High Energy Accelerator Research Organization (KEK)
Public Relation Office, Head
Research and Development on the Accelerator Target and Beam Window Materials
by RaDIATE International Collaboration
The large-scale proton accelerator facilities around the world, such as Femi National Accelerator Laboratory (FNAL) at Illinois, U.S.A. and Japan Proton Accelerator Research Complex (J-PARC) at Tokai- village, Ibaraki-prefecture, Japan, accelerate proton beams and collide them with target materials (referred to as “irradiation”). The collisions produce particles, such as neutrinos, hadrons, neutrons, and muons, which are subsequently used for research into elementary particle and nuclear physics, material and life sciences, and for the development of fusion reactors and accelerator-driven nuclear transmutation systems. The accelerator operates under vacuum to lower the probability of scattering the accelerated protons by air molecules. The target is situated inside of a helium-filled or nitrogen-filled chamber referred to as the target station that must be separated from the accelerator chamber by a thin metal membrane referred to as the “beam window” (Fig.1). The beam window is repeatedly exposed to a high-intensity proton beam accelerated towards the target, subjecting the metal window to instantaneous thermal shocks that create pressure waves.
For the beam window, thin, lightweight materials are chosen to minimize the deposited energy and subsequent heating, and high strength is desired to withstand the repeated thermal shocks. However, when beam windows and target materials are exposed to the proton beam, atomic displacements (referred to as “radiation damage”) occur that knock atoms and clusters of atoms from their atomic lattice sites in metals. Radiation damage is a serious problem that degrades the mechanical properties of the material, and depending on the temperature, can cause dimensional changes due to void swelling and accumulation of defects.
For the validation of the leptonic charge-parity (CP) violation (#1), both FNAL and J-PARC are planning to increase their beam intensities to Mega-Watt class, which is much higher than the current power. To enable this push to the frontier of high energy physics, it is important to predict and even increase the lifetime of targets and beam windows by developing or choosing radiation damage tolerant materials.
To address this problem, several leading accelerator laboratories and reactor/fusion research facilities in the U.S.A., Europe, and Japan are cooperating under the RaDIATE international collaboration (*2). From 2017 to 2018, the RaDIATE collaboration performed a proton irradiation experiment in the Brookhaven Linac Isotope Producer (BLIP) at Brookhaven National Laboratory (BNL), the aim of which was to expose various candidate materials for beam windows and targets to a high-intensity proton beam. Titanium alloys were included in the irradiated materials of the experiment, motivated by the current and future use of the titanium alloys for the beam windows at the J-PARC neutrino experimental facility and the potential use of Ti alloys for beam windows for neutrino beam facilities at Fermilab (Long-Baseline Neutrino Facility). There are concerns that the beam windows may not withstand the continual thermal shocks at the expected much higher beam powers because of radiation-induced changes in mechanical properties. After irradiation, material specimens were then transported to Pacific Northwest National Laboratory (PNNL) for detailed examinations by the state-of-the-art analytical equipment. Figure 2 shows some of the titanium alloy material specimens assembled inside a container, referred to as an irradiation capsule, prior to capsule sealing and irradiation.
Research Methods and Achievements
Up to now, the J-PARC neutrino experimental facility employs titanium alloy Ti-6Al-4V, ze., titanium (Ti) with the addition of 6% aluminum (Al) and 4% vanadium (V), for its beam window, which has a high strength among lightweight titanium alloys. When pure Ti is heated to 885°C, the titanium undergoes a phase transformation from the lower temperature α-phase to the higher temperature β-phase.
The Al and V are intentionally added because they stabilize the α-phase and β-phase, respectively, producing an alloy that can be heat treated to produce a dual-phase structure that can be tailored to yield desired mechanical properties (Fig. 3).
