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5. Spin Physics at COSY (2021-2024 and beyond) -- Pathfinder investigations toward an EDM storage ring and Spin-for-FAIR

Author

Gebel, R., Hejny, V., Kacharava, A., Lehrach, A., Lenisa, P., Nass, A., Pretz, J., Rathmann, F., Ströher, H., Keshelashvili, I., Stephenson, E. J., Filatov, A. Wrońska Y., Kondratenko, A., Kondratenko, M., Nikolaev, N., Melnikov, A., Senichev, Y., Aksentyev, A., Butenko, A., Syresin, E., Saleev, A., Shmakova, V., Karanth, S., Breitkreutz, B., Shurkhno, N., Stassen, R., and Pesce, A.

Subjects
Physics - Accelerator Physics, Nuclear Experiment
Abstract

The unique global feature of COSY is its ability to accelerate, store and manipulate polarized proton and deuteron beams. In the recent past, these beams have been used primarily for precision measurements, in particular in connection with the study of charged particle EDMs (Electric Dipole Moment) in storage rings. The role of COSY as a R&D facility and for initial (static and oscillating) EDM measurements can hardly be overestimated. Unfortunately, as a consequence of the strategic decisions of Forschungszentrum J\"ulich and the subsequent "TransFAIR" agreement between FZJ and GSI Darmstadt, it is currently planned to stop the operation of COSY by the end of 2024. The various groups working with polarized beams at COSY felt it important to collect information on essential measurements to be performed until the termination of machine operation. These experiments, briefly described in this document along with an estimate of the beam time required, serve as pathfinder investigations toward an EDM storage ring and Spin for FAIR., Comment: 40 pages, 17 figures

