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High Energy Physics (Experiment)

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Physics
DOI: 10.54546/NaturalSciRev.100902

The muon collider: Expected physics, technological challenges, and the prospects for reusing the 21 km UNK tunnel

A multi-TeV muon collider is now among the main options considered for the post-LHC energy frontier. The muon is an elementary particle that radiates ∼10 9 times less synchrotron power than an electron of the same energy. A circular muon collider would therefore deliver the full beam energy to the hard collision in a compact collider ring, although its acceleration chain needs a longer tunnel. It combines the energy reach of a 100 TeV-class proton machine with the clean final states of a lepton collider. This review summarizes the expected physics results. They include Higgs couplings and selfcouplings, electroweak and vector-boson-fusion processes, the top quark, and a broad programme of searches beyond the Standard Model. The programme would close nearly all of the thermal window for electroweak WIMP dark matter. The review also covers the technological challenges, namely muon production, ionization cooling, rapid acceleration, high-field high-temperature-superconductor (HTS) magnets, the machine–detector interface, and the neutrino-flux constraint. For each, the review describes the proposed solution, its present status, and the open issues. None of these technologies has yet been demonstrated at the required performance, and the design luminosity is a target. The review then examines three ways of reusing the existing 21 km UNK tunnel near Protvino, by scaling the parameters of the International Muon Collider Collaboration (IMCC). If the tunnel houses the last rapid-cycling synchrotron, as the LHC tunnel does in the IMCC option at CERN, this synchrotron limits the centre-of-mass energy to about 6 TeV. A new collider ring of about 7−9 km is then needed. If the tunnel houses the collider ring, arc dipoles of 11−14 T give about 14−18 TeV, and aspirational 16 T dipoles about 21 TeV. The acceleration chain then needs a separate tunnel of about 50−73 km. If the tunnel houses both the collider ring and the last synchrotron, as proposed earlier for the LHC tunnel, only the first synchrotrons need new ring tunnels. This layout gives about 6 TeV with the IMCC baseline magnets and about 10 TeV only with 16 T fixed and ±3.8 T pulsed synchrotron dipoles, neither yet demonstrated, at 35−57% of the target luminosity. Such a facility would also support a programme of non-collider applications of intense muon beams, such as an aimed neutrino beam, as well as muon-catalyzed fusion, muography, muonic-atom isotopic analysis, and muon spin spectroscopy. Some of these directions have a long history in the Russian physics institutes.
L. V. Dudko
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Physics
DOI: 10.54546/NaturalSciRev.100801

Perturbative  QCD fitting of  KEDR and BESIII  ℯ+ℯ- data  for R(s) and αs determination

The experimental data collected by KEDR and BESIII collaborations at the energies below charm quark thresholds are compared with the massless QCD expressions for the \(e^+e^-\) annihilation R-ratio truncated at different orders of perturbation theory. The fits demonstrate the dependence of the extracted \(\alpha_s(M_Z)\) values on the orders of truncation of the corresponding approximations. The next-to-leading order, next-to-next-to-leading order and next-to-next-to-next-to-leading order fits of the combined KEDR data and BESIII data , truncated at the scale of mass of \(J/\Psi\) meson, give the following results \(\alpha_s(M_Z)=0.1151_{-0.0069}^{+0.0052}\), \(\alpha_s(M_Z)=0.1190_{-0.0081}^{+0.0064}\) and \(\alpha_s(M_Z)=0.1283_{-0.0075}^{+0.0028}\). The increasing tendency of fitted \(\alpha_s(M_Z)\) value is associated with the effects of not totally controlled within asymptotic perturbation theory expansions kinematical \(\pi^2\) contributions to R-ratio coefficients due to analytical continuation from the space-like to time-like energy regions. The applications of the fixed orders of perturbation theory expansions and careful treatment of the analytical continuation effects are commented.   Corrected: 28 July 2026 (changes have been made in Eqs. (12)–(14) and an expression has been added after them)
A. L. Kataev, K. Yu. Todyshev
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Physics 70th anniversary of JINR
DOI: 10.54546/NaturalSciRev.200708

Searching for Light Dark Matter and Dark Sectors with the NA64 experiment at the CERN SPS: et al.

