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Dark photons are hypothetical massive vector particles that could mix with ordinary photons. The simplest theoretical model is fully characterised by only two parameters: the mass of the dark photon m$_{\gamma^{\mathrm{D}}}$ and its mixing…

High Energy Physics - Experiment · Physics 2023-01-11 SHiP Collaboration , C. Ahdida , A. Akmete , R. Albanese , A. Alexandrov , A. Anokhina , S. Aoki , G. Arduini , E. Atkin , N. Azorskiy , J. J. Back , A. Bagulya , F. Baaltasar Dos Santos , A. Baranov , F. Bardou , G. J. Barker , M. Battistin , J. Bauche , A. Bay , V. Bayliss , G. Bencivenni , A. Y. Berdnikov , Y. A. Berdnikov , M. Bertani , C. Betancourt , I. Bezshyiko , O. Bezshyyko , D. Bick , S. Bieschke , A. Blanco , J. Boehm , M. Bogomilov , I. Boiarska , K. Bondarenko , W. M. Bonivento , J. Borburgh , A. Boyarsky , R. Brenner , D. Breton , V. Büscher , A. Buonaura , S. Buontempo , S. Cadeddu , A. Calcaterra , M. Calviani , M. Campanelli , M. Casolino , N. Charitonidis , P. Chau , J. Chauveau , A. Chepurnov , M. Chernyavskiy , K. -Y. Choi , A. Chumakov , P. Ciambrone , V. Cicero , L. Congedo , K. Cornelis , M. Cristinziani , A. Crupano , G. M. Dallavalle , A. Datwyler , N. D'Ambrosio , G. D'Appollonio , R. de Asmundis , J. De Carvalho Saraiva , G. De Lellis , M. de Magistris , A. De Roeck , M. De Serio , D. De Simone , L. Dedenko , P. Dergachev , A. Di Crescenzo , L. Di Giulio , N. Di Marco , C. Dib , H. Dijkstra , V. Dmitrenko , L. A. Dougherty , A. Dolmatov , D. Domenici , S. Donskov , V. Drohan , A. Dubreuil , O. Durhan , M. Ehlert , E. Elikkaya , T. Enik , A. Etenko , F. Fabbri , O. Fedin , F. Fedotovs , G. Felici , M. Ferrillo , M. Ferro-Luzzi , K. Filippov , R. A. Fini , P. Fonte , C. Franco , M. Fraser , R. Fresa , R. Froeschl , T. Fukuda , G. Galati , J. Gall , L. Gatignon , G. Gavrilov , V. Gentile , B. Goddard , L. Golinka-Bezshyyko , A. Golovatiuk , V. Golovtsov , D. Golubkov , A. Golutvin , P. Gorbounov , D. Gorbunov , S. Gorbunov , V. Gorkavenko , M. Gorshenkov , V. Grachev , A. L. Grandchamp , E. Graverini , J. -L. Grenard , D. Grenier , V. Grichine , N. Gruzinskii , A. M. Guler , Yu. Guz , G. J. Haefeli , C. Hagner , H. Hakobyan , I. W. Harris , E. van Herwijnen , C. Hessler , A. Hollnagel , B. Hosseini , M. Hushchyn , G. Iaselli , A. Iuliano , R. Jacobsson , D. Joković , M. Jonker , I. Kadenko , V. Kain , B. Kaiser , C. Kamiscioglu , D. Karpenkov , K. Kershaw , M. Khabibullin , E. Khalikov , G. Khaustov , G. Khoriauli , A. Khotyantsev , Y. G. Kim , V. Kim , N. Kitagawa , J. -W. Ko , K. Kodama , A. Kolesnikov , D. I. Kolev , V. Kolosov , M. Komatsu , A. Kono , N. Konovalova , S. Kormannshaus , I. Korol , I. Korol'ko , A. Korzenev , V. Kostyukhin , E. Koukovini Platia , S. Kovalenko , I. Krasilnikova , Y. Kudenko , E. Kurbatov , P. Kurbatov , V. Kurochka , E. Kuznetsova , H. M. Lacker , M. Lamont , G. Lanfranchi , O. Lantwin , A. Lauria , K. S. Lee , K. Y. Lee , J. -M. Lévy , V. P. Loschiavo , L. Lopes , E. Lopez Sola , V. Lyubovitskij , J. Maalmi , A. -M. Magnan , V. Maleev , A. Malinin , Y. Manabe , A. K. Managadze , M. Manfredi , S. Marsh , A. M. Marshall , A. Mefodev , P. Mermod , A. Miano , S. Mikado , Yu. Mikhaylov , D. A. Milstead , O. Mineev , A. Montanari , M. C. Montesi , K. Morishima , S. Movchan , Y. Muttoni , N. Naganawa , M. Nakamura , T. Nakano , S. Nasybulin , P. Ninin , A. Nishio , A. Novikov , B. Obinyakov , S. Ogawa , N. Okateva , B. Opitz , J. Osborne , M. Ovchynnikov , N. Owtscharenko , P. H. Owen , P. Pacholek , A. Paoloni , B. D. Park , A. Pastore , M. Patel , D. Pereyma , A. Perillo-Marcone , G. L. Petkov , K. Petridis , A. Petrov , D. Podgrudkov , V. Poliakov , N. Polukhina , J. Prieto Prieto , M. Prokudin , A. Prota , A. Quercia , A. Rademakers , A. Rakai , F. Ratnikov , T. Rawlings , F. Redi , S. Ricciardi , M. Rinaldesi , Volodymyr Rodin , Viktor Rodin , P. Robbe , A. B. Rodrigues Cavalcante , T. Roganova , H. Rokujo , G. Rosa , T. Rovelli , O. Ruchayskiy , T. Ruf , V. Samoylenko , V. Samsonov , F. Sanchez Galan , P. Santos Diaz , A. Sanz Ull , A. Saputi , O. Sato , E. S. Savchenko , J. S. Schliwinski , W. Schmidt-Parzefall , N. Serra , S. Sgobba , O. Shadura , A. Shakin , M. Shaposhnikov , P. Shatalov , T. Shchedrina , L. Shchutska , V. Shevchenko , H. Shibuya , S. Shirobokov , A. Shustov , S. B. Silverstein , S. Simone , R. Simoniello , M. Skorokhvatov , S. Smirnov , J. Y. Sohn , A. Sokolenko , E. Solodko , N. Starkov , L. Stoel , M. E. Stramaglia , D. Sukhonos , Y. Suzuki , S. Takahashi , J. L. Tastet , P. Teterin , S. Than Naing , I. Timiryasov , V. Tioukov , D. Tommasini , M. Torii , N. Tosi , D. Treille , R. Tsenov , S. Ulin , E. Ursov , A. Ustyuzhanin , Z. Uteshev , L. Uvarov , G. Vankova-Kirilova , F. Vannucci , V. Venturi , S. Vilchinski , Heinz Vincke , Helmut Vincke , C. Visone , K. Vlasik , A. Volkov , R. Voronkov , S. van Waasen , R. Wanke , P. Wertelaers , O. Williams , J. -K. Woo , M. Wurm , S. Xella , D. Yilmaz , A. U. Yilmazer , C. S. Yoon , Yu. Zaytsev , A. Zelenov , J. Zimmerman

