WO2015169011A1 - Extra high energy electron beam or photon beam radiotherapy robot system - Google Patents
Extra high energy electron beam or photon beam radiotherapy robot system Download PDFInfo
- Publication number
- WO2015169011A1 WO2015169011A1 PCT/CN2014/085119 CN2014085119W WO2015169011A1 WO 2015169011 A1 WO2015169011 A1 WO 2015169011A1 CN 2014085119 W CN2014085119 W CN 2014085119W WO 2015169011 A1 WO2015169011 A1 WO 2015169011A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- laser
- electron beam
- photon
- robot
- ultra
- Prior art date
Links
- 238000010894 electron beam technology Methods 0.000 title claims abstract description 113
- 238000001959 radiotherapy Methods 0.000 title claims abstract description 43
- 230000006641 stabilisation Effects 0.000 claims abstract description 17
- 238000011105 stabilization Methods 0.000 claims abstract description 17
- 239000007789 gas Substances 0.000 claims description 45
- 230000003287 optical effect Effects 0.000 claims description 12
- 229910052734 helium Inorganic materials 0.000 claims description 7
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 claims description 7
- 230000005855 radiation Effects 0.000 claims description 7
- 239000001307 helium Substances 0.000 claims description 6
- 230000000644 propagated effect Effects 0.000 claims description 5
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 claims description 4
- 239000001257 hydrogen Substances 0.000 claims description 4
- 229910052739 hydrogen Inorganic materials 0.000 claims description 4
- 230000029058 respiratory gaseous exchange Effects 0.000 claims description 2
- 230000000087 stabilizing effect Effects 0.000 claims 1
- 230000006835 compression Effects 0.000 description 17
- 238000007906 compression Methods 0.000 description 17
- 206010028980 Neoplasm Diseases 0.000 description 8
- 238000010586 diagram Methods 0.000 description 7
- 239000006096 absorbing agent Substances 0.000 description 6
- 201000011510 cancer Diseases 0.000 description 6
- 230000000694 effects Effects 0.000 description 6
- 230000005684 electric field Effects 0.000 description 6
- 230000005438 electron bubble Effects 0.000 description 6
- 230000005461 Bremsstrahlung Effects 0.000 description 5
- 230000001133 acceleration Effects 0.000 description 5
- 210000004027 cell Anatomy 0.000 description 5
- 238000006243 chemical reaction Methods 0.000 description 5
- 230000007246 mechanism Effects 0.000 description 5
- 238000000034 method Methods 0.000 description 5
- 238000003491 array Methods 0.000 description 4
- 238000011347 external beam therapy Methods 0.000 description 4
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 3
- 238000005286 illumination Methods 0.000 description 3
- 238000002721 intensity-modulated radiation therapy Methods 0.000 description 3
- 230000008569 process Effects 0.000 description 3
- 238000002560 therapeutic procedure Methods 0.000 description 3
- 210000001519 tissue Anatomy 0.000 description 3
- 238000011455 3D conformal radiation therapy Methods 0.000 description 2
- 230000009286 beneficial effect Effects 0.000 description 2
- 230000005489 elastic deformation Effects 0.000 description 2
- 238000002710 external beam radiation therapy Methods 0.000 description 2
- 238000002513 implantation Methods 0.000 description 2
- 238000002347 injection Methods 0.000 description 2
- 239000007924 injection Substances 0.000 description 2
- 150000002500 ions Chemical class 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 230000035515 penetration Effects 0.000 description 2
- 238000012546 transfer Methods 0.000 description 2
- 238000002729 3-dimensional conformal radiation therapy Methods 0.000 description 1
- 241000238631 Hexapoda Species 0.000 description 1
- 229910052689 Holmium Inorganic materials 0.000 description 1
- 238000000342 Monte Carlo simulation Methods 0.000 description 1
- 206010060862 Prostate cancer Diseases 0.000 description 1
- 208000000236 Prostatic Neoplasms Diseases 0.000 description 1
- UDWPONKAYSRBTJ-UHFFFAOYSA-N [He].[N] Chemical compound [He].[N] UDWPONKAYSRBTJ-UHFFFAOYSA-N 0.000 description 1
- 238000004458 analytical method Methods 0.000 description 1
- 238000005452 bending Methods 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000007812 deficiency Effects 0.000 description 1
- 238000011982 device technology Methods 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 229910001873 dinitrogen Inorganic materials 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 239000011888 foil Substances 0.000 description 1
- 239000003574 free electron Substances 0.000 description 1
- 230000005251 gamma ray Effects 0.000 description 1
- KJZYNXUDTRRSPN-UHFFFAOYSA-N holmium atom Chemical compound [Ho] KJZYNXUDTRRSPN-UHFFFAOYSA-N 0.000 description 1
- 238000003384 imaging method Methods 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 230000003993 interaction Effects 0.000 description 1
- 208000037841 lung tumor Diseases 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 230000005415 magnetization Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 229910001172 neodymium magnet Inorganic materials 0.000 description 1
- 230000007935 neutral effect Effects 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 238000005381 potential energy Methods 0.000 description 1
- 230000000191 radiation effect Effects 0.000 description 1
- 239000000941 radioactive substance Substances 0.000 description 1
- 238000002673 radiosurgery Methods 0.000 description 1
- 229910052761 rare earth metal Inorganic materials 0.000 description 1
- 150000002910 rare earth metals Chemical class 0.000 description 1
- 238000012552 review Methods 0.000 description 1
- 239000011163 secondary particle Substances 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 238000002720 stereotactic body radiation therapy Methods 0.000 description 1
- 230000001225 therapeutic effect Effects 0.000 description 1
- 210000003934 vacuole Anatomy 0.000 description 1
- 238000012795 verification Methods 0.000 description 1
Classifications
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61N—ELECTROTHERAPY; MAGNETOTHERAPY; RADIATION THERAPY; ULTRASOUND THERAPY
- A61N5/00—Radiation therapy
- A61N5/06—Radiation therapy using light
Definitions
- Ultra high energy electron beam or photon beam radiation therapy robot system Ultra high energy electron beam or photon beam radiation therapy robot system
- the present invention relates to an external radiation therapy robot system in the field of new medical device technology, and in particular to a robot system using ultra high energy electron beam or photon beam radiation therapy. Background technique
- Radiation therapy uses high-energy radiation such as X-rays, gamma rays, electrons, protons, heavy ions, and neutrons to destroy the cancer cell's DNA to kill it. Since radiotherapy kills cancer cells while also damaging normal cells, treatment must be carefully planned to minimize this side effect. Radiation for cancer treatment can come from devices outside the body, called external radiation therapy, or from radioactive substances implanted in the body close to cancer cells, known as internal or external radiotherapy. External beam radiation therapy usually uses a photon beam (X-ray or gamma-ray). The electron beam decreases rapidly after a finite distance, and thus does not affect deeper normal tissues.
- Electron beam therapy is commonly used for the treatment of cancer in shallow tumors such as the skin area or in the skin, limbs and other parts of the body. For deeper areas, surgical electron radiation therapy is used. Many types of external radiation therapy use a device called a medical linear accelerator driven by a radio frequency (RF) power amplifier, such as a magnetron or a klystron, to produce an electron beam with an energy of 6-20 MeV.
- RF radio frequency
- external beam radiotherapy can provide an effective three-dimensional dose distribution shape and accurate spatial dose-delivery map through image verification.
- These techniques including three-dimensional conformal radiotherapy (3D-CRT), intensity-modulated radiation therapy (IMRT), image-guided radiotherapy (IGRT), and hadron therapy, enhance radiation doses to tumor areas and reduce specific sensitive areas of surrounding normal tissue. Radiation effects.
- body stereotactic radiotherapy SBRT uses a smaller radiation field and higher in most cases than 3D-CRT. Dose, but more accurately target the target area and shorten the course of treatment.
- a radiotherapy apparatus using X-rays that is, a small linear accelerator is mounted on a multi-joint robot arm or a rotary table, and the position of the robot arm or the rotary table is controlled, thereby generating a small size.
- the X-rays of the grating are concentrated to the center point for illumination.
- ultra-high energy electron beams are significantly better than photon beams in avoiding dose effects on sensitive structures and normal tissues.
- neutron doses such as ultra-high energy electron beams applied to the whole body are one to two orders of magnitude lower than proton beam therapy and photon intensity modulated radiation therapy.
- the ultra-high energy electron beam used in the ultra-high energy electron beam treatment can be generated by a conventional radio frequency-based linear accelerator, including an electronic ejection device, a main acceleration structure called LINAC, an electron beam propagation system, and a final console.
- Electrospray devices are typically comprised of a photocathode microwave electron gun or a thermionic high voltage direct current gun and several bunching chambers for generating an electron beam.
- the LINAC consists of a series of room temperature or superconducting RF cavities with an acceleration gradient of 10 MV/m.
- the electron beam propagation system includes an electron beam focusing and defocusing electric quadrupole magnet.
- the operator station is equipped with a vacuum electron beam propagation system and a series of electron beam bending and focusing electromagnets.
- the overall size of the RF linac is estimated to be about 50 meters long. Together with the return table that can guide the electron beam in multiple directions, the total weight can reach hundreds of tons.
- the cost of construction and operation of such facilities is enormous, which has made it difficult to popularize ultra-high-energy electron beam radiotherapy systems based on conventional accelerators to small-scale hospitals.
- a high-energy electron beam radiation therapy system using a more compact LINAC accelerator and a gantry turret is disclosed in the literature 3, since the principle is still based on a linear accelerator, the structure is still not more compact and compact.
- Literature 2 David H. Whittum, “Microwave Electron Linacs for Oncology", Reviews of Accelerator Science and Technology, pp. 63-92, Vol.2, Iss. l, 2009;
- the ultra high energy electron beam or photon beam radiation therapy robot system of the present invention comprises the following parts: a laser driving system, forming a strong laser pulse; a laser plasma accelerator, the intense laser pulse is directed and focused thereto to generate an electron beam; an electron beam focusing system for directing an electron beam from the laser plasma accelerator to a patient's patient to perform ultra-high energy electrons Beam radiotherapy
- the electron beam from the laser plasma accelerator generates a high energy photon beam for treatment;
- the robot body is provided with a vacuum optical system, and the strong laser pulse is guided and focused to the laser in the vacuum optical system Plasma accelerator
- a laser beam stabilization system monitors the position of the laser beam and corrects their errors in a vacuum optical system.
- the laser driving system comprises:
- the front end is capable of generating low energy laser pulses
- An amplifier chain that amplifies the energy of the low energy laser pulse to form a high energy laser pulse
- a pulse compression chamber that converts the high energy laser pulse into a strong laser pulse
- the laser plasma accelerator comprises:
- a first gas chamber filled with a mixed gas, which is used to generate plasma and electrons by gas;
- the intense laser pulse output by the laser drive system is focused by a spherical mirror or an off-axis parabolic mirror into the laser plasma accelerator.
- the strong laser pulse ionizes the mixed gas in the first chamber to generate plasma and electrons, and the strong laser pulse is in the second gas.
- the chamber continues to generate and accelerate the electrons, and the gas flow control system controls and delivers the gases into the first and second chambers at different pressures, respectively.
- This laser plasma accelerator can efficiently generate ultra-high-energy and high-quality electron beams using a high-acceleration electric field.
- the laser plasma accelerator can generate electron beam energy between l-250 MeV and better between 50-250 MeV.
- the laser plasma accelerator is capable of adjusting the second chamber length to control electron beam energy. More preferably, the bellows structure can be driven by the power element to adjust the second chamber length.
- the laser plasma accelerator is connected to an external transfer chamber, and the electron beam focusing system is mounted in an external transfer chamber of the laser plasma accelerator.
- the electron beam focusing system has means for providing a thin layer pencil beam output. More preferably, the Ministry The piece can be a four-pole permanent magnet array structure.
- the electron beam focusing system is expandable without damaging the vacuum of the laser plasma accelerator.
- the photon beam sighting system comprises a conventional bremsstrahlung conversion target and a collimator, and the electron beam output by the laser plasma accelerator produces a therapeutic high energy photon beam in the photon beam sighting system.
- the electron beam focusing system and the photon beam aiming system are detachable and easy to assemble and replace.
- the robot body has various forms, and may be a multi-joint robot or a parallel robot or a robot turret.
- the robot body can propagate an electron beam or a photon beam from a plurality of directions to a patient's patient site, and can provide a raster scan of the pencil-shaped harness in combination with the treatment bed and the laser beam stabilization system.
- the end of the robot body is provided with an accelerator cavity, and the laser plasma accelerator is installed in the accelerator cavity at the end of the robot body.
- the robot body comprises a base, a rotary table, a rotary drive mechanism, a first rotating shaft, a second rotating shaft, a boom and a third rotating shaft, wherein: the rotary driving mechanism is mounted on the rotary table, thereby realizing the relative rotation of the rotary table
- the base is the rotation of the first rotating shaft; the second rotating shaft connects the rotating table and the arm frame to achieve relative rotation, and the third rotating shaft connects the arm frame and the accelerator cavity to realize the rotation.
- the laser beam stabilization system is arranged along the inner arm frame and the axis of the robot body to monitor the position of the laser beam and correct the error, so that the propagation direction of the strong laser pulse always coincides with the rotation axis of each joint of the robot.
- the laser plasma accelerator, the vacuum optical system, and the laser beam stabilization system are all installed in a vacuum environment, and the inside of the robot body is a hollow vacuum structure, and the vacuum pump system maintains a certain vacuum pressure.
- the duration of the electron beam or photon beam irradiation is controllable from single pulse irradiation to continuous illumination, if it is faster than the breathing interval of the human body, if it is smaller than the heartbeat interval, if it is smaller than the single pulse pulse of the laser driving pulse.
- the width is best.
- the present invention has the following beneficial effects:
- the laser drive system of the present invention produces an energy amplified high energy laser pulse and further forms a strong laser pulse.
- the intense laser pulse is directed inside the robot body having a hollow vacuum structure and focused into a laser plasma accelerator mounted in an accelerator cavity at the end of the robot body to produce an electron beam.
- the electron beam focusing system directs the electron beam to the patient's patient or produces a high-energy photon beam in the photon beam aiming system for ultra-high energy electron beam or photon beam radiation therapy.
- the robot body enables the propagation of electron beams or photon beams from multiple directions to the patient's patient.
- the laser beam stabilization system monitors the position of the laser beam and corrects the error. Compared with the prior art, the present invention has the following beneficial effects:
- Ultra-high-energy electron beam is generated by laser plasma accelerator instead of linear accelerator.
