Description:FORM 2
THE PATENT ACT, 1970
(39 of 1970)
&
The Patent Rules, 2003
COMPLETE SPECIFICATION
(See section 10 and rule 13)

1. TITLE OF THE INVENTION:
A Bremsstrahlung Collider System for Photon-Mediated Particle Collisions and Method Thereof
2. APPLICANT:
Name: Sanghamitra Foundation
Nationality: Indian Registered Society
Address: 2-32, Nizampet Road, Hydernagar, Kukatpally, Hyderabad-500085, Telangana, INDIA
3. PREAMBLE TO THE DESCRIPTION:
The following specification particularly describes the invention and the manner in which it is to be performed: 
4. DESCRIPTION:
Field of the invention:
[0001] The present disclosure generally relates to the technical field of particle accelerator systems and photon-based collision technologies, and in specific, relates to a bremsstrahlung collider system that is configured to generate photon radiation and facilitate photon-mediated particle interactions in a controlled collision region, thereby enabling a compact architecture adapted for laboratory-scale implementation and improved efficiency in photon flux utilization.
Background of the invention:
[0002] Particle accelerator systems constitute a fundamental class of apparatus configured to accelerate charged particles to high kinetic energy levels using electromagnetic fields for applications in scientific research, medical therapy, and industrial processing, while photon generation technologies are employed to produce high-energy electromagnetic radiation through mechanisms such as Bremsstrahlung emission, synchrotron radiation, and inverse Compton scattering, and high-energy collision systems are designed to facilitate controlled interactions between particles or between particles and photons to investigate fundamental physical phenomena, material properties, and radiation effects, where such systems are typically implemented in specialized facilities requiring precise control over beam dynamics, energy distribution, and interaction environments to achieve reproducible and measurable experimental outcomes.
[0003] Conventional particle accelerators include linear accelerators, synchrotrons, and cyclotrons, each configured to impart energy to charged particles through distinct acceleration mechanisms involving radiofrequency fields, magnetic confinement, or cyclic acceleration paths, while Bremsstrahlung photon generation technologies utilize high atomic number conversion targets, such as tungsten or gold, to produce high-energy photons upon interaction with relativistic electron beams, and large-scale particle colliders are adapted to enable particle–particle interactions at extremely high energies using complex beam alignment, focusing, and collision systems, where such colliders often incorporate extensive infrastructure, multiple beamlines, and high-precision synchronization mechanisms to facilitate experimental investigations in high-energy physics and related domains.
[0004] However, existing particle accelerator systems and associated photon generation technologies exhibit several technical limitations, where conventional accelerators primarily function as particle acceleration devices without integrated mechanisms for controlled photon-mediated collision processes, while Bremsstrahlung photon generation systems are typically configured for radiation production rather than directed interaction within a defined collision region, and large-scale particle colliders are predominantly adapted for particle–particle interactions without efficient utilization of generated photon radiation for collision purposes, thereby resulting in fragmented system architectures that lack functional integration between photon generation and collision processes, leading to reduced operational efficiency, limited experimental flexibility, and suboptimal utilization of generated high-energy photon flux within compact and practical configurations.
[0005] Furthermore, conventional and existing technologies are associated with additional drawbacks including large physical size and extensive infrastructure requirements, high energy consumption due to continuous operation of high-power acceleration and beam control systems, lack of compact and modular configurations suitable for laboratory-scale implementation, separation of photon generation units from collision systems resulting in inefficient coupling and energy losses, and limited accessibility for small-scale research institutions due to high cost, complexity, and operational constraints, thereby creating a need for an integrated system capable of generating and utilizing photon radiation within a unified architecture that enables controlled photon-mediated particle interactions while reducing system size, improving energy efficiency, and enhancing practical applicability in diverse research and industrial environments.
[0006] In prior art, WO2012005629A1 discloses a device for generating Bremsstrahlung radiation. The device comprises an accelerating structure configured to accelerate charged particles, an electron gun configured to generate and inject pulsed electron beams, a high-frequency power system, and a target configured to produce Bremsstrahlung radiation upon interaction with accelerated electron beams. The device enables pulse-to-pulse variation of beam energy and radiation intensity through controlled modulation of beam current and accelerating fields, and includes control and cooling subsystems operatively connected to maintain stable operation. However, the device lacks a controlled collision region and does not disclose integration of photon generation with photon-mediated particle collision mechanisms in a compact modular system.
[0007] Therefore, there is a need for a bremsstrahlung collider system that is configured to generate photon radiation and facilitate photon-mediated particle interactions in a controlled collision region, thereby enabling a compact architecture adapted for laboratory-scale implementation and improved efficiency in photon flux utilization. There is also a need for a bremsstrahlung collider system that incorporates a compact and modular configuration, thereby enabling laboratory-scale deployment while reducing spatial footprint and infrastructure requirements associated with conventional large-scale particle accelerator and collider systems. Furthermore, there is also a need for a bremsstrahlung collider system that supports photon-mediated interactions, including photon–photon, photon–electron, and photon–ion collisions, thereby expanding experimental capabilities and enabling versatile investigation of particle interaction phenomena within a single system.
Objectives of the invention:
[0008] The primary objective of the present invention is to provide a bremsstrahlung collider system that is configured to generate photon radiation and facilitate photon-mediated particle interactions in a controlled collision region, thereby enabling a compact architecture adapted for laboratory-scale implementation and improved efficiency in photon flux utilization.
[0009] Another objective of the present invention is to provide a bremsstrahlung collider system that enables integrated generation and utilization of photon radiation within a unified architecture, thereby facilitating efficient photon-mediated particle interactions with improved collision probability and system-level operational coherence.
[0010] Another objective of the present invention is to provide a bremsstrahlung collider system that incorporates a compact and modular configuration, thereby enabling laboratory-scale deployment while reducing spatial footprint and infrastructure requirements associated with conventional large-scale particle accelerator and collider systems.
[0011] Another objective of the present invention is to provide a bremsstrahlung collider system that enhances photon flux density through coordinated beam alignment, focusing, and collimation assemblies, thereby improving interaction efficiency and enabling precise control over photon beam direction and intensity distribution.
[0012] Another objective of the present invention is to provide a bremsstrahlung collider system that supports photon-mediated interactions, including photon–photon, photon–electron, and photon–ion collisions, thereby expanding experimental capabilities and enabling versatile investigation of particle interaction phenomena within a single system.
[0013] Another objective of the present invention is to provide a bremsstrahlung collider system that enables adjustable energy operation of the accelerated electron beam and resulting photon spectrum, thereby allowing optimization of collision conditions for different particle types and experimental requirements.