Dark matter is a well-established theoretical addition to the Standard Model supported by many observations in modern astrophysics and cosmology. In this context, the existence of weakly interacting massive particles represents an appealing…

High Energy Physics - Experiment · Physics 2021-06-03 SHiP Collaboration

The Search for Hidden Particles (SHiP) Collaboration has proposed a general-purpose experimental facility operating in beam-dump mode at the CERN SPS accelerator to search for light, feebly interacting particles. The SHiP experiment…

Instrumentation and Detectors · Physics 2022-05-23 SHIP Collaboration

Several models of dark matter suggest the existence of dark sectors consisting of SU(3)_C x SU(2)_L x U(1)_Y singlet fields. These sectors of particles do not interact with the ordinary matter directly but could couple to it via gravity. In…

We consider current observational constraints on the electromagnetic charge of dark matter. The velocity dependence of the scattering cross-section through the photon gives rise to qualitatively different constraints than standard dark…

High Energy Physics - Phenomenology · Physics 2011-03-22 Samuel D. McDermott , Hai-Bo Yu , Kathryn M. Zurek

Pions of a dark sector gauge group can be strongly interacting massive particle (SIMP) dark matter, produced by the freeze-out of $3 \to 2$ interactions, with naturally large self-interactions. We study if adding a dark photon to the set-up…

High Energy Physics - Phenomenology · Physics 2023-04-14 Pieter Braat , Marieke Postma