However, after irradiation, tensile tests on the Ti-6Al-4V specimens irradiated to relatively low doses exhibited almost complete loss of uniform elongation and the associated increase in the yield point (termed embrittlement}, which may impact the performance of the beam window (*3). On the other hand, the Ti-3Al-2.5V alloy, another dual α+β phase alloy but with less β-phase, retained uniform elongation of three percent, even after three times more irradiation (Fig. 4).
To begin to understand the cause of this remarkable difference of tensile behavior between these two alloys, the irradiated Ti-6Al-4V has been investigated using a state-of-the-art transmission electron microscope capable of atomic resolution and various analytical modes to probe chemical and structural changes at the nanoscale and above. As a result, a high density of defect clusters forming small dislocation loops was found in the α-phase, and an even higher density of very fine precipitates, referred to as “ω-phase”, evolved during irradiation in the β-phase (Fig. 5). A precursor to the ω-phase was present in the alloy before irradiation, but irradiation accelerated the precipitation of this phase, which is known to significantly reduce the ductility of the alloy. All these facts suggest that the significant loss of uniform elongation in the Ti-6AI-4V alloy after irradiation is due to the high density of small defect clusters in the a-phase, further exacerbated by the evolution of the ω-phase in the intergranular β-phase. Further work is needed to completely understand the differences between the two alloys.
Significance of the Achievement and Expectation for Future Studies
So far, the titanium alloy Ti-6AI-4V has been utilized as the beam window at the high-intensity proton accelerator facilities. However, it has now been shown that the alloy loses uniform elongation after exposure to relatively low proton doses. It may not be applicable as a beam window for the next-generation of neutrino experimental facilities at FNAL and J-PARC at much higher beam power. Exploration of other alloys and different thermomechanical processing was pursued to identify an acceptable candidate material that can handle the high beam power. Through this research, insight has been gained into how the different titanium alloy grades respond to irradiation. In fact, according to research by the RaDIATE Collaboration, one alloy in particular exhibited much less degradation of material properties after irradiation. This research achieved a major milestone towards the development of a suitable beam window material to handle the higher power beam operations. This research also can be beneficial to the development of radiation- resistant Ti alloys, which may play a role in fusion reactors and accelerator-driven nuclear transmutation systems.
The RaDIATE international collaboration engages in collaborative research to find solutions for the target and beam window materials, which impact all of the premier extensive accelerator facilities in the world. The collaborative approach of international research activities are imperative to help realize the selection of suitable materials for unprecedented high-intensity accelerator operation, which will help drive the breakthroughs in particle and nuclear physics, material and life sciences, and accelerator-driven nuclear transformation technologies.
Tensile behavior of dual-phase titanium alloys under high-intensity proton beam exposure: radiation-induced omega phase transformation in Ti-6Al-4V
Taku Ishida1,2, Eiichi Wakai1,3,Shunsuke Makimura1,2, Andrew M. Casella4, Danny J. Edwards4,Ramprashad Prabhakaran4, David J. Senor4,Kavin Ammigan5, Sujit Bidhar5, Patrick G. Hurh5, Frederique Pellemoine5, Christopher J. Densham6, Michael D. Fitton
On behalf of the RaDIATE COLLABORATION
1J-PARC, 2KEK, 3JAEA, 4PNNL, 5FNAL, 6STFC RAL, 7BNL
Journal of Nuclear Materials
Media Contacts for Further Inquiries
Minako Abe, PR section, J-PARC
Hajime Hikino, PR office, High Energy Accelerator Research Organization (KEK, Japan)
Hiroko Tada, PR office, Institute of Particle and Nuclear Studies, High Energy Accelerator Research Organization (KEK, Japan)
Globally and in Japan:
Dr. Taku Ishida, neutrino section, J-PARC center
Globally and in United States:
Dr. David Senor, Energy and Environment Directorate, Pacific Northwest National Laboratory
Phone: +1-(509) 371-6936
Globally and in Europe:
Dr. Christopher J. Densham, High Power Targets Group, Rutherford Appleton Laboratory