[0014] Yet another objective of the present invention is to provide a bremsstrahlung collider system that improves energy utilization efficiency by directing generated Bremsstrahlung photons into a controlled collision region, thereby minimizing energy losses and enhancing effective conversion of beam energy into usable interaction events.
[0015] Further objective of the present invention is to provide a bremsstrahlung collider system that integrates detection mechanisms, including photon and particle detectors configured to measure interaction outcomes, thereby enabling accurate analysis, monitoring, and characterization of photon-mediated collision processes within the system.
Summary of the invention:
[0016] The present disclosure proposes a bremsstrahlung collider system for photon-mediated particle collisions and method thereof. The following presents a simplified summary in order to provide a basic understanding of some aspects of the claimed subject matter. This summary is not an extensive overview. It is not intended to identify key/critical elements or to delineate the scope of the claimed subject matter. Its sole purpose is to present some concepts in a simplified form as a prelude to the more detailed description that is presented later.
[0017] In order to overcome the above deficiencies of the prior art, the present disclosure is to solve the technical problem to provide a bremsstrahlung collider system that is configured to generate photon radiation and facilitate photon-mediated particle interactions in a controlled collision region, thereby enabling a compact architecture adapted for laboratory-scale implementation and improved efficiency in photon flux utilization.
[0018] According to one aspect, the invention provides a bremsstrahlung collider system for photon-mediated particle collisions. In one embodiment herein, the bremsstrahlung collider system comprises a primary charged particle accelerator, a beam path, plurality of dipole magnets, plurality of quadrupole magnets, plurality of radio-frequency (RF) cavities, a cryogenic cooling system, a beam dump, a photon converter, a beam alignment and focusing assembly, a photon collimation unit, a collision region, a detection unit, one or more energy recovery subsystems, and an energy management system.
[0019] In one embodiment herein, the primary charged particle accelerator includes a beam path configured to guide a circulating relativistic electron beam along a closed-loop path. In one embodiment herein, the dipole magnets are arranged along the beam path. The dipole magnets are configured to bend the electron beam trajectory. In one embodiment herein, the quadrupole magnets are arranged along the beam path. The quadrupole magnets are configured to focus the electron beam.
[0020] In one embodiment herein, the radio-frequency (RF) cavities are operatively coupled to the beam path for accelerating the electron beam to relativistic energy levels during repeated circulation within the closed-loop path. In one embodiment herein, the cryogenic cooling system is thermally coupled to the RF cavities and the dipole and quadrupole magnets. The cryogenic cooling system is configured to maintain superconducting operating conditions and extract thermal energy generated during operation.
[0021] In one embodiment herein, the photon converter having a high atomic number material and is positioned along the beam path within the primary charged particle accelerator. The photon converter is configured to generate a photon radiation upon interaction with the relativistic electron beam. In another embodiment herein, the photon converter is selected from a group consisting of tungsten, gold, tantalum, platinum, lead, and combinations thereof. Additionally, the primary charged particle accelerator is selected from a group consisting of a linear accelerator, a synchrotron, a cyclotron, and a plasma-based accelerator.
[0022] In one embodiment herein, the beam dump is operatively connected to the beam path. The beam dump is configured to receive the electron beam after interaction with the photon converter and convert residual beam energy into thermal energy. In one embodiment herein, the beam alignment and focusing assembly having at least the quadrupole magnets and electromagnetic lenses. The beam alignment and focusing assembly is configured to receive the generated photon radiation and to focus, align, and direct the photon radiation, and to optimize photon flux density and collision probability.
[0023] In one embodiment herein, the photon collimation unit is configured to restrict the angular dispersion of the photon radiation and to form a directional photon beam. In another embodiment herein, the photon collimation unit comprises one or more apertures or collimators configured to restrict the angular dispersion of a photon beam
[0024] In one embodiment herein, the collision region is located downstream of the photon converter. The collision region is configured to receive the directional photon radiation and to enable controlled interaction with at least one secondary particle beam. Additionally, the collision region comprises a vacuum chamber configured to reduce scattering losses and improve interaction efficiency. The interaction achieved through spatial alignment of photon and particle beams within a defined collision volume. In one embodiment herein, the secondary particle beam is configured to collide with the generated photons. The secondary particle beam comprises electrons, positrons, protons, ions, and neutral particles.
[0025] In one embodiment herein, the detection unit is configured to measure interaction outcomes within the collision region. The detection unit includes at least one of a photon detector, particle detector, and spectrometer. In one embodiment herein, the energy recovery subsystems are operatively coupled to at least one of the dipole magnets for capturing radiation losses generated during beam bending, the RF cavities for capturing radio-frequency losses, the beam dump for capturing thermal energy generated from beam termination, and the cryogenic cooling system for capturing extracted thermal energy.
[0026] In one embodiment herein, the energy management system is electrically coupled to the energy recovery subsystems and the RF cavities. The energy management system is arranged to convert captured energy into usable electrical or thermal power and to redistribute the usable power to at least the RF cavities. The bremsstrahlung collider system is adapted to perform photon-mediated particle interactions using the directional photon beam.
[0027] In another embodiment herein, the bremsstrahlung collider system is configured to operate at adjustable energy levels to control the photon energy spectrum, and recovers energy losses from the RF cavities, the dipole magnets, the beam dump, and the cryogenic cooling system for reutilization within the accelerator, thereby enabling photon-photon, photon-electron, photon-ion, and photon-particle collisions in an energy-efficient manner.
[0028] According to another aspect, the invention provides a method for performing energy-efficient photon-mediated particle interactions using the bremsstrahlung collider system. At one step, the electron beam is generated by using the primary charged particle accelerator, guides the electron beam through the beam path along a closed-loop path using the plurality of dipole magnets. At another step, the electron beam is focused and stabilized using the quadrupole magnets and accelerated to relativistic energy levels using one or more radio-frequency (RF) cavities. At another step, the superconducting operating conditions of the RF cavities are maintained, and the dipole and quadrupole magnets are used with the cryogenic cooling system.
[0029] At another step, the relativistic electron beam is directed onto the photon converter, comprising a high atomic number material to generate photon radiation, and receives and conditions the generated photon radiation using the beam alignment and focusing assembly. At another step, the photon radiation is collimated using the photon collimation unit to form the directional photon beam and is delivered into the collision region. At another step, at least one secondary particle beam or target is introduced into the collision region and detecting outcomes using the detection unit. At another step, the energy losses are captured and generated during beam acceleration, beam bending, beam termination, and thermal dissipation using one or more energy recovery subsystems. Further, at another step, captured energy losses are converted into usable electrical and thermal power using the energy management system and redistributed the usable power to at least the RF cavities to support continued operation of the bremsstrahlung collider system.
