Patent Grant
11160159
This application is based upon and claims the benefit of prior European Patent Application No. 20161640.6, filed on Mar. 6, 2020, the entire contents of which are incorporated by reference herein.
The present disclosure concerns extraction of a beam of accelerated charged particles out of a synchrocyclotron (SC) comprising hill sectors and valley sectors alternatively distributed around the central axis (z) with a symmetry (N) of at least three, at different energies ranging between a low energy (E1) and a high energy (E2) corresponding to low and high average radii (R1, R2) of the trajectory followed by the beam. In particular, the extraction of the beam is triggered by a magnetic perturbation or field bump, having a magnitude which can be controlled over an azimuthal sector. of a given azimuthal angle (θc) (defining the aperture of the azimuthal sector) and comprised between the low and high average radii (R1, R2) to be equal to the offset amplitude (ΔBz0(Ri, νr)·θc/2π) at the average instability onset radius (Ri) and at the radial tune (νr), wherein,
The synchrocyclotron of the present invention is particularly advantageous in that it can extract beams of charged particles at a range of energies varying from 20% to 100% of the nominal energy of the synchrocyclotron. For example, for a 230 MeV synchrocyclotron, the present invention can very easily extract beams of charged particles of energies ranging from 46 MeV to 230 MeV
A cyclotron is a type of circular particle accelerator in which negatively or positively charged particles accelerate outwards from the center of the cyclotron along a spiral path forming successive concentric orbits up to energies of several MeV. The acceleration of the particles is driven by a radio frequency (RF)-alternating electric field, and the trajectory of the particles is guided along successively larger orbits on a plane (X, Y) of average radius (R) by the z-component (Bz) of a main magnetic field (B). There are various types of cyclotrons. In isochronous cyclotrons, both Bz and the frequency of the RF field are constant, so that the particle beam runs each successive cycle or cycle fraction of the spiral path in the same time. A synchrocyclotron is a special type of cyclotron, in which the frequency of the RF-alternating electric field varies to compensate for relativistic effects as the particles' velocity approaches the speed of light. This is in contrast to the isochronous cyclotrons, where this frequency is constant. Cyclotrons are used in various fields, for example in nuclear physics, in medical treatment such as proton-therapy, or in radio pharmacology.
The present disclosure concerns synchrocyclotrons. In a synchrocyclotron, the particles form longitudinal phase oscillations around a synchronous phase, typically of a few degrees to about 30 degrees, in such way that they are alternatively accelerated for a number of revolutions, then decelerated for another period of a number of revolutions. The resulting acceleration is slower in a synchrocyclotron than in an isochronous cyclotron, but due to the high longitudinal stability of the beam, many particles can be accelerated at each duty cycle.
A cyclotron comprises several elements including an injection unit, a RF accelerating system for accelerating the charged particles, a magnetic system for guiding the accelerated particles along a precise path, an extraction system for collecting the thus accelerated particles, and a vacuum system for creating and maintaining a vacuum in the cyclotron. Superconducting cyclotrons require a cryocooling system for maintaining the superconducting elements thereof at their superconducting temperatures.
An injection system introduces a particle beam with a relatively low initial velocity into an acceleration gap at or near the center of the cyclotron. The RF accelerating system sequentially and repetitively accelerates this particle beam, guided outwards along a spiral path within the acceleration gap by a magnetic field generated by the magnetic unit.
The magnetic unit generates a magnetic field that guides and focuses the beam of charged particles along the spiral path until reaching its target energy, Ei. The main magnetic field is generated in the gap defined between two field shaping units arranged parallel to one another on either side of a median plane (P) normal to the central axis (z) and defining a symmetry plane of the cyclotron, by two solenoid main coils wound around these field shaping units. The field shaping units can be magnet poles or superconducting coils separated from one another by the acceleration gap. The main magnetic field must be controlled to limit defocusing of the beam due to relativistic effects, inter alia.
