{"title":"大质量自旋为2的暗物质介质的类似轫致辐射的产生","authors":"I. Voronchikhin, D. Kirpichnikov","doi":"10.1140/epjc/s10052-025-14868-6","DOIUrl":null,"url":null,"abstract":"<div><p>The link between Standard Model (SM) particles and dark matter (DM) can be introduced via spin-2 massive mediator, <span>\\( {\\text {G}}\\)</span>, that couples to photon and charged leptons. Moreover, in a mediator mass range from sub-MeV to sub-GeV, fixed-target facilities such as NA64e, LDMX, NA64<span>\\(\\mu \\)</span>, <span>\\(\\hbox {M}^3\\)</span>, and E137, can potentially probe such particle of the hidden sector via the signatures that are described by the bremsstrahlung-like process involving tensor mediator. We compare numerically the Weizsaker–Williams (WW) approximation and the exact tree-level (ETL) method for the bremsstrahlung-like mediator production cross section by choosing various parameters of the fixed-target experiments. To be more specific, the determination of WW validity region (in the parameter space of spin-2 DM mediator scenario, that can be examined in the laboratory facilities) is of particular interest of the present manuscript. In addition, we derive novel constraints on spin-2 DM mediator parameter space from the data of the E137 fixed-target experiment. In particular, we demonstrate that the E137 experiment has been ruled out the couplings of the spin-2 mediator at the level of <span>\\(8~\\times ~10^{-8}~\\text{ GeV}^{-1}~\\lesssim ~c^{\\text {G}}_{ee}~\\lesssim ~10^{-5}~\\text{ GeV}^{-1}\\)</span> for the typical masses in the range <span>\\(100~\\text{ MeV }~\\lesssim ~m_{\\text {G}}~\\lesssim 800~\\text{ MeV }\\)</span>, that corresponds to the statistics of <span>\\(1.87~\\times ~10^{20}\\)</span> electrons accumulated on target. The latter implies its universal coupling to photons and electrons, <span>\\(c^{\\textrm{G}}_{\\gamma \\gamma }~=~c^{\\textrm{G}}_{ee}\\)</span>.\n\n</p></div>","PeriodicalId":788,"journal":{"name":"The European Physical Journal C","volume":"85 10","pages":""},"PeriodicalIF":4.8000,"publicationDate":"2025-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1140/epjc/s10052-025-14868-6.pdf","citationCount":"0","resultStr":"{\"title\":\"The bremsstrahlung-like production of the massive spin-2 dark matter mediator\",\"authors\":\"I. Voronchikhin, D. Kirpichnikov\",\"doi\":\"10.1140/epjc/s10052-025-14868-6\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>The link between Standard Model (SM) particles and dark matter (DM) can be introduced via spin-2 massive mediator, <span>\\\\( {\\\\text {G}}\\\\)</span>, that couples to photon and charged leptons. Moreover, in a mediator mass range from sub-MeV to sub-GeV, fixed-target facilities such as NA64e, LDMX, NA64<span>\\\\(\\\\mu \\\\)</span>, <span>\\\\(\\\\hbox {M}^3\\\\)</span>, and E137, can potentially probe such particle of the hidden sector via the signatures that are described by the bremsstrahlung-like process involving tensor mediator. We compare numerically the Weizsaker–Williams (WW) approximation and the exact tree-level (ETL) method for the bremsstrahlung-like mediator production cross section by choosing various parameters of the fixed-target experiments. To be more specific, the determination of WW validity region (in the parameter space of spin-2 DM mediator scenario, that can be examined in the laboratory facilities) is of particular interest of the present manuscript. In addition, we derive novel constraints on spin-2 DM mediator parameter space from the data of the E137 fixed-target experiment. In particular, we demonstrate that the E137 experiment has been ruled out the couplings of the spin-2 mediator at the level of <span>\\\\(8~\\\\times ~10^{-8}~\\\\text{ GeV}^{-1}~\\\\lesssim ~c^{\\\\text {G}}_{ee}~\\\\lesssim ~10^{-5}~\\\\text{ GeV}^{-1}\\\\)</span> for the typical masses in the range <span>\\\\(100~\\\\text{ MeV }~\\\\lesssim ~m_{\\\\text {G}}~\\\\lesssim 800~\\\\text{ MeV }\\\\)</span>, that corresponds to the statistics of <span>\\\\(1.87~\\\\times ~10^{20}\\\\)</span> electrons accumulated on target. The latter implies its universal coupling to photons and electrons, <span>\\\\(c^{\\\\textrm{G}}_{\\\\gamma \\\\gamma }~=~c^{\\\\textrm{G}}_{ee}\\\\)</span>.