_version_ 1866917713301995520
author Andreev, Yu. M.
Antonov, A.
Banerjee, D.
Oberhauser, B. Banto
Bernhard, J.
Bisio, P.
Celentano, A.
Charitonidis, N.
Cooke, D.
Crivelli, P.
Depero, E.
Dermenev, A. V.
Donskov, S. V.
Dusaev, R. R.
Enik, T.
Frolov, V. N.
Gardikiotis, A.
Gninenko, S. N.
Hösgen, M.
Kachanov, V. A.
Kambar, Y.
Karneyeu, A. E.
Kekelidze, G.
Ketzer, B.
Kirpichnikov, D. V.
Kirsanov, M. M.
Kolosov, V. N.
Gertsenberger, S. V.
Girod, S.
Kasianova, E. A.
Kramarenko, V. A.
Kravchuk, L. V.
Krasnikov, N. V.
Kuleshov, S. V.
Lyubovitskij, V. E.
Lysan, V.
Marini, A.
Marsicano, L.
Matveev, V. A.
Fredes, R. Mena
Yanssen, R. Mena
Bueno, L. Molina
Mongillo, M.
Peshekhonov, D. V.
Polyakov, V. A.
Radics, B.
Salamatin, K.
Samoylenko, V. D.
Sieber, H.
Shchukin, D.
Soto, O.
Tikhomirov, V. O.
Tlisova, I.
Toropin, A. N.
Tuzi, M.
Ulloa, P.
Volkov, P. V.
Volkov, V. Yu.
Voronchikhin, I. V.
Zamora-Saá, J.
Zhevlako, A. S.
author_facet Andreev, Yu. M.
Antonov, A.
Banerjee, D.
Oberhauser, B. Banto
Bernhard, J.
Bisio, P.
Celentano, A.
Charitonidis, N.
Cooke, D.
Crivelli, P.
Depero, E.
Dermenev, A. V.
Donskov, S. V.
Dusaev, R. R.
Enik, T.
Frolov, V. N.
Gardikiotis, A.
Gninenko, S. N.
Hösgen, M.
Kachanov, V. A.
Kambar, Y.
Karneyeu, A. E.
Kekelidze, G.
Ketzer, B.
Kirpichnikov, D. V.
Kirsanov, M. M.
Kolosov, V. N.
Gertsenberger, S. V.
Girod, S.
Kasianova, E. A.
Kramarenko, V. A.
Kravchuk, L. V.
Krasnikov, N. V.
Kuleshov, S. V.
Lyubovitskij, V. E.
Lysan, V.
Marini, A.
Marsicano, L.
Matveev, V. A.
Fredes, R. Mena
Yanssen, R. Mena
Bueno, L. Molina
Mongillo, M.
Peshekhonov, D. V.
Polyakov, V. A.
Radics, B.
Salamatin, K.
Samoylenko, V. D.
Sieber, H.
Shchukin, D.
Soto, O.
Tikhomirov, V. O.
Tlisova, I.
Toropin, A. N.
Tuzi, M.
Ulloa, P.
Volkov, P. V.
Volkov, V. Yu.
Voronchikhin, I. V.
Zamora-Saá, J.
Zhevlako, A. S.
contents The inclusion of an additional $U(1)$ gauge $L_μ-L_τ$ symmetry would release the tension between the measured and the predicted value of the anomalous muon magnetic moment: this paradigm assumes the existence of a new, light $Z^\prime$ vector boson, with dominant coupling to $μ$ and $τ$ leptons and interacting with electrons via a loop mechanism. The $L_μ-L_τ$ model can also explain the Dark Matter relic abundance, by assuming that the $Z'$ boson acts as a "portal" to a new Dark Sector of particles in Nature, not charged under known interactions. In this work we present the results of the $Z'$ search performed by the NA64-$e$ experiment at CERN SPS, that collected $\sim 9\times10^{11}$ 100 GeV electrons impinging on an active thick target. Despite the suppressed $Z'$ production yield with an electron beam, NA64-$e$ provides the first accelerator-based results excluding the $g-2$ preferred band of the $Z'$ parameter space in the 1 keV $ < m_{Z'} \lesssim 2$ MeV range, in complementarity with the limits recently obtained by the NA64-$μ$ experiment with a muon beam.
format Preprint
id arxiv_https___arxiv_org_abs_2404_06982
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle First constraints on the $L_μ-L_τ$ explanation of the muon $g-2$ anomaly from NA64-$e$ at CERN
Andreev, Yu. M.
Antonov, A.
Banerjee, D.
Oberhauser, B. Banto
Bernhard, J.
Bisio, P.
Celentano, A.
Charitonidis, N.
Cooke, D.
Crivelli, P.
Depero, E.
Dermenev, A. V.
Donskov, S. V.
Dusaev, R. R.
Enik, T.
Frolov, V. N.
Gardikiotis, A.
Gninenko, S. N.
Hösgen, M.
Kachanov, V. A.
Kambar, Y.
Karneyeu, A. E.
Kekelidze, G.
Ketzer, B.
Kirpichnikov, D. V.
Kirsanov, M. M.
Kolosov, V. N.
Gertsenberger, S. V.
Girod, S.
Kasianova, E. A.
Kramarenko, V. A.
Kravchuk, L. V.
Krasnikov, N. V.
Kuleshov, S. V.
Lyubovitskij, V. E.
Lysan, V.
Marini, A.
Marsicano, L.
Matveev, V. A.
Fredes, R. Mena
Yanssen, R. Mena
Bueno, L. Molina
Mongillo, M.
Peshekhonov, D. V.
Polyakov, V. A.
Radics, B.
Salamatin, K.
Samoylenko, V. D.
Sieber, H.
Shchukin, D.
Soto, O.
Tikhomirov, V. O.
Tlisova, I.
Toropin, A. N.
Tuzi, M.
Ulloa, P.
Volkov, P. V.
Volkov, V. Yu.
Voronchikhin, I. V.
Zamora-Saá, J.
Zhevlako, A. S.
High Energy Physics - Experiment
High Energy Physics - Phenomenology
The inclusion of an additional $U(1)$ gauge $L_μ-L_τ$ symmetry would release the tension between the measured and the predicted value of the anomalous muon magnetic moment: this paradigm assumes the existence of a new, light $Z^\prime$ vector boson, with dominant coupling to $μ$ and $τ$ leptons and interacting with electrons via a loop mechanism. The $L_μ-L_τ$ model can also explain the Dark Matter relic abundance, by assuming that the $Z'$ boson