[0030] Further, objects and advantages of the present invention will be apparent from a study of the following portion of the specification, the claims, and the attached drawings.
Detailed description of drawings:
[0031] The accompanying drawings, which are incorporated in and constitute a part of the specification, illustrate an embodiment of the invention, and, together with the description, explain the principles of the invention.
[0032] FIG. 1 illustrates a schematic view of a bremsstrahlung collider system for photon-mediated particle collisions, in accordance to an exemplary embodiment of the invention.
[0033] FIG. 2A illustrates a schematic view of radio-frequency cavities, in accordance to an exemplary embodiment of the invention.
[0034] FIG. 2B illustrates a perspective view of the bremsstrahlung collider system with resistive losses, in accordance to an exemplary embodiment of the invention.
[0035] FIG. 2C illustrates a perspective view of a beam dump, in accordance to an exemplary embodiment of the invention.
[0036] FIG. 4 illustrates a flowchart of a method for performing energy-efficient photon-mediated particle interactions using the bremsstrahlung collider system, in accordance to an exemplary embodiment of the invention.
Detailed invention disclosure:
[0037] Various embodiments of the present invention will be described in reference to the accompanying drawings. Wherever possible, same or similar reference numerals are used in the drawings and the description to refer to the same or like parts or steps.
[0038] The present disclosure has been made with a view towards solving the problem with the prior art described above, and it is an object of the present invention to provide a bremsstrahlung collider system that is configured to generate photon radiation and facilitate photon-mediated particle interactions in a controlled collision region, thereby enabling a compact architecture adapted for laboratory-scale implementation and improved efficiency in photon flux utilization.
[0039] According to one exemplary embodiment of the invention, FIG. 1 refers to a schematic view of the bremsstrahlung collider system 100 for photon-mediated particle collisions. In one embodiment herein, the bremsstrahlung collider system 100 enables integrated generation and utilization of photon radiation within a unified architecture, thereby facilitating efficient photon-mediated particle interactions with improved collision probability and system-level operational coherence. The bremsstrahlung collider system 100 incorporates a compact and modular configuration, thereby enabling laboratory-scale deployment while reducing spatial footprint and infrastructure requirements associated with conventional large-scale particle accelerator and collider systems. The bremsstrahlung collider system 100 enhances photon flux density through coordinated beam alignment, focusing, and collimation assemblies, thereby improving interaction efficiency and enabling precise control over photon beam direction and intensity distribution.
[0040] In another embodiment herein, the bremsstrahlung collider system 100 comprises a primary charged particle accelerator 102, a beam path 104, plurality of dipole magnets 106, plurality of quadrupole magnets 108, plurality of radio-frequency (RF) cavities 110, a cryogenic cooling system 112, a beam dump 114, a photon converter 116, a beam alignment and focusing assembly 118, a photon collimation unit 120, a collision region 122, a detection unit 124, one or more energy recovery subsystems 126, and an energy management system 128. In one embodiment herein, the primary charged particle accelerator 102 is configured to generate the electron beam, which is the primary charged particle used in the bremsstrahlung collider system 100. The charged particle source is responsible for creating the electron beam that will be injected into the accelerator system for further manipulation and interaction with other components. This could be an electron gun or a photo-emissive source depending on the accelerator setup. Additionally, the beam path 104 is configured to guide a circulating relativistic electron beam along a closed-loop path.
[0041] In one embodiment herein, the beam path 104 is the central pathway that guides the circulating electron beam. Once generated by the charged particle source 102, the electron beam is injected into the beam path 104, where it will be directed through the accelerator and interaction areas. The closed-loop configuration ensures continuous circulation of the beam. Additionally, the beam path 104 is typically a vacuum chamber that reduces scattering and maintains high beam quality. In one embodiment herein, the dipole magnets 106 are arranged along the beam path 104. The dipole magnets 106 are configured to bend the electron beam trajectory. The dipole magnets 106 are configured for bending the electron beams trajectory, allowing it to follow the closed-loop path within the bremsstrahlung collider system 100. The dipole magnets 106 adjust the path of the beam as it travels through the accelerator ring, helping to guide it toward the photon converter 116. Additionally, the dipole magnets 106 are typically superconducting or normal conducting, depending on the energy requirements of the bremsstrahlung collider system 100.
[0042] In one embodiment herein, the quadrupole magnets 108 are arranged along the beam path 104. The quadrupole magnets 108 are configured to focus and stabilize the electron beam. After the electron beam is bent by the dipole magnets 106, the quadrupole magnets 108 ensure the beam remains tight and focused, maintaining high beam quality and precision as it travels through the bremsstrahlung collider system 100. Additionally, the quadrupole magnets 108 are typically used for beam focusing in high-energy accelerators. In one embodiment herein, the radio-frequency (RF) cavities 110 are operatively coupled to the beam path 104. The RF cavities 110 are configured for accelerating the electron beam to relativistic energy levels during repeated circulation within the closed-loop path. The RF cavities 110 increase the energy of the circulating electron beam by applying high-frequency electromagnetic fields, ensuring that the beam reaches the necessary energies for efficient photon production.
[0043] In one embodiment herein, the cryogenic cooling system 112 is thermally coupled to the RF cavities 110 and the dipole and quadrupole magnets (106, 108). The cryogenic cooling system 112 is configured to maintain superconducting operating conditions and extract thermal energy generated during operation. The cryogenic cooling system 112 cools the components to extremely low temperatures, reducing electrical resistance and ensuring that the accelerator operates with minimal energy loss. Additionally, the cryogenic cooling system 112 is used in accelerator facilities to maintain optimal temperatures for superconducting components. In one embodiment herein, the photon converter 116 having a high atomic number material and is positioned along the beam path 104 within the primary charged particle accelerator 102. The photon converter 116 is configured to generate a photon radiation upon interaction with the relativistic electron beam. The high-energy electron beam generated by the primary charged particle accelerator 102 is directed toward the photon converter 116, where it produces Bremsstrahlung radiation. This radiation is used for subsequent photon-mediated particle interactions.
[0044] In one embodiment herein, the beam dump 114 is operatively connected to the beam path 104. The beam dump 114 is configured to receive the electron beam after interaction with the photon converter 116 and convert residual beam energy into thermal energy. After the electron beam interacts with the photon converter 116, any remaining energy in the beam is safely absorbed by the beam dump 114. This component prevents unwanted beam energy from interfering with the bremsstrahlung collider system 100. In one embodiment herein, the beam alignment and focusing assembly 118 having at least the quadrupole magnets 108 and electromagnetic lenses. The beam alignment and focusing assembly 118 is configured to receive the generated photon radiation and to focus, align, and direct the photon radiation, and to optimize photon flux density and collision probability. After the photon radiation is generated in the photon converter 116, it passes through the beam alignment system 118, which focuses and aligns a photon beam to ensure maximum collision efficiency. The alignment and focusing assembly 118 with the quadrupole magnets 108 that direct the photon beam or radiation.