Focusing can be improved by providing hill and valley sectors alternatively distributed around the central axis (z) with a symmetry (N) of at least three for shaping the main magnetic field with a symmetry of same order (N). The focusing and defocusing effects generated by radial and azimuthal components of the thus varying magnetic field near the median plane (P) affect the value of the tunes of the beam. The tunes of the beam are the fractions of periods each particle makes around a closed orbit during one revolution. At a given energy (Ei) (or at a given average radius (Ri)), tunes have a radial component (νr) and a normal component (νz). A perfectly flat main magnetic field (Bz) has a radial tune νr=1, resulting in an instable beam of charged particles. In a main magnetic field of tune νr=1, a not perfectly aligned particle would slip out of the orbit it is meant to follow and drift away, which must be avoided during the acceleration phase.
The main coils are enclosed within a flux return or yoke, which restricts the magnetic field within the cyclotron. Vacuum is extracted at least within the acceleration gap. Any one of the field shaping units and flux return can be made of magnetic materials, such as iron or low carbon steel, or can consist of coils activated by electrical energy. Said coils, as well as the main coils can be made of superconducting materials. In this case, the superconducting coils must be cooled below their critical temperature. Cryocoolers can be used to cool the superconducting components of a cyclotron below their critical temperature which can be of the order of between 2 and 10 K, typically around 4 K for low temperature superconductors (LTS) and of the order of between 20 and 75 K for high temperature superconductors (HTS). The flux return is provided with one or more exit ports for allowing the extraction of the charged particles out of the (synchro)cyclotron.
When the particle beam reaches its target energy, the extraction system extracts it from the cyclotron through an exit port and guides it towards an extraction channel. Several extraction systems exist and are known to a person of ordinary skill in the art, including stripping (mostly in isochronous cyclotrons), electrostatic extraction (also mostly in isochronous cyclotrons), and regenerative extraction, wherein a resonant perturbation is created by a field bump (possible in both synchrocyclotrons and isochronous cyclotrons).
Regenerative extraction creates a resonant perturbation in an orbit of a particle beam by applying a magnetic field bump (ΔBz). Iron bars with a well-defined azimuthal and radial extension (called “regenerator”) are often used to generate a magnetic field bump. For example, U.S. Pat. No. 8,581,525 and WO2013098089 describe iron-based regenerators. A first drawback with iron-based regenerators includes that the magnitude of the magnetic field bump cannot be varied easily, and certainly not during operation of the cyclotron. This is a drawback when a same cyclotron is used to extract particles at different energies. A second drawback is that the energy of the extracted particle beam cannot be varied. If a particle beam of a given energy (Ei) is required for an application, the particle beam must be extracted at the nominal energy of the cyclotron, and the energy of the beam must be reduced by energy control devices located downstream of the exit port, outside of the synchrocyclotron, such as energy selection systems (ESS), degraders, range-shifters, collimators, and the like.
Iron-based regenerators can be replaced by coils, in particular by superconducting coils which can generate higher magnetic fields. The use of coils allows the magnitude, (ΔBz), of the field bump to be varied independently of the magnitude of the z-component (Bz) of the main magnetic field (B).
Solutions have been proposed for extracting a particle beam out of a synchrocyclotron at different energies (Ei) (or average radii (Ri)). U.S. Pat. No. 9,302,384 describes a synchrocyclotron comprising an extraction structure arranged proximate to the entry point of the extraction channel to change an energy level of the particles, wherein the extraction structure has multiple thicknesses and is movable relative to the extraction channel to place one of the multiple thicknesses in a path of the particles. This solution is not suitable for extracting beams of energies varying over a broad range [E1, E2].
