Scientific Purpose: Provide unique information about the structure and properties of materials across the spectrum of biology, chemistry, physics, and engineering.
The European Spallation Source ERIC (ESS) is a multi-disciplinaryresearch facility currently under construction[1] in Lund, Sweden.[2] Its Data Management and Software Centre (DMSC) is co-located with DTU in Lyngby, Denmark.[3][4][5] Its 13 European contributor countries are partners in the construction and operation of the ESS.[6] The ESS is scheduled to begin its scientific user program in 2027, when the construction phase is set to be completed.[7] The ESS will assist scientists in the tasks of observing and understanding basic atomic structures and forces, which are more challenging to do with other neutron sources in terms of lengths and time scales.[8] The research facility is located near the MAX IV Laboratory, which conducts synchrotron radiation research. The construction of the facility began in the summer of 2014 and the first science results are planned for 2027.
During operation, the ESS will use nuclear spallation, a process in which neutrons are liberated from heavy elements by high energy protons. This is considered to be a safer process than uranium fission since the reaction requires an external energy supply which can be stopped easily. This facility is an example of a "long pulse" source (milliseconds).[9][10] Furthermore, spallation produces more usable neutrons for a given amount of waste heat than fission.
The facility consists of a linear accelerator, in which protons are accelerated and collide with a rotating, helium-cooled tungsten target, generating intense pulses of neutrons. Surrounding the tungsten are baths of cryogenic hydrogen, which feed neutron supermirror guides. It operates similarly to optical fibres, directing the beams of neutrons to experimental stations, where research is performed on a range of materials.
Neutron scattering can be applied to a range of scientific explorations in physics, chemistry, geology, biology, and medicine. Neutrons serve as a probe for revealing the structure and function of matter from the microscopic down to the atomic scale, with the potential for development of new materials and processes.[11]
During the construction, the ESS became a European Research Infrastructure Consortium, or ERIC, on 1 October 2015.
When the ISIS neutron source was built in England in 1985, its success in producing indirect images of molecular structures eventually raised the possibility of a far more powerful spallation source. By 1993, the European Neutron Scattering Association began to advocate for the construction of a new spallation source, and the project would eventually become known as the ESS.[15]
Neutron science soon became a critical tool in the development of industrial and consumer products worldwide. So much so that the Organization for Economic Development (OECD), declared in 1999 that a new generation of high-intensity neutron sources should be built, one each in North America, Asia and Europe.[15] Europe's challenge was its diverse collection of national governments, and an active research community numbering in the thousands. In 2001, a European roadmap for developing accelerator driven systems for nuclear waste incineration estimated that the ESS could have the beam ready for users in 2010.[16] A European international task force gathered in Bonn, Germany in 2002 to review the findings and a positive consensus emerged to build ESS. The stakeholders group met a year later to review the task force's progress, and in 2003 a new design concept was adopted that set the course for beginning operations by 2019.[15]
Over the next five years a selection process chose Lund, Sweden as the site of the ESS; the definitive selection of Lund was announced in Brussels, Belgium, on 28 May 2009.[15] On 1 July 2010, the staff and operations of ESS Scandinavia were transferred from Lund University to 'European Spallation Source ESS AB', a limited liability company set up to design, construct and operate the European Spallation Source in Lund. The company's headquarters are situated in central Lund.[17]
ESS became a European Research Infrastructure Consortium, or ERIC, on 1 October 2015. The Founding Members of the European Spallation Source ERIC are the Czech Republic, Denmark, Estonia, France, Germany, Hungary, Italy, Norway, Poland, Spain, Sweden, Switzerland and the United Kingdom.[18]
As of 2013, the estimated cost of the facility will be about €1.843 bn. (or $1.958 bn.) Host nations Sweden and Denmark each plan to cover about half of the sum. However the negotiations about the exact contributions from every partner were still in progress.[19] From 2010 to 30 September 2015, ESS was operated as a Swedish aktiebolag, or AB.[15]
Originally, three possible sites for the ESS were under consideration: Bilbao (Spain), Debrecen (Hungary) and Lund (Sweden).[20]
On 28 May 2009, seven countries indicated support for placing ESS in Sweden. Furthermore, Switzerland and Italy indicated that they would support the site in majority.[21] On 6 June 2009, Spain withdrew the Bilbao candidacy and signed a collaboration agreement with Sweden, supporting Lund as the main site, but with key component development work being performed in Bilbao. This effectively settled the location of the ESS; detailed economical negotiations between the participating countries then took place.[22] On 18 December 2009, Hungary also chose to tentatively support ESS in Lund, thus withdrawing the candidacy of Debrecen.[20][23]
The facility's construction began in early 2014, with an event held in September of that year. The user programme will start in 2027.[7] The site is accessible via Lund tramway, the first new tram system in Sweden in over a century.