[0045] In one embodiment herein, the photon collimation unit 120 is configured to restrict the angular dispersion of the photon radiation and to form a directional photon beam. The photon collimation unit 120 ensures that the photon beam is focused and aligned as it is directed into the collision region 122, improving interaction efficiency. The photon collimation unit 120 typically involves apertures or collimators that limit the angular spread of the photon beam. In one embodiment herein, the collision region 122 is located downstream of the photon converter 116. The collision region 122 is configured to receive the directional photon radiation and to enable controlled interaction with at least one secondary particle beam. The interaction achieved through spatial alignment of photon and particle beams within a defined collision volume. The directional photon beam, after being conditioned and collimated, enters the collision region 122, where it interacts with a secondary particle beam or target, facilitating photon-mediated particle interactions. This region may include a vacuum chamber or other systems to reduce scattering losses and improve collision efficiency. Additionally, the secondary particle beam is configured to collide with the generated photons. The secondary particle beam comprises electrons, positrons, protons, ions, and neutral particles.
[0046] In one embodiment herein, the detection unit 124 is configured to measure interaction outcomes within the collision region 122. The detection unit 124 includes at least one of a photon detector, particle detector, and spectrometer. The detection unit 124 captures the results of the interactions, which are then analysed to provide experimental data. The detection unit 124 may include photon detectors, particle detectors, and spectrometers for measuring the interaction products.
[0047] In one embodiment herein, the one or more energy recovery subsystems 126 are operatively coupled to at least one of the dipole magnets 106 for capturing radiation losses generated during beam bending, the RF cavities 110 for capturing radio-frequency losses, the beam dump 114 for capturing thermal energy generated from beam termination, and the cryogenic cooling system 112 for capturing extracted thermal energy. These subsystems convert waste energy from various sources back into usable power, improving the overall energy efficiency of the bremsstrahlung collider system 100. Additionally, the energy recovery subsystems 126 include thermal energy recovery modules, electromagnetic induction units, or thermoelectric generators.
[0048] In one embodiment herein, the energy management system 128 is electrically coupled to the energy recovery subsystems 126 and the RF cavities 110. The energy management system 128 is arranged to convert captured energy into usable electrical or thermal power and to redistribute the usable power to at least the RF cavities 110. The bremsstrahlung collider system 100 ensures that recovered energy is converted into usable electrical or thermal power and redistributed to the necessary components of the accelerator and collider. The bremsstrahlung collider system 100 is adapted to perform photon-mediated particle interactions using the directional photon beam.
[0049] In another embodiment herein, the bremsstrahlung collider system 100 is configured to operate at adjustable energy levels to control the photon energy spectrum, and recovers energy losses from the RF cavities 110, the dipole magnets 106, the beam dump 114, and the cryogenic cooling system 112 for reutilization within the accelerator, thereby enabling photon-photon, photon-electron, photon-ion, and photon-particle collisions in an energy-efficient manner. The photon converter 116 is selected from a group consisting of tungsten, gold, tantalum, platinum, lead, and combinations thereof. The Bremsstrahlung collider system 100 is industrial-applicable as it is compact, energy-efficient, and capable of supporting laboratory-scale experiments, research institutions, and even potential industrial applications in material science and particle physics.
[0050] In another embodiment herein, the primary charged particle accelerator 102 is selected from a group consisting of a linear accelerator, a synchrotron, a cyclotron, and a plasma-based accelerator. The collision region 122 comprises a vacuum chamber configured to reduce scattering losses and improve interaction efficiency. The photon collimation unit 120 comprises one or more apertures or collimators configured to restrict angular dispersion of the photon beam. The charged particle source 102 may comprise a thermionic electron gun capable of emitting an electron beam for injection into the beam path 104, or a photo emissive source that generates electrons via light-induced emission.
[0051] In one embodiment herein, the cryogenic cooling system 112 may consist of liquid nitrogen-based cooling loops for superconducting magnets and RF cavities 110, and a helium-based cooling system for more advanced superconducting applications requiring lower temperatures. The photon converter 116 could be made of high atomic number materials such as tungsten, gold, or tantalum, or it could use composite materials designed to enhance photon generation efficiency in specialized energy ranges. The beam alignment and focusing assembly 118 may incorporate quadrupole magnets 108 for beam focusing, along with electromagnetic lenses designed to fine-tune the photon beam path 104, ensuring minimal beam loss and maximum photon density at the collision region 122.
[0052] In one embodiment herein, the detection system 124 could include photon detectors such as silicon photomultipliers or scintillation detectors to measure photon energy and particle velocity, and particle detectors like time-of-flight (TOF) detectors to track the secondary particle behavior. The energy recovery subsystems 126 could include thermoelectric generators that capture waste heat from the RF cavities 110 and the beam dump 114, or magnetic recovery coils designed to capture and convert electromagnetic radiation into usable electrical energy. The energy management system 128 could incorporate power electronics such as voltage regulators, capacitors, or battery storage systems to store and manage recovered energy, redistributing it as needed to maintain operational efficiency of the primary charged particle accelerator 102.
[0053] In one embodiment herein, a method for controlling adjustable energy levels utilizes real-time feedback to adjust the RF field strength in the RF cavities 110. This is achieved using variable RF power amplifiers that continuously monitor the electron beam energy and adjust the field amplitude and frequency in the RF cavities 110 to maintain the desired energy level for photon generation. This allows the bremsstrahlung collider system 100 to optimize the photon energy spectrum dynamically. Next, the magnetic field generated by the dipole magnets 106 may be adjusted in real-time by varying the current supplied to the magnet coils. This allows the bremsstrahlung collider system 100 to control the curvature of the electron beam, thus influencing the photon energy by adjusting the beam’s interaction time with the photon converter 116. The field strength is dynamically altered based on energy feedback from the RF cavities 110 and beam energy sensors, ensuring that the energy of the photon beam remains within the required parameters for each experiment. The modulation can be adjusted based on the experimental conditions, allowing for the generation of a variable photon spectrum.