Since its approval in 2016, NA64 has pioneered Light Dark Matter (LDM) searches with electron [1], positron [2], muon [3], and hadron [4] beams. The experiment has successfully met its primary objectives, as outlined in the EPPS input (2018), and even exceed them producing results that demonstrate its ability to operate in a near background-free environment. The Physics Beyond Collider (PBC) initiative at CERN recognizes NA64’s contributions as complementary and worthy of continued exploration. Its key advantage over beam dump approaches is that the signal rate scales as (coupling) 2 rather than (coupling) 4 , reducing the required beam particles for the same sensitivity. To fully exploit the NA64 physics potential, an upgrade during LS3 will enable NA64 to run in background-free mode at higher SPS beam rates. Planned upgrades include (a) improved detector hermeticity with a new veto hadron calorimeter, (b) enhanced particle identification with a synchrotron radiation detector, and (c) increased beam rates via upgraded electronics. With the recently strengthened NA64 collaboration, stable operations and timely data analysis are planned for LHC Run 4. The expected ∼ 10 13 electrons, ∼ 10 11 positrons (40 and 60 GeV), and ∼ 2×10 13 muons on target will allow NA64 to explore new light dark matter regions, with the potential for discovery or conclusive exclusion of many well-motivated LDM models.
Yu. M. Andreev, A. Antonov, M. A. Ayala Torres, D. Banerjee, B. Banto Oberhauser, V. Bautin, J. Bernhard, P. Bisio, A. Celentano, N. Charitonidis, P. Crivelli, A. V. Dermenev, S. V. Donskov, R. R. Dusaev, V. N. Frolov, S. V. Gertsenberger, S. Girod, S. N. Gninenko, A. V. Ivanov, Y. Kambar, A. E. Karneyeu, G. Kekelidze, B. Ketzer, D. V. Kirpichnikov, M. M. Kirsanov, V. A. Kramarenko, N. V. Krasnikov, S. V. Kuleshov, V. E. Lyubovitskij, A. Marini, L. Marsicano, V. A. Matveev, R. Mena Fredes, R. Mena Yanssen, L. Molina Bueno, M. Mongillo, D. V. Peshekhonov, V. A. Polyakov, B. Radics, K. Salamatin, V. D. Samoylenko, H. Sieber, D. Shchukin, O. Soto, V. O. Tikhomirov, I. Tlisova, A. N. Toropin, M. Tuzi, P. V. Volkov, I. V. Voronchikhin, J. Zamora-Saá, A. S. Zhevlakov
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Physics Mathematical and Computer Sciences 70th anniversary of JINR
DOI: 10.54546/NaturalSciRev.200701

Multifunctional Information and Computing Complex of JINR

The Multifunctional Information and Computing Complex (MICC) of the JINR Meshcheryakov Laboratory of Information Technologies (MLIT) is a key element of the JINR network and information and computing infrastructures. The MICC is regarded as JINR’s unique basic facility and plays a decisive role in scientific research, which entails advanced computing power and storage systems. Its uniqueness is ensured by the consolidation of all state-of-the-art information technologies for data processing and storage, united by the network infrastructure with a bandwidth of up to 4 × 100 Gbps. It consists of distributed data processing and storage systems based on both grid and cloud technologies and the hyperconverged computing infrastructure with liquid cooling. Multifunctionality, high reliability, and availability in 24 × 7 × 365 mode, scalability and high performance, information security and an advanced software environment are the main requirements that the MICC meets. The reliability and availability are ensured by the enhanced high-speed telecommunication system and the modern local network infrastructure, as well as by the reliable engineering infrastructure that provides guaranteed power supply and cooling for server hardware. This infrastructure is a staple for computing the experiments at the NICA accelerator complex. The BM@N, MPD, and SPD experiments intensively use all computational components and storage systems. Being part of the Worldwide LHC Computing Grid, the MICC serves as the Tier1 grid site for the CMS experiment at the LHC and as the Tier2 grid site that provides support for the experiments at the LHC and other world’s large-scale experiments in high-energy physics. The integrated cloud environment of the JINR Member States focuses on supporting users and experiments in Russia, China, the USA, etc. (e.g., NICA, NOvA, BaikalGVD, JUNO). The HybriLIT platform comprising the Govorun supercomputer provides capabilities for elaborating mathematical models and algorithms and performing resource-intensive computations, including on graphics accelerators that enable the development of the ecosystem for machine and deep learning tasks, Big Data analysis, and quantum computing on simulators.
A. I. Balandin, N. A. Balashov, O. Yu. Derenovskaya, A. G. Dolbilov, A. P. Gavrish, A. O. Golunov, N. I. Gromova, A. V. Evlanov, I. A. Kashunin, V. V. Korenkov, N. A. Kutovskiy, V. V. Mitsyn, A. N. Moibenko, I. S. Pelevanyuk, D. V. Podgainy, O. I. Streltsova, S. V. Shmatov, T. A. Strizh, V. V. Trofimov, A. S. Vorontsov, N. N. Voytishin, M. I. Zuev
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Physics 70th anniversary of JINR
DOI: 10.54546/NaturalSciRev.200602