WO2013142409 describes a synchrocyclotron comprising a series of magnetic extraction bumps extending in series radially from the central axis on opposite sides of the median acceleration plane. WO2017160758 describes a synchrocyclotron wherein an RF-frequency versus ion-time-of-flight scenario is set such that the frequency versus time scenario is the same for any ion extraction energy from the given design range, and a constant-or-variable-RF-voltage versus ion-time-of-flight scenario is adjusted to provide ion acceleration from injection to extraction for ions with different respective extraction energy levels within the given design range; and the ions are extracted at the different energy levels at the shared extraction radius. WO2019146211 describes a synchrocyclotron wherein a high-frequency wave of a different frequency from that of the high-frequency wave used for the acceleration is applied to the charged particle beam to eject the charged particle beam. Thus, in the circular accelerator that accelerates the charged particle beam while increasing the trajectory radius by applying the high-frequency wave within the main magnetic field, the ejection of the charged particle beam from the circular accelerator can thereby be controlled with high accuracy. These solutions require the intensity of the magnetic field or the frequency of the RF acceleration electric field to be varied, which requires time for large variations thereof.
US20190239333 describes a miniaturized and variable energy accelerator wherein a plurality of ring-shaped beam closed orbits of the trajectory of the particle beam followed by charged particles of corresponding energies, are offset on one side relative to the center of the synchrocyclotron. The frequency of the radiofrequency electric field fed to the charged particles by the acceleration electrode is modulated by the beam closed orbits. The offset of the orbits thus generated forms aggregated regions where adjacent orbits are very close to one another and discrete regions where adjacent orbits are separated by a larger distance in the radial direction.
US20150084548 describes a synchrocyclotron comprising an electrode that applies an RF electric field to accelerate the charged particle beam; and further comprising a DC power supply device that applies a DC electric field to the electrode. When the charged particle beam is accelerated while applying a DC voltage to the dummy dee electrode from outside a radius re. an E×B drift is generated along the spiral-shaped orbit to the radius re by the beam bending magnetic field B and the electric field E from the DC voltage Vdc at the outer side from re, the beam orbit drifts from the center to the outer side, and the charged particle beam is extracted by an electrostatic deflector electrode.
The solution proposed in the latter two documents is challenging for extracting charged particles at low energies, of the order of 25 to 50% of the nominal energy (Em) of the synchrocyclotron.
There therefore remains a need for a synchrocyclotron capable of delivering beams with fast variable energy having simplified and easy beam extraction, in that the energies may be switched rapidly with high dose rates. The present disclosure proposes a synchrocyclotron provided with a first and second instability coil units configured for creating a magnetic field bump of varying magnitudes for selecting the energy of the particles to be extracted. The perturbation thus created enters into resonance due to the specific magnetic field conditions the perturbed orbits are exposed to. The synchrocyclotron of the present disclosure fulfils the foregoing requirements. The following sections describe these and other advantages in more details.
The present disclosure concerns a synchrocyclotron for extracting charged particles such as hadrons (e.g., protons), accelerated to an extraction energy (Ei) between a low energy (E1) and a high energy (E2). The synchrocyclotron comprises:
In some embodiments, the hill sectors and valley sectors may have a symmetry (N) of N=2n+1 with n∈N. For example, N may be equal to 3. The z-component (Bz) of the main magnetic field may be controlled such that the radial tune (νr) of the successive orbits is not equal to 1 and is comprised within 1±0.1, or, in alterative embodiments, within 1±0.025 or 1.002≤|νr|≤1.015, for all values of the average radius (R), comprised between a low radius (R1) and a high radius (R2), corresponding to respective average radial positions of the charged particles at the low and high energies (E1, E2).
The first and second instability coil units may be configured for creating the field bump within an azimuthal sector of azimuthal angle (θc), with an amplitude (ΔBz(R)) increasing radially, and in some embodiments monotonically, between a first field bump amplitude value (ΔBz(R1)) at the low radius (R1) and a second field bump amplitude value (ΔBz(R2)) at the high radius (R2).