Published
2021

6. Conceptual design of the Spin Physics Detector

Author

Abazov, V. M., Abramov, V., Afanasyev, L. G., Akhunzyanov, R. R., Akindinov, A. V., Akopov, N., Alekseev, I. G., Aleshko, A. M., Alexakhin, V. Yu., Alexeev, G. D., Alexeev, M., Amoroso, A., Anikin, I. V., Andreev, V. F., Anosov, V. A., Arbuzov, A. B., Azorskiy, N. I., Baldin, A. A., Balandina, V. V., Baldina, E. G., Barabanov, M. Yu., Barsov, S. G., Baskov, V. A., Beloborodov, A. N., Belov, I. N., Belova, A. P., Belyaev, A. V., Berdnikov, A. Ya., Berdnikov, Ya. A., Berezhnoy, A. V., Bleko, V. V., Bobkov, A. V., Bogoslovsky, D. N., Boguslavsky, I. N., Boltushkin, E. V., Boos, E. E., Burtsev, V. E., Chen, Lei, Chepurnov, A. S., Chiosso, M., Chumakov, A., Dalkarov, O. D., Datta, A., Demikhov, E. I., Denisenko, I. I., Denisov, O. Yu., Duginov, V. N., Dunin, V. B., Dygnarowicz, K., Efremov, A. V., El-Kholy, R., Eliseev, D. A., Enik, T. L., Fedin, O. L., Feofilov, G. A., Filatov, Yu. N., Finger, M., Frolov, V. N., Galinski, G., Galoyan, A. S., Trapaga, C. E Garsia, Gavrishchuk, O. P., Gerasimov, S. G., Glonti, L., Goloskokov, S. V., Golovanov, G. A., Golubev, A. A., M., Golubykh S., V., Goncharov P., O., Grafov N., Y., Gribkov D., Gribovsky, A. S., Gridin, A. O., Grinyov, B. V., Gritsay, K. I., Gromov, S. A., Gromov, V. A., Gurchin, Yu. V., Gusakov, Yu. V., Guskov, A. V., Guzman, F., Haidenbauer, J., Havranek, M., Ivanov, A. V., Ivanov, N. Ya., Isupov, A. Yu., Jary, V., Jia, Shi-Hai, Jokovic, D., Kaplii, A., Karpishkov, A. V., Kasianova, E. A., Kekelidze, G. D., Khabarov, S. V., Kharusov, P. R., Khrenov, A. N., Kim, V. T., Kirichkov, N. V., Kirin, D. Yu., Kishchin, I., Klekotko, A., Klopot, Ya., Kluev, A., Kokoulina, E. S., Komarov, V. I., Kondratenko, A. M., Kondratenko, M. A., Konorov, I., Kopylov, Yu. A., Korjik, M. V., Korovkin, P. S., Korzenev, A. Yu., Kostukov, E. V., Kotzinian, A., Kovalenko, A. D., Kovalenko, V. N., A., Kozhin M., Kramarenko, V. A., Kruglov, V. N., Kubankin, A., Kubankin, Yu., Kuleshov, S., Kovtun, V. E., Kulikov, A. V., Kurbatov, V. S., Kurjata, R., Kutuzov, S. A., Kuznetsova, E. V., Ladygin, E. A., Ladygin, V. P., Larionova, D. M., Lednicky, D., Lednicky, R., Li, Pei-Yu, Li, Xiao-Mei, Lobko, A. S., Luschevskaya, E., L'vov, A. I., Lyashchenko, V. N., Lysan, V. M., Lyubovitskij, V., Maggiora, A., Maleev, V. P., Maltsev, A., Malykhina, T. V., Makankin, A. M., Makarenko, V. V., Maletic, D., Malkevich, D. B., Marcisovsky, M., Martovitsky, E. V., Marzec, J., Merkin, M. M., Meshcheriakov, G. V., Mitrankov, Yu. M., Mitrankova, M. M., Mitrofanov, E. O., Morozov, B., Moshkovsky, I. V., Movsisyan, A., Nagorniy, S. N., Nechaeva, P. Yu., Nefedov, M. A., Nefedov, Yu. A., Negodaev, M. A., Neue, G., Nikiforov, D. N., Nikitin, V. A., Nikolaev, A. S., Oleynik, D. A., Ososkov, G. A., Panzieri, D., Parsamyan, B., Parzhitsky, S. S., Pastuszak, G., Pavlov, V. V., Pavlova, A. A., Pelevanyuk, I. S., Perepelkin, E. E., Peshekhonov, D. V., Petrosyan, A. Sh., Piskun, A. A., Plotnikov, V. V., Podgainy, D. V., Polozov, P., Polyakova, R. V., Polyansky, V. V., Popov, V. V., Popule, J., Prochazka, I., Prokhorov, I. K., Reva, S. N., Reznikov, S. G., Rezvaya, E. P., Richard, J. -M., Rogachevsky, O. V., Romanov, V. M., Rudenko, A. I., Rumyantsev, M. A., Rusinov, V., Rybakov, N. A., Rychter, A., Rymbekova, A., Safonov, A. B., Salamatin, K. M., Saleev, V. A., Samartsev, A. G., Savenkov, A. A., Savic, M., Semak, A. A., Shaikovsky, V. N., Shavrin, A. A., Sheremeteva, A. I., Shimanskii, S. S., Shipilova, A. V., Shtejer, K., Shulyakovsky, R., Sinitsa, A. A., Skachkov, N. B., Skachkova, A. N., Slunecka, M., Sluneckova, V., Solin, A. A., Solin, A. V., Song, Jin-Xin, Sotnikov, V. V., Sun, Peng-Fei, Starikova, S. Yu., Stavinskiy, A. V., Streletskaya, E. A., Strikman, M., Strusik-Kotlozh, D., Suchkov, S. I., Sultanov, R. I., Sun, Hao, Svirida, D. N., Tarasov, O. G., Tarkovskyi, E. I., Temerbayev, A., Terekhin, A. A., V., Tereschenko V., R., Terkulov A., V., Teryaev O., V., Tishevsky A., V., Tkachenko A., Tokmenin, A. A. V. V., Tomasek, L., Tomasi-Gustafsson, E., Topchiev, N. P., Topilin, N. D., Topko, B. L., Tosello, F., Trifonov, A., Troyan., Yu. A., Trunov, N. O., Tsenov, R., Usenko, E. A., Uzhinsky, V. V., Uzikov, Yu. N., Valiev, F. F., Vasilieva, E. V., Vechernin, V. V., Verkheev, A. Yu., Vertogradov, L. S., Vertogradova, Yu. L., Vesenkov, V. A., Virius, M., Volchansky, N. I., Volkov, I. S., Volkov, P. V., Vorobiev, A., Vrba, V., Wang, Qian, Yudin, I. P., Zamora, J., Zamyatin, N. I., Zaremba, K., Zelenov, A. V., Zemlyanichkina, E. V., Zhang, Yun-Yu, Zhang, Jun-Wei, Zhao, Ming-Rui, Zhao, Qiang, Zhi, Yu, Zhemchugov, A. S., Zhevlakov, A., Zhigareva, N. M., Zhmurin, P. N., Zhukov, I. A., Zhuravlev., N. I, Ziembicki, M., Zinin, A. V., Zubarev, E. V., and Zuev, M. I.