- the volume and quality advantages of laser plasma accelerator make the whole device miniaturized, and the price and installation site layout advantages are obvious;
- Multi-angle illumination and scanning are realized by the robot body, and vacuum propagation of the strong pulse laser is realized by the robot body;
- the ultra high energy electron beam or photon beam radiotherapy robot system of the present invention is more compact, efficient, inexpensive, simpler to operate, and has higher performance than prior art external beam radiation therapy systems.
- FIG. 1a and 1b are schematic diagrams showing the system structure of an embodiment of the present invention.
- Figure 2 is a schematic view of a first air chamber and a second air chamber of the laser plasma accelerator of the system shown in Figures la, lb;
- Figure 3 is a schematic diagram of an electron acceleration mechanism based on a laser wake field
- FIGS. la and 1b are schematic diagrams of a laser plasma accelerator of the ultra high energy electron beam or photon beam radiation therapy robot system shown in Figs. la and 1b, including the first gas chamber and the second gas chamber of Fig. 2;
- FIG. 5 is a schematic view of a miniature quadrupole permanent magnet (PMQ);
- FIG. 6 is a schematic diagram of an electron beam focusing system according to an embodiment of the present invention, which is composed of three quadrupole permanent magnets (PMQ) shown in FIG. 5;
- PMQ quadrupole permanent magnets
- FIG. 7a, 7b are schematic views of a vacuum optical system embedded in the robot body of the ultra high energy electron beam or photon beam radiation therapy robot system shown in Figs.
- FIG. 8 is a schematic diagram of a laser beam stabilization system according to an embodiment of the present invention.
- FIG. 9 is a schematic diagram of an embodiment of a parallel robot according to another embodiment of the present invention.
- 1 is the front end
- 10 is the low energy laser pulse
- 11 is the high energy laser pulse
- 12 is the strong laser pulse
- 13 and 14 are the mirrors
- 15 is the off-axis parabolic mirror
- 2 is the laser drive system
- 21 is the amplifier chain
- 22 is the pulse compression chamber
- 23 is the pulse compression optics.
- 3 is a laser plasma accelerator
- 30 is a gas flow control system
- 31 is a first gas chamber
- 32 is a second gas chamber
- 33 is a mixed gas
- 34 is a pure gas
- 35 is a joint
- 36 is a power component
- 37 is a corrugation Tube structure
- 38 is a multi-degree of freedom adjustment table
- 39 is a laser absorber
- 4 is the electron beam focusing system
- 40 is the outer casing
- 41 is the adapter
- 42 is the magnet array
- 43 and 44 are the four-pole permanent magnets (wedge permanent magnets)
- 45 is the central cavity
- 46 is the outer cavity
- 47 is Bracket
- 48 is a vacuum linear movement system
- 49 is a linear guide;
- 5 is a photon beam aiming system, 51 is a bremsstrahlung conversion target, and 52 is a collimator;
- 6 is the robot body, 60 is the base, 61 is the rotary table, 62 is the rotary drive, 63 is the first rotating shaft, 64 is the second rotating shaft, 65 is the boom, 66 is the third rotating shaft, 67 is the light guiding arm, 68 For the rotary axis, 69 is a parallel drive unit;
- 7 is a laser beam stabilization system, 70 is a laser source, 71 is a calibration beam, 72 is a CCD camera, 73 is a mirror bracket, and 74 is a precision motor;
- 8 is an accelerator cavity, 80 is a vacuum window, 81 is a linear guide, and 82 is a base mechanism;
- 100 is an electron beam
- 101 is a photon beam
- 200 is a patient
- 201 is a treatment bed
- 303 is a fine dotted line
- 304 is a thick dotted line
- 305 is a thick solid line
- 306 is a thin dotted line
- 307 is an electronic vacuole
- 308 is strong
- the longitudinal electric field 309 is the electron trajectory
- 310 is the trajectory.
- the embodiment provides an ultra-high energy electron beam or photon beam radiation therapy robot system, including: a laser driving system 2, a laser plasma accelerator 3, an electron beam focusing system 4, a photon beam aiming system 5, and a robot.
- the body 6 and the laser beam stabilization system 7, the laser drive system 2 produces an energy amplified high energy laser pulse and further forms a strong laser pulse.
- the intense laser pulse is guided inside the robot body 6 having a hollow vacuum structure and focused into a laser plasma accelerator 3 installed in an accelerator chamber at the end of the robot body, thereby generating an electron beam.
- the electron beam focusing system 4 directs the electron beam to the patient's patient, photon beam imaging
- the quasi-system 5 produces a high-energy photon beam by means of an electron beam for ultra-high energy electron beam or photon beam radiation therapy.
- the robot body 6 enables the propagation of electron beams or photon beams from a plurality of directions to a patient's patient.
- the laser beam stabilization system 7 monitors the position of the laser beam and corrects the error.
- the laser drive system 2 includes a front end 1, an amplifier chain 21, a pulse compression chamber 22, and a vacuum pump system 24.
- the front end 1 is used to generate and output a low energy laser pulse 10.
- the low energy laser pulse 10 enters and passes through the amplifier chain 21 to be amplified and forms a high energy laser pulse 11.
- a pulse compression optics 23 is mounted in the pulse compression chamber 22, and the amplified high energy laser pulse 11 is compressed in the pulse compression optics 23 in the time domain.
- the pulse compression chamber 22 is evacuated by a vacuum pump system 24 to maintain a pressure of 10 - 3 - 10 - 4 Pa.
- the strong laser pulse 12 formed by the compression of the pulse compression chamber 22 is propagated to the laser plasma accelerator 3 mounted at the end of the robot body 6.
- the outer casing 29 serves to protect the entire laser drive system 2.
- the pulse compression optics 23 includes a pair of diffraction gratings 25, 26, a vertical reflector 27 and a fixed mirror 28 that combine the various spectral components of the pulse in the time domain.
- the output intense laser pulse 12 generated by the pulse compression optics 23 then has ultra-high energy and ultra-short pulse width, so its energy and pulse width can be further optimized to accelerate the electron beam 100.
- Laser plasma accelerator 3
- the laser plasma accelerator comprises: a first gas chamber filled with a mixed gas; a second gas chamber filled with pure hydrogen or helium; and a gas flow control system.
- the intense laser pulse 12 compressed in the pulse compression chamber 22 is focused by a spherical mirror or an off-axis parabolic mirror 15 at the entrance of the laser plasma accelerator 3.
- the first gas chamber 31, referred to as the injection stage is filled with a mixed gas 33, such as a helium-nitrogen mixed gas composed of 98% helium gas and 2% nitrogen gas.
- the second gas chamber 32, called the acceleration stage is filled with a clean gas 34 such as hydrogen or helium. These gases are propagated through the joint 35 to the laser plasma accelerator 3 at different pressures under the control of the gas flow control system 30, respectively.
- the length of the second plenum 32 can be adjusted by the power element 36 driving the bellows structure 37.
- the laser plasma accelerator 3 is mounted above a multi-degree of freedom adjustment stage 38, such as a commercial Hexapod six-axis precision platform.
- the alignment of the laser plasma accelerator 3 with the intense laser pulse 12 is accomplished by a multi-degree of freedom adjustment stage 38.
- the residual intense laser pulse 12 passing through the laser plasma accelerator 3 is finally absorbed by the laser absorber 39 mounted at the bottom of the multi-degree of freedom adjustment stage 38.
- the intense laser pulse 12 excites a large amplitude plasma wake field, wherein the accelerating electric field captures the plasma inner electrons and induces electrons by ionization.
- the intense laser pulse 12 produces a plasma wake field of the order of 100 GV/m in the second plenum 32.
- the electron beam 100 pre-accelerated in the first gas chamber 31 is further accelerated to the lGeV level in the second gas chamber 32.
- Figure 3 illustrates the physical process of the wake field excitation and the capture and acceleration of electrons in the wake field. This produces a wake field when the strong laser pulse 12 propagates in the neutral mixed gas 33 of the first gas chamber 31.
- the plasma electron density change curve is shown in the upper diagram 301, and the excited longitudinal tail field is shown in the lower portion 302.
- the outer electrons of ⁇ and up to N 5+ are completely ionized at the front of the intense laser pulse 12 having a light intensity of 1.5 x 10 16 W/cm 2 and plasma electrons are formed around the strong laser pulse 12 .
- the boundary of the intense laser pulse 12 is indicated by a thin dotted line 303 in the figure. Since the two inner shell (K-shell) electrons of N 6+ and N 7+ need to be laser ionized with a light intensity higher than 1 X 10 19 ATM 2 , the inner shell electrons only peak at the strong laser pulse 12 Ionization near the light intensity.
- a strong laser with a normalized laser field (a 0 0.
- the intensity map of pulse 12 is indicated by thick dotted line 304.
- the thick solid line 305 indicates the degree of progress of nitrogen ionization along the propagation axis (the number of electrons of the ionized helium atom).
- the boundaries of the plasma region including the inner shell electrons ionized from N 6+ and N 7+ are indicated by thin dashed lines 306.
- the plasma electrons in the boundary of the fine dotted line 303 are pushed away by the radiation pressure (mass dynamic) of the strong laser pulse 12 having a relative intensity of ⁇ >>1, and a narrow electron sheath is formed behind the laser pulse to surround the spherical-like ions.
- the zone also often referred to as electron bubble 307.
- This charge separation produces a strong longitudinal electric field 308 on the order of 100 GV/m with a plasma electron density of 10 18 cm- 3 , which is three orders of magnitude higher than the amplitude of the accelerating electric field of a conventional RF accelerator.
- the electrons are simultaneously subjected to a strong focusing force. Therefore, once the electron beams 100 are captured into the electron cells 307, they are rapidly accelerated to a high energy level of 1 GeV within a length of 1 cm.
- the inner shell electrons ionized from N 6+ and N 7+ are close to the center of the electron bubble, where the wake potential has a maximum value and the laser pulse has the lowest kinetic power.
- the pre-ionized free electron trajectory is mostly a narrow sheath movement along the outside of the electron bubble.
- the electrons ionized from the inner shell layer move closer to the electron bubble axis to the electron bubble tail, where the tail wave potential energy is the smallest, if the electron is obtained With sufficient kinetic energy, they will eventually be captured into the wake field as shown by electron trace 309. However, the electrons shown by trace 310 are off-axis and ionized earlier, and slip away from the potential well will not be captured.
- This mechanism can occur at intensity as low as the light field ionization threshold of the inner shell electrons of the mixed gas, and greatly increases the trapped charge. Since the capture occurs near the bubble axis, the amplitude of the oscillation is reduced after capture compared to the free injection from the electron sheath.
- the electron beam focusing system 4 has means for providing a thin layer of pencil beam output using a four pole permanent magnet array.
- the electron beam 100 output from the laser plasma accelerator 3 is collimated by the four-pole permanent magnet array of the electron beam focusing system 4 and then propagated to the patient of the patient 200 to form a thin-layer pencil beam.
- the electron beam focusing system 4 is mounted in an adapter 41 outside the plasma accelerator 3, and the electron beam focusing system 4 can be expanded and contracted without damaging the vacuum of the plasma accelerator 3.
- Figure 5 shows a four-pole permanent magnet array structure consisting of 12 symmetrically arranged Halbach type quadrupole permanent magnets (PMQ) 43, 44, comprising a central cavity 45 and an outer cavity 46, and a bracket 47 for supporting And positioning.
- PMQ Halbach type quadrupole permanent magnets
- the quadrupole magnetic field is composed of four radial wedge-shaped permanent magnets 43 having a high remanence material, such as Nd 2 FeuB or S m CO, etc., whose magnetization directions are indicated by arrows.
- the external magnetic field closure is formed by an additional eight wedge shaped permanent magnets 44. Since the four main wedge blocks are strongly attracted to the center of the quadrupole, the mechanical position accuracy and magnetic field accuracy must be obtained by inserting the central cavity 45 and the outer cavity 46 of the magnet array 42 with a non-magnetic material precision hollow cylinder.
- the electron beam focusing system 4 includes two or three sets of magnet arrays 42.
- the magnetic field gradient of the two-dimensional Halbach type quadrupole permanent magnet (PMQ) 2 (r, - 1 - ⁇ - 1 ), where is the tip field strength, r, the inner hole radius, r. The outer radius of the PMQ.
- the magnetic field gradient 1160 [77 ] (l-2.5/r. [ ] ).
- two or three sets of magnet arrays 42 mounted in the outer casing 40 of the electron beam focusing system 4 constitute a binary (FD) or triplet (FDF) structure.
- the vacuum linear motion system 48 and the linear guides 49 are both parallel to the longitudinal axis of the electron beam 100 and are fixed inside the outer casing 40, and all of the magnet arrays 42 pass through and are linearly movable along the linear guides 49.
- the number of linear movement systems 48 is the same as the number of magnet arrays 42, and each linear movement system 48 controls only one and a different position of the magnet array 42 along the longitudinal axis of the electron beam 100, which is separately adjusted and optimized by the computer.
- the linear guides 49 ensure the structural alignment and rigidity of the magnet array 42.
- the photon beam sighting system 5 includes a bremsstrahlung conversion target 51 and a collimator 52 installed therein, and the electron beam 101 generated by the laser plasma accelerator 3 is incident on the bremsstrahlung conversion target. 51 and collimator 52 produce photon beam 101.
- the photon beam sighting system 5 and the electron beam focusing system 4 can be disassembled and replaced in a simple manner. Robot body 6 and accelerator cavity 8
- the intense laser pulse 12 from the pulse compression chamber 22 is propagated through the robot body 6 to the accelerator chamber 8 mounted at the end of the robot body 6, and is then focused to the entrance of the laser plasma accelerator 3, ultimately producing an electron beam 100 or a photon beam 101.
- the robot body 6 is capable of manipulating and adjusting the position and posture of the electron beam 100 or the photon beam 101 to effect radiotherapy of the patient 200.
- the robot body 6 can also manipulate the electron beam 100 to achieve fine scanning treatment.
- the laser beam stabilization system 7 is arranged along the inner arm frame and the axis of the robot body 6, so that the propagation direction of the strong laser pulse 12 always coincides with the rotation axis of each joint of the robot.
- the interior of the robot body 6 is a hollow vacuum structure that is evacuated by a vacuum pump system 24 to maintain a pressure of 10 - 3 - 10 - 4 Pa.
- the robot body 6 has various forms.
- Figure la is a schematic view of the robot body 6 using a multi-joint robotic arm.
- Fig. 9 is a schematic view of the robot body 6 realized by a parallel robot.
- the robot body 6 includes a base 60, a turntable 61, a swing drive 62, a first rotating shaft 63, a second rotating shaft 64, a boom 65, and a third rotating shaft 66.
- the slewing drive 62 is mounted on the turntable 61 to effect rotation of the turntable 61 relative to the base 60, i.e., the first rotating shaft 63.