[0054] According to another exemplary embodiment of the invention, FIG. 2A refers to a schematic view of the radio-frequency cavities 110. In one embodiment herein, the radio-frequency cavities 110 comprise a resonant cavity body defining an enclosed conductive chamber. The internal geometry of the radio-frequency cavities 110 is configured to support standing electromagnetic wave modes, thereby generating an oscillating electric field within the cavity volume. The beam path 104 passes through the radio-frequency cavities 110 along a longitudinal axis, thereby enabling the relativistic electron beam to traverse the cavity while interacting with the electric field established therein. An RF input coupler is operatively connected to the resonant cavity body. The RF input coupler is configured to introduce high-frequency electromagnetic power into the radio-frequency cavities 110 from an external RF power source. Within the radio-frequency cavities 110, an oscillating electric field is generated across the cavity gap. The electric field is oriented along the beam propagation direction defined by the beam path 104. The electric field accelerates charged particles by imparting kinetic energy to the electron beam each time the beam traverses the cavity during circulation within the closed-loop structure of the bremsstrahlung collider system 100.
[0055] The radio-frequency cavities 110 are structurally coupled to the cryogenic cooling system 112. The cryogenic cooling system 112 maintains superconducting operating conditions of the cavity walls to reduce resistive losses and enhance quality factor of the resonant structure. The thermal energy generated due to RF losses within the cavity walls is extracted through the cryogenic cooling system 112 and is further available for capture by the energy recovery subsystems 126 for subsequent conversion and reutilization. In operation, the electron beam generated by the charged particle source accelerator 102 is guided through the beam path 104 and repeatedly passes through the radio-frequency cavities 110, where synchronized RF excitation produces a time-varying electric field 110B that accelerates the electron beam to relativistic energy levels. The phase of the RF field is controlled such that the electron beam experiences a net accelerating force during each pass through the cavity, thereby progressively increasing beam energy over multiple cycles.
[0056] The radio-frequency cavities 110 further enable controlled energy modulation of the electron beam by adjusting RF amplitude, frequency, and phase parameters, thereby facilitating precise control of beam energy prior to interaction with the Bremsstrahlung conversion target 116. The RF input coupler may be configured to support variable power input, thereby enabling dynamic tuning of the accelerating gradient within the cavity. In one embodiment, the radio-frequency cavities 110 comprise superconducting cavities fabricated from niobium or niobium-based alloys. The superconducting material enables operation at cryogenic temperatures with minimal surface resistance and high energy efficiency. In another embodiment, the radio-frequency cavities 110 comprise normal-conducting metallic cavities constructed from copper or copper alloys, suitable for lower energy or compact configurations.
[0057] In one embodiment herein, the RF input coupler comprises a waveguide-based coupler or coaxial coupler. The coupling strength is adjustable to optimize power transfer efficiency and maintain stable cavity operation. The internal geometry of the radio-frequency cavities 110 may be configured as elliptical, cylindrical, or re-entrant structures to support desired resonant modes and enhance accelerating field uniformity. Additionally, the radio-frequency cavities 110 are configured in a multi-cell arrangement, where multiple resonant sections are coupled together to increase the effective accelerating length and improve overall acceleration efficiency of the electron beam. During operation, the RF losses generated within the cavity walls and coupler interfaces are captured as thermal energy by the cryogenic cooling system 112, and the extracted thermal energy is transferred to the energy recovery subsystems 126. The energy recovery subsystems 126 convert the thermal energy into usable electrical or thermal power. The converted energy is subsequently managed by the energy management system 128 and redistributed to power the radio-frequency cavities 110 and associated components, thereby reducing net external energy consumption.
[0058] According to another exemplary embodiment of the invention, FIG. 2B refers to a perspective view of the bremsstrahlung collider system 100 with resistive losses. In one embodiment herein, the dipole magnets 106 in the bremsstrahlung collider system 100 are crucial for bending the electron beam that circulates through the beam path 104. The primary function of the dipole magnets 106 is to ensure that the electron beam follows the correct curved path within the closed-loop accelerator. The dipole magnets 106 generate a magnetic field that interacts with the charged electron beam, causing it to deviate from a straight line and follow a circular trajectory, as required for the system’s operation. As the electron beam interacts with the magnetic field of the dipole magnets 106, resistive losses occur due to the inherent resistance of the materials used in the dipole magnets 106, such as copper or superconducting alloys. These losses are manifested as thermal energy, which is dissipated from the dipole magnets 106 into the surrounding environment. The resistive losses must be managed to ensure that the bremsstrahlung collider system 100 operates efficiently, with thermal energy being captured and dealt with appropriately.
[0059] To minimize the resistive losses, the dipole magnets 106 may be fabricated using superconducting materials, such as niobium-titanium or niobium-tin alloys. These superconducting magnets require cryogenic cooling to maintain superconducting conditions, which are critical for reducing resistive losses and improving overall system efficiency. The cryogenic cooling system 112 is thermally coupled to the dipole magnets 106, ensuring that they operate in a superconducting state and that thermal dissipation is minimized during operation. The resistive losses generated by the dipole magnets 106 are captured by the cryogenic cooling system 112 in the case of superconducting magnets, or by thermal recovery systems 126 in the case of normal-conducting magnets. These systems convert the waste thermal energy into usable power, improving the overall energy efficiency of the bremsstrahlung collider system 100.
[0060] According to another exemplary embodiment of the invention, FIG. 2C refers to a perspective view of the beam dump 114. Once the electron beam passes through the photon converter 116 and generates the Bremsstrahlung radiation, any remaining energy in the beam that has not been utilized in photon generation is directed towards the beam dump 114. The beam dump 114 is strategically placed to ensure that all residual energy from the electron beam is safely absorbed. The beam dump 114 might be coupled with a thermal management system to prevent overheating, and it may be adapted to convert the captured energy into usable thermal power, which might be captured by the energy recovery subsystems 126 for further utilization in the bremsstrahlung collider system 100.
[0061] In one embodiment herein, the beam dump 114 is liquid-cooled, where water or another cooling fluid circulates through the beam dump 114 to carry away the heat generated by the electron beam’s energy. This cooling mechanism ensures that the thermal load on the bremsstrahlung collider system 100 does not exceed safe operating limits. Another embodiment may involve a solid-state beam dump 114, which utilizes high-density materials like tungsten to directly absorb and dissipate the heat generated by the electron beam. In this case, the beam dump 114 may be equipped with high-efficiency heat exchangers to manage the thermal energy effectively. Additionally, the beam dump 114 is an integral part of the energy recovery loop. The energy that is not converted into photon radiation in the photon converter 116 is absorbed by the beam dump 114. In systems with superconducting magnets or high-energy RF cavities 110, the residual heat from the beam dump 114 is captured and managed by the cryogenic cooling system 112 or other thermal recovery systems 126. The energy that is recovered from the beam dump 114 may be converted into usable electrical or thermal power and redistributed throughout the bremsstrahlung collider system 100 via the energy management system 128. This process significantly enhances the overall energy efficiency of the bremsstrahlung collider system 100 by minimizing waste and optimizing energy usage.