Dark matter produced from thermal freeze-out is typically restricted to have masses above roughly 1 MeV. However, if the couplings are small, the freeze-in mechanism allows for production of dark matter down to keV masses. We consider dark…

High Energy Physics - Phenomenology · Physics 2025-11-04 Jae Hyeok Chang , Rouven Essig , Annika Reinert

Dark matter could be made up of dark photons, massive but very light particles whose interactions with matter resemble those of usual photons but suppressed by a small mixing parameter. We analyze the main approaches to dark photon…

High Energy Physics - Phenomenology · Physics 2019-09-13 C. Álvarez-Luna , J. A. R. Cembranos

We report direction detection constraints on the presence of hidden photon dark matter with masses between 20-30 ueV using a cryogenic emitter-receiver-amplifier spectroscopy setup designed as the first iteration of QUALIPHIDE (QUantum…

Cosmology and Nongalactic Astrophysics · Physics 2023-06-21 Karthik Ramanathan , Nikita Klimovich , Ritoban Basu Thakur , Byeong Ho Eom , Henry G. LeDuc , Shibo Shu , Andrew D. Beyer , Peter K. Day

DarkSHINE is an electron fixed target experiment under proposal that aims to probe light dark matter in the MeV-GeV mass range via the invisible decay of dark photons, leveraging the High repetition rate 8 GeV electron beam from the…

High Energy Physics - Experiment · Physics 2025-12-16 Haijun Yang

Dark matter detectors built primarily to probe elastic scattering of WIMPs on nuclei are also precise probes of light, weakly coupled particles that may be absorbed by the detector material. In this paper, we derive constraints on the…

High Energy Physics - Phenomenology · Physics 2015-07-23 Haipeng An , Maxim Pospelov , Josef Pradler , Adam Ritz

New gauge bosons at the MeV scale with tiny gauge couplings (so-called dark photons) can be responsible for the freeze-in production of dark matter and provide a clear target for present and future experiments. We study the effects of…

High Energy Physics - Phenomenology · Physics 2020-03-04 Saniya Heeba , Felix Kahlhoefer

We report new limits on the kinetic mixing strength of the dark photon spanning the mass range 0.21 -- 1.24 $\mu$eV corresponding to a frequency span of 50 -- 300 MHz. The Dark E-Field Radio experiment is a wide-band search for dark photon…

High Energy Physics - Experiment · Physics 2024-06-03 Joseph Levine , Benjamin Godfrey , J. Anthony Tyson , S. Mani Tripathi , Daniel Polin , Amin Aminaei , Brian H. Kolner , Paul Stucky

Searches for dark matter with liquid xenon time projection chamber experiments have traditionally focused on the region of the parameter space that is characteristic of weakly interacting massive particles, ranging from a few GeV/$c^2$ to a…