- the second rotating shaft 64 is connected to the rotary table 61 to perform relative rotation with the boom 65, and the third rotating shaft 66 is coupled to the boom 65 and the accelerator chamber 8 for rotation. Both the second shaft 64 and the third shaft 66 take an external drive system similar to 62.
- the number of shafts can be increased or decreased, and the present invention is not limited thereto.
- Figure 9 shows another robot body 6 implemented in parallel robot mode.
- the light guide arm 67 is formed by repeated series connection of the plurality of booms 65 and the rotary shaft 68, and is connected to the pulse compression chamber 22 and the accelerator chamber 8 at both ends of the light guide arm 67 to form an internal hollow vacuum structure that communicates with each other, by a vacuum pump system. 24 Pump to vacuum to maintain a pressure of 10 - 3 -10 - 4 Pa.
- a plurality of parallel drive units 69 are mounted external to the accelerator chamber 8 and can be realized by a power element such as a commercially available electric push rod.
- the position and attitude adjustment of the accelerator chamber 8, that is, the electron beam 100 or the photon number 101, relative to the patient 200 is achieved by controlling the relative length of the parallel drive unit 69.
- the number of the boom 65, the rotary shaft 68, and the parallel drive unit 69 may vary depending on the particular implementation, and the present invention is not limited thereto.
- the accelerator chamber 8 is mounted at the end of the robot body 6. Inside the accelerator chamber 8, there are mainly linear guides 81, a base structure 82, a vacuum window 80, a mirror 14, an off-axis parabolic mirror 15, a laser plasma accelerator 3, a multi-degree-of-freedom adjustment stage 38, and a laser absorber 39.
- the base structure 82 is fixed inside the accelerator chamber 8, and the linear guide 81 is mounted on the base structure 82, thereby preventing the linear guide 81 from being deformed when the accelerator chamber 8 is drawn to a vacuum.
- the mirror 14, the off-axis parabolic mirror 15, the laser plasma accelerator 3, the multi-degree-of-freedom adjustment stage 38 and the laser absorber 39 are mounted coaxially on the linear guide 81 so that the lateral and longitudinal alignment are easy Adjust and ensure accuracy.
- the mirror 14 is located opposite the entrance of the intense pulsed laser 12
- the off-axis parabolic mirror 15 is located at the top of the accelerator chamber 8
- the laser plasma accelerator 3 is mounted above the multi-degree of freedom adjustment stage 38
- the laser absorber 39 is mounted in multiple freedoms.
- the laser plasma accelerator 3 and the multi-degree of freedom adjustment stage 38 and the laser absorber 39 are co-located at the bottom of the accelerator chamber 8, and the intense pulsed laser 12 enters the accelerator chamber 8 and is reflected by the radiation mirror 14 to the off-axis paraboloid.
- the mirror 15 is focused at the entrance of the laser plasma accelerator 3.
- a vacuum window 80 is mounted at the bottom outlet of the accelerator chamber 8 to separate the vacuum optical system and the laser plasma accelerator 3 from the outside air and the patient 200. Because the significant diffusion of the angle will affect beam performance and clinical accuracy, the vacuum window 80 uses a thin foil of low atomic number elements such as helium.
- the alignment of the vacuum optical system due to the movement and elastic deformation of the robot body 6 can be corrected by the laser beam stabilization system 7, as shown in Figs. la and 8.
- the intense laser pulse 12 is transmitted from the fixed mirror 28 to the vacuum optical system composed of the mirrors 13, 14 and the off-axis parabolic mirror 15 in the pulse compression chamber 22, and reaches the entrance of the laser plasma accelerator 3.
- the mirror 13 is used to adjust the propagation direction of the intense pulsed laser 12, and is arranged at an angle of 45 degrees with the propagation axis of the intense pulsed laser 12.
- a laser source 70 such as a holmium laser, provides a calibration beam 71.
- the position of the collimated beam 71 transmitted by each of the mirrors is detected using a CCD camera 72.
- the mirror will pass through two or three precision motors 74, such as piezoelectric, integrated on the mirror holder 73.
- the motor is adjusted to its position and attitude to ensure that the intense pulsed laser 12 can accurately focus on the entrance of the laser plasma accelerator 3, as shown in Figures 7a and 7b. This process of detecting the position of the laser beam on each mirror and then correcting the position and attitude of the corresponding mirror will be repeated until the laser beam position is stabilized.
- different electron beam energies are provided according to specific requirements, for example: 50 MeV, 100 MeV, 150 MeV, 200 MeV and 250 MeV.
- the requirements for electron beam power are determined by the radiotherapy program. For example, the treatment of lOcc lung tumors requires a dose of 100 mega volts electrons in 10 seconds in 1 second. From this it is possible to derive various specific parameter requirements including the wavelength or energy of the intense laser pulse 12 and the laser plasma accelerator 3.
- the content of the present invention is not limited to a specific technical parameter configuration.
Landscapes
- Health & Medical Sciences (AREA)
- Engineering & Computer Science (AREA)
- Biomedical Technology (AREA)
- Pathology (AREA)
- Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
- Radiology & Medical Imaging (AREA)
- Life Sciences & Earth Sciences (AREA)
- Animal Behavior & Ethology (AREA)
- General Health & Medical Sciences (AREA)
- Public Health (AREA)
- Veterinary Medicine (AREA)
- Radiation-Therapy Devices (AREA)
Abstract
Provided in the present invention is an extra high energy electron beam (100) or photon beam (101) radiotherapy robot system, comprising a laser driving system (2), a laser plasma accelerator (3), an electron beam focusing system (4), a photon beam aiming system (5), a robot body (6) and a laser beam stabilization system (7), wherein the laser driving system (2) generates intense laser pulses (12) and spreads same to the laser plasma accelerator (3) installed at the tail end of the robot body (6) to generate electron beams (100); the electron beam focusing system (4) guides the electron beams (100) to diseased parts of a patient (200); the photon beam aiming system (5) enables the electron beams (100) to generate high energy photon beams (101) to perform extra high energy electron beam (100) or photon beam (101) radiotherapy; the robot body (6) spreads the electron beams (100) or the photon beams (101) to the diseased parts of the patient (200) in multiple directions; and the laser beam stabilization system (7) monitors the positions of the laser beams and corrects errors. The extra high energy electron beam (100) or photon beam (101) radiotherapy robot system of the present invention is more compact, more efficient, cheaper and easier to operate, and has a higher performance than an external irradiation radiation therapy system in the prior art.
Description
超高能电子束或光子束放射治疗机器人系统 技术领域 Ultra high energy electron beam or photon beam radiation therapy robot system
本发明涉及一种新型医疗器械技术领域的外放射治疗机器人系统, 具体地, 涉及 一种使用超高能电子束或光子束放射治疗的机器人系统。 背景技术 The present invention relates to an external radiation therapy robot system in the field of new medical device technology, and in particular to a robot system using ultra high energy electron beam or photon beam radiation therapy. Background technique
放射治疗利用高能量辐射如 X射线、 γ射线、 电子、 质子、 重离子和中子来破坏癌 细胞的 DNA以将其杀死。 由于放射治疗在杀死癌细胞的同时也损害正常细胞, 必须仔 细规划治疗以尽量减少这种副作用。 用于癌症治疗的辐射可以来自体外的装置, 被称为 外照射放疗, 也可以来自植入体内靠近癌细胞的放射性物质, 被称为内照射放疗或近距 离放疗。 外照射放疗通常使用光子束 (X射线或 γ射线)。 电子束在有限距离之后剂量 迅速下降, 也因此影响不到较深的正常组织, 电子束治疗通常用于浅层肿瘤如皮肤区域 或全身皮肤、 四肢等部位的癌症治疗。 对于较深的区域, 会采用手术电子放射治疗。 众 多类型的外照射放疗均使用称为医用直线加速器的设备,由射频(RF)功率放大器驱动, 如磁控管或速调管, 产生具有 6-20MeV能量的电子束。 Radiation therapy uses high-energy radiation such as X-rays, gamma rays, electrons, protons, heavy ions, and neutrons to destroy the cancer cell's DNA to kill it. Since radiotherapy kills cancer cells while also damaging normal cells, treatment must be carefully planned to minimize this side effect. Radiation for cancer treatment can come from devices outside the body, called external radiation therapy, or from radioactive substances implanted in the body close to cancer cells, known as internal or external radiotherapy. External beam radiation therapy usually uses a photon beam (X-ray or gamma-ray). The electron beam decreases rapidly after a finite distance, and thus does not affect deeper normal tissues. Electron beam therapy is commonly used for the treatment of cancer in shallow tumors such as the skin area or in the skin, limbs and other parts of the body. For deeper areas, surgical electron radiation therapy is used. Many types of external radiation therapy use a device called a medical linear accelerator driven by a radio frequency (RF) power amplifier, such as a magnetron or a klystron, to produce an electron beam with an energy of 6-20 MeV.
外照射放疗的技术优势可以通过图像验证提供有效的三维剂量分布形状和精确的 空间剂量传递图。 这些技术, 包括三维适形放疗 (3D-CRT)、调强放疗 (IMRT)、 影像引导 放疗 (IGRT)和强子治疗, 加强对肿瘤区域的放射剂量并减少对周围正常组织的特定敏感 区域的放射影响。 凭借复杂的计算软件和先进的治疗设备(包括精密机械臂和紧凑型医 用加速器), 体部立体定向放疗 (SBRT)在绝大多数情况下比 3D-CRT使用更小的辐射场 和更高的剂量, 但更精确地瞄准目标区域并缩短疗程。 The technical advantages of external beam radiotherapy can provide an effective three-dimensional dose distribution shape and accurate spatial dose-delivery map through image verification. These techniques, including three-dimensional conformal radiotherapy (3D-CRT), intensity-modulated radiation therapy (IMRT), image-guided radiotherapy (IGRT), and hadron therapy, enhance radiation doses to tumor areas and reduce specific sensitive areas of surrounding normal tissue. Radiation effects. With sophisticated computing software and advanced treatment equipment (including precision robotic arms and compact medical accelerators), body stereotactic radiotherapy (SBRT) uses a smaller radiation field and higher in most cases than 3D-CRT. Dose, but more accurately target the target area and shorten the course of treatment.
如文献 1、 文献 2中均公开了一种利用 X射线的放射治疗装置, 即把小型直线加速 器安装到多关节机械臂或回转台上, 控制机械臂或者回转台位置姿态, 从而把产生于小 型光栅的 X射线集中到中心点进行照射。 As disclosed in Document 1 and Document 2, a radiotherapy apparatus using X-rays is disclosed, that is, a small linear accelerator is mounted on a multi-joint robot arm or a rotary table, and the position of the robot arm or the rotary table is controlled, thereby generating a small size. The X-rays of the grating are concentrated to the center point for illumination.
然而, 在目前的医用射频直线加速器所产生的上述电子束能级范围下, 最大穿透深 度和横向半影品质都制约了这种先进模式在实际癌症治疗中的应用。一旦电子能级高于 50MeV, 这些问题都可以克服, 穿透深度更加深, 横向半影也更加尖锐, 尽管纵向半影
也有所增加。 Monte Carlo模拟研究中对比了光子, 质子和超高能电子束在调强放疗前 列腺癌症的效果, 最吻合目标剂量的是质子束, 而电子束的目标覆盖范围度是和光子束 的效果相比拟的,有时好过光子束。此外,在避免剂量影响到敏感结构和正常组织方面, 超高能电子束明显好过光子束。至于由轫致辐射和电子核反应相互作用产生的次级粒子 的剂量影响, 如超高能电子束施加于全身的中子剂量低于质子束治疗和光子调强放疗一 到二个数量级。 However, under the above-mentioned range of electron beam levels generated by current medical RF linear accelerators, the maximum penetration depth and lateral penumbra quality all restrict the application of this advanced mode in actual cancer treatment. Once the electronic energy level is higher than 50MeV, these problems can be overcome, the penetration depth is deeper, and the horizontal penumbra is sharper, even though the vertical penumbra Also increased. The Monte Carlo simulation study compared the effects of photon, proton and ultra-high-energy electron beams on intensity-modulated radiotherapy for prostate cancer. The best target dose is the proton beam, and the target coverage of the electron beam is comparable to that of the photon beam. Sometimes better than a photon beam. In addition, ultra-high energy electron beams are significantly better than photon beams in avoiding dose effects on sensitive structures and normal tissues. As for the dose effects of secondary particles produced by the interaction of bremsstrahlung and electron nuclear reactions, neutron doses such as ultra-high energy electron beams applied to the whole body are one to two orders of magnitude lower than proton beam therapy and photon intensity modulated radiation therapy.
所述的超高能电子束治疗使用的超高能电子束,可以由传统的基于射频的直线加速 器产生, 包括一个电子喷射装置, 称作 LINAC的主加速结构, 电子束传播系统, 以及 最终的操作台。 电子喷射装置通常由光阴极微波电子枪或热离子高压直流电枪和几个用 于产生电子束的聚束腔组成。 LINAC 由一系列室温或者超导射频腔体组成, 加速梯度 为 10 MV/m。 电子束传播系统包括电子束聚焦和散焦电四极磁铁。操作台装有真空电子 束传播系统和一系列的电子束弯转和聚焦电磁铁。为实现基于射频直线加速器的外照射 放疗, 射频直线加速器整体尺寸估计要在 50米长左右。 加上能多方向引导电子束的回 转台, 总重量可达上百吨级。 因此, 这类设施的建设和运营成本大到难以置信, 由此导 致基于常规加速器的超高能电子束放疗系统很难普及到小规模医院。虽然文献 3中公开 了一种使用更加紧凑的 LINAC加速器及龙门式转台的超高能电子束放射治疗系统, 但 由于其原理仍然基于直线加速器, 因此结构上还是无法做到更加紧凑小巧。 The ultra-high energy electron beam used in the ultra-high energy electron beam treatment can be generated by a conventional radio frequency-based linear accelerator, including an electronic ejection device, a main acceleration structure called LINAC, an electron beam propagation system, and a final console. . Electrospray devices are typically comprised of a photocathode microwave electron gun or a thermionic high voltage direct current gun and several bunching chambers for generating an electron beam. The LINAC consists of a series of room temperature or superconducting RF cavities with an acceleration gradient of 10 MV/m. The electron beam propagation system includes an electron beam focusing and defocusing electric quadrupole magnet. The operator station is equipped with a vacuum electron beam propagation system and a series of electron beam bending and focusing electromagnets. In order to achieve external beam radiotherapy based on RF linacs, the overall size of the RF linac is estimated to be about 50 meters long. Together with the return table that can guide the electron beam in multiple directions, the total weight can reach hundreds of tons. As a result, the cost of construction and operation of such facilities is unbelievable, which has made it difficult to popularize ultra-high-energy electron beam radiotherapy systems based on conventional accelerators to small-scale hospitals. Although a high-energy electron beam radiation therapy system using a more compact LINAC accelerator and a gantry turret is disclosed in the literature 3, since the principle is still based on a linear accelerator, the structure is still not more compact and compact.