[0062] In one embodiment herein, the primary charged particle accelerator 102 may be configured as a laser-driven plasma accelerator, which uses high-intensity lasers to generate electron beams in a compact manner. This setup could be advantageous for smaller-scale applications or portable accelerator systems. The beam path 104 could be constructed as a magnetically levitated beam path, using magnetic fields to levitate the electron beam, thereby reducing friction and improving the efficiency of beam transport. This would reduce power consumption in the beam guidance system and enhance system longevity. The dipole magnets 106 may be designed with superconducting coil windings that allow for extremely high magnetic field strengths with minimal resistive losses. This would increase the beam bending efficiency and reduce the power consumption for higher-energy applications.
[0063] The quadrupole magnets 108 may be multifunctional, incorporating adjustable magnetic gradients that can be dynamically tuned during operation to compensate for variations in beam stability or to optimize focusing at various energy levels. The radio-frequency (RF) cavities 110 could be dual-mode cavities, capable of providing both longitudinal and transverse electromagnetic fields for dual purposes, acceleration and focusing of the electron beam, allowing for a more compact and energy-efficient system. The photon converter 116 may be constructed using nanostructured materials, such as nanotube-based composites, to enhance photon generation efficiency. The materials would allow for better interaction with high-energy electrons, leading to an increase in the number of high-energy photons generated.
[0064] The beam dump 114 may feature multi-layered absorption modules, where each layer is optimized for absorbing a specific energy range of residual beam energy. This would improve the overall thermal management and beam termination efficiency. The cryogenic cooling system 112 could integrate regenerative heat exchangers that capture the waste heat from the system, which could then be reused to pre-cool incoming coolant, increasing overall cooling efficiency. The energy recovery subsystems 126 may include a high-efficiency thermophotovoltaic (TPV) system, which converts the thermal energy from the beam dump 114 into usable electrical power, enhancing the energy efficiency of the bremsstrahlung collider system 100. The bremsstrahlung collider system 100 may be configured in a modular design, where key components such as the photon converter 116, the beam dump 114, and the RF cavities 110 are designed for easy replacement or upgrade. This modular approach would enable scalability and ease of maintenance for various applications, from research labs to industrial facilities.
[0065] The collision region 122 could be designed with adjustable vacuum levels to reduce scattering losses, allowing for precise control over particle interactions. Additionally, this collision region 122 could incorporate targeted electromagnetic shielding to minimize interference from external fields. The detection system 124 could include multiple detection modules, including time-of-flight (TOF) detectors, silicon photomultipliers, and calorimeters, integrated into a multi-layered detector array. This bremsstrahlung collider system 100 would allow for a comprehensive analysis of photon-mediated particle interactions at different energy levels and angles. The energy management system 128 could be enhanced with machine learning algorithms to dynamically adjust power distribution based on real-time performance metrics, optimizing energy usage across the system. The bremsstrahlung collider system 100 could also be integrated with smart grid technologies for future scalability in industrial applications.
[0066] In one embodiment herein, the bremsstrahlung collider system 100 includes variable power RF amplifiers or feedback-controlled RF systems for dynamic tuning of the photon energy spectrum. The bremsstrahlung collider system 100 comprises real-time beam alignment feedback mechanisms using beam position sensors and adaptive magnetic steering coils, continuously optimizing photon beam trajectory to ensure the highest interaction efficiency. The beam dump 114 includes liquid-metal cooling systems for high thermal energy absorption, coupled with thermoelectric generators for converting residual heat into electrical power, which is then redirected to support system components. In another embodiment herein, the bremsstrahlung collider system 100 is configured to generate multiple electron beams in parallel, enabling simultaneous photon generation and interaction across several experimental regions. Additionally, the bremsstrahlung collider system 100 is designed in a modular fashion, where components such as the photon converter 116, beam dump 114, and RF cavities 110 can be easily replaced or upgraded, offering scalability for diverse applications.
[0067] In another embodiment herein, the dipole magnets 106 are configured to support dynamic field adjustment, where the magnetic field strength can be varied in real-time to correct beam deviations and ensure precise photon generation. The detection system 124 comprises multi-modal sensors, including time-of-flight (TOF) detectors for particle velocity analysis, scintillation detectors for high-energy photon detection, and calorimeters for precise energy measurement during photon-mediated particle collisions. The cryogenic cooling system 112 uses liquid helium for ultra-low-temperature cooling, supporting superconducting magnets and minimizing resistive losses in high-energy systems. The bremsstrahlung collider system 100 is integrated with smart power management technologies, including AI-driven control systems, to optimize the energy distribution across components based on real-time load and power requirements.
[0068] According to another exemplary embodiment of the invention, FIG. 3 refers to a flowchart 300 of a method for performing energy-efficient photon-mediated particle interactions using the bremsstrahlung collider system 100. At step 302, the electron beam is generated by using the primary charged particle accelerator 102 and guides the electron beam through the beam path 104 along the closed-loop path using the plurality of dipole magnets 106. At step 304, the electron beam is focused and stabilized using the plurality of quadrupole magnets 108 and accelerated to relativistic energy levels using one or more radio-frequency (RF) cavities 110.
[0069] At step 306, the superconducting operating conditions of the RF cavities 110 are maintained, and the dipole and quadrupole magnets (106, 108) are used with the cryogenic cooling system 112. At step 308, the relativistic electron beam is directed onto the photon converter 116, comprising a high atomic number material to generate photon radiation, and receives the generated photon radiation using the beam alignment and focusing assembly 118.
[0070] At step 310, the photon radiation is collimated using the photon collimation unit 120 to form the directional photon beam and is delivered into the collision region 122. At step 312, at least one secondary particle beam or target is introduced into the collision region 122 to enable photon-mediated particle interactions and detect the outcomes using the detection unit 124. At step 314, the energy losses are captured and generated during beam acceleration, beam bending, beam termination, and thermal dissipation using one or more energy recovery subsystems 126. At step 316, captured energy losses are converted into usable electrical and thermal power using the energy management system 128 and redistributed the usable power to at least the RF cavities 110 to support continued operation of the bremsstrahlung collider system 100.
