Yu. M. Andreev, D. Banerjee, B. Banto Oberhauser, J. Bernhard, P. Bisio, N. Charitonidis, P. Crivelli, E. Depero, A. V. Dermenev, S. V. Donskov, R. R. Dusaev, T. Enik, V. N. Frolov, A. Gardikiotis, S. V. Gertsenberger, S. Girod, S. N. Gninenko, M. Hösgen, R. Joosten, V. A. Kachanov, Y. Kambar, A. E. Karneyeu, E. A. Kasianova, G. Kekelidze, B. Ketzer, D. V. Kirpichnikov, M. M. Kirsanov, V. N. Kolosov, V. A. Kramarenko, L. V. Kravchuk, N. V. Krasnikov, S. V. Kuleshov, V. E. Lyubovitskij, V. Lysan, V. A. Matveev, R. Mena Fredes, R. G. Mena Yanssen, L. Molina Bueno, M. Mongillo, D. V. Peshekhonov, V. A. Polyakov, B. Radics, K. M. Salamatin, V. D. Samoylenko, D. A. Shchukin, O. Soto, H. Sieber, V. O. Tikhomirov, I. V. Tlisova, A. N. Toropin, M. Tuzi, B. M. Veit, P. V. Volkov, V. Yu. Volkov, I. V. Voronchikhin, J. Zamora-Saá, A. S. Zhevlakov
{"title":"在欧洲核子研究中心空间站的 NA64 实验中利用高能μ介子揭示暗黑扇区","authors":"Yu. M. Andreev, D. Banerjee, B. Banto Oberhauser, J. Bernhard, P. Bisio, N. Charitonidis, P. Crivelli, E. Depero, A. V. Dermenev, S. V. Donskov, R. R. Dusaev, T. Enik, V. N. Frolov, A. Gardikiotis, S. V. Gertsenberger, S. Girod, S. N. Gninenko, M. Hösgen, R. Joosten, V. A. Kachanov, Y. Kambar, A. E. Karneyeu, E. A. Kasianova, G. Kekelidze, B. Ketzer, D. V. Kirpichnikov, M. M. Kirsanov, V. N. Kolosov, V. A. Kramarenko, L. V. Kravchuk, N. V. Krasnikov, S. V. Kuleshov, V. E. Lyubovitskij, V. Lysan, V. A. Matveev, R. Mena Fredes, R. G. Mena Yanssen, L. Molina Bueno, M. Mongillo, D. V. Peshekhonov, V. A. Polyakov, B. Radics, K. M. Salamatin, V. D. Samoylenko, D. A. Shchukin, O. Soto, H. Sieber, V. O. Tikhomirov, I. V. Tlisova, A. N. Toropin, M. Tuzi, B. M. Veit, P. V. Volkov, V. Yu. Volkov, I. V. Voronchikhin, J. Zamora-Saá, A. S. Zhevlakov","doi":"arxiv-2409.10128","DOIUrl":null,"url":null,"abstract":"A search for Dark Sectors is performed using the unique M2 beam line at the\nCERN Super Proton Synchrotron. New particles ($X$) could be produced in the\nbremsstrahlung-like reaction of high energy 160 GeV muons impinging on an\nactive target, $\\mu N\\rightarrow\\mu NX$, followed by their decays,\n$X\\rightarrow\\text{invisible}$. The experimental signature would be a scattered\nsingle muon from the target, with about less than half of its initial energy\nand no activity in the sub-detectors located downstream the interaction point.\nThe full sample of the 2022 run is analyzed through the missing energy/momentum\nchannel, with a total statistics of $(1.98\\pm0.02)\\times10^{10}$ muons on\ntarget. We demonstrate that various muon-philic scenarios involving different\ntypes of mediators, such as scalar or vector particles, can be probed\nsimultaneously with such a technique. For the vector-case, besides a\n$L_\\mu-L_\\tau$ $Z'$ vector boson, we also consider an invisibly decaying dark\nphoton ($A'\\rightarrow\\text{invisible}$). This search is complementary to NA64\nrunning with electrons and positrons, thus, opening the possibility to expand\nthe exploration of the thermal light dark matter parameter space by combining\nthe results obtained with the three beams.","PeriodicalId":501181,"journal":{"name":"arXiv - PHYS - High Energy Physics - Experiment","volume":"69 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Shedding light on Dark Sectors with high-energy muons at the NA64 experiment at the CERN SPS\",\"authors\":\"Yu. M. Andreev, D. Banerjee, B. Banto Oberhauser, J. Bernhard, P. Bisio, N. Charitonidis, P. Crivelli, E. Depero, A. V. Dermenev, S. V. Donskov, R. R. Dusaev, T. Enik, V. N. Frolov, A. Gardikiotis, S. V. Gertsenberger, S. Girod, S. N. Gninenko, M. Hösgen, R. Joosten, V. A. Kachanov, Y. Kambar, A. E. Karneyeu, E. A. Kasianova, G. Kekelidze, B. Ketzer, D. V. Kirpichnikov, M. M. Kirsanov, V. N. Kolosov, V. A. Kramarenko, L. V. Kravchuk, N. V. Krasnikov, S. V. Kuleshov, V. E. Lyubovitskij, V. Lysan, V. A. Matveev, R. Mena