文献 1: Adler Jr Jr, Chang SD, Murphy MJ, Doty J, Geis P and Hancock SL, "The Cyberknife: a frameless robotic system for radiosurgery", Stereotactic Functional Neurosurgery, pp.124-128, 69(1-4 Pt 2), 1997; Document 1: Adler Jr Jr, Chang SD, Murphy MJ, Doty J, Geis P and Hancock SL, "The Cyberknife: a frameless robotic system for radiosurgery", Stereotactic Functional Neurosurgery, pp.124-128, 69 (1-4 Pt 2), 1997;
文献 2: David H. Whittum, "Microwave Electron Linacs for Oncology", Reviews of Accelerator Science and Technology, pp.63-92, Vol.2, Iss. l, 2009; Literature 2: David H. Whittum, "Microwave Electron Linacs for Oncology", Reviews of Accelerator Science and Technology, pp. 63-92, Vol.2, Iss. l, 2009;
文献 3: U.S. patent application No. 13/765,017, filed on Feb. 12, 2013, entitled PLURIDIRECTIONAL VERY HIGH ELECTRON ENERGY RADIATION THERAPY SYSTEMS AND PROCESSES, Pub. No. US 20130231516 Al ; 发明内容 Document 3: US patent application No. 13/765,017, filed on Feb. 12, 2013, entitled PLURIDIRECTIONAL VERY HIGH ELECTRON ENERGY RADIATION THERAPY SYSTEMS AND PROCESSES, Pub. No. US 20130231516 Al ;
针对现有技术中的缺陷,本发明的目的是提供一种使用超高能电子束或光子束进 行外放射治疗的机器人系统。 In view of the deficiencies in the prior art, it is an object of the present invention to provide a robotic system for performing external radiation therapy using an ultra-high energy electron beam or a photon beam.
本发明所述的超高能电子束或光子束放射治疗机器人系统, 包括以下部分: 激光驱动系统, 形成强激光脉冲;
激光等离子体加速器, 所述的强激光脉冲被引导并聚焦到此从而产生电子束; 电子束聚焦系统, 用于将来自激光等离子体加速器的电子束导向到患者病患处, 从 而进行超高能电子束放疗; The ultra high energy electron beam or photon beam radiation therapy robot system of the present invention comprises the following parts: a laser driving system, forming a strong laser pulse; a laser plasma accelerator, the intense laser pulse is directed and focused thereto to generate an electron beam; an electron beam focusing system for directing an electron beam from the laser plasma accelerator to a patient's patient to perform ultra-high energy electrons Beam radiotherapy
光子束瞄准系统, 将来自激光等离子体加速器的电子束产生治疗用的高能光子束; 机器人本体, 其内设有真空光学系统, 所述强激光脉冲在真空光学系统中被引导并 聚焦到上述激光等离子体加速器; a photon beam aiming system, the electron beam from the laser plasma accelerator generates a high energy photon beam for treatment; the robot body is provided with a vacuum optical system, and the strong laser pulse is guided and focused to the laser in the vacuum optical system Plasma accelerator
激光束稳定系统, 在真空光学系统中监控激光束位置并纠正它们的误差。 优选地, 所述激光驱动系统, 包括: A laser beam stabilization system monitors the position of the laser beam and corrects their errors in a vacuum optical system. Preferably, the laser driving system comprises:
前端, 能够产生低能激光脉冲; The front end is capable of generating low energy laser pulses;
放大器链, 放大上述低能激光脉冲的能量形成高能激光脉冲; An amplifier chain that amplifies the energy of the low energy laser pulse to form a high energy laser pulse;
脉冲压缩室, 将所述高能激光脉冲转换为强激光脉冲; a pulse compression chamber that converts the high energy laser pulse into a strong laser pulse;
真空泵系统, 保持脉冲压缩室、 机器人本体的内部以及加速器腔的真空压力。 优选地, 所述激光等离子体加速器包括: The vacuum pump system maintains the pulse compression chamber, the interior of the robot body, and the vacuum pressure of the accelerator chamber. Preferably, the laser plasma accelerator comprises:
充有混合气体的第一气室, 用来电离气体产生等离子体和电子; a first gas chamber filled with a mixed gas, which is used to generate plasma and electrons by gas;
充有纯净氢气或氦气的第二气室, 用来加速电子; a second chamber filled with pure hydrogen or helium to accelerate the electrons;
气体流量控制系统; Gas flow control system;
激光驱动系统输出的强激光脉冲由球面反射镜或离轴抛物面反射镜聚焦后进入激 光等离子体加速器, 强激光脉冲在第一气室电离混合气体产生等离子体和电子、 强激光 脉冲在第二气室继续产生并加速电子,气体流量控制系统分别以不同的压力控制并输送 气体进入第一气室和第二气室中。 The intense laser pulse output by the laser drive system is focused by a spherical mirror or an off-axis parabolic mirror into the laser plasma accelerator. The strong laser pulse ionizes the mixed gas in the first chamber to generate plasma and electrons, and the strong laser pulse is in the second gas. The chamber continues to generate and accelerate the electrons, and the gas flow control system controls and delivers the gases into the first and second chambers at different pressures, respectively.
这种激光等离子体加速器可以利用高加速电场高效的产生超高能高品质电子束。所 述的激光等离子体加速器能够产生的电子束能量应在 l-250MeV之间, 50-250MeV之间 更好。 This laser plasma accelerator can efficiently generate ultra-high-energy and high-quality electron beams using a high-acceleration electric field. The laser plasma accelerator can generate electron beam energy between l-250 MeV and better between 50-250 MeV.
优选地, 所述激光等离子体加速器能调整第二气室长度以控制电子束能量。 更优选 地, 可以由动力元件驱动波纹管结构来调整第二气室长度。 Preferably, the laser plasma accelerator is capable of adjusting the second chamber length to control electron beam energy. More preferably, the bellows structure can be driven by the power element to adjust the second chamber length.
优选地, 所述激光等离子体加速器连接有外部转接室, 电子束聚焦系统安装在激光 等离子体加速器的外部转接室中。 Preferably, the laser plasma accelerator is connected to an external transfer chamber, and the electron beam focusing system is mounted in an external transfer chamber of the laser plasma accelerator.
优选地, 所述电子束聚焦系统具有提供薄层笔形波束输出的部件。 更优选地, 该部
件可以采用四极永磁铁阵列结构。 Preferably, the electron beam focusing system has means for providing a thin layer pencil beam output. More preferably, the Ministry The piece can be a four-pole permanent magnet array structure.
优选地,所述电子束聚焦系统在不破坏激光等离子体加速器的真空情况下可进行伸 缩。 Preferably, the electron beam focusing system is expandable without damaging the vacuum of the laser plasma accelerator.
优选地, 所述光子束瞄准系统, 包括常规的轫致辐射转换靶和准直器, 激光等离子 体加速器输出的电子束在光子束瞄准系统中产生治疗用的高能光子束。所述电子束聚焦 系统和光子束瞄准系统为可拆卸安装方式, 方便拆装和更换使用。 Preferably, the photon beam sighting system comprises a conventional bremsstrahlung conversion target and a collimator, and the electron beam output by the laser plasma accelerator produces a therapeutic high energy photon beam in the photon beam sighting system. The electron beam focusing system and the photon beam aiming system are detachable and easy to assemble and replace.
优选地, 所述机器人本体, 其具有多种形态, 可以是多关节机械臂或并联机器人或 机器人转台。所述机器人本体可以从多个方向向患者病患部位传播电子束或光子束, 并 能够结合治疗床和激光束稳定系统, 提供笔形线束的光栅扫描。 Preferably, the robot body has various forms, and may be a multi-joint robot or a parallel robot or a robot turret. The robot body can propagate an electron beam or a photon beam from a plurality of directions to a patient's patient site, and can provide a raster scan of the pencil-shaped harness in combination with the treatment bed and the laser beam stabilization system.
优选地, 所述机器人本体末端设有加速器腔, 激光等离子体加速器安装于机器人本 体末端的加速器腔内。 Preferably, the end of the robot body is provided with an accelerator cavity, and the laser plasma accelerator is installed in the accelerator cavity at the end of the robot body.
更优选地, 所述机器人本体包括基座、 回转台、 回转驱动机构、 第一转轴、 第二 转轴、 臂架和第三转轴, 其中: 回转驱动机构安装在回转台上, 从而实现回转台相对于 基座即第一转轴的转动; 第二转轴连接回转台与臂架实现相对转动, 第三转轴连接臂架 与加速器腔实现转动。 More preferably, the robot body comprises a base, a rotary table, a rotary drive mechanism, a first rotating shaft, a second rotating shaft, a boom and a third rotating shaft, wherein: the rotary driving mechanism is mounted on the rotary table, thereby realizing the relative rotation of the rotary table The base is the rotation of the first rotating shaft; the second rotating shaft connects the rotating table and the arm frame to achieve relative rotation, and the third rotating shaft connects the arm frame and the accelerator cavity to realize the rotation.
优选地, 所述激光束稳定系统沿机器人本体内部臂架及轴线布置, 用以监控激光束 位置并纠正误差, 使得强激光脉冲的传播方向始终与机器人各个关节的转动轴线重合。 Preferably, the laser beam stabilization system is arranged along the inner arm frame and the axis of the robot body to monitor the position of the laser beam and correct the error, so that the propagation direction of the strong laser pulse always coincides with the rotation axis of each joint of the robot.
优选地, 所述的激光等离子体加速器、 真空光学系统、 激光束稳定系统均安装 在真空环境中, 并且所述的机器人本体内部为中空真空结构, 由真空泵系统保持其 一定的真空压力。 Preferably, the laser plasma accelerator, the vacuum optical system, and the laser beam stabilization system are all installed in a vacuum environment, and the inside of the robot body is a hollow vacuum structure, and the vacuum pump system maintains a certain vacuum pressure.
优选地, 电子束或光子束放射照射的时长从单脉冲照射到连续照射可控, 如果快于 人体的呼吸间隔则比较好, 如果小于心跳间隔则更好, 如果小于激光驱动脉冲的单个脉 冲脉宽则最好。 Preferably, the duration of the electron beam or photon beam irradiation is controllable from single pulse irradiation to continuous illumination, if it is faster than the breathing interval of the human body, if it is smaller than the heartbeat interval, if it is smaller than the single pulse pulse of the laser driving pulse. The width is best.
与现有技术相比, 本发明具有如下的有益效果: Compared with the prior art, the present invention has the following beneficial effects:
本发明激光驱动系统产生能量放大的高能激光脉冲并进一步形成强激光脉冲。 该强激光脉冲沿具有中空真空结构的机器人本体内部被引导并聚焦到安装在机器 人本体末端的加速器腔内的激光等离子体加速器中, 从而产生电子束。 电子束聚焦 系统把电子束导向到患者病患处, 或在光子束瞄准系统中产生高能光子束, 从而进 行超高能电子束或光子束放射治疗。 机器人本体实现从多个方向向患者病患处传播 电子束或光子束。 激光束稳定系统监控激光束位置并纠正误差。
与现有技术相比, 本发明具有以下有益效果: The laser drive system of the present invention produces an energy amplified high energy laser pulse and further forms a strong laser pulse. The intense laser pulse is directed inside the robot body having a hollow vacuum structure and focused into a laser plasma accelerator mounted in an accelerator cavity at the end of the robot body to produce an electron beam. The electron beam focusing system directs the electron beam to the patient's patient or produces a high-energy photon beam in the photon beam aiming system for ultra-high energy electron beam or photon beam radiation therapy. The robot body enables the propagation of electron beams or photon beams from multiple directions to the patient's patient. The laser beam stabilization system monitors the position of the laser beam and corrects the error. Compared with the prior art, the present invention has the following beneficial effects:
1.通过激光等离子体加速器而不是直线加速器 LINAC产生超高能电子束,激光 等离子体加速器的体积和质量优势使得设备整体小型化, 价格和安装场地布置优势 很明显; 1. Ultra-high-energy electron beam is generated by laser plasma accelerator instead of linear accelerator. The volume and quality advantages of laser plasma accelerator make the whole device miniaturized, and the price and installation site layout advantages are obvious;
2.通过机器人本体实现多角度照射和扫描, 通过机器人本体实现强脉冲激光的 真空传播; 2. Multi-angle illumination and scanning are realized by the robot body, and vacuum propagation of the strong pulse laser is realized by the robot body;
3.可以简易更换为通过电子束或者光子束进行治疗; 3. Can be easily replaced by treatment with electron beam or photon beam;
本发明的超高能电子束或光子束放射治疗机器人系统更紧凑、 高效、廉价, 操作更 简单, 比现有技术的外照射放疗系统具有更高性能。 附图说明 The ultra high energy electron beam or photon beam radiotherapy robot system of the present invention is more compact, efficient, inexpensive, simpler to operate, and has higher performance than prior art external beam radiation therapy systems. DRAWINGS
通过阅读参照以下附图对非限制性实施例所作的详细描述, 本发明的其它特 征、 目的和优点将会变得更明显: Other features, objects, and advantages of the present invention will become more apparent from the Detailed Description of Description
图 la、 lb为本发明一实施例系统结构示意图; 1a and 1b are schematic diagrams showing the system structure of an embodiment of the present invention;
图 2为图 la、 lb所示的系统的激光等离子体加速器的第一气室和第二气室的示意 图; Figure 2 is a schematic view of a first air chamber and a second air chamber of the laser plasma accelerator of the system shown in Figures la, lb;
图 3为基于激光尾波场的电子加速机制示意图; Figure 3 is a schematic diagram of an electron acceleration mechanism based on a laser wake field;
图 4a、 4b为图 la、 lb所示的超高能电子束或光子束放射治疗机器人系统的激光等 离子体加速器的示意图, 包括图 2中的第一气室和第二气室; 4a, 4b are schematic diagrams of a laser plasma accelerator of the ultra high energy electron beam or photon beam radiation therapy robot system shown in Figs. la and 1b, including the first gas chamber and the second gas chamber of Fig. 2;
图 5为微型四极永磁铁 (PMQ) 的示意图; Figure 5 is a schematic view of a miniature quadrupole permanent magnet (PMQ);
图 6为本发明实施例的电子束聚焦系统的示意图, 由三个图 5 所示的四极永磁铁 (PMQ) 组成; 6 is a schematic diagram of an electron beam focusing system according to an embodiment of the present invention, which is composed of three quadrupole permanent magnets (PMQ) shown in FIG. 5;
图 7a、 7b为嵌入于图 la、 lb所示的超高能电子束或光子束放射治疗机器人系统的 机器人本体中的真空光学系统的示意图; 7a, 7b are schematic views of a vacuum optical system embedded in the robot body of the ultra high energy electron beam or photon beam radiation therapy robot system shown in Figs.