The linear accelerator
The ESS uses a linear accelerator[24] (linac) to accelerate a beam of protons from the exit of its ion source at 75 keV to 2 GeV, at the entrance of the accelerator, protons are traveling at ~1% of the speed of light and at the end of the accelerator, they reach a velocity of ~95% speed of light. The accelerator uses both normal conducting and superconducting cavities.
The normal conducting cavities are Radio frequencyQuadrupole, RFQ, working at a frequency of 352.21 MHz, and accelerating the proton beam up to an energy of 3.62 MeV. The next structure is a transport line for the medium energy protons, MEBT which transports the beam from the RFQ to the next structure for further acceleration. In the MEBT, the beam properties are measured, the beam is cleaned from the transverse halo around the beam, and also the head and tail of the beam pulse are cleaned using a transversally deflecting electromagnetic chopper. The Drift Tube Linac, DTL, which is the structure downstream of the MEBT accelerates the beam further to ~90 MeV. At this energy, there is a transition from normal conducting cavities to superconducting cavities.
Three families of superconducting cavities accelerate the beam to its final energy of 2 GeV, firstly a section using double-spoke cavities up to an energy of ~216 Mev, then two families of elliptical cavities which are optimized for medium and high energy proton acceleration at a frequency of 704.42 MHz. Following the elliptical cavities, a transfer-line guides the beam to the target, and just before sending the beam to the target for producing spallation neutrons expands the beam and paints the target to dissipate the generated heat over a larger area.
The linac repetition rate is 14 Hz, and the pulses of protons are 2.86 ms long, making the duty factor of the linac 4%. The beam current within the pulse is 62.5 mA, and the average beam current is 2.5 mA.
Except in the RFQ which uses the same structure and field to accelerate and focus the beam, the transverse focusing of the beam of protons is performed using magnetic lenses. In the low energy beam transport, right after the ion source, magnetic solenoids are used, in the DTL permanent quadrupolemagnets are used and the rest of the linac uses electromagnetic quadrupoles.
The spallation target and its environmental impact
Radioactive substances will be generated by the spallation process, but the solid target makes the handling of these materials easier and safer than if a liquid target had been used.
ESS, E.on, and Lunds Energi are collaborating in a project aiming to get the facility to be the world's first completely sustainable large-scale research centre through investment in wind power.[28] The ESS project is expected to include an extension of the Nysted Wind Farm.
Recent design improvements will decrease energy usage at ESS.[30][31]
Neutron Scattering and Imaging Instruments at ESS
The target station is surrounded by instrument halls with scientific instruments placed in four sections in the cardinal directions.[32] In the western section, science instruments are located 156 meters from the center of the target station. The distance is between 50 and 80 meters in the southern one, and the science instruments located closest to the target station are in the northern and eastern sections.[32]
Initially, 15 different scientific instruments will be erected:[33]
The European Spallation Source neutrino Super Beam (ESSnuSB) project aims to measure leptonic CP violation at the second neutrino oscillation maximum, offering higher sensitivity than the first maximum. After 10 years of data collection, ESSnuSB is expected to cover over 70% of the CP-violating phase range with 5σ confidence level, achieving a precision better than 8° for all δCP values. The ESSnuSB+ extension project focuses on measuring neutrino-nucleus cross-sections in the 0.2–0.6 GeV energy range to address systematic uncertainties . This will be accomplished using two new facilities: a Low Energy nuSTORM (LEnuSTORM) and a Low Energy Monitored Neutrino Beam (LEMNB). The project also includes the development of a target station prototype, a common near detector, and studies on gadolinium-doped water Cherenkov detectors.[34][35]
^Mezei, Ferenc (1996). "The raison d'être of long pulse spallation sources". Journal of Neutron Research. 6 (1–3): 3–32. doi:10.1080/10238169708200095.
^Alekou, A.; Baussan, E.; Kraljevic, N. Blaskovic; Blennow, M.; Bogomilov, M.; Bouquerel, E.; Burgman, A.; Carlile, C. J.; Cederkall, J.; Christiansen, P.; Collins, M.; Morales, E. Cristaldo; D'Alessi, L.; Danared, H.; de André, J. P. A. M. (December 2021). "Updated physics performance of the ESSnuSB experiment". The European Physical Journal C. 81 (12): 1130. arXiv:2107.07585. Bibcode:2021EPJC...81.1130A. doi:10.1140/epjc/s10052-021-09845-8. ISSN1434-6044. S2CID236033945.
Hallonsten, O. 2012. Introduction: In pursuit of a Promise. In O. Hallonsten (ed.) In pursuit of a Promise: Perspectives on the political process to establish the European Spallation Source (ESS) in Lund, Sweden (pp. 11–19). Lund: Arkiv Academic Press, 2012, p. 12.
Prolingheuer, N.; Herbst, M.; Heuel-Fabianek, B.; Moormann, R.; Nabbi, R.; Schlögl, B., Vanderborght, J. 2009: Estimating Dose Rates from Activated Groundwater at Accelerator Sites. Nuclear Technology, Vol. 168, No. 3, December 2009, pp. 924–930.
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