High Energy Physics - Experiment · Physics 2024-06-19 J. Aalbers , D. S. Akerib , A. K. Al Musalhi , C. S. Amarasinghe , A. Ames , T. J. Anderson , N. Angelides , H. M. Araújo , J. E. Armstrong , M. Arthurs , A. Baker , S. Balashov , J. Bang , J. W. Bargemann , A. Baxter , K. Beattie , T. Benson , A. Bhatti , A. Biekert , T. P. Biesiadzinski , H. J. Birch , E. Bishop , G. M. Blockinger , B. Boxer , C. A. J. Brew , P. Brás , S. Burdin , M. Buuck , M. C. Carmona-Benitez , M. Carter , A. Chawla , H. Chen , J. J. Cherwinka , N. I. Chott , M. V. Converse , A. Cottle , G. Cox , D. Curran , C. E. Dahl , A. David , J. Delgaudio , S. Dey , L. de Viveiros , C. Ding , J. E. Y. Dobson , E. Druszkiewicz , S. R. Eriksen , A. Fan , N. M. Fearon , S. Fiorucci , H. Flaecher , E. D. Fraser , T. M. A. Fruth , R. J. Gaitskell , A. Geffre , J. Genovesi , C. Ghag , R. Gibbons , S. Gokhale , J. Green , M. G. D. van der Grinten , C. R. Hall , S. Han , E. Hartigan-O'Connor , S. J. Haselschwardt , S. A. Hertel , G. Heuermann , G. J. Homenides , M. Horn , D. Q. Huang , D. Hunt , C. M. Ignarra , E. Jacquet , R. S. James , J. Johnson , A. C. Kaboth , A. C. Kamaha , D. Khaitan , A. Khazov , I. Khurana , J. Kim , J. Kingston , R. Kirk , D. Kodroff , L. Korley , E. V. Korolkova , H. Kraus , S. Kravitz , L. Kreczko , B. Krikler , V. A. Kudryavtsev , J. Lee , D. S. Leonard , K. T. Lesko , C. Levy , J. Lin , A. Lindote , R. Linehan , W. H. Lippincott , M. I. Lopes , E. Lopez Asamar , W. Lorenzon , C. Lu , S. Luitz , P. A. Majewski , A. Manalaysay , R. L. Mannino , C. Maupin , M. E. McCarthy , G. McDowell , D. N. McKinsey , J. McLaughlin , R. McMonigle , E. H. Miller , E. Mizrachi , A. Monte , M. E. Monzani , J. D. Morales Mendoza , E. Morrison , B. J. Mount , M. Murdy , A. St. J. Murphy , A. Naylor , C. Nedlik , H. N. Nelson , F. Neves , A. Nguyen , J. A. Nikoleyczik , I. Olcina , K. C. Oliver-Mallory , J. Orpwood , K. J. Palladino , J. Palmer , N. J. Pannifer , N. Parveen , S. J. Patton , B. Penning , G. Pereira , E. Perry , T. Pershing , A. Piepke , Y. Qie , J. Reichenbacher , C. A. Rhyne , Q. Riffard , G. R. C. Rischbieter , H. S. Riyat , R. Rosero , T. Rushton , D. Rynders , D. Santone , A. B. M. R. Sazzad , R. W. Schnee , S. Shaw , T. Shutt , J. J. Silk , C. Silva , G. Sinev , R. Smith , V. N. Solovov , P. Sorensen , J. Soria , I. Stancu , A. Stevens , K. Stifter , B. Suerfu , T. J. Sumner , M. Szydagis , W. C. Taylor , D. R. Tiedt , M. Timalsina , Z. Tong , D. R. Tovey , J. Tranter , M. Trask , M. Tripathi , D. R. Tronstad , W. Turner , A. Vacheret , A. C. Vaitkus , V. Velan , A. Wang , J. J. Wang , Y. Wang , J. R. Watson , R. C. Webb , L. Weeldreyer , T. J. Whitis , M. Williams , W. J. Wisniewski , F. L. H. Wolfs , S. Woodford , D. Woodward , C. J. Wright , Q. Xia , X. Xiang , J. Xu , M. Yeh , E. A. Zweig

We investigate a dark sector containing a pair of light non-degenerate scalar particles, with masses in the MeV-GeV range, coupled to the visible sector through heavier mediators. The heaviest dark state is long-lived, and its decays offer…

High Energy Physics - Phenomenology · Physics 2022-05-17 Enrico Bertuzzo , Marco Taoso

In this work, we present UV completions of the recently proposed number-changing Co-SIMP freeze-out mechanism. In contrast to the standard cannibalistic-type dark matter picture that occurs entirely in the dark sector, the $3\to 2$ process…

High Energy Physics - Phenomenology · Physics 2023-08-28 Aditya Parikh , Juri Smirnov , Weishuang Linda Xu , Bei Zhou

Motivated by various kinds of new physics models, a new light neutral vector boson (the dark photon) connected to the Standard Model of particle physics only through the kinetic mixing with the U(1)_Y factor has been studied extensively.…

High Energy Physics - Phenomenology · Physics 2014-02-03 Haipeng An , Maxim Pospelov , Josef Pradler

Dark photons, hypothesized to be sufficiently light and/or weakly interacting, offer a compelling candidate for dark matter. Their decay into three photons, referred to as the "dark photon trident" process, becomes the dominant channel when…

High Energy Physics - Phenomenology · Physics 2025-06-17 Thong T. Q. Nguyen

The dark photon is widely predicted in many new physics beyond the Standard Model. In this work, we propose to utilize the polarized lepton cross section in neutral current DIS process at the HERA and upcoming Electron-Ion Collider (EIC) to…

High Energy Physics - Phenomenology · Physics 2022-08-24 Bin Yan

SHiP is a newly proposed fixed-target experiment at the CERN SPS with the aim of searching for hidden particles that interact very weakly with SM particles. The work presented in this document investigates SHiP's physics reach in the…

High Energy Physics - Experiment · Physics 2015-07-09 Elena Graverini , Nicola Serra , Barbara Storaci
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