图 8为本发明一实施例的激光束稳定系统的示意图; FIG. 8 is a schematic diagram of a laser beam stabilization system according to an embodiment of the present invention; FIG.
图 9为本发明另一实施例通过并联机器人的实施例示意图。 FIG. 9 is a schematic diagram of an embodiment of a parallel robot according to another embodiment of the present invention.
上述图中: In the above picture:
1 为前端, 10为低能激光脉冲, 11 为高能激光脉冲, 12为强激光脉冲, 13、 14为反射镜, 15为离轴抛物面反射镜; 1 is the front end, 10 is the low energy laser pulse, 11 is the high energy laser pulse, 12 is the strong laser pulse, 13 and 14 are the mirrors, and 15 is the off-axis parabolic mirror;
2为激光驱动系统, 21 为放大器链, 22为脉冲压缩室, 23 为脉冲压缩光学器
件, 24为真空泵系统, 25、 26为衍射光栅, 27为垂直发射器, 28为固定反射镜, 29 为外壳; 2 is the laser drive system, 21 is the amplifier chain, 22 is the pulse compression chamber, and 23 is the pulse compression optics. 24, vacuum pump system, 25, 26 for the diffraction grating, 27 for the vertical transmitter, 28 for the fixed mirror, 29 for the outer casing;
3为激光等离子体加速器, 30为气体流量控制系统, 31为第一气室, 32为第二气 室, 33为混合气体, 34为纯净气体, 35为接头, 36为动力元件, 37为波纹管结构, 38 为多自由度调整台, 39为激光吸收器; 3 is a laser plasma accelerator, 30 is a gas flow control system, 31 is a first gas chamber, 32 is a second gas chamber, 33 is a mixed gas, 34 is a pure gas, 35 is a joint, 36 is a power component, 37 is a corrugation Tube structure, 38 is a multi-degree of freedom adjustment table, 39 is a laser absorber;
4为电子束聚焦系统, 40为外壳, 41为转接器, 42为磁铁阵列, 43、 44为四极 永磁铁 (楔形永磁铁), 45为中心空腔, 46为外空腔, 47为支架, 48为真空直线移动系 统, 49为直线导轨; 4 is the electron beam focusing system, 40 is the outer casing, 41 is the adapter, 42 is the magnet array, 43 and 44 are the four-pole permanent magnets (wedge permanent magnets), 45 is the central cavity, 46 is the outer cavity, 47 is Bracket, 48 is a vacuum linear movement system, and 49 is a linear guide;
5为光子束瞄准系统, 51为轫致辐射转换靶, 52为准直器; 5 is a photon beam aiming system, 51 is a bremsstrahlung conversion target, and 52 is a collimator;
6为机器人本体, 60为基座, 61为回转台, 62为回转驱动, 63为第一转轴, 64 为第二转轴, 65为臂架, 66为第三转轴, 67为导光臂, 68为回转轴, 69为并联驱动单 元; 6 is the robot body, 60 is the base, 61 is the rotary table, 62 is the rotary drive, 63 is the first rotating shaft, 64 is the second rotating shaft, 65 is the boom, 66 is the third rotating shaft, 67 is the light guiding arm, 68 For the rotary axis, 69 is a parallel drive unit;
7为激光束稳定系统, 70为激光源, 71为校准光束, 72为 CCD摄像头, 73为反 射镜支架, 74为精密电机; 7 is a laser beam stabilization system, 70 is a laser source, 71 is a calibration beam, 72 is a CCD camera, 73 is a mirror bracket, and 74 is a precision motor;
8为加速器腔, 80为真空窗, 81为直线导轨, 82为基座机构; 8 is an accelerator cavity, 80 is a vacuum window, 81 is a linear guide, and 82 is a base mechanism;
100为电子束, 101为光子束, 200为患者, 201为治疗床, 303为细点线, 304为 粗点线, 305为粗实线, 306为细虚线, 307为电子空泡, 308为强纵向电场, 309为电 子轨迹, 310为轨迹。 具体实施方式 100 is an electron beam, 101 is a photon beam, 200 is a patient, 201 is a treatment bed, 303 is a fine dotted line, 304 is a thick dotted line, 305 is a thick solid line, 306 is a thin dotted line, 307 is an electronic vacuole, 308 is strong The longitudinal electric field, 309 is the electron trajectory, and 310 is the trajectory. detailed description
下面结合具体实施例对本发明进行详细说明。 以下实施例将有助于本领域的技术人 员进一步理解本发明, 但不以任何形式限制本发明。 应当指出的是, 对本领域的普通技 术人员来说, 在不脱离本发明构思的前提下, 还可以做出若干变形和改进。 这些都属于 本发明的保护范围。 The invention will now be described in detail in connection with specific embodiments. The following examples are intended to further understand the present invention by those skilled in the art, but are not intended to limit the invention in any way. It should be noted that a number of variations and modifications may be made by those skilled in the art without departing from the inventive concept. These are all within the scope of protection of the present invention.
如图 l a所示, 本实施例提供一种超高能电子束或光子束放射治疗机器人系统, 包括: 激光驱动系统 2、 激光等离子体加速器 3、 电子束聚焦系统 4、 光子束瞄准系 统 5、 机器人本体 6和激光束稳定系统 7, 激光驱动系统 2产生能量放大的高能激 光脉冲并进一步形成强激光脉冲。 该强激光脉冲沿具有中空真空结构的机器人本体 6 内部被引导并聚焦到安装在机器人本体末端的加速器腔内的激光等离子体加速器 3 中, 从而产生电子束。 电子束聚焦系统 4把电子束导向到患者病患处, 光子束瞄
准系统 5通过电子束产生高能光子束, 从而进行超高能电子束或光子束放射治疗。 机器人本体 6实现从多个方向向患者病患处传播电子束或光子束。 激光束稳定系统 7监控激光束位置并纠正误差。 以下对涉及的各个部分进行详细说明。 激光驱动系统 2 As shown in FIG. 1A, the embodiment provides an ultra-high energy electron beam or photon beam radiation therapy robot system, including: a laser driving system 2, a laser plasma accelerator 3, an electron beam focusing system 4, a photon beam aiming system 5, and a robot. The body 6 and the laser beam stabilization system 7, the laser drive system 2 produces an energy amplified high energy laser pulse and further forms a strong laser pulse. The intense laser pulse is guided inside the robot body 6 having a hollow vacuum structure and focused into a laser plasma accelerator 3 installed in an accelerator chamber at the end of the robot body, thereby generating an electron beam. The electron beam focusing system 4 directs the electron beam to the patient's patient, photon beam imaging The quasi-system 5 produces a high-energy photon beam by means of an electron beam for ultra-high energy electron beam or photon beam radiation therapy. The robot body 6 enables the propagation of electron beams or photon beams from a plurality of directions to a patient's patient. The laser beam stabilization system 7 monitors the position of the laser beam and corrects the error. The various parts involved are described in detail below. Laser drive system 2
如图 1所示, 所述激光驱动系统 2包括前端 1, 放大器链 21, 脉冲压缩室 22, 真空 泵系统 24。 前端 1用于产生并输出低能激光脉冲 10。 低能激光脉冲 10进入并通过放大 器链 21从而被放大并形成高能激光脉冲 11。脉冲压缩室 22中安装有脉冲压缩光学器件 23, 放大的高能激光脉冲 11在脉冲压缩光学器件 23 中在时域上压缩。 脉冲压缩室 22 由真空泵系统 24抽至真空, 以保持为 10—3-10—4Pa的压力。 经过脉冲压缩室 22压缩后形 成的强激光脉冲 12传播到安装在所述机器人本体 6末端的所述激光等离子体加速器 3 里。 外壳 29用来保护整个激光驱动系统 2。 As shown in FIG. 1, the laser drive system 2 includes a front end 1, an amplifier chain 21, a pulse compression chamber 22, and a vacuum pump system 24. The front end 1 is used to generate and output a low energy laser pulse 10. The low energy laser pulse 10 enters and passes through the amplifier chain 21 to be amplified and forms a high energy laser pulse 11. A pulse compression optics 23 is mounted in the pulse compression chamber 22, and the amplified high energy laser pulse 11 is compressed in the pulse compression optics 23 in the time domain. The pulse compression chamber 22 is evacuated by a vacuum pump system 24 to maintain a pressure of 10 - 3 - 10 - 4 Pa. The strong laser pulse 12 formed by the compression of the pulse compression chamber 22 is propagated to the laser plasma accelerator 3 mounted at the end of the robot body 6. The outer casing 29 serves to protect the entire laser drive system 2.
所述脉冲压缩光学器件 23包括一对衍射光栅 25、 26, 一个垂直反射器 27和一个固 定反射镜 28, 在时域上把脉冲的各种频谱分量组合在一起。 产生于脉冲压缩光学器件 23的输出强激光脉冲 12于是具有超高能量和超短脉宽, 因此其能量和脉宽可以进一步 优化来加速电子束 100。 激光等离子体加速器 3 The pulse compression optics 23 includes a pair of diffraction gratings 25, 26, a vertical reflector 27 and a fixed mirror 28 that combine the various spectral components of the pulse in the time domain. The output intense laser pulse 12 generated by the pulse compression optics 23 then has ultra-high energy and ultra-short pulse width, so its energy and pulse width can be further optimized to accelerate the electron beam 100. Laser plasma accelerator 3
如图 la、 图 2和图 4a所示, 所述激光等离子体加速器包括: 充有混合气体的第一 气室; 充有纯净氢气或氦气的第二气室; 气体流量控制系统。 As shown in Figures la, 2 and 4a, the laser plasma accelerator comprises: a first gas chamber filled with a mixed gas; a second gas chamber filled with pure hydrogen or helium; and a gas flow control system.
在脉冲压缩室 22压缩的强激光脉冲 12在激光等离子体加速器 3的入口由球面反射 镜或离轴抛物面反射镜 15聚焦。被称作注入级的第一气室 31填充有混和气体 33,例如 由 98%氦气和 2%氮气组成的氦氮混合气体。被称作加速级的第二气室 32填充有如氢气 或氦气的纯净气体 34。 这些气体在气体流量控制系统 30的控制下分别以不同的压力通 过接头 35传播到激光等离子体加速器 3。第二气室 32的长度可由动力元件 36驱动波纹 管结构 37来调整。 The intense laser pulse 12 compressed in the pulse compression chamber 22 is focused by a spherical mirror or an off-axis parabolic mirror 15 at the entrance of the laser plasma accelerator 3. The first gas chamber 31, referred to as the injection stage, is filled with a mixed gas 33, such as a helium-nitrogen mixed gas composed of 98% helium gas and 2% nitrogen gas. The second gas chamber 32, called the acceleration stage, is filled with a clean gas 34 such as hydrogen or helium. These gases are propagated through the joint 35 to the laser plasma accelerator 3 at different pressures under the control of the gas flow control system 30, respectively. The length of the second plenum 32 can be adjusted by the power element 36 driving the bellows structure 37.
如图 4a所示, 激光等离子体加速器 3安装在多自由度调整台 38上方, 例如商品化 的 Hexapod六轴精密平台。 激光等离子体加速器 3与强激光脉冲 12的位姿对准通过多 自由度调整台 38来完成。穿过激光等离子体加速器 3的残余的强激光脉冲 12最后被安 装在多自由度调整台 38底部的激光吸收器 39吸收。
如图 2和图 4a所示, 在第一气室 31中, 所述的强激光脉冲 12激发大振幅等离子 体尾波场, 其中的加速电场可以捕获等离子体内层电子并用电离诱导注入加速电子。 强 激光脉冲 12在第二气室 32中产生 100GV/m量级的等离子体尾波场。在第一气室 31中 预加速的电子束 100在第二气室 32中被进一步加速到 lGeV级别。 As shown in Figure 4a, the laser plasma accelerator 3 is mounted above a multi-degree of freedom adjustment stage 38, such as a commercial Hexapod six-axis precision platform. The alignment of the laser plasma accelerator 3 with the intense laser pulse 12 is accomplished by a multi-degree of freedom adjustment stage 38. The residual intense laser pulse 12 passing through the laser plasma accelerator 3 is finally absorbed by the laser absorber 39 mounted at the bottom of the multi-degree of freedom adjustment stage 38. As shown in Figures 2 and 4a, in the first plenum 31, the intense laser pulse 12 excites a large amplitude plasma wake field, wherein the accelerating electric field captures the plasma inner electrons and induces electrons by ionization. The intense laser pulse 12 produces a plasma wake field of the order of 100 GV/m in the second plenum 32. The electron beam 100 pre-accelerated in the first gas chamber 31 is further accelerated to the lGeV level in the second gas chamber 32.
图 3说明了尾波场激发和在尾波场中捕获并加速电子的物理过程 300。 当强激光脉 冲 12在第一气室 31的中性混合气体 33中传播时该产生尾波场。 图 3中, 等离子体电 子密度变化曲线表示在上部的图 301中, 激发的纵向尾场表示在下部 302中。 Figure 3 illustrates the physical process of the wake field excitation and the capture and acceleration of electrons in the wake field. This produces a wake field when the strong laser pulse 12 propagates in the neutral mixed gas 33 of the first gas chamber 31. In Fig. 3, the plasma electron density change curve is shown in the upper diagram 301, and the excited longitudinal tail field is shown in the lower portion 302.
如图 3中部的 300所示, 氦和直到 N5+的外层电子在光强为 1.5 x l016W/cm2的强激 光脉冲 12前沿完全电离并在强激光脉冲 12外围形成等离子体电子, 强激光脉冲 12的 边界在图中用细点线 303表示。 由于 N6+和 N7+的两个内壳层 (K壳层) 电子需要用光 强高于 1 X 1019 A™2的激光电离,因此内壳层电子仅在强激光脉冲 12的峰值光强附近电 离。具有归一化激光场(a0 0.855 x l0-9/1/2[f A™2 [ ^]=2,其中 /[f A™2]为光强, 为激光波长) 的强激光脉冲 12的强度图用粗点线 304表示。 在图上部的 301中, 粗实 线 305表示沿传播轴的氮电离进展程度(已电离的氦原子的电子数量)。包括电离自 N6+ 和 N7+的内壳层电子的等离子区域的边界用细虚线 306表示。 As shown by 300 in the middle of Fig. 3, the outer electrons of 氦 and up to N 5+ are completely ionized at the front of the intense laser pulse 12 having a light intensity of 1.5 x 10 16 W/cm 2 and plasma electrons are formed around the strong laser pulse 12 . The boundary of the intense laser pulse 12 is indicated by a thin dotted line 303 in the figure. Since the two inner shell (K-shell) electrons of N 6+ and N 7+ need to be laser ionized with a light intensity higher than 1 X 10 19 ATM 2 , the inner shell electrons only peak at the strong laser pulse 12 Ionization near the light intensity. A strong laser with a normalized laser field (a 0 0. 855 x l0- 9 / 1/2 [f ATM 2 [ ^] = 2 , where /[f ATM 2 ] is the light intensity, the laser wavelength) The intensity map of pulse 12 is indicated by thick dotted line 304. In the upper portion of the figure 301, the thick solid line 305 indicates the degree of progress of nitrogen ionization along the propagation axis (the number of electrons of the ionized helium atom). The boundaries of the plasma region including the inner shell electrons ionized from N 6+ and N 7+ are indicated by thin dashed lines 306.