Subjects
High Energy Physics - Experiment, Physics - Instrumentation and Detectors
Abstract

The Spin Physics Detector, a universal facility for studying the nucleon spin structure and other spin-related phenomena with polarized proton and deuteron beams, is proposed to be placed in one of the two interaction points of the NICA collider that is under construction at the Joint Institute for Nuclear Research (Dubna, Russia). At the heart of the project there is huge experience with polarized beams at JINR. The main objective of the proposed experiment is the comprehensive study of the unpolarized and polarized gluon content of the nucleon. Spin measurements at the Spin Physics Detector at the NICA collider have bright perspectives to make a unique contribution and challenge our understanding of the spin structure of the nucleon. In this document the Conceptual Design of the Spin Physics Detector is presented.

Published
2021

7. Transparent Spin Method for Spin Control of Hadron Beams in Colliders

Author

Filatov, Yu. N., Kondratenko, A. M., Kondratenko, M. A., Derbenev, Ya. S., and Morozov, V. S.

Subjects
Physics - Accelerator Physics
Abstract

We present a concept for control of the ion polarization, called a transparent spin method. The spin transparency is achieved by designing such a synchrotron structure that the net spin rotation angle in one particle turn is zero. The polarization direction of any ions including deuterons can be efficiently controlled using weak quasi-static fields. These fields allow for dynamic adjustment of the polarization direction during an experiment. The main features of the Transparent Spin method are illustrated in a figure-8 collider. The results are relevant to the Electron-Ion Collider considered in the US, the ion-ion collider NICA constructed in Russia, and a polarized Electron-ion collider planned in China.

Published
2020
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9. First results on the measurements of the proton beam polarization at internal target at Nuclotron

Author

Ladygin, V. P., Gurchin, Yu. V., Isupov, A. Yu., Janek, M., Khrenov, A. N., Kurilkin, P. K., Livanov, A. N., Piyadin, S. M., Reznikov, S. G., Skhomenko, Ya. T., Terekhin, A. A., Tishevsky, A. V., Averyanov, A. V., Bazylev, S. N., Belov, A. S., Butenko, A. V., Chernykh, E. V., Filatov, Yu. N., Fimushkin, V. V., Krivenkov, D. O., Kondratenko, A. M., Kondratenko, M. A., Kovalenko, A. D., Slepnev, I. V., Slepnev, V. M., Shutov, A. V., Sidorin, A. O., Vnukov, I. E., and Volkov, V. S.

Subjects
Physics - Instrumentation and Detectors, Nuclear Experiment
Abstract

The spin program at NICA using SPD and MPD requires high intensity polarized proton beam with high value of the beam polarization. First results on the measurements of the proton beam polarization performed at internal target at Nuclotron are reported. The polarization of the proton beam provided by new source of polarized ions has been measured at 500 MeV using quasielastic proton-proton scattering and DSS setup at internal target. The obtained value of the vertical polarization of ~35 % is consistent with the calculations taking into account the current magnetic optics of the Nuclotron injection line., Comment: 4 pages, 2 figures

Published
2017
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10. Ion Polarization Scheme for MEIC

Author

Kondratenko, A. M., Kondratenko, M. A., Filatov, Yu. N., Derbenev, Ya. S., Lin, F., Morozov, V. S., and Zhang, Y.