[0071] Numerous advantages of the present disclosure may be apparent from the discussion above. In accordance with the present disclosure, the bremsstrahlung collider system 100 is disclosed. The proposed bremsstrahlung collider system 100 enables integrated generation and utilization of photon radiation within a unified architecture, thereby facilitating efficient photon-mediated particle interactions with improved collision probability and system-level operational coherence. The bremsstrahlung collider system 100 incorporates a compact and modular configuration, thereby enabling laboratory-scale deployment while reducing spatial footprint and infrastructure requirements associated with conventional large-scale particle accelerator and collider systems.
[0072] The bremsstrahlung collider system 100 enhances photon flux density through coordinated beam alignment, focusing, and collimation assemblies, thereby improving interaction efficiency and enabling precise control over photon beam direction and intensity distribution. The bremsstrahlung collider system 100 supports photon-mediated interactions, including photon–photon, photon–electron, and photon–ion collisions, thereby expanding experimental capabilities and enabling versatile investigation of particle interaction phenomena within a single system. The bremsstrahlung collider system 100 enables adjustable energy operation of the accelerated electron beam and resulting photon spectrum, thereby allowing optimization of collision conditions for different particle types and experimental requirements.
[0073] The bremsstrahlung collider system 100 improves energy utilization efficiency by directing generated Bremsstrahlung photons into a controlled collision region 122, thereby minimizing energy losses and enhancing effective conversion of beam energy into usable interaction events. The bremsstrahlung collider system 100 integrates detection mechanisms, including photon and particle detectors configured to measure interaction outcomes, thereby enabling accurate analysis, monitoring, and characterization of photon-mediated collision processes within the bremsstrahlung collider system 100.
[0074] It will readily be apparent that numerous modifications and alterations can be made to the processes described in the foregoing examples without departing from the principles underlying the invention, and all such modifications and alterations are intended to be embraced by this application. 
5. CLAIMS:
We Claim:
1. A bremsstrahlung collider system (100) for photon-mediated particle collisions, comprising:
a primary charged particle accelerator (102) including a beam path (104) configured to guide a circulating relativistic electron beam along a closed-loop path;
plurality of dipole magnets (106) arranged along the beam path (104), wherein the dipole magnets (106) are configured to bend a trajectory of the electron beam;
plurality of quadrupole magnets (108) arranged along the beam path (104), wherein the quadrupole magnets (108) are configured to focus and stabilize the electron beam;
one or more radio-frequency (RF) cavities (110) operatively coupled to the beam path (104), wherein the RF cavities (110) are configured to accelerate the electron beam to relativistic energy levels during circulation within the closed-loop path;
a cryogenic cooling system (112) thermally coupled to the RF cavities (110) and the dipole and quadrupole magnets (106, 108), wherein the cryogenic cooling system (112) is configured to maintain superconducting operating conditions and extract thermal energy generated during operation;
a photon converter (116) having a high atomic number material and positioned along a beam path (104) within the primary charged particle accelerator (102), wherein the photon converter (116) is configured to generate a photon radiation upon interaction with the relativistic electron beam;
a beam dump (114) operatively connected to the beam path (104), wherein the beam dump (114) is configured to receive the electron beam after interaction with the photon converter (116) and convert residual beam energy into thermal energy;
a beam alignment and focusing assembly (118) having at least one set of electromagnetic lenses and quadrupole magnets, wherein the beam alignment and focusing assembly (118) is arranged along a photon path to focus and direct photon radiation;
a photon collimation unit (120) configured to restrict angular dispersion of the photon radiation to form a directional photon beam;
a collision region (122) located downstream of the photon converter (116), wherein the collision region (122) having a vacuum chamber configured to receive the directional photon beam and to enable controlled interaction with at least one secondary particle beam;
a detection unit (124) configured to measure interaction outcomes within the collision region (122), wherein the detection unit (124) includes at least one of a photon detector, particle detector, and spectrometer;
one or more energy recovery subsystems (126) operatively coupled to at least one of the dipole magnets (106), the RF cavities (110), the beam dump (114), and the cryogenic cooling system (112) to capture energy losses generated during operation; and
an energy management system (128) electrically coupled to the energy recovery subsystems (126) and the RF cavities (110), wherein the energy management system (128) is arranged to convert captured energy into usable electrical or thermal power and to redistribute the usable power to at least the RF cavities (110),
wherein the bremsstrahlung collider system (100) is adapted to perform photon-mediated particle interactions using the directional photon beam.
2. The bremsstrahlung collider system (100) as claimed in claim 1, wherein the bremsstrahlung collider system (100) is configured to operate at adjustable energy levels to control a photon energy spectrum, and to recover energy losses from the RF cavities (110), the dipole magnets (106), the beam dump (114), and the cryogenic cooling system (112) for reutilization within the accelerator.
3. The bremsstrahlung collider system (100) as claimed in claim 1, wherein the secondary particle beam comprises electrons, positrons, protons, ions, or neutral particles configured to interact with the photon radiation within the collision region (122).
4. The bremsstrahlung collider system (100) as claimed in claim 1, wherein the photon converter (116) comprises tungsten, gold, tantalum, platinum, lead, or combinations thereof.
5. The bremsstrahlung collider system (100) as claimed in claim 1, wherein the primary charged particle accelerator (102) comprises a linear accelerator, a synchrotron, a cyclotron, or a plasma-based accelerator.
6. The bremsstrahlung collider system (100) as claimed in claim 1, wherein the collision region (122) comprises the vacuum chamber configured to reduce scattering losses and improve interaction efficiency.
7. The bremsstrahlung collider system (100) as claimed in claim 1, wherein the photon collimation unit (120) comprises one or more apertures or collimators arranged to restrict angular dispersion of a photon beam.
8. A method for performing energy-efficient photon-mediated particle interactions using a bremsstrahlung collider system (100), comprising:
generating an electron beam using the primary charged particle accelerator (102) and guiding the electron beam through a beam path (104) along a closed-loop path using the plurality of dipole magnets (106);
focusing and stabilizing the electron beam using plurality of quadrupole magnets (108) and accelerating the electron beam to relativistic energy levels using one or more radio-frequency (RF) cavities (110);
maintaining superconducting operating conditions of the RF cavities (110) and the dipole and quadrupole magnets (106, 108) using a cryogenic cooling system (112);
directing the relativistic electron beam onto the photon converter (116) comprising a high atomic number material to generate photon radiation, and receiving the generated photon radiation using a beam alignment and focusing assembly (118);
collimating the photon radiation using a photon collimation unit (120) to form a directional photon beam and delivering the directional photon beam into a collision region (122);
introducing at least one secondary particle beam or target into the collision region (122) to enable photon-mediated particle interactions and detecting outcomes using a detection unit (124);
capturing energy losses generated during beam acceleration, beam bending, beam termination, and thermal dissipation using one or more energy recovery subsystems (126); and
converting the captured energy losses into usable electrical and thermal power using an energy management system (128) and redistributing the usable power to at least the RF cavities (110) to support continued operation of the bremsstrahlung collider system (100).