在细点线 303边界内的等离子体电子被相对强度为 ^>>1的强激光脉冲 12的辐射 压力 (有质动力) 推开, 并在激光脉冲后面形成一个窄电子鞘包围着类球形的离子区, 也经常被称作电子空泡 307。 这种电荷分离产生 100GV/m量级的强纵向电场 308, 等离 子体电子密度为 1018cm—3, 比常规的射频加速器的加速电场在幅值上高三个数量级。 在 电子空泡 307中, 电子同时承受着强聚焦力。 因此, 一旦电子束 100被捕获到电子空泡 307中, 它们会被迅速的在 1cm的长度内加速到 lGeV级别的高能。 The plasma electrons in the boundary of the fine dotted line 303 are pushed away by the radiation pressure (mass dynamic) of the strong laser pulse 12 having a relative intensity of ^>>1, and a narrow electron sheath is formed behind the laser pulse to surround the spherical-like ions. The zone, also often referred to as electron bubble 307. This charge separation produces a strong longitudinal electric field 308 on the order of 100 GV/m with a plasma electron density of 10 18 cm- 3 , which is three orders of magnitude higher than the amplitude of the accelerating electric field of a conventional RF accelerator. In the electron bubble 307, the electrons are simultaneously subjected to a strong focusing force. Therefore, once the electron beams 100 are captured into the electron cells 307, they are rapidly accelerated to a high energy level of 1 GeV within a length of 1 cm.
所述的电离自 N6+和 N7+的内壳层电子靠近电子空泡中心, 在这里尾波势能具有最 大值, 激光脉冲的有质动力最小。 预电离的自由电子的轨迹多是沿电子空泡外部的窄鞘 运动, 相反地, 电离自内壳层的电子靠近电子空泡轴移动到电子空泡尾部, 那里尾波势 能最小,如果电子获得足够的动能,它们最后将被捕获进尾波场,如电子轨迹 309所示。 但是轨迹 310所示的电子, 偏离轴向并且电离较早, 会滑离势阱不会被捕获。 这个被称 作电离诱导注入的机制在强度低至混和气体的内壳层电子的光场电离阈值时均可发生, 并且极大的增加捕获电荷。 由于捕获发生在靠近空泡轴附近, 相比于源自电子鞘的自由 注入, 振荡的幅度在捕获后有所降低。 参考电离诱导注入的理论分析, 为了捕获在激光 电场的峰值处电离的电子, 最小的激光强度必须为 1- ≤0.64 , 其中 ^ = (1 1/2为
洛仑兹因子, 为等离子体尾波的相速度。 为使电子在激光包络前端被捕获, 强度必须 a0≥\ .23 , 此时 ^ = 33。 电子束聚焦系统 4和光子束瞄准系统 5 The inner shell electrons ionized from N 6+ and N 7+ are close to the center of the electron bubble, where the wake potential has a maximum value and the laser pulse has the lowest kinetic power. The pre-ionized free electron trajectory is mostly a narrow sheath movement along the outside of the electron bubble. Conversely, the electrons ionized from the inner shell layer move closer to the electron bubble axis to the electron bubble tail, where the tail wave potential energy is the smallest, if the electron is obtained With sufficient kinetic energy, they will eventually be captured into the wake field as shown by electron trace 309. However, the electrons shown by trace 310 are off-axis and ionized earlier, and slip away from the potential well will not be captured. This mechanism, known as ionization-induced implantation, can occur at intensity as low as the light field ionization threshold of the inner shell electrons of the mixed gas, and greatly increases the trapped charge. Since the capture occurs near the bubble axis, the amplitude of the oscillation is reduced after capture compared to the free injection from the electron sheath. Theoretical analysis of reference ionization induced implantation, in order to capture electrons ionized at the peak of the laser electric field, the minimum laser intensity must be 1- ≤ 0.64, where ^ = (1 1/2 is The Lorentz factor is the phase velocity of the plasma wake. In order for the electron to be captured at the front end of the laser envelope, the intensity must be a 0 ≥ \ .23, at this time ^ = 33. Electron beam focusing system 4 and photon beam aiming system 5
如图 la和图 4a所示, 所述电子束聚焦系统 4具有提供薄层笔形波束输出的部件, 该部件采用四极永磁铁阵列。从激光等离子体加速器 3输出的电子束 100通过电子束聚 焦系统 4的四极永磁铁阵列准直后传播至患者 200的病患处, 形成薄层笔形波束。 该电 子束聚焦系统 4安装在等离子体加速器 3外部的转接器 41中, 电子束聚焦系统 4在不 破坏等离子体加速器 3的真空情况下可进行伸缩。 As shown in Figures la and 4a, the electron beam focusing system 4 has means for providing a thin layer of pencil beam output using a four pole permanent magnet array. The electron beam 100 output from the laser plasma accelerator 3 is collimated by the four-pole permanent magnet array of the electron beam focusing system 4 and then propagated to the patient of the patient 200 to form a thin-layer pencil beam. The electron beam focusing system 4 is mounted in an adapter 41 outside the plasma accelerator 3, and the electron beam focusing system 4 can be expanded and contracted without damaging the vacuum of the plasma accelerator 3.
图 5展示四极永磁铁阵列结构, 由 12块对称布置的 Halbach型四极永磁铁(PMQ ) 43、 44组成磁铁阵列 42, 包括中心空腔 45和外空腔 46, 以及支架 47用于支撑和定位。 Figure 5 shows a four-pole permanent magnet array structure consisting of 12 symmetrically arranged Halbach type quadrupole permanent magnets (PMQ) 43, 44, comprising a central cavity 45 and an outer cavity 46, and a bracket 47 for supporting And positioning.
四极磁场是由四个具有高剩磁材料的径向楔形永磁铁 43 组成, 其如 Nd2FeuB或 SmCO等, 其磁化方向由箭头表示。外磁场闭合由另外八个楔形永磁铁 44形成。 由于四 个主要楔形块被强烈吸向四极中心, 必须借由非磁材料精密空心圆柱插入磁铁阵列 42 的中心空腔 45和外空腔 46来获得机械位置精度和磁场准确性。 The quadrupole magnetic field is composed of four radial wedge-shaped permanent magnets 43 having a high remanence material, such as Nd 2 FeuB or S m CO, etc., whose magnetization directions are indicated by arrows. The external magnetic field closure is formed by an additional eight wedge shaped permanent magnets 44. Since the four main wedge blocks are strongly attracted to the center of the quadrupole, the mechanical position accuracy and magnetic field accuracy must be obtained by inserting the central cavity 45 and the outer cavity 46 of the magnet array 42 with a non-magnetic material precision hollow cylinder.
如图 6所示,电子束聚焦系统 4包括两或三组磁铁阵列 42。如图 5所示,二维 Halbach 型四极永磁铁 (PMQ ) 的磁场梯度为 =2 (r,—1-^—1), 其中 为尖端场强度, r,为内孔 半径, r。为 PMQ的外半径。 对于 PM为 N50级的钕铁硼型稀土磁铁 (N ¾145) , 如果 βΓ=1.45Γ且 r尸 2.5mm, 可得磁场梯度为 =1160[77 ](l-2.5/r。[ ])。 As shown in FIG. 6, the electron beam focusing system 4 includes two or three sets of magnet arrays 42. As shown in Fig. 5, the magnetic field gradient of the two-dimensional Halbach type quadrupole permanent magnet (PMQ) is =2 (r, - 1 -^- 1 ), where is the tip field strength, r, the inner hole radius, r. The outer radius of the PMQ. For NdFeB rare earth magnets with a mass of N50 (N 3⁄4 14 5), if β Γ = 1.45 Γ and r corp. 2.5 mm, the magnetic field gradient is = 1160 [77 ] (l-2.5/r. [ ] ).
如图 6所示, 安装在电子束聚焦系统 4外壳 40内的两或三组磁铁阵列 42, 组成双 元组 (FD ) 或三元组 (FDF ) 结构。 真空直线移动系统 48与直线导轨 49均与电子束 100纵轴向平行且都固定在外壳 40内部,所有磁铁阵列 42均穿过并且可以沿直线导轨 49直线移动。 直线移动系统 48的数量与磁铁阵列 42的数量一致, 并且每个直线移动 系统 48只控制一个且不同的磁铁阵列 42沿电子束 100纵轴向的位置, 由计算机分别 调整并优化。 直线导轨 49保证磁铁阵列 42的结构对齐及刚度。 As shown in Fig. 6, two or three sets of magnet arrays 42 mounted in the outer casing 40 of the electron beam focusing system 4 constitute a binary (FD) or triplet (FDF) structure. The vacuum linear motion system 48 and the linear guides 49 are both parallel to the longitudinal axis of the electron beam 100 and are fixed inside the outer casing 40, and all of the magnet arrays 42 pass through and are linearly movable along the linear guides 49. The number of linear movement systems 48 is the same as the number of magnet arrays 42, and each linear movement system 48 controls only one and a different position of the magnet array 42 along the longitudinal axis of the electron beam 100, which is separately adjusted and optimized by the computer. The linear guides 49 ensure the structural alignment and rigidity of the magnet array 42.
如图 lb和图 4b所示, 光子束瞄准系统 5包括安装在其内部的轫致辐射转换靶 51 和准直器 52, 由激光等离子体加速器 3产生的电子束 101入射到轫致辐射转换靶 51和 准直器 52产生光子束 101。光子束瞄准系统 5与电子束聚焦系统 4可以通过简易方式拆 装并更换使用。
机器人本体 6和加速器腔 8 As shown in FIGS. 1b and 4b, the photon beam sighting system 5 includes a bremsstrahlung conversion target 51 and a collimator 52 installed therein, and the electron beam 101 generated by the laser plasma accelerator 3 is incident on the bremsstrahlung conversion target. 51 and collimator 52 produce photon beam 101. The photon beam sighting system 5 and the electron beam focusing system 4 can be disassembled and replaced in a simple manner. Robot body 6 and accelerator cavity 8
来自脉冲压缩室 22的强激光脉冲 12通过机器人本体 6传播至安装在机器人本体 6 末端的加速器腔 8中, 进而聚焦到激光等离子体加速器 3的入口, 最终产生电子束 100 或光子束 101。 机器人本体 6能够操控并调整电子束 100或光子束 101的位置及姿态实 现对患者 200的放射性治疗。 同时, 在治疗床 201的运动配合下, 机器人本体 6也能够 操控所述电子束 100实现精细扫描治疗。 The intense laser pulse 12 from the pulse compression chamber 22 is propagated through the robot body 6 to the accelerator chamber 8 mounted at the end of the robot body 6, and is then focused to the entrance of the laser plasma accelerator 3, ultimately producing an electron beam 100 or a photon beam 101. The robot body 6 is capable of manipulating and adjusting the position and posture of the electron beam 100 or the photon beam 101 to effect radiotherapy of the patient 200. At the same time, under the motion cooperation of the treatment bed 201, the robot body 6 can also manipulate the electron beam 100 to achieve fine scanning treatment.
激光束稳定系统 7沿机器人本体 6内部臂架及轴线布置, 使得强激光脉冲 12的传 播方向始终与机器人各个关节的转动轴线重合。 机器人本体 6的内部为中空真空结构, 由真空泵系统 24抽至真空, 以保持为 10—3-10—4Pa的压力。 The laser beam stabilization system 7 is arranged along the inner arm frame and the axis of the robot body 6, so that the propagation direction of the strong laser pulse 12 always coincides with the rotation axis of each joint of the robot. The interior of the robot body 6 is a hollow vacuum structure that is evacuated by a vacuum pump system 24 to maintain a pressure of 10 - 3 - 10 - 4 Pa.
机器人本体 6具有多种形态。 图 la是使用多关节机械臂实现机器人本体 6的示意 图。 图 9是通过并联机器人方式实现机器人本体 6的示意图。 The robot body 6 has various forms. Figure la is a schematic view of the robot body 6 using a multi-joint robotic arm. Fig. 9 is a schematic view of the robot body 6 realized by a parallel robot.
如图 la所示, 所述的机器人本体 6包括基座 60, 回转台 61, 回转驱动 62, 第一转 轴 63, 第二转轴 64, 臂架 65, 第三转轴 66。 其中回转驱动 62安装在回转台 61上, 实 现回转台 61相对于基座 60也就是第一转轴 63的转动。 第二转轴 64连接回转台 61与 臂架 65实现相对转动, 第三转轴 66连接臂架 65与加速器腔 8实现转动。 第二转轴 64 与第三转轴 66都采取外置的类似 62的驱动系统。 根据具体实现, 转轴的数量可以增加 或减少, 本发明内容并不局限于此。 As shown in FIG. la, the robot body 6 includes a base 60, a turntable 61, a swing drive 62, a first rotating shaft 63, a second rotating shaft 64, a boom 65, and a third rotating shaft 66. The slewing drive 62 is mounted on the turntable 61 to effect rotation of the turntable 61 relative to the base 60, i.e., the first rotating shaft 63. The second rotating shaft 64 is connected to the rotary table 61 to perform relative rotation with the boom 65, and the third rotating shaft 66 is coupled to the boom 65 and the accelerator chamber 8 for rotation. Both the second shaft 64 and the third shaft 66 take an external drive system similar to 62. Depending on the implementation, the number of shafts can be increased or decreased, and the present invention is not limited thereto.