Subjects
Physics - Accelerator Physics
Abstract

The choice of a figure 8 shape for the booster and collider rings of MEIC opens wide possibilities for preservation of the ion polarization during beam acceleration as well as for control of the polarization at the collider's interaction points. As in the case of accelerators with Siberian snakes, the spin tune is energy independent but is equal to zero instead of one half. The figure-8 topology eliminates the effect of arcs on the spin motion. There appears a unique opportunity to control the polarization of any particle species including deuterons, using longitudinal fields of small integrated strength (weak solenoids). Contrary to existing schemes, using weak solenoids in figure-8 colliders, one can control the polarization at the interaction points without essentially any effect on the beam's orbital characteristics. A universal scheme for control of the polarization using weak solenoids provides an elegant solution to the problem of ion acceleration completely eliminating resonant beam depolarization. It allows one to easily adjust the polarization in any direction at any orbital location, which becomes necessary when transferring the beam from one ring into another or when measuring the polarization by polarimeters. It also allows for an easy manipulation of the spin direction at an interaction point during an experiment. The latter feature allows one to set up a spin-flipping system with a spin reversal time of less than a second. By compensating the coherent part of the zero-integer spin resonance strength, which arises due to errors in alignment of the magnetic element of the lattice, one can reduce the field integrals of the control solenoids by a few orders of magnitude.

Published
2016

11. MEIC Design Summary

Author

Abeyratne, S., Barber, D., Bogacz, A., Brindza, P., Cai, Y., Camsonne, A., Castilla, A., Chevtsov, P., Daly, E., Derbenev, Y. S., Douglas, D., Dudnikov, V., Ent, R., Erdelyi, B., Filatov, Y., Gaskell, D., Grames, J., Guo, J., Harwood, L., Hutton, A., Hyde, C., Jordan, K., Kimber, A., Krafft, G. A., Kondratenko, A., Kondratenko, M., Li, R., Lin, F., Mann, T., McIntyre, P., Michalski, T., Morozov, V. S., Nadel-Turonski, P., Nosochkov, Y. M., Ostroumov, P. N., Park, K., Pilat, F., Poelker, M., Pogue, N. J., Rimmer, R., Roblin, Y., Satogata, T., Sattarov, A., Spata, M., Suleiman, R., Sullivan, M., Sy, A., Tennant, C., Wang, H., Wang, M-H, Wang, S., Wienands, U., Zhang, H., Zhang, Y., and Zhao, Z.

Subjects
Physics - Accelerator Physics
Abstract

This document summarizes the design of Jefferson Lab's electron-ion collider, MEIC, as of January 20, 2015, and describes the facility whose cost was estimated for the United States Department of Energy Nuclear Sciences Advisory Committee EIC cost review of January 26-28, 2015. In particular, each of the main technical systems within the collider is presented to the level of the best current information.

Published
2015

20. Science Requirements and Conceptual Design for a Polarized Medium Energy Electron-Ion Collider at Jefferson Lab

Author

Abeyratne, S., Accardi, A., Ahmed, S., Barber, D., Bisognano, J., Bogacz, A., Castilla, A., Chevtsov, P., Corneliussen, S., Deconinck, W., Degtiarenko, P., Delayen, J., Derbenev, Ya., DeSilva, S., Douglas, D., Dudnikov, V., Ent, R., Erdelyi, B., Evtushenko, P., Filatov, Yu., Gaskell, D., Geng, R., Guzey, V., Horn, T., Hutton, A., Hyde, C., Johnson, R., Kim, Y., Klein, F., Kondratenko, A., Kondratenko, M., Krafft, G., Li, R., Lin, F., Manikonda, S., Marhauser, F., McKeown, R., Morozov, V., Nadel-Turonski, P., Nissen, E., Ostroumov, P., Pivi, M., Pilat, F., Poelker, M., Prokudin, A., Rimmer, R., Satogata, T., Sayed, H., Spata, M., Sullivan, M., Tennant, C., Terzić, B., Tiefenback, M., Wang, H., Wang, S., Weiss, C., Yunn, B., and Zhang, Y.

Subjects
Physics - Accelerator Physics, High Energy Physics - Experiment
Abstract

This report presents a brief summary of the science opportunities and program of a polarized medium energy electron-ion collider at Jefferson Lab and a comprehensive description of the conceptual design of such a collider based on the CEBAF electron accelerator facility., Comment: 160 pages, ~93 figures This work was supported by the U.S. Department of Energy, Office of Nuclear Physics, under Contract No. DE-AC05-06OR23177, DE-AC02-06CH11357, DE-AC05-060R23177, and DESC0005823. The U.S. Government retains a non-exclusive, paid-up, irrevocable, world-wide license to publish or reproduce this manuscript for U.S. Government purposes

Published
2012

22. Physical Programm and Acceleration of Polarized Light Nuclei Beams at Jinr Nuclotron

Author

Vokal, S., Kovalenko, A. D., Kondratenko, A. M., Kondratenko, M. A., Mikhailov, V. A., Filatov, Yu. N., and Shimanskiy, S. S.