Study of low-energy QCD in meson reactions with the Coulomb field of atomic nuclei

This paper reviews the development of theoretical and experimental studies of low-energy QCD parameters starting from early investigations at the JINR Laboratory of Theoretical Physics and ending with modern measurements at CERN. We summarize the historical background and the pioneering theoretical approaches used at JINR to calculate meson parameters in various hadronic models which have laid the foundation for the experimental proposal to investigate the pion polarizability via radiative scattering off nuclei. The first observation of the Compton effect on the pion and the first measurements of the charged pion polarizability and the γ → 3 π constant performed with the U-70 accelerator are discussed as key milestones enabling quantitative studies of the meson structure and highlighting their impact on the low-energy QCD phenomenology. Continued advances in theoretical predictions have underscored the need for higher-precision experimental data and motivated new measurements carried out with pion beams in the COMPASS experiment at CERN. Finally, we outline the prospects for future studies within the AMBER experiment where kaon beams will enable a precision determination of kaon polarizabilities and related low-energy constants further advancing our understanding of dynamics of the strong interaction.
A. Guskov, A. Maltsev, A. Olshevskiy
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Physics
DOI: 10.54546/NaturalSciRev.100101

Technical Design Report of the Spin Physics Detector at NICA: et al. (SPD  Collaboration).