图 9显示另一种并联机器人方式实现的机器人本体 6。 通过多个臂架 65和回转轴 68的反复串联形成导光臂 67, 并在导光臂 67两端分别与脉冲压缩室 22和加速器腔 8 连接形成彼此连通的内部中空真空结构, 由真空泵系统 24 抽至真空, 以保持为 10—3-10—4Pa的压力。多个并联驱动单元 69安装在加速器腔 8外部,可以通过商品化的电 动推杆等动力元件进行实现。 通过控制并联驱动单元 69的相对长度实现对加速器腔 8, 也就是电子束 100或光子数 101, 相对于患者 200的位置及姿态调整。 根据具体实现, 臂架 65, 回转轴 68, 以及并联驱动单元 69的数量可以不同,本发明内容并不局限于此。 Figure 9 shows another robot body 6 implemented in parallel robot mode. The light guide arm 67 is formed by repeated series connection of the plurality of booms 65 and the rotary shaft 68, and is connected to the pulse compression chamber 22 and the accelerator chamber 8 at both ends of the light guide arm 67 to form an internal hollow vacuum structure that communicates with each other, by a vacuum pump system. 24 Pump to vacuum to maintain a pressure of 10 - 3 -10 - 4 Pa. A plurality of parallel drive units 69 are mounted external to the accelerator chamber 8 and can be realized by a power element such as a commercially available electric push rod. The position and attitude adjustment of the accelerator chamber 8, that is, the electron beam 100 or the photon number 101, relative to the patient 200 is achieved by controlling the relative length of the parallel drive unit 69. The number of the boom 65, the rotary shaft 68, and the parallel drive unit 69 may vary depending on the particular implementation, and the present invention is not limited thereto.
如图 la和图 4a所示, 加速器腔 8安装在机器人本体 6的末端。 加速器腔 8内部主 要有直线导轨 81, 基座结构 82, 真空窗 80, 反射镜 14, 离轴抛物面反射镜 15, 激光等 离子体加速器 3, 多自由度调整台 38和激光吸收器 39。 其中基座结构 82固定在加速器 腔 8内部, 直线导轨 81安装在基座结构 82上, 由此防止直线导轨 81在加速器腔 8抽 至真空时变形。 反射镜 14, 离轴抛物面反射镜 15, 激光等离子体加速器 3, 多自由度调 整台 38和激光吸收器 39均同轴方式安装在直线导轨 81上, 使得横向和纵向对齐容易
调节并确保精度。其中反射镜 14位于强脉冲激光 12的入口对面,离轴抛物面反射镜 15 位于加速器腔 8的顶部, 激光等离子体加速器 3安装在多自由度调整台 38的上方, 激 光吸收器 39安装在多自由度调整台 38的底部,激光等离子体加速器 3和多自由度调整 台 38以及激光吸收器 39共同位于加速器腔 8的底部, 强脉冲激光 12进入加速器腔 8 后由放射镜 14反射到离轴抛物面反射镜 15并在激光等离子体加速器 3的入口处聚焦。 真空窗 80安装在加速器腔 8底部出口, 以把真空光学系统和激光等离子体加速器 3相 对于外部空气和患者 200分隔开。 因为角度的明显扩散将影响光束性能和临床准确度, 真空窗 80使用例如铍等低原子序数元素的薄箔。 激光束稳定系统 7 As shown in FIGS. 1a and 4a, the accelerator chamber 8 is mounted at the end of the robot body 6. Inside the accelerator chamber 8, there are mainly linear guides 81, a base structure 82, a vacuum window 80, a mirror 14, an off-axis parabolic mirror 15, a laser plasma accelerator 3, a multi-degree-of-freedom adjustment stage 38, and a laser absorber 39. The base structure 82 is fixed inside the accelerator chamber 8, and the linear guide 81 is mounted on the base structure 82, thereby preventing the linear guide 81 from being deformed when the accelerator chamber 8 is drawn to a vacuum. The mirror 14, the off-axis parabolic mirror 15, the laser plasma accelerator 3, the multi-degree-of-freedom adjustment stage 38 and the laser absorber 39 are mounted coaxially on the linear guide 81 so that the lateral and longitudinal alignment are easy Adjust and ensure accuracy. Wherein the mirror 14 is located opposite the entrance of the intense pulsed laser 12, the off-axis parabolic mirror 15 is located at the top of the accelerator chamber 8, the laser plasma accelerator 3 is mounted above the multi-degree of freedom adjustment stage 38, and the laser absorber 39 is mounted in multiple freedoms. At the bottom of the adjustment stage 38, the laser plasma accelerator 3 and the multi-degree of freedom adjustment stage 38 and the laser absorber 39 are co-located at the bottom of the accelerator chamber 8, and the intense pulsed laser 12 enters the accelerator chamber 8 and is reflected by the radiation mirror 14 to the off-axis paraboloid. The mirror 15 is focused at the entrance of the laser plasma accelerator 3. A vacuum window 80 is mounted at the bottom outlet of the accelerator chamber 8 to separate the vacuum optical system and the laser plasma accelerator 3 from the outside air and the patient 200. Because the significant diffusion of the angle will affect beam performance and clinical accuracy, the vacuum window 80 uses a thin foil of low atomic number elements such as helium. Laser beam stabilization system 7
由于机器人本体 6的运动和弹性形变导致的真空光学系统的偏准可通过激光束稳定 系统 7进行纠正, 如图 la和图 8所示。 强激光脉冲 12在脉冲压缩室 22内从固定反射 镜 28传输到由反射镜 13、 14和离轴抛物面反射镜 15等组成的真空光学系统后到达激 光等离子体加速器 3的入口。 反射镜 13用于调整强脉冲激光 12的传播方向, 与强脉冲 激光 12的传播轴成 45度角布置。例如氦氖激光的激光源 70提供校准光束 71。使用 CCD 摄像头 72检测各个反射镜透射出来的校准光束 71的位置。 通常, 一旦机器人本体 6的 运动或弹性形变导致校准光束 71在某个反射镜处有位移, 该反射镜将会通过集成在反 射镜支架 73上的两个或三个精密电机 74,例如压电电机,来调整其自身的位置和姿态, 以保证强脉冲激光 12能够准确的对焦到激光等离子体加速器 3的入口, 如图 7a和 7b 所示。这个检测激光束在每个反射镜上的位置然后校正相应反射镜的位置和姿态的过程 将一直被重复直至激光束位置稳定。 The alignment of the vacuum optical system due to the movement and elastic deformation of the robot body 6 can be corrected by the laser beam stabilization system 7, as shown in Figs. la and 8. The intense laser pulse 12 is transmitted from the fixed mirror 28 to the vacuum optical system composed of the mirrors 13, 14 and the off-axis parabolic mirror 15 in the pulse compression chamber 22, and reaches the entrance of the laser plasma accelerator 3. The mirror 13 is used to adjust the propagation direction of the intense pulsed laser 12, and is arranged at an angle of 45 degrees with the propagation axis of the intense pulsed laser 12. A laser source 70, such as a holmium laser, provides a calibration beam 71. The position of the collimated beam 71 transmitted by each of the mirrors is detected using a CCD camera 72. Generally, once the motion or elastic deformation of the robot body 6 causes the calibration beam 71 to be displaced at a certain mirror, the mirror will pass through two or three precision motors 74, such as piezoelectric, integrated on the mirror holder 73. The motor is adjusted to its position and attitude to ensure that the intense pulsed laser 12 can accurately focus on the entrance of the laser plasma accelerator 3, as shown in Figures 7a and 7b. This process of detecting the position of the laser beam on each mirror and then correcting the position and attitude of the corresponding mirror will be repeated until the laser beam position is stabilized.
在本发明的激光等离子体加速器驱动的超高能电子束或光子束放射治疗机器人系 统的具体实施例中, 根据具体要求, 提供了不同电子束能量, 例如: 50兆电子伏、 100 兆电子伏、 150兆电子伏、 200兆电子伏和 250兆电子伏。 电子束电量的要求是由放射 治疗计划决定的, 例如, lOcc肺肿瘤的治疗需要 100兆电子伏电子在 1秒内 10戈瑞的 剂量。 由此可以推算出包括强激光脉冲 12 的波长或能量, 以及激光等离子体加速器 3 在内的各种具体参数要求。 本发明内容并不局限于具体的技术参数配置。 In a specific embodiment of the ultra-high energy electron beam or photon beam radiotherapy robot system driven by the laser plasma accelerator of the present invention, different electron beam energies are provided according to specific requirements, for example: 50 MeV, 100 MeV, 150 MeV, 200 MeV and 250 MeV. The requirements for electron beam power are determined by the radiotherapy program. For example, the treatment of lOcc lung tumors requires a dose of 100 mega volts electrons in 10 seconds in 1 second. From this it is possible to derive various specific parameter requirements including the wavelength or energy of the intense laser pulse 12 and the laser plasma accelerator 3. The content of the present invention is not limited to a specific technical parameter configuration.
以上对本发明的具体实施例进行了描述。 需要理解的是, 本发明并不局限于上 述特定实施方式, 本领域技术人员可以在权利要求的范围内做出各种变形或修改, 这并不影响本发明的实质内容。
The specific embodiments of the present invention have been described above. It is to be understood that the invention is not limited to the specific embodiments described above, and various modifications and changes may be made by those skilled in the art without departing from the scope of the invention.
Claims
1、 一种超高能电子束或光子束放射治疗机器人系统, 其特征在于, 包括以下部分: 激光驱动系统, 形成强激光脉冲; 1. An ultra-high-energy electron beam or photon beam radiotherapy robot system, characterized by including the following parts: a laser drive system to form strong laser pulses;
激光等离子体加速器,激光驱动系统产生的强激光脉冲被引导并聚焦到激光等离子 体加速器, 从而产生电子束; Laser plasma accelerator, the intense laser pulse generated by the laser drive system is guided and focused to the laser plasma accelerator, thereby generating an electron beam;
电子束聚焦系统, 用于将来自激光等离子体加速器的电子束导向到患者病患处, 从 而进行超高能电子束放疗; The electron beam focusing system is used to guide the electron beam from the laser plasma accelerator to the patient's site to perform ultra-high-energy electron beam radiotherapy;
光子束瞄准系统,用于把来自激光等离子体加速器的电子束产生治疗用的高能光子 束; Photon beam aiming system for converting electron beams from laser plasma accelerators into high-energy photon beams for treatment;
机器人本体, 其内设有真空光学系统, 所述强激光脉冲在真空光学系统中被引导并 聚焦到上述激光等离子体加速器; The robot body is equipped with a vacuum optical system, and the strong laser pulse is guided and focused into the above-mentioned laser plasma accelerator in the vacuum optical system;
激光束稳定系统, 在真空光学系统中监控激光束位置并纠正它们的误差。 Laser beam stabilization system monitors laser beam positions and corrects their errors in vacuum optical systems.
2、 根据权利要求 1所述的一种超高能电子束或光子束放射治疗机器人系统, 其特 征在于, 所述激光等离子体加速器包括: 2. An ultra-high-energy electron beam or photon beam radiotherapy robot system according to claim 1, characterized in that the laser plasma accelerator includes:
充有混合气体的第一气室, 用来电离气体产生等离子体和电子; The first gas chamber filled with mixed gas is used to ionize the gas to generate plasma and electrons;
充有纯净氢气或氦气的第二气室, 用来加速电子; A second gas chamber filled with pure hydrogen or helium to accelerate electrons;
气体流量控制系统; Gas flow control system;
激光驱动系统输出的强激光脉冲由球面反射镜或离轴抛物面反射镜聚焦后进入激 光等离子体加速器, 强激光脉冲在第一气室电离混合气体产生等离子体和电子、 强激光 脉冲在第二气室继续产生并加速电子,气体流量控制系统分别以不同的压力控制并输送 气体进入第一气室和第二气室中。 The strong laser pulse output from the laser drive system is focused by a spherical mirror or an off-axis parabolic mirror and then enters the laser plasma accelerator. The strong laser pulse ionizes the mixed gas in the first gas chamber to generate plasma and electrons. The strong laser pulse ionizes the mixed gas in the first gas chamber to generate plasma and electrons. The chamber continues to generate and accelerate electrons, and the gas flow control system controls and delivers gas into the first gas chamber and the second gas chamber respectively at different pressures.
3、 根据权利要求 2所述的一种超高能电子束或光子束放射治疗机器人系统, 其特 征在于,所述激光等离子体加速器的第二气室长度由动力元件驱动波纹管结构来调整以 控制电子束能量。 3. An ultra-high-energy electron beam or photon beam radiotherapy robot system according to claim 2, characterized in that the length of the second air chamber of the laser plasma accelerator is adjusted and controlled by a power element driving a bellows structure. Electron beam energy.
4、 根据权利要求 1-3任一项所述的一种超高能电子束或光子束放射治疗机器人系 统, 其特征在于, 所述激光等离子体加速器的位姿对准通过多自由度调整台来完成。 4. An ultra-high-energy electron beam or photon beam radiotherapy robot system according to any one of claims 1 to 3, characterized in that the posture alignment of the laser plasma accelerator is achieved through a multi-degree-of-freedom adjustment table. Finish.
5、 根据权利要求 1所述的一种超高能电子束或光子束放射治疗机器人系统, 其特 征在于, 所述电子束聚焦系统具有提供薄层笔形波束输出的四极永磁铁阵列结构。 5. An ultra-high-energy electron beam or photon beam radiotherapy robot system according to claim 1, characterized in that the electron beam focusing system has a four-pole permanent magnet array structure that provides thin-layer pencil beam output.
6、 根据权利要求 1或 5所述的一种超高能电子束或光子束放射治疗机器人系统,
其特征在于, 所述电子束聚焦系统在不破坏等离子体加速器的真空情况下可进行伸缩。 6. An ultra-high-energy electron beam or photon beam radiotherapy robot system according to claim 1 or 5, It is characterized in that the electron beam focusing system can be expanded and retracted without destroying the vacuum of the plasma accelerator.
7、 根据权利要求 6所述的一种超高能电子束或光子束放射治疗机器人系统, 其特 征在于, 所述电子束聚焦系统和光子束瞄准系统为可拆卸安装方式, 方便拆装和更换使 用。 7. An ultra-high-energy electron beam or photon beam radiotherapy robot system according to claim 6, characterized in that the electron beam focusing system and the photon beam aiming system are detachable and easy to disassemble and replace. .
8、 根据权利要求 1所述的一种超高能电子束或光子束放射治疗机器人系统, 其特 征在于, 所述机器人本体末端设有加速器腔, 激光等离子体加速器安装于加速器腔内, 来自激光驱动系统的强激光脉冲通过机器人本体传播至加速器腔中,进而聚焦到激光等 离子体加速器的入口, 最终产生电子束或光子束。 8. An ultra-high-energy electron beam or photon beam radiotherapy robot system according to claim 1, characterized in that an accelerator cavity is provided at the end of the robot body, and a laser plasma accelerator is installed in the accelerator cavity, driven by the laser The strong laser pulse of the system is propagated into the accelerator cavity through the robot body, and then focused to the entrance of the laser plasma accelerator, ultimately producing an electron beam or photon beam.