Subjects
High Energy Physics - Experiment
Abstract

The physical spin program at high $p_T$ region and energies $s^{1/2}_{NN} \sim 10 GeV$ is discussed. It's shown that cumulative processes, color transparency problem and polarization phenomenons directly connect with properties new form of the nuclear matter as Color Quark Condensate(CQC). Studies of CQC one of the most important physical problem and can be realized using polarized ion beams at JINR nuclotron-M (and in future at NICA). The calculations of spin resonance strengthes in the linear approximation for p, d, t and $^3He$ beams in the JINR nuclotron are presented. The methods to preserve the degree of polarization during crossing the spin resonances are examined. The method of matching the direction of polarization vector during the beam injection in to the ring of the nuclotron is given. These methods of spin resonance crossing can be used to accelerate polarized beams in the other cyclic accelerators., Comment: 8 pages, Will be published in Proceedings of XII Workshop on High Energy Spin Physics DSPIN-07, Dubna, September 3 - 7, 2007

Published
2008

34. Conception of High Intensive Polarized Proton Beam Formation in NICA Collider

Author

Syresin, Evgeny, Butenko, Andrey, Filatov, Yury, Kolokolchikov, Sergey, Kondratenko, Anatoliy, Kondratenko, M., Kostromin, Sergey, Kozlov, Oleg, Meshkov, Igor, Mityanina, Natalya, Senichev, Yury, Sidorin, Anatoly, Trubnikov, Grigoriy, Tuzikov, Alexey, and Zenkevich, Pavel

Subjects
MC1: Circular and Linear Colliders, Physics::Accelerator Physics, Nuclear Experiment, Accelerator Physics
Abstract

NICA (Nuclotron-based Ion Collider fAcility) is a new accelerator complex being assembled at JINR to search for the mixed phase of baryonic matter and to investigate the nature of nucleon/particle spin. The polarized proton beams will be operated at the energy range of 5-12.6 GeV, the beam intensity in each ring of 2.2x10¹³ and the luminosity of 1x10³² cm⁻² s⁻¹. The conception of formation of high intensive proton beams is discussed for two different schemes. In first scheme the protons are injected from Nuclotron to Collider at an energy of 2-2.5 GeV to provide the cooling and the storage at this energy and then they are accelerated up to energy of experiments. In the second scheme the cooling of protons is realized in one from accelerators of the injection chain and the protons are injected from Nuclotron to Collider at energy of experiments, where they are stored up required intensity., Proceedings of the 13th International Particle Accelerator Conference, IPAC2022, Bangkok, Thailand

Published
2022
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46. Spin Resonance Strength in the Transparent Spin Mode of the NICA Collider

Author

Filatov, Yury, Kondratenko, Anatoliy, Kondratenko, M., Kovalenko, Alexander, and Vinogradov, Stanislav

Subjects
MC1: Circular and Linear Colliders, Physics::Accelerator Physics, Accelerator Physics
Abstract

To implement the polarization program at the NICA complex (Dubna, Russia) the novel mode of ion polarization control - the transparent spin mode - is planned to use. To set up the transparent spin mode in the NICA collider two solenoidal snakes will be placed in straights of the Multi Purpose Detector (MPD) and the Spin Physics Detector (SPD). The beam polarization at SPD will be controlled by means of ‘‘weak’’ solenoids. The main characteristic of the transparent spin mode is the spin resonance strength, which consists of two parts: a coherent part arising due to additional transverse and longitudinal fields on the beam trajectory deviating from the design orbit and an incoherent part associated with the particles’ betatron and synchrotron oscillations (beam emittances). The resonance strength allows one to formulate requirements on the magnitudes of the control solenoids’ fields. The theoretical analysis, calculation and spin tracking simulation of the spin resonance strength in the whole momentum range of the NICA collider are presented., Proceedings of the 10th Int. Particle Accelerator Conf., IPAC2019, Melbourne, Australia