Dr. Kavin Ammigan, High-Power High-Intensity Targetry R&D Group, Target Systems Department, Fermi National Accelerator Laboratory
Dr. Dohyun Kim, Medical Isotope Research & Production group
Phone: +1 (631) 344-7850
About RaDIATE International Collaboration:
Dr. Frederique Pellemoine, High-Power High-Intensity Targetry R&D Group, Target Systems Department, Fermi National Accelerator Laboratory
Phone: +1 (630) 840-6267
*1 Leptonic CP violation
The reason for the overwhelming existence of matter relative to anti-matter in our universe is a fundamental mystery. Modern cosmology posits that this condition originated from the “violation” of a fundamental law of physics. The laws of physics are basically symmetric, and the laws applicable to matter particles are also valid for anti-matter particles. Meanwhile, it is known that there is a tiny amount of violation in the symmetry between quarks (elementary particles that constitute matter) and anti-quarks. This symmetry breaking, referred to as “Charge-conjugation (C)- Parity (P) symmetry violation”, has not been observed yet on the other fundamental particle group called “leptons”, which consists of electrons, muons, and neutrinos. Recently, the T2K international collaboration made an announcement that they obtained an indication of a fairly large CP violation between neutrinos and anti-neutrinos, which were generated at J-PARC, and detected at an underground neutrino observatory 295 km away called “SuperKamiokande” (check reference). To confirm this indication, a project is underway in Japan to increase the beam power at J-PARC and to construct the “Hyper-Kamiokande” detector with 8 times larger fiducial volume than Super-Kamiokande. In the U.S.A., a project is underway to direct neutrinos from the LongBaseline Neutrino Facility (LBNF), under construction at FNAL in Illinois, to a detector 1,300 km away at the Deep Underground Neutrino Experiment (DUNE) in South Dakota. To perform these experiments, scheduled to start around 2027, it is necessary to increase the beam power of the proton accelerators that produce neutrinos to Mega-Watt class. Thus, developing materials for targets and beam windows that can tolerate radiation damage from the unprecedented high beam power is crucial.
(reference)：J-PARC press release (2020.04.16)
Published in Nature, the results are a major step forward in the study of difference between matter and antimatter
*2 RaDIATE International Collaboration
RaDIATE is an abbreviation of “Radiation Damage In Accelerator Target Environments”. In 2012, FNAL and STFC advocated the necessity to promote research and development for materials under accelerator target environments, i.e., materials employed for targets, beam windows, collimators, and beam dumps, which suffer direct impingement of high-intensity proton beams, and initiated an international collaboration with FNAL as the lead organization. As of 2020, the collaboration has grown to more than 70 members at 13 institutions in the U.S.A., Europe and Japan, including high-intensity proton accelerator facilities for particle and nuclear physics, spallation neutron sources, and nuclear transmutation research (FNAL, STFC, ORNL, ESS, CERN, J-PARC=KEK&JAEA, etc) and of nuclear research facilities that have rich expertise and technologies to study radiation damage effects on fission and fusion reactor materials (PNNL, Oxford University, JAEA, etc). The collaboration promotes research at the forefront of radiation damage tolerance and thermal shock resistance of materials in challenging irradiation environments.
(reference)RaDIATE International Collaboration Website:
*3 Tensile tests and uniform elongation
When tensile tests are performed, the material initially deforms in proportion to the applied stress. When the stress increases beyond the yield stress, the specimen starts to elongate, and the stress-strain curve departs from linearity. If stress continues to increase, the material elongates uniformly, and the elongation up to the maximum-stress point is referred to as “uniform elongation” (Fig.6). It is important to retain uniform elongation in a structural material because it allows graceful failure without the rapid growth of cracks. Materials are typically hardened after irradiation due to the accumulation of radiation defects, which increases the yield stress of the material. At the same time, uniform elongation is reduced. This behavior is referred to as radiation hardening and embrittlement.