取所述治疗对象的CT图像,The CT acquisition module is configured to acquire the CT image of the treatment subject,
    其中,所述预测模块还配置成将所述CT获取模块获取的所述治疗对象的CT图像以及基于所述治疗对象的CT图像转换获得的阻止本领输入所述经训练的递归神经网络模型。Wherein, the prediction module is further configured to input the CT image of the treatment subject acquired by the CT acquisition module and the stopping power obtained based on the conversion of the CT image of the treatment subject into the trained recurrent neural network model.
  10. 一种质子治疗的参数监测系统,其特征在于,包括:A parameter monitoring system for proton therapy, which is characterized in that it comprises:
    CT系统,配置成提供治疗对象的CT图像;CT system, configured to provide CT images of the subject;
    蒙特卡洛系统,配置成基于治疗对象的三维体模构建治疗对象,并模拟获得质子束的剂量分布和正电子核素活度分布,所述三维体模根据所述治疗对象的CT图像构建;The Monte Carlo system is configured to construct a treatment object based on a three-dimensional phantom of the treatment object, and to obtain a dose distribution of a proton beam and a positron nuclide activity distribution by simulating, the three-dimensional phantom is constructed based on a CT image of the treatment object;
    PET系统,配置成提供质子与组织发生反应产生的正电子核素活度分布的PET图像;以及A PET system configured to provide PET images of the activity distribution of positron nuclides produced by the reaction between protons and tissues; and
    如权利要求1至9任一项所述的质子治疗的参数监测装置。The parameter monitoring device for proton therapy according to any one of claims 1 to 9.
PCT/CN2020/099492 2020-05-26 2020-06-30 Parameter monitoring device and system for proton therapy WO2021237869A1 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
CN202010453061.9A CN111569279B (en) 2020-05-26 2020-05-26 Parameter monitoring device and system for proton treatment
CN202010453061.9 2020-05-26

Publications (1)

Publication Number Publication Date
WO2021237869A1 true WO2021237869A1 (en) 2021-12-02

Family

ID=72121477

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/CN2020/099492 WO2021237869A1 (en) 2020-05-26 2020-06-30 Parameter monitoring device and system for proton therapy

Country Status (2)

Country Link
CN (1) CN111569279B (en)
WO (1) WO2021237869A1 (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111991711A (en) * 2020-09-07 2020-11-27 杭州珞珈质子科技有限公司 Parameter monitoring device and system for proton treatment
CN112023279A (en) * 2020-09-11 2020-12-04 杭州珞珈质子科技有限公司 Parameter monitoring device and system for proton treatment
CN113426030B (en) * 2021-05-25 2023-12-05 海创时代(深圳)医疗科技有限公司 Proton dosage calculation method and device
CN113744331B (en) * 2021-08-26 2024-03-22 上海联影医疗科技股份有限公司 Energy determination method, device, equipment and storage medium
CN116236704A (en) * 2021-12-07 2023-06-09 苏州瑞派宁科技有限公司 Proton range verification method, proton range verification device and computer-readable storage medium

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106772546A (en) * 2016-12-29 2017-05-31 中科超精(安徽)科技有限公司 One kind is considered by medium to heteropical charged particle equivalent depth acquisition methods
US20190175952A1 (en) * 2017-12-08 2019-06-13 Elekta, Inc. Determining parameters for a beam model of a radiation machine using deep convolutional neural networks
CN110270016A (en) * 2019-05-27 2019-09-24 彭浩 Proton therapeutic monitoring method, device and system neural network based

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP3305200A1 (en) * 2016-10-07 2018-04-11 Ion Beam Applications S.A. Medical apparatus comprising a hadron therapy device, a mri, and a prompt-gamma system
US10898727B2 (en) * 2017-08-23 2021-01-26 Siemens Healthcare Gmbh Method for providing result data which is suitable for use in planning the irradiation of a patient
CN110215619B (en) * 2018-03-03 2022-03-08 彭浩 Intelligent proton on-line monitoring system
CN110270014B (en) * 2019-05-07 2022-01-04 彭浩 Proton or heavy ion radiotherapy dose real-time monitoring method and system

