Electron–ion collider

An electron–ion collider (EIC) is a type of particle accelerator collider designed to collide spin-polarized beams of electrons and ions, in order to study the properties of nuclear matter in detail via deep inelastic scattering. In 2012, a whitepaper^[1] was published, proposing the developing and building of an EIC accelerator, and in 2015, the Department of Energy Nuclear Science Advisory Committee (NSAC) named the construction of an electron–ion collider one of the top priorities for the near future in nuclear physics in the United States.^[2]

In 2020, The United States Department of Energy announced that an EIC will be built over the next ten years at Brookhaven National Laboratory (BNL) in Upton, New York, at an estimated cost of $1.6 to $2.6 billion.^[3]

On 18 September 2020, a ribbon-cutting ceremony was held at BNL, officially launching the development and building of the EIC.^[4]

Proposed designs

In the US, Brookhaven National Laboratory has a declared design for an EIC scheduled to be built in the 2020 decade. In Europe, CERN has plans for the LHeC. There are also Chinese and Russian plans for an electron–ion collider.

eRHIC

Brookhaven National Laboratory's conceptual design, eRHIC, proposes upgrading the existing Relativistic Heavy Ion Collider, which collides beams of light to heavy ions including polarized protons, with a polarized electron facility.^[5] On January 9, 2020, It was announced by Paul Dabbar, undersecretary of the US Department of Energy Office of Science, that the BNL eRHIC design was selected over the conceptual design put forward by Thomas Jefferson National Accelerator Facility as the design of a future EIC in the United States. In addition to the site selection, it was announced that the BNL EIC had acquired CD-0 (mission need) from the Department of Energy.^[3]

LHeC

The LHeC would make use of the existing LHC accelerator and add an electron accelerator to collide electrons with the hadrons.^[6]^[7]

Technical challenges

Polarization

In order to allow understanding of spin dependence of the electron-nucleon collisions, both the ion beam and the electron beam must be polarized. Achieving and maintaining high levels of polarization is challenging. Nucleons and electrons pose different issues. Electron polarization is affected by synchrotron radiation. This gives rise to both self polarization via the Sokolov–Ternov effect and depolarization due to the effects of quantum fluctuations. Ignoring the effects of synchrotron radiation, the motion of the spin follows the Thomas BMT equation.

High luminosity achievement

The luminosity determines the rates of interactions between electrons and nucleons. The weaker a mode of interaction is, the higher luminosity is required to reach an adequate measurement of the process. The luminosity is inversely proportional to the product of the beam sizes of the two colliding species, which implies that the smaller the emittances of the beams, the larger the luminosity. Whereas the electron beam emittance (for a storage ring) is determined by an equilibrium between damping and diffusion from synchrotrotron radiation, the emittance for the ion beam is determined by the initially injected value. The ion beam emittance may be decreased via various methods of beam cooling, such as electron cooling or stochastic cooling. In addition, one must consider the effect of intrabeam scattering, which is largely a heating effect.

Scientific purpose

An electron–ion collider allows probing of the substructure of protons and neutrons via a high energy electron. Protons and neutrons are composed of quarks, interacting via the strong interaction mediated by gluons. The general domain encompassing the study of these fundamental phenomena is nuclear physics, with the low level generally accepted framework being quantum chromodynamics, the 'chromo' resulting from the fact that quarks are described as having three different possible values for color charge (red, green or blue).

Some of the remaining mysteries associated with atomic nuclei include how nuclear properties such as spin and mass emerge from the lower level constituent dynamics of quarks and gluons. Formulations of these mysteries, encompassing research projects, include the proton spin crisis and the proton radius puzzle.

Collaboration

The Electron–Ion Collider user group consists of more than 1400 physicists from over 290 laboratories and universities from 38 countries around the world.^[8]

Funding

In the year 2022, the Office of Science in Department of Energy reported that the budget for Electron–Ion Collider would be $30M, while the project required $120M to meet its defined milestone in 2023, causing the EIC pre-construction schedule to be "stretched".^[9]

Previous EICs

One electron–ion collider in the past was HERA in Hamburg, Germany. Hera ran from 1992 to 2007 and collided electrons and protons at a center of mass energy of 318 GeV.