The synchrocyclotron may also comprise a controlling unit configured for adjusting the amplitude (ΔBz(R)) of the field bump at various levels comprised between low values and high values, such that, for all values of an average instability onset radius (Ri) comprised between the low and high radii (R1, R2), the value of the amplitude of the field bump (ΔBz(Ri)) at the average instability onset radius (Ri), is equal to a value of an offset amplitude (ΔBz0(Ri, νr)) at the average instability onset radius (Ri), and is lower than the values of the offset amplitude (ΔBz0(R, νr)) for all values of the average radius (R) smaller than the average instability onset radius (Ri), wherein the offset amplitude (ΔBz0(Ri, νr)·θc/2π) is the minimal amplitude of the field bump at the average instability onset radius (Ri) required for sufficiently offsetting the center of the orbit of average instability onset radius (Ri) along which the charged particles are guided, such that a combination of an amplitude of the harmonic 2 and a radial gradient of the amplitude of the harmonic 2 on this orbit is produced by the main magnetic field (B) of symmetry (N) on a thus offset orbit, and is large enough to generate a resonance instability of the successive orbits of average radius, R≥Ri.
The first and second instability coil units may be defined such that a projection of the first and second instability coil units are located within an area defined circumferentially by an azimuthal section comprised within the azimuthal angle (θc) which can be smaller than π/3, or, in alternative embodiments, smaller than π/4, or smaller than π/6. Further, the area may be defined radially between the low and high radii (R1, R2).
In an embodiment, the first and second instability coil units can be in the form of a pair of trapezoidal or triangular coils of dimensions fitting the azimuthal sector of azimuthal angle (θc) and of length at least equal to (R2−R1) in the radial direction. The distance separating the first and second instability coil units can decrease radially, so that the amplitude (ΔBz(R1)) at the low radius (R1) is smaller than the amplitude (ΔBz(R2)) at the high radius (R2). The distance separating the first and second instability coil units may decrease linearly along the radial direction, wherein each of the first and second instability coil unit forms an angle with the median plane (P) comprised between 5 and 30 degrees, or, in alternative embodiments, between 10 and 25 deg.
In an embodiment, the first and second instability coil units may be formed by a series of two or more pairs of coils radially aligned within the azimuthal sector, each pair of coils being configured for generating a field bump of amplitude (ΔBz(R)) higher than the adjacent pair of coils located closer to the central axis (z), or of amplitude (ΔBz(R)) lower than the adjacent pair of coils located further away from the central axis (z).
The offset amplitude (ΔBz0(Ri, νr)·θc/2π) at the average instability onset radius (Ri) may be defined such that ΔBz0(Ri,νr)·θc/2π is between 0.001% and 1% of an average value of the z-component (Bz) of the main magnetic field (B) at the average instability onset radius (Ri), or, in alternative embodiments, between 0.005% and 0.05% thereof.
For a synchrocyclotron having a nominal energy (Em) of extraction, the low energy (E1) may be comprised between 20% and 75% of Em, or, in alternative embodiments, between 30% and 50% of Em. The high energy (E2) can be comprised between 80% and 100% of Em, or between 90% or 95% and 99% of Em,
The present disclosure also concerns a method for extracting charged particles out of a synchrocyclotron at any given value of an extraction energy (Ei) between a low energy (E1) and a high energy (E2). The method comprises the steps of:
In some embodiments, the radial tune of successive orbits may be within 1±0.025, or 1.002≤|νr|≤1.015,
For a fuller understanding of the nature of the present disclosure, reference is made to the following detailed description taken in conjunction with the accompanying drawings in which:
The present disclosure concerns accelerated particle beam extraction systems applied to synchrocyclotrons producing beams of charged particles such as hadrons and, in particular, protons having a maximal or nominal target energy (Em). The nominal target energy (Em) of the particle beam may be of the order of 15 to 400 MeV/nucleon. In alternative embodiments, the nominal target energy may be between 60 and 350 MeV/nucleon, or between 70 and 300 MeV/nucleon. The nominal energy (Em) of a synchrocyclotron may be set when designing the synchrocyclotron. The synchrocyclotron (1) of the present disclosure is capable of extracting beams of charged particles at varying energies comprised between a low energy (E1) and a high energy (E2) of extraction, wherein E1<Em≤E2. The low energy (E1) may be of the order of between 20% and 75% of Em or between 30% and 50% of Em, and wherein the high energy (E2) may be between 80% and 100% of Em or between 90% or 95% and 99% of Em. A beam of charged particles has a given energy (Ei) when it rotates at a corresponding orbit of radius (Ri), as illustrated in
The extraction at varying energies by the synchrocyclotron of the present disclosure is made possible by, on the one hand, creating a field bump which amplitude (ΔBz(Ri)) at any orbit of average radius (Ri) comprised between R1 and R2 can be varied to reach the value of the offset amplitude (ΔBz0(Ri, νr)) required for offsetting the center of the orbit of average radius (Ri) sufficiently for creating a resonant instability and, on the other hand, by creating the conditions for the offset amplitude (ΔBz0(R, νr)) to be sufficiently high to allow a stable and reproducible acceleration of the beam and sufficiently low to limit the magnitude (ΔBz(Ri)) of the field bump. The foregoing features can be combined in a synchrocyclotron according to the present disclosure as explained below. Additionally, the beam may be extracted at the maximum target energy (Em).
The present invention can be implemented on conventional synchrocyclotrons. A synchrocyclotron according to the present disclosure includes the following components.
As illustrated in
The synchrocyclotron further comprises a magnetic unit comprising main coils (31, 32) and field shaping units (41, 42) for bending into concentrically larger orbits (=spiral) the trajectory of the beam of charged particles as it is being accelerated by the RF-oscillating electric field. As illustrated in
The magnetic unit also comprises a first field shaping unit (41) and a second field shaping unit (42). The first and second field shaping units (41, 42) are arranged within the first and second main coils on either side of the median plane (P) and are separated from one another by a gap (6). The orbits of the beam of charged particles are comprised within or oscillate about the median plane. The first and second field shaping units (41, 42) may be in the form of magnet poles made of ferromagnetic metal (e.g., steel) or may be formed by a series of coils, such as superconducting coils. for shaping the main magnetic field (B) and thus guiding the charged particles along successive orbits of increasing average radii (R) (=spiral path) centered on the central axis (z). In particular, the first and second field shaping units (41,42) may be configured for controlling a z-component (Bz) of the main magnetic field between the first and second field shaping units, which is parallel to the central axis (z) such that the revolution speed of the particles around each orbit is synchronized with the RF-oscillating electric field, for all values of the radius (R) of the orbits. An example of z-component (Bz) of the main magnetic field is illustrated in
The first and second field shaping units (41, 42) comprise hill sectors (44h) and valley sectors (44v) alternatively distributed around the central axis (z) with a symmetry (N) of at least three. In some embodiments, N may be an odd number (N=2n+1, with n∈N) such as N=3, for shaping the z-component of the main magnetic field with a symmetry of same order (N), as shown in
Once the beam of charged particles has reached the target energy, it must be extracted from the synchrocyclotron. The synchrocyclotron of the present disclosure uses a novel regenerative device for creating an instability to a given orbit of radius (Ri) of the trajectory of the beam ranging between R1 and R2, which enters into resonance as will be explained below. The synchrocyclotron comprises first and second instability coil units (51, 52), each comprising at least a coil which can be energized to create an instability to a given orbit. Once the charged particles of the beam reach a region of the gap where they are not bent by the main magnetic field to remain within the gap (i.e., a stray field region), the beam can be extracted through one or more exit ports (49). Since the main magnetic field is lower in the valleys than in the hills (cf.