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106772546A (en) * 2016-12-29 2017-05-31 中科超精(安徽)科技有限公司 One kind is considered by medium to heteropical charged particle equivalent depth acquisition methods
US20190175952A1 (en) * 2017-12-08 2019-06-13 Elekta, Inc. Determining parameters for a beam model of a radiation machine using deep convolutional neural networks
CN110270016A (en) * 2019-05-27 2019-09-24 彭浩 Proton therapeutic monitoring method, device and system neural network based

Also Published As

Publication number Publication date
CN111569279A (en) 2020-08-25
CN111569279B (en) 2021-08-17

Similar Documents

Publication Publication Date Title
WO2021237869A1 (en) Parameter monitoring device and system for proton therapy
Van Elmpt et al. A literature review of electronic portal imaging for radiotherapy dosimetry
JP6754841B2 (en) How to set a geometric model based on medical image data
TWI646945B (en) Deconstruction method of tissue element mass ratio based on medical image and establishment method of geometric model
Fiorina et al. Monte Carlo simulation tool for online treatment monitoring in hadrontherapy with in-beam PET: a patient study
WO2022078175A1 (en) Boron neutron capture therapy system and treatment plan generation method therefor
CN108310677B (en) Smooth geometric model establishing method based on medical image data
Jones et al. Characterization of Compton-scatter imaging with an analytical simulation method
Ferrero et al. Evaluation of in-beam PET treatment verification in proton therapy with different reconstruction methods
Masuda et al. ML-EM algorithm for dose estimation using PET in proton therapy
CN111991711A (en) Parameter monitoring device and system for proton treatment
Lozano et al. Comparison of reconstructed prompt gamma emissions using maximum likelihood estimation and origin ensemble algorithms for a Compton camera system tailored to proton range monitoring
CN112330626A (en) Boron neutron capture treatment dose distribution prediction method based on artificial intelligence and application and device thereof
Rucinski et al. Secondary radiation measurements for particle therapy applications: Charged secondaries produced by 16O ion beams in a PMMA target at large angles
CN112023279A (en) Parameter monitoring device and system for proton treatment
CN114566252A (en) Nuclear medicine activity-dose automatic conversion method based on generation countermeasure network
RU2824926C1 (en) Boron-neutron capture therapy system and method of creating treatment plan therefor
Siebers et al. Monte Carlo simulation of EPIDs
CN116052839B (en) Dose verification method and device based on Cerenkov radiation
Bălan et al. Particle tracking, recognition and LET evaluation of out-of-field proton therapy delivered to a phantom with implants
Tajaldeen Dosimetric impact of organ motion with 4D-CT based treatment planning in lung stereotactic ablative radiotherapy
Huisman Accelerated clinical prompt gamma simulations for proton therapy
Gaitan et al. DESIGN AND METHODOLOGY OF A PROSPECTIVE TRIAL TO IMPROVE THE UNDERSTANDING OF KIDNEY RADIATION DOSE
Antoniou Assessment of Adaptive Radiotherapy Workflows for Head and Neck Cancer
CN115445102A (en) Boron neutron capture treatment method and device

Legal Events

Date Code Title Description
121 Ep: the epo has been informed by wipo that ep was designated in this application

Ref document number: 20937489

Country of ref document: EP

Kind code of ref document: A1

NENP Non-entry into the national phase

Ref country code: DE

122 Ep: pct application non-entry in european phase

Ref document number: 20937489

Country of ref document: EP

Kind code of ref document: A1

32PN Ep: public notification in the ep bulletin as address of the adressee cannot be established

Free format text: NOTING OF LOSS OF RIGHTS PURSUANT TO RULE 112(1) EPC (EPO FORM 1205A DATED 21.06.2023)

122 Ep: pct application non-entry in european phase

Ref document number: 20937489

Country of ref document: EP

Kind code of ref document: A1