The Spin Physics Detector Collaboration proposes to install a universal detector in the second interaction point of the NICA collider under construction (JINR, Dubna) to study the spin structure of the proton and deuteron and other spin-related phenomena using a unique possibility to operate with polarized proton and deuteron beams at a collision energy up to 27 GeV and a luminosity up to 10 32 cm −2 s −1 . As the main goal, the experiment aims to provide access to the gluon TMD PDFs in the proton and deuteron, as well as the gluon transversity distribution and tensor PDFs in the deuteron, via the measurement of specific single- and double-spin asymmetries using different complementary probes, such as charmonia, open charm, and prompt photon production processes. Other polarized and unpolarized physics is possible, especially at the first stage of NICA operation with reduced luminosity and collision energy of the proton and ion beams. This paper is dedicated exclusively to technical issues of the SPD setup construction. Corrected: 5 February 2025 (the surname of one of the authors was initially misspelled (M. Bolsunovskya), the correct spelling is M. Bolsunovskaya). 23 April 2025 (the surname of one of the authors was initially misspelled (A. Seleznev), the correct spelling is A. Selezenev).
V. Abazov, V. Abramov, L. Afanasyev, R. Akhunzyanov, A. Akindinov, I. Alekseev, A. Aleshko, V. Alexakhin, G. Alexeev, L. Alimov, A. Allakhverdieva, A. Amoroso, V. Andreev, V. Andreev, E. Andronov, Yu. Anikin, S. Anischenko, A. Anisenkov, V. Anosov, E. Antokhin, A. Antonov, S. Antsupov, A. Anufriev, K. Asadova, S. Ashraf, V. Astakhov, A. Aynikeev, M. Azarkin, N. Azorskiy, A. Bagulya, D. Baigarashev, A. Baldin, E. Baldina, N. Barbashina, A. Barnyakov, S. Barsov, A. Bartkevich, V. Baryshevsky, K. Basharina, A. Baskakov, V. Baskov, M. Batista, M. Baturitsky, V. Bautin, T. Bedareva, S. Belokurova, A. Belova, E. Belyaeva, A. Berdnikov, Ya. Berdnikov, A. Berezhnoy, A. Berngardt, Yu. Bespalov, V. Bleko, L. Bliznyuk, D. Bogoslovskii, A. Boiko, A. Boikov, M. Bolsunovskaya, E. Boos, V. Borisov, V. Borsch, D. Budkouski, S. Bulanova, O. Bulekov, V. Bunichev, N. Burtebayev, D. Bychanok, A. Casanova, G. Cesar, D. Chemezov, L. Chen, A. Chepurnov, V. Chmill, A. Chukanov, A. Chuzo, A. Danilyuk, A. Datta, D. Dedovich, M. Demichev, G. Deng, I. Denisenko, O. Denisov, T. Derbysheva, D. Derkach, A. Didorenko, M.-O. Dima, A. Doinikov, S. Doronin, V. Dronik, F. Dubinin, V. Dunin, A. Durum, A. Egorov, R. El-Kholy, T. Enik, D. Ermak, D. Erofeev, A. Erokhin, D. Ezhov, O. Fedin, Ju. Fedotova, G. Feofilov, Yu. Filatov, S. Filimonov, V. Frolov, K. Galaktionov, A. Galoyan, A. Garkun, O. Gavrishchuk, S. Gerasimov, M. Gilts, L. Gladilin, G. Golovanov, S. Golovnya, V. Golovtsov, A. Golubev, S. Golubykh, P. Goncharov, A. Gongadze, N. Greben, A. Gregoryev, D. Gribkov, A. Gridin, K. Gritsay, D. Gubachev, J. Guo, Yu. Gurchin, A. Gurinovich, Yu. Gurov, A. Guskov, D. Gutierrez, F. Guzman, A. Hakobyan, D. Han, S. Harkusha, Sh. Hu, S. Igolkin, A. Isupov, A. Ivanov, N. Ivanov, V. Ivantchenko, Sh. Jin, S. Kakurin, N. Kalinichenko, Y. Kambar, A. Kantsyrev, I. Kapitonov, V. Karjavine, A. Karpishkov, A. Katcin, G. Kekelidze, D. Kereibay, S. Khabarov, P. Kharyuzov, H. Khodzhibagiyan, E. Kidanov, E. Kidanova, V. Kim, A. Kiryanov