As shown in
Thus, the extraction system may combine:
The radial tune is a measure of the oscillations in the radial direction of the beam over the orbits forming its trajectory. In other words, a tune is the ratio of oscillations to revolutions of the beam. At a given energy, tunes are defined in both transverse direction to the trajectory of the beam: the radial tune (νr) in the radial direction and the normal tune (νz) normal to the median plane (P). A perfectly flat magnetic field in the radial direction has a radial tune, νr=1, and is unstable, in that particles which are not perfectly aligned on a closed orbit would slip out of the orbit along the median plane and drift in a given direction. Such drift must be avoided or at least minimized at least during the acceleration phase of the beam, before reaching the target energy. By design, in isochronous cyclotrons, νr>1 and cannot be selected very close to unity, as in such conditions the field could not increase sufficiently with the radius to compensate relativistic effects at high energies. This is not the case with synchrocyclotron since there is no isochronism conditions imposed when designing the magnetic field.
In the present disclosure, the radial tune (νr) of the successive orbits comprised between the low average radius (R1) and the high average radius (R2), is not equal to 1 as the beam would be too unstable to be accelerated along the orbits. The radial tune (νr) may be comprised within 1±0.1, or within 1±0.025, such as 1.002≤|νr|≤1.015. The radial tune (νr) may be excluded from the range, |1−νr|<0.002, to give the beam sufficient stability to reach the target energy. For instance, the beam may have sufficient stability to reach the target energy when 0.002≤|1−νr|≤0.015 or 0.004≤|1−νr|≤0.012. An example of the radial tune (νr) (solid line) as a function of the radius (R) is illustrated in
Selecting the radial tune (νr) within the foregoing ranges ensures, on the one hand, that it is sufficiently high for all the orbits of average radius comprised between (R1) and (R2) which is smaller than the average instability onset radius to be sufficiently stable to accelerate the beam to the target energy and, on the other hand, that it is sufficiently low to require only a small perturbation, either electric or magnetic, to offset the orbits. In the present disclosure, a magnetic perturbation is used. This is may initiate a resonant process leading to the extraction of the beam.
With the values of the radial tune (νr) as discussed supra, a small magnetic perturbation suffices to offset an orbit of given radius (Ri) comprised between R1 and R2. The magnetic perturbation is created by a first instability coil unit (51) and a second instability coil unit (52) arranged on either side of the median plane (P) as shown in
As shown in
A controlling unit is configured for adjusting the amplitude (ΔBz(R)) of the profile of the field bump at various levels comprised between low values and high values, such that, the value of the amplitude (ΔBz(Ri)) at any average radius (Ri) comprised between R1 and R2 can be varied up and down within a given range. For example, the amplitude of the field bump can be increased from the low values (ΔBz(R1)) to the high values (ΔBz(R2)) by scaling or by shifting up the amplitude of the field bump, or combination thereof. This can be done by simply varying the amount of current fed to the first and second instability coils (51, 52).
The values of the offset amplitude (ΔBz0(Ri, νr)·θc/2π) at any average instability onset radius (Ri) comprised between (R1) and (R2) may be determined and entered into the controlling unit. The offset amplitude (ΔBz0(Ri, νr)·θc/2π) is the minimal amplitude of the field bump at the average instability onset radius (Ri) required for sufficiently offsetting the center of the orbit of average instability onset radius (Ri) along which the charged particles are guided. The offset must be sufficient for producing a combination of harmonic 2 and gradient of harmonic 2 on this orbit by the main magnetic field (B) of symmetry (N) on a thus offset orbit. This combination must be large enough to generate a resonance instability of the successive orbits of average radius, R≥Ri. Knowing the values of the main parameters of the synchrocyclotron, including the radial tune (νr), the z-component of the main magnetic field (Bz), the degree of symmetry (N), and the like, a person skilled in the art may determine the offset amplitude for any value of the average radius (R) when designing the synchrocyclotron. An example of the offset amplitude (ΔBz0(R, νr)) is schematically represented with the thick continuous line of
Referring to
If a different orbit of average instability onset radius (Rj) or (Rk) is to be offset for extraction of a beam of energy (Ej) or (Ek), the amplitude (ΔBz(Rj)) or (ΔBz(Rk)) of the field bump is set as follows, ΔBz(Rj)=ΔBz0(Rj, νr), and ΔBz(R)<ΔBz0(Rj, νr), ∀R<Rj, as illustrated with the short dashed line (ij) in
The values of the offset amplitude (ΔBz0(Ri, νr). θc/2π) at any average instability onset radius (Ri) comprised between (R1) and (R2) may be of the order of 0.001% to 1% of an average value of the z-component (Bz) of the main magnetic field at the average instability onset radius (Ri), such as 0.002% to 0.7%. In alternative embodiments, the offset amplitude may be 0.005% to 0.05% or 0.021%±0.02% of Bz(Ri). For example, for a z-component (Bz) of the main magnetic field of the order of 4 T at an average instability onset radius (Ri), the offset amplitude (ΔBz0(Ri, νr)·θc/2π) may be of the order of 0.025 T±0.02 T, depending on the values of the radial tune (νr(Ri)) at the average instability onset radius (Ri).