6. DATE AND SIGNATURE:
Dated this 22nd day of April, 2026

 
7. ABSTRACT:
Title: A Bremsstrahlung Collider System for Photon-Mediated Particle Collisions and Method Thereof
The present disclosure proposes a bremsstrahlung collider system (100) that is configured to generate photon radiation and facilitate photon-mediated particle interactions in a controlled collision region, thereby enabling a compact architecture adapted for laboratory-scale implementation and improved efficiency in photon flux utilization. The bremsstrahlung collider system (100) comprises a primary charged particle accelerator (102), a beam path (104), plurality of dipole magnets (106), plurality of quadrupole magnets (108), plurality of radio-frequency (RF) cavities (110), a cryogenic cooling system (112), a beam dump (114), a photon converter (116), a beam alignment and focusing assembly (118), a photon collimation unit (120), a collision region (122), a detection unit (124), one or more energy recovery subsystems (126), and an energy management system (128). The bremsstrahlung collider system (100) supports photon-mediated interactions, including photon–photon, photon–electron, and photon–ion collisions, expanding experimental capabilities and enabling versatile investigation of particle interaction phenomena.

, Claims:We Claim:
1. A bremsstrahlung collider system (100) for photon-mediated particle collisions, comprising:
a primary charged particle accelerator (102) including a beam path (104) configured to guide a circulating relativistic electron beam along a closed-loop path;
plurality of dipole magnets (106) arranged along the beam path (104), wherein the dipole magnets (106) are configured to bend a trajectory of the electron beam;
plurality of quadrupole magnets (108) arranged along the beam path (104), wherein the quadrupole magnets (108) are configured to focus and stabilize the electron beam;
one or more radio-frequency (RF) cavities (110) operatively coupled to the beam path (104), wherein the RF cavities (110) are configured to accelerate the electron beam to relativistic energy levels during circulation within the closed-loop path;
a cryogenic cooling system (112) thermally coupled to the RF cavities (110) and the dipole and quadrupole magnets (106, 108), wherein the cryogenic cooling system (112) is configured to maintain superconducting operating conditions and extract thermal energy generated during operation;
a photon converter (116) having a high atomic number material and positioned along a beam path (104) within the primary charged particle accelerator (102), wherein the photon converter (116) is configured to generate a photon radiation upon interaction with the relativistic electron beam;
a beam dump (114) operatively connected to the beam path (104), wherein the beam dump (114) is configured to receive the electron beam after interaction with the photon converter (116) and convert residual beam energy into thermal energy;
a beam alignment and focusing assembly (118) having at least one set of electromagnetic lenses and quadrupole magnets, wherein the beam alignment and focusing assembly (118) is arranged along a photon path to focus and direct photon radiation;
a photon collimation unit (120) configured to restrict angular dispersion of the photon radiation to form a directional photon beam;
a collision region (122) located downstream of the photon converter (116), wherein the collision region (122) having a vacuum chamber configured to receive the directional photon beam and to enable controlled interaction with at least one secondary particle beam;
a detection unit (124) configured to measure interaction outcomes within the collision region (122), wherein the detection unit (124) includes at least one of a photon detector, particle detector, and spectrometer;
one or more energy recovery subsystems (126) operatively coupled to at least one of the dipole magnets (106), the RF cavities (110), the beam dump (114), and the cryogenic cooling system (112) to capture energy losses generated during operation; and
an energy management system (128) electrically coupled to the energy recovery subsystems (126) and the RF cavities (110), wherein the energy management system (128) is arranged to convert captured energy into usable electrical or thermal power and to redistribute the usable power to at least the RF cavities (110),
wherein the bremsstrahlung collider system (100) is adapted to perform photon-mediated particle interactions using the directional photon beam.
2. The bremsstrahlung collider system (100) as claimed in claim 1, wherein the bremsstrahlung collider system (100) is configured to operate at adjustable energy levels to control a photon energy spectrum, and to recover energy losses from the RF cavities (110), the dipole magnets (106), the beam dump (114), and the cryogenic cooling system (112) for reutilization within the accelerator.
3. The bremsstrahlung collider system (100) as claimed in claim 1, wherein the secondary particle beam comprises electrons, positrons, protons, ions, or neutral particles configured to interact with the photon radiation within the collision region (122).
4. The bremsstrahlung collider system (100) as claimed in claim 1, wherein the photon converter (116) comprises tungsten, gold, tantalum, platinum, lead, or combinations thereof.
5. The bremsstrahlung collider system (100) as claimed in claim 1, wherein the primary charged particle accelerator (102) comprises a linear accelerator, a synchrotron, a cyclotron, or a plasma-based accelerator.
6. The bremsstrahlung collider system (100) as claimed in claim 1, wherein the collision region (122) comprises the vacuum chamber configured to reduce scattering losses and improve interaction efficiency.
7. The bremsstrahlung collider system (100) as claimed in claim 1, wherein the photon collimation unit (120) comprises one or more apertures or collimators arranged to restrict angular dispersion of a photon beam.
8. A method for performing energy-efficient photon-mediated particle interactions using a bremsstrahlung collider system (100), comprising:
generating an electron beam using the primary charged particle accelerator (102) and guiding the electron beam through a beam path (104) along a closed-loop path using the plurality of dipole magnets (106);
focusing and stabilizing the electron beam using plurality of quadrupole magnets (108) and accelerating the electron beam to relativistic energy levels using one or more radio-frequency (RF) cavities (110);
maintaining superconducting operating conditions of the RF cavities (110) and the dipole and quadrupole magnets (106, 108) using a cryogenic cooling system (112);
directing the relativistic electron beam onto the photon converter (116) comprising a high atomic number material to generate photon radiation, and receiving the generated photon radiation using a beam alignment and focusing assembly (118);
collimating the photon radiation using a photon collimation unit (120) to form a directional photon beam and delivering the directional photon beam into a collision region (122);
introducing at least one secondary particle beam or target into the collision region (122) to enable photon-mediated particle interactions and detecting outcomes using a detection unit (124);
capturing energy losses generated during beam acceleration, beam bending, beam termination, and thermal dissipation using one or more energy recovery subsystems (126); and
converting the captured energy losses into usable electrical and thermal power using an energy management system (128) and redistributing the usable power to at least the RF cavities (110) to support continued operation of the bremsstrahlung collider system (100).