, I. Kishchin, E. Kokoulina, A. Kolbasin, V. Komarov, A. Konak, Yu. Kopylov, M. Korjik, M. Korotkov, D. Korovkin, A. Korzenev, B. Kostenko, A. Kotova, A. Kotzinian, V. Kovalenko, N. Kovyazina, M. Kozhin, A. Kraeva, V. Kramarenko, A. Kremnev, U. Kruchonak, A. Kubankin, O. Kuchinskaia, Yu. Kulchitsky, S. Kuleshov, A. Kulikov, V. Kulikov, V. Kurbatov, Zh. Kurmanaliev, Yu. Kurochkin, S. Kutuzov, E. Kuznetsova, I. Kuyanov, E. Ladygin, V. Ladygin, D. Larionova, V. Lebedev, R. Lednicki, M. Levchuk, P. Li, X. Li, Y. Li, A. Livanov, A. Lobanov, A. Lobko, K. Loshmanova, S. Lukashevich, E. Luschevskaya, A. L’vov, I. Lyashko, V. Lysan, V. Lyubovitskij, D. Madigozhin, V. Makarenko, N. Makarov, R. Makhmanazarov, V. Maleev, D. Maletic, A. Malinin, A. Malkhasyan, A. Maltsev, N. Maltsev, M. Malyshev, O. Mamoutova, A. Manakonov, A. Marova, M. Merkin, I. Meshkov, V. Metchinsky, O. Minko, Yu. Mitrankov, M. Mitrankova, A. Mkrtchyan, H. Mkrtchyan, R. Mohamed, A. Morozikhin, S. Morozova, E. Mosolova, V. Mossolov, S. Movchan, Y. Mukhamejanov, A. Mukhamejanova, E. Muzyaev, D. Myktybekov, S. Nagorniy, M. Nassurlla, P. Nechaeva, M. Negodaev, V. Nesterov, M. Nevmerzhitsky, G. Nigmatkulov, D. Nikiforov, V. Nikitin, A. Nikolaev, D. Oleynik, V. Onuchin, I. Orlov, A. Orlova, G. Ososkov, D. Panzieri, B. Parsamyan, V. Pavlov, P. Pavzderin, M. Pedraza, V. Perelygin, D. Peshkov, A. Petrosyan, M. Petrov, V. Petrov, K. Petrukhin, A. Piskun, S. Pivovarov, I. Polishchuk, P. Polozov, V. Polyanskii, A. Ponomarev, V. Popov, V. Popov, S. Popovich, D. Prokhorova, N. Prokofiev, F. Prokoshin, A. Puchkov, I. Pudin, E. Pyata, V. Rasin, F. Ratnikov, V. Red’kov, A. Reshetin, S. Reznikov, N. Rogacheva, S. Romakhov, A. Rouba, V. Rudnev, V. Rusinov, D. Rusov, V. Ryltsov, N. Saduyev, A. Safonov, S. Sakhiyev, K. Salamatin, V. Saleev, A. Samartsev, E. Samigullin, O. Samoylov, E. Saprunov, A. Savenkov, A. Seleznev, A. Semak, D. Senkov, A. Sergeev, L. Seryogin, S. Seryubin, A. Shabanov, A. Shahinyan, A. Shavrin, I. Shein, A. Sheremeteva, V. Shevchenko, K. Shilyaev, S. Shimansky, S. Shinbulatov, F. Shipilov, A. Shipilova, S. Shkarovskiy, Dz. Shoukovy, K. Shpakov, I. Shreyber, K. Shtejer, R. Shulyakovsky, A. Shunko, S. Sinelshchikova, A. Skachkova, A. Skalnenkov, A. Smirnov, S. Smirnov, A. Snesarev, E. Soldatov, A. Solin, A. Solin jr., V. Solovtsov, J. Song, D. Sosnov, A. Stavinskiy, D. Stekacheva, E. Streletskaya, M. Strikhanov, O. Suarez, A. Sukhikh, S. Sukhovarov, V. Sulin, R. Sultanov, P. Sun, D. Svirida, E. Syresin, V. Tadevosyan, O. Tarasov, E. Tarkovsky, V. Tchekhovsky, E. Tcherniaev, A. Terekhin, A. Terkulov, V. Tereshchenko, O. Teryaev, P. Teterin, A. Tishevsky, V. Tokmenin, N. Topilin, P. Tsiareshka, A. Tumasyan, G. Tyumenkov, E. Usenko, L. Uvarov, V. Uzhinsky, Yu. Uzikov, F. Valiev, E. Vasilieva, A. Vasyukov, V. Vechernin, A. Verkheev, L. Vertogradov, Yu. Vertogradova, R. Vidal, N. Voitishin, I. Volkov, P. Volkov, A. Vorobyov, H. Voskanyan, H. Wang, Y. Wang, T. Xu, A. Yanovich, I. Yeletskikh, N. Yerezhep, S. Yurchenko, A. Zakharov, N. Zamiatin, J. Zamora-Sa´a, A. Zarochentsev, A Zelenov, E. Zemlyanichkina, M. Zhabitsky, J. Zhang, Zh. Zhang, A. Zhemchugov, V. Zherebchevsky, A. Zhevlakov, N. Zhigareva, J. Zhou, X. Zhuang, I. Zhukov, N. Zhuravlev, A. Zinin, S. Zmeev, D. Zolotykh, E. Zubarev, A. Zvyagina, S. Gerassimov