9、 根据权利要求 1或 8所述的一种超高能电子束或光子束放射治疗机器人系统, 其特征在于, 所述机器人本体是多关节机械臂或并联机器人或机器人转台, 所述机器人 本体可以从多个方向向患者病患部位传播电子束或光子束, 并能够结合治疗床和激光束 稳定系统, 提供笔形线束的光栅扫描。 9. An ultra-high-energy electron beam or photon beam radiotherapy robot system according to claim 1 or 8, characterized in that the robot body is a multi-joint mechanical arm or a parallel robot or a robot turntable, and the robot body can Propagates an electron or photon beam to the patient's site from multiple directions and can be combined with a treatment table and laser beam stabilization system to provide raster scanning of a pencil beam.
10、根据权利要求 1-3任一项所述的一种超高能电子束或光子束放射治疗机器人系 统, 其特征在于, 所述激光束稳定系统沿机器人本体内部臂架及轴线布置, 用以监控激 光束位置并纠正误差, 使得强激光脉冲的传播方向始终与机器人各个关节的转动轴线重 合。 10. An ultra-high-energy electron beam or photon beam radiotherapy robot system according to any one of claims 1 to 3, characterized in that the laser beam stabilizing system is arranged along the internal arm frame and axis of the robot body to Monitor the position of the laser beam and correct the error so that the propagation direction of the strong laser pulse always coincides with the rotation axis of each joint of the robot.
11、 根据权利要求 1-3任一项所述的一种超高能电子束或光子束放射治疗机器人系 统, 其特征在于, 所述的激光等离子体加速器、 真空光学系统、 激光束稳定系统均 安装在真空环境中, 并且所述的机器人本体内部为中空真空结构, 由真空泵系统保 持其一定的真空压力。 11. An ultra-high-energy electron beam or photon beam radiotherapy robot system according to any one of claims 1 to 3, characterized in that the laser plasma accelerator, vacuum optical system, and laser beam stabilization system are all installed In a vacuum environment, and the inside of the robot body is a hollow vacuum structure, a certain vacuum pressure is maintained by the vacuum pump system.
12、根据权利要求 1-3任一项所述的一种超高能电子束或光子束放射治疗机器人系 统, 其特征在于, 电子束或光子束放射照射的时长从单脉冲照射到连续照射可控, 该时 长快于人体的呼吸间隔, 或者小于心跳间隔, 或者小于激光驱动脉冲的单个脉冲脉宽。
12. An ultra-high-energy electron beam or photon beam radiation therapy robot system according to any one of claims 1 to 3, characterized in that the duration of electron beam or photon beam radiation irradiation is controllable from single pulse irradiation to continuous irradiation. , this duration is faster than the breathing interval of the human body, or shorter than the heartbeat interval, or shorter than the single pulse width of the laser driving pulse.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201410191339.4 | 2014-05-07 | ||
CN201410191339.4A CN104001270B (en) | 2014-05-07 | 2014-05-07 | Extrahigh energy electron beam or photon beam radiation treatment robot system |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2015169011A1 true WO2015169011A1 (en) | 2015-11-12 |
Family
ID=51362350
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/CN2014/085119 WO2015169011A1 (en) | 2014-05-07 | 2014-08-25 | Extra high energy electron beam or photon beam radiotherapy robot system |
Country Status (2)
Country | Link |
---|---|
CN (1) | CN104001270B (en) |
WO (1) | WO2015169011A1 (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
LT6816B (en) | 2019-10-03 | 2021-05-10 | Valstybinis mokslinių tyrimų institutas Fizinių ir technologijos mokslų centras | Laser-driven high-dose-rate generating device of ionizing radiation |
US11013100B2 (en) | 2016-10-10 | 2021-05-18 | University Of Strathclyde | Plasma accelerator |
EP3749065A4 (en) * | 2019-03-27 | 2021-09-01 | Huazhong University of Science and Technology | Electron radiation system |
US11483919B2 (en) | 2019-03-27 | 2022-10-25 | Huazhong University Of Science And Technology | System of electron irradiation |
Families Citing this family (31)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104873345A (en) * | 2015-04-26 | 2015-09-02 | 王颖 | Partial laser therapy bed for dermatological departments |
CN105148412B (en) * | 2015-09-09 | 2019-01-11 | 上海联影医疗科技有限公司 | Target optimization method and imaging system is imaged |
CN105288865B (en) * | 2015-11-10 | 2018-05-18 | 康健 | Skin laser treatment auxiliary robot and its householder method |
US9855445B2 (en) | 2016-04-01 | 2018-01-02 | Varian Medical Systems, Inc. | Radiation therapy systems and methods for delivering doses to a target volume |
CN106669050A (en) * | 2017-03-08 | 2017-05-17 | 中国科学院上海应用物理研究所 | Compact rotating frame |
CN110650778A (en) * | 2017-03-24 | 2020-01-03 | 加利福尼亚大学董事会 | System and method for delivering radiation therapy |
CN107185111A (en) * | 2017-07-19 | 2017-09-22 | 烟台海灵健康科技有限公司 | Intelligent plasma physiotherapy equipment |
US11590364B2 (en) | 2017-07-21 | 2023-02-28 | Varian Medical Systems International Ag | Material inserts for radiation therapy |
US11712579B2 (en) | 2017-07-21 | 2023-08-01 | Varian Medical Systems, Inc. | Range compensators for radiation therapy |
US10843011B2 (en) | 2017-07-21 | 2020-11-24 | Varian Medical Systems, Inc. | Particle beam gun control systems and methods |
US10092774B1 (en) | 2017-07-21 | 2018-10-09 | Varian Medical Systems International, AG | Dose aspects of radiation therapy planning and treatment |
US10549117B2 (en) | 2017-07-21 | 2020-02-04 | Varian Medical Systems, Inc | Geometric aspects of radiation therapy planning and treatment |
US10183179B1 (en) | 2017-07-21 | 2019-01-22 | Varian Medical Systems, Inc. | Triggered treatment systems and methods |
CN115282504A (en) | 2017-11-16 | 2022-11-04 | 瓦里安医疗系统公司 | Radiation therapy treatment system and method in a radiation therapy treatment system |
US10910188B2 (en) | 2018-07-25 | 2021-02-02 | Varian Medical Systems, Inc. | Radiation anode target systems and methods |
CN111420290A (en) * | 2019-01-10 | 2020-07-17 | 中国科学院沈阳自动化研究所 | Robotized laser cosmetic and therapeutic system |
US10814144B2 (en) | 2019-03-06 | 2020-10-27 | Varian Medical Systems, Inc. | Radiation treatment based on dose rate |
US11116995B2 (en) | 2019-03-06 | 2021-09-14 | Varian Medical Systems, Inc. | Radiation treatment planning based on dose rate |
US11103727B2 (en) | 2019-03-08 | 2021-08-31 | Varian Medical Systems International Ag | Model based PBS optimization for flash therapy treatment planning and oncology information system |
US11090508B2 (en) | 2019-03-08 | 2021-08-17 | Varian Medical Systems Particle Therapy Gmbh & Co. Kg | System and method for biological treatment planning and decision support |
CN111821583A (en) * | 2019-04-22 | 2020-10-27 | 苏州雷泰医疗科技有限公司 | Accelerator treatment device and treatment method |
US10918886B2 (en) | 2019-06-10 | 2021-02-16 | Varian Medical Systems, Inc. | Flash therapy treatment planning and oncology information system having dose rate prescription and dose rate mapping |
US11291859B2 (en) | 2019-10-03 | 2022-04-05 | Varian Medical Systems, Inc. | Radiation treatment planning for delivering high dose rates to spots in a target |
CN111132441A (en) * | 2019-12-31 | 2020-05-08 | 清华大学 | Permanent magnet type quadrupole magnet and assembling method thereof |
US11865361B2 (en) | 2020-04-03 | 2024-01-09 | Varian Medical Systems, Inc. | System and method for scanning pattern optimization for flash therapy treatment planning |
US11541252B2 (en) | 2020-06-23 | 2023-01-03 | Varian Medical Systems, Inc. | Defining dose rate for pencil beam scanning |
US11957934B2 (en) | 2020-07-01 | 2024-04-16 | Siemens Healthineers International Ag | Methods and systems using modeling of crystalline materials for spot placement for radiation therapy |
US12064645B2 (en) | 2020-07-02 | 2024-08-20 | Siemens Healthineers International Ag | Methods and systems used for planning radiation treatment |
CN112996212A (en) * | 2021-02-05 | 2021-06-18 | 北京大学 | Plasma channel generating device |
CN217745384U (en) * | 2021-03-31 | 2022-11-08 | 中硼(厦门)医疗器械有限公司 | Neutron capture therapy system |
CN113225890B (en) * | 2021-05-08 | 2024-03-29 | 湖南太观科技有限公司 | Micro accelerator based on intelligent metamaterial and acceleration method thereof |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101237908A (en) * | 2005-08-04 | 2008-08-06 | 马尔科·苏米尼 | Device for generating electron beams and X-ray beams for interstitial intraoperative radiation therapy |
CN102113419A (en) * | 2008-05-22 | 2011-06-29 | 弗拉迪米尔·叶戈罗维奇·巴拉金 | Multi-axis charged particle cancer therapy method and apparatus |
WO2013133936A1 (en) * | 2012-03-03 | 2013-09-12 | The Board Of Trustees Of The Leland Stanford Junior University | Pluridirectional very high electron energy radiation therapy systems and processes |
CN103745760A (en) * | 2014-01-16 | 2014-04-23 | 上海交通大学 | All-optical laser plasma accelerator-based Gamma ray source |
Family Cites Families (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE10014034C2 (en) * | 2000-03-22 | 2002-01-24 | Thomson Tubes Electroniques Gm | Plasma accelerator arrangement |
DE102010061121B4 (en) * | 2010-12-08 | 2013-03-07 | Gsi Helmholtzzentrum Für Schwerionenforschung Gmbh | Irradiation phantom with at least one movement device for moving a first portion |
CN103336295A (en) * | 2013-06-19 | 2013-10-02 | 南京航空航天大学 | Method for acquiring photon beam energy spectrum of medical electric linear accelerator |
CN103619118B (en) * | 2013-12-13 | 2016-04-13 | 上海交通大学 | The method of laser plasma accelerator and generation high-quality electron beam |
-
2014
- 2014-05-07 CN CN201410191339.4A patent/CN104001270B/en not_active Expired - Fee Related
- 2014-08-25 WO PCT/CN2014/085119 patent/WO2015169011A1/en active Application Filing
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101237908A (en) * | 2005-08-04 | 2008-08-06 | 马尔科·苏米尼 | Device for generating electron beams and X-ray beams for interstitial intraoperative radiation therapy |
CN102113419A (en) * | 2008-05-22 | 2011-06-29 | 弗拉迪米尔·叶戈罗维奇·巴拉金 | Multi-axis charged particle cancer therapy method and apparatus |
WO2013133936A1 (en) * | 2012-03-03 | 2013-09-12 | The Board Of Trustees Of The Leland Stanford Junior University | Pluridirectional very high electron energy radiation therapy systems and processes |
CN103745760A (en) * | 2014-01-16 | 2014-04-23 | 上海交通大学 | All-optical laser plasma accelerator-based Gamma ray source |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US11013100B2 (en) | 2016-10-10 | 2021-05-18 | University Of Strathclyde | Plasma accelerator |
EP3749065A4 (en) * | 2019-03-27 | 2021-09-01 | Huazhong University of Science and Technology | Electron radiation system |
US11483919B2 (en) | 2019-03-27 | 2022-10-25 | Huazhong University Of Science And Technology | System of electron irradiation |
LT6816B (en) | 2019-10-03 | 2021-05-10 | Valstybinis mokslinių tyrimų institutas Fizinių ir technologijos mokslų centras | Laser-driven high-dose-rate generating device of ionizing radiation |
Also Published As
Publication number | Publication date |
---|---|
CN104001270A (en) | 2014-08-27 |
CN104001270B (en) | 2016-07-06 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
WO2015169011A1 (en) | Extra high energy electron beam or photon beam radiotherapy robot system | |
US9283406B2 (en) | Charged hadron beam delivery | |
US7940894B2 (en) | Elongated lifetime X-ray method and apparatus used in conjunction with a charged particle cancer therapy system | |
US8045679B2 (en) | Charged particle cancer therapy X-ray method and apparatus | |
JP5497750B2 (en) | X-ray method and apparatus used in combination with a charged particle cancer treatment system | |
US7939809B2 (en) | Charged particle beam extraction method and apparatus used in conjunction with a charged particle cancer therapy system | |
JP5450602B2 (en) | Tumor treatment device for treating tumor using charged particles accelerated by synchrotron | |
US5471516A (en) | Radiotherapy apparatus equipped with low dose localizing and portal imaging X-ray source | |
US8415643B2 (en) | Charged particle beam acceleration and extraction method and apparatus used in conjunction with a charged particle cancer therapy system | |
US8625739B2 (en) | Charged particle cancer therapy x-ray method and apparatus | |
US20100006106A1 (en) | Semi-vertical positioning method and apparatus used in conjunction with a charged particle cancer therapy system | |
US8229072B2 (en) | Elongated lifetime X-ray method and apparatus used in conjunction with a charged particle cancer therapy system | |
US10485991B2 (en) | Methods and systems for RF power generation and distribution to facilitate rapid radiation therapies | |
JP2009511222A (en) | Integrated system of external beam radiation therapy and MRI | |
AU2009249867A1 (en) | Charged particle beam extraction method and apparatus used in conjunction with a charged particle cancer therapy system | |
Kutsaev et al. | Compact X-Band electron linac for radiotherapy and security applications | |
JP6126153B2 (en) | Charged particle beam acceleration method and apparatus as part of a charged particle cancer treatment system | |
KR102068326B1 (en) | Radiation therapy apparatus for animals | |
JP2010251275A (en) | Ion collective accelerator and application thereof | |
US20110092759A1 (en) | Mobile system for electron beam intraoperative radiation therapy | |
JP2018146265A (en) | Electron beam irradiation device and method for operating electron beam irradiation device | |
Lim et al. | Design of a radiotherapy machine using the 6-MeV C-band standing-wave accelerator | |
KR20210131778A (en) | Magnetic field generating apparatus and control method thereof | |
IT201800006452A1 (en) | Beam transport line with 2 or 4 quadrant fast-varying power supplies to perform a "Fast Adaptative Spot Scanning Therapy" (FASST) with proton beams |
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: 14891412 Country of ref document: EP Kind code of ref document: A1 |
|
NENP | Non-entry into the national phase |
Ref country code: DE |
|
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 04/04/2017) |
|
122 | Ep: pct application non-entry in european phase |
Ref document number: 14891412 Country of ref document: EP Kind code of ref document: A1 |