Fredes, R. G. Mena Yanssen, L. Molina Bueno, M. Mongillo, D. V. Peshekhonov, V. A. Polyakov, B. Radics, K. M. Salamatin, V. D. Samoylenko, D. A. Shchukin, O. Soto, H. Sieber, V. O. Tikhomirov, I. V. Tlisova, A. N. Toropin, M. Tuzi, B. M. Veit, P. V. Volkov, V. Yu. Volkov, I. V. Voronchikhin, J. Zamora-Saá, A. S. Zhevlakov\",\"doi\":\"arxiv-2409.10128\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A search for Dark Sectors is performed using the unique M2 beam line at the\\nCERN Super Proton Synchrotron. New particles ($X$) could be produced in the\\nbremsstrahlung-like reaction of high energy 160 GeV muons impinging on an\\nactive target, $\\\\mu N\\\\rightarrow\\\\mu NX$, followed by their decays,\\n$X\\\\rightarrow\\\\text{invisible}$. The experimental signature would be a scattered\\nsingle muon from the target, with about less than half of its initial energy\\nand no activity in the sub-detectors located downstream the interaction point.\\nThe full sample of the 2022 run is analyzed through the missing energy/momentum\\nchannel, with a total statistics of $(1.98\\\\pm0.02)\\\\times10^{10}$ muons on\\ntarget. We demonstrate that various muon-philic scenarios involving different\\ntypes of mediators, such as scalar or vector particles, can be probed\\nsimultaneously with such a technique. For the vector-case, besides a\\n$L_\\\\mu-L_\\\\tau$ $Z'$ vector boson, we also consider an invisibly decaying dark\\nphoton ($A'\\\\rightarrow\\\\text{invisible}$). This search is complementary to NA64\\nrunning with electrons and positrons, thus, opening the possibility to expand\\nthe exploration of the thermal light dark matter parameter space by combining\\nthe results obtained with the three beams.\",\"PeriodicalId\":501181,\"journal\":{\"name\":\"arXiv - PHYS - High Energy Physics - Experiment\",\"volume\":\"69 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-16\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - High Energy Physics - Experiment\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.10128\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Physics - Experiment","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.10128","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Shedding light on Dark Sectors with high-energy muons at the NA64 experiment at the CERN SPS
A search for Dark Sectors is performed using the unique M2 beam line at the
CERN Super Proton Synchrotron. New particles ($X$) could be produced in the
bremsstrahlung-like reaction of high energy 160 GeV muons impinging on an
active target, $\mu N\rightarrow\mu NX$, followed by their decays,
$X\rightarrow\text{invisible}$. The experimental signature would be a scattered
single muon from the target, with about less than half of its initial energy
and no activity in the sub-detectors located downstream the interaction point.
The full sample of the 2022 run is analyzed through the missing energy/momentum
channel, with a total statistics of $(1.98\pm0.02)\times10^{10}$ muons on
target. We demonstrate that various muon-philic scenarios involving different
types of mediators, such as scalar or vector particles, can be probed
simultaneously with such a technique. For the vector-case, besides a
$L_\mu-L_\tau$ $Z'$ vector boson, we also consider an invisibly decaying dark
photon ($A'\rightarrow\text{invisible}$). This search is complementary to NA64
running with electrons and positrons, thus, opening the possibility to expand
the exploration of the thermal light dark matter parameter space by combining
the results obtained with the three beams.