Published
2019
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47. Simulation of Transparent Spin Experiment in RHIC

Author

Huang, He, Adams, Petra, Derbenev, Yaroslav, Filatov, Yury, Huang, Haixin, Kondratenko, Anatoliy, Kondratenko, M., Lin, Fanglei, Méot, Francois, Morozov, Vasiliy, Ptitsyn, Vadim, Schmidke, William, and Zhang, Yuhong

Subjects
Physics::Accelerator Physics, 05: Beam Dynamics and EM Fields, Nuclear Experiment, Accelerator Physics
Abstract

The transparent spin mode has been proposed as a new technique for preservation and control of the spin polari-zation of ion beams in a synchrotron. The ion rings of the proposed Jefferson Lab Electron-Ion Collider (JLEIC) adopted this technique in their figure-8 design. The transparent spin mode can also be setup in a racetrack with two identical Siberian snakes. There is a proposal to test the predicted features of the spin transparent mode in Relativistic Heavy Ion Collider (RHIC), which already has all of the necessary hardware capabilities. We have earlier analytically estimated the setup parameters and developed a preliminary experimental plan. In this paper we describe simulation setup and benchmarking for the proposed experiment using a Zgoubi model of RHIC., Proceedings of the North American Particle Accelerator Conference, NAPAC2019, Lansing, MI, USA

Published
2019
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48. Spin Response Function for Spin Transparency Mode of RHIC

Author

Morozov, Vasiliy, Adams, Petra, Derbenev, Yaroslav, Filatov, Yury, Huang, Haixin, Huang, He, Kondratenko, Anatoliy, Kondratenko, M., Lin, Fanglei, Méot, Francois, Ptitsyn, Vadim, Schmidke, William, and Zhang, Yuhong

Subjects
MC1: Circular and Linear Colliders, Physics::Accelerator Physics, Condensed Matter::Strongly Correlated Electrons, Accelerator Physics
Abstract

In the Spin Transparency (ST) mode of RHIC, the axes of its Siberian snakes are parallel. The spin tune in the ST mode is zero and the spin motion becomes degenerate: any spin direction repeats every particle turn. In contrast, the lattice of a conventional collider determines a unique stable periodic spin direction, so that the collider operates in the Preferred Spin (PS) mode. Contributions of perturbing magnetic fields to the spin resonance strengths in the PS mode are usually calculated using the spin response function. However, in that form, it is not applicable in the ST mode. This paper presents a response function formalism expanded for the ST mode of operation of conventional colliders with two identical Siberian snakes in the highly-relativistic limit. We present calculations of the spin response function for RHIC in the ST mode., Proceedings of the 10th Int. Particle Accelerator Conf., IPAC2019, Melbourne, Australia

Published
2019
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49. EXPERIMENTAL VERIFICATION OF TRANSPARENT SPIN MODE IN RHIC

Author

Morozov, Vasiliy, Adams, Petra, Derbenev, Yaroslav, Filatov, Yury, Huang, Haixin, Huang, He, Kondratenko, Anatoliy, Kondratenko, M., Lin, Fanglei, Méot, Francois, Ptitsyn, Vadim, Schmidke, William, and Zhang, Yuhong

Subjects
MC1: Circular and Linear Colliders, Physics::Accelerator Physics, Accelerator Physics
Abstract

High electron and ion polarizations are some of the key design requirements of a future Electron Ion Collider (EIC). The transparent spin mode, a concept inspired by the figure 8 ring design of JLEIC, is a novel technique for preservation and control of electron and ion spin polarizations in a collider or storage ring. It makes the ring lattice "invisible" to the spin and allows for polarization control by small quasi-static magnetic fields with practically no effect on the beam’s orbital characteristics. It offers unique opportunities for polarization maintenance and control in Jefferson Lab’s JLEIC and in BNL’s eRHIC. The transparent spin mode has been demonstrated in simulations and we now plan to test it experimentally. We present a design of an experiment using a polarized proton beam stored in one of the RHIC rings. In the experiment, one of the RHIC rings is configured in the transparent spin mode by aligning the axes of its two Siberian snakes. The experiment goals, procedures, hardware requirements and expected results are presented., Proceedings of the 10th Int. Particle Accelerator Conf., IPAC2019, Melbourne, Australia

Published
2019
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