An orbit of average instability onset radius (Ri) can be offset relative to the center of the synchrocyclotron as described herein. The offset of the orbit thus created may be taken advantage of by generating a resonance instability in the orbit that drifts the following orbits. The “following orbits” are defined herein as the orbits of average radii equal to or larger than the average instability onset radius (Ri). A condition for creating resonance is generally accepted that k νr+l νz=m, with k, l, m∈N. For example, l=0 and k=m=2, yielding 2 νr=2, may be used for extracting a beam driven by a combination of an amplitude of the harmonic 2 and a radial gradient of the amplitude of the harmonic 2 in the magnetic field. This may be generated in synchrocyclotrons by sets of iron bars or coils called a peeler-regenerator system.
In the present disclosure, once the orbit of average instability onset radius (Ri) has been offset relative to the central axis (z), the following orbits are exposed to a main magnetic field which z-component (Bz) has a symmetry (N) relative to the central axis (z) as illustrated in
The symmetry (N) of the first and second filed shaping units (41, 42) may be configured to preserve the vertical stability (in the z-direction) of the beam as the centers of following orbits drift away from the central axis (z). The field bump magnitude (ΔBz(Ri)) may generate a sufficient offset for the drifting following orbits to generate a strong 2nd harmonic component in the following orbits. The symmetry (N) of the first and second field shaping units may be an odd number (N=2n+1, with n∈N), as it facilitates the formation of a resonance harmonic 2 in the orbits. A 2nd harmonic component may be generated in the following orbits with a symmetry (N) wherein N is an even number (N=2n, with n>1 and n∈N) with a field bump having a slightly higher amplitude (ΔBz(Ri)) than with an odd symmetry (N=2n+1). In some embodiments, N may be equal to 3 (i.e., N=3).
The separation between the following orbits increases with the number of revolutions during which the unstable drift lasts before extraction. For example, the unstable drift of the following orbits may last at least 5 revolutions, at least 10 revolutions, or at least 20 revolutions, to build up sufficient separation between successive orbits to yield larger offset in angle and position between energies when the orbits reach the stray field of the field shaping units.
A field bump defined within an azimuthal sector of relative angle (θc/2π) and having a magnitude ΔBz(Ri)=ΔBz0(Ri, νr), at any orbit of average radius (Ri) comprised between the low radius (R1) and the high radius (R2) and, at the same time, ΔBz(Rk)<ΔBz0(Rk, νr), V Rk<Ri, may be formed by first and second instability coil units (51, 52) extending radially at least between the low and high radii (R1, R2). As illustrated in
As illustrated in
Alternatively, the amplitude (ΔBz(R)·θc/2π) of the field bump may increase radially by aligning radially a series of two or more pairs of coils within the azimuthal sector, each configured for generating a field bump of amplitude (ΔBz(R)·θc/2π) higher than the adjacent pair of coils located closer to the central axis (z) or of amplitude (ΔBz(R)·θc/2π) lower than the adjacent pair of coils located further away from the central axis (z)
By using coils for creating a field bump, the amplitude profile (ΔBz(R)) of the field bump may be varied at various levels comprised between low values and high values by simply varying the amount of current fed to the coils. The whole profile of the amplitude of the field bump (ΔBz(R)) may be varied, for example, by scaling, by shifting up and down, or by a combination of both.