\\n\\n</p></div>\",\"PeriodicalId\":788,\"journal\":{\"name\":\"The European Physical Journal C\",\"volume\":\"85 10\",\"pages\":\"\"},\"PeriodicalIF\":4.8000,\"publicationDate\":\"2025-10-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://link.springer.com/content/pdf/10.1140/epjc/s10052-025-14868-6.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The European Physical Journal C\",\"FirstCategoryId\":\"4\",\"ListUrlMain\":\"https://link.springer.com/article/10.1140/epjc/s10052-025-14868-6\",\"RegionNum\":2,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, PARTICLES & FIELDS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The European Physical Journal C","FirstCategoryId":"4","ListUrlMain":"https://link.springer.com/article/10.1140/epjc/s10052-025-14868-6","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, PARTICLES & FIELDS","Score":null,"Total":0}
The bremsstrahlung-like production of the massive spin-2 dark matter mediator
The link between Standard Model (SM) particles and dark matter (DM) can be introduced via spin-2 massive mediator, \( {\text {G}}\), that couples to photon and charged leptons. Moreover, in a mediator mass range from sub-MeV to sub-GeV, fixed-target facilities such as NA64e, LDMX, NA64\(\mu \), \(\hbox {M}^3\), and E137, can potentially probe such particle of the hidden sector via the signatures that are described by the bremsstrahlung-like process involving tensor mediator. We compare numerically the Weizsaker–Williams (WW) approximation and the exact tree-level (ETL) method for the bremsstrahlung-like mediator production cross section by choosing various parameters of the fixed-target experiments. To be more specific, the determination of WW validity region (in the parameter space of spin-2 DM mediator scenario, that can be examined in the laboratory facilities) is of particular interest of the present manuscript. In addition, we derive novel constraints on spin-2 DM mediator parameter space from the data of the E137 fixed-target experiment. In particular, we demonstrate that the E137 experiment has been ruled out the couplings of the spin-2 mediator at the level of \(8~\times ~10^{-8}~\text{ GeV}^{-1}~\lesssim ~c^{\text {G}}_{ee}~\lesssim ~10^{-5}~\text{ GeV}^{-1}\) for the typical masses in the range \(100~\text{ MeV }~\lesssim ~m_{\text {G}}~\lesssim 800~\text{ MeV }\), that corresponds to the statistics of \(1.87~\times ~10^{20}\) electrons accumulated on target. The latter implies its universal coupling to photons and electrons, \(c^{\textrm{G}}_{\gamma \gamma }~=~c^{\textrm{G}}_{ee}\).
期刊介绍:
Experimental Physics I: Accelerator Based High-Energy Physics
Hadron and lepton collider physics
Lepton-nucleon scattering
High-energy nuclear reactions
Standard model precision tests
Search for new physics beyond the standard model
Heavy flavour physics
Neutrino properties
Particle detector developments
Computational methods and analysis tools
Experimental Physics II: Astroparticle Physics
Dark matter searches
High-energy cosmic rays
Double beta decay
Long baseline neutrino experiments
Neutrino astronomy
Axions and other weakly interacting light particles
Gravitational waves and observational cosmology
Particle detector developments
Computational methods and analysis tools
Theoretical Physics I: Phenomenology of the Standard Model and Beyond
Electroweak interactions
Quantum chromo dynamics
Heavy quark physics and quark flavour mixing
Neutrino physics
Phenomenology of astro- and cosmoparticle physics
Meson spectroscopy and non-perturbative QCD
Low-energy effective field theories
Lattice field theory
High temperature QCD and heavy ion physics
Phenomenology of supersymmetric extensions of the SM
Phenomenology of non-supersymmetric extensions of the SM
Model building and alternative models of electroweak symmetry breaking
Flavour physics beyond the SM
Computational algorithms and tools...etc.