References

^ A. Accardi et al., "Electron Ion Collider: The Next QCD Frontier – Understanding the glue that binds us all", 2012.
^ "Office of Science" (PDF).
^ ^a ^b “U.S. Department of Energy Selects Brookhaven National Laboratory to Host Major New Nuclear Physics Facility” 2020.
^ "Brookhaven launches electron-ion collider". 21 September 2020.
^ E. C. Aschenauer et al., “eRHIC Design Study: An Electron–Ion Collider at BNL,” 2014.
^ Abelleira Fernandez, J. L.; Adolphsen, C.; Akay, A. N.; Aksakal, H.; Albacete, J. L.; Alekhin, S.; Allport, P.; Andreev, V.; Appleby, R. B.; Arikan, E.; Armesto, N.; Azuelos, G.; Bai, M.; Barber, D.; Bartels, J.; Behnke, O.; Behr, J.; Belyaev, A. S.; Ben-Zvi, I.; Bernard, N.; Bertolucci, S.; Bettoni, S.; Biswal, S.; Blümlein, J.; Böttcher, H.; Bogacz, A.; Bracco, C.; Brandt, G.; Braun, H.; et al. (2012). "A Large Hadron Electron Collider at CERN Report on the Physics and Design Concepts for Machine and Detector". Journal of Physics G: Nuclear and Particle Physics. 39 (7): 075001. arXiv:1206.2913. Bibcode:2012JPhG...39g5001A. doi:10.1088/0954-3899/39/7/075001. S2CID 52498118.
^ "A Large Hadron electron Collider at CERN".
^ "Welcome! | Electron–Ion Collider User Group".
^ Thomas, Will (January 7, 2022). "DOE Nuclear Physics Program Approaches Pivot Point". FYI, American Institute of Physics. Retrieved 15 April 2022.

[EICwhitepaper-1] A. Accardi et al., "Electron Ion Collider: The Next QCD Frontier – Understanding the glue that binds us all", 2012.

[2] "Office of Science" (PDF).

[DOE-BH-2020-3] “U.S. Department of Energy Selects Brookhaven National Laboratory to Host Major New Nuclear Physics Facility” 2020.

[4] "Brookhaven launches electron-ion collider". 21 September 2020.

[5] E. C. Aschenauer et al., “eRHIC Design Study: An Electron–Ion Collider at BNL,” 2014.

[6] Abelleira Fernandez, J. L.; Adolphsen, C.; Akay, A. N.; Aksakal, H.; Albacete, J. L.; Alekhin, S.; Allport, P.; Andreev, V.; Appleby, R. B.; Arikan, E.; Armesto, N.; Azuelos, G.; Bai, M.; Barber, D.; Bartels, J.; Behnke, O.; Behr, J.; Belyaev, A. S.; Ben-Zvi, I.; Bernard, N.; Bertolucci, S.; Bettoni, S.; Biswal, S.; Blümlein, J.; Böttcher, H.; Bogacz, A.; Bracco, C.; Brandt, G.; Braun, H.; et al. (2012). "A Large Hadron Electron Collider at CERN Report on the Physics and Design Concepts for Machine and Detector". Journal of Physics G: Nuclear and Particle Physics. 39 (7): 075001. arXiv:1206.2913. Bibcode:2012JPhG...39g5001A. doi:10.1088/0954-3899/39/7/075001. S2CID 52498118.

[7] "A Large Hadron electron Collider at CERN".

[8] "Welcome! | Electron–Ion Collider User Group".

[9] Thomas, Will (January 7, 2022). "DOE Nuclear Physics Program Approaches Pivot Point". FYI, American Institute of Physics. Retrieved 15 April 2022.

[1]

[2]

[3]

[4]

[5]

[6]

[7]

[8]

[9]