The first and second instability coil units (51, 52) may be located in a valley sector (44v). This has two main advantages. First, since the gap height (Hv) in a valley sector (44v) is larger than the gap height (Hh) in a hill sector (44h), there is more room for installing the first and second instability coil units (51, 52). Second, since the z-component (Bz) of the main magnetic field is lower in the valley sectors than in the hill sectors (cf.
As illustrated in
The angle and entry point of a beam into the stray field depends on the energy of the beam. By controlling the direction and building process of the drift of a beam, the angles and entry points of beams of different energies, albeit different, may be concentrated in a limited region, where a magnetic channel can drive the beams of different energies through a single exit port (49). Guiding beams of different energies entering the stray field at different positions and angles through a single exit port can be carried out by a skilled person, such as described e.g., in EP3503693.
The synchrocyclotron of the present disclosure is advantageous in that beams of widely varying energies between low and high energies (E1, E2) can be extracted by a simple tuning of the first and second instability coil units (51, 52) by a method comprising the following steps.
First, providing a synchrocyclotron as discussed supra configured, such that,
In some embodiments, the radial tune of successive orbits may be within 1±0.025, or 1.002≤|νr|≤1.015,
Then selecting a value of the extraction energy (Ei) of the charged particles to be extracted, and determining the value of the offset amplitude (ΔBz0(Ri, νr)·θc/2π) required for offsetting the center of the orbit of average radius (Ri) of the charged particles at the extraction energy (Ei) such that a resonance instability of the successive orbits of average radius, R≥Ri, is generated. The present disclosure allows for adjustment of the amplitude of the field bump such that the amplitude (ΔBz(Ri)) of the field bump equals the offset amplitude (ΔBz0(Ri, νr)) at the average instability onset radius (Ri) and is lower than the offset amplitude (ΔBz0(R, νr)) for all values of the average radius smaller than the average radius (Ri). This may be performed by varying the amount of current fed to the first and second instability coil units (51, 52), such that the profile of the amplitude (ΔBz(R)) varies, for example by scaling, shifting up and down, or combination of the two.
The present disclosure is advantageous in that the tuning of the extraction energies is easy and quick to perform, and in that it is possible to equip existing synchrocyclotrons with a main magnetic field that may be adapted to yield the desired profile and radial tune (νr), with first and second instability coil units (51, 52) to perform the method of the present disclosure.
| Number | Date | Country | Kind |
|---|---|---|---|
| EP20161640 | Mar 2020 | EP | regional |
| Number | Name | Date | Kind |
|---|---|---|---|
| 8581525 | Antaya et al. | Mar 2013 | B2 |
| 20130141019 | Kleeven | Jun 2013 | A1 |
| 20160143124 | Kleeven | May 2016 | A1 |
| 20170332475 | Kleeven | Nov 2017 | A1 |
| 20180132342 | Abs | May 2018 | A1 |
| 20200170099 | Abs | May 2020 | A1 |
| Number | Date | Country |
|---|---|---|
| 206 061 269 | Mar 2017 | CN |
| 2446718 | Mar 2018 | EP |
| 3503693 | Jun 2019 | EP |
| WO 2013098089 | Jul 2013 | WO |
| WO 2020044604 | Mar 2020 | WO |
| Entry |
|---|
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| Extended European Search Report issued in corresponding European Patent Application 20161640.6 dated Sep. 9, 2020. |
| Number | Date | Country | |
|---|---|---|---|
| 20210282257 A1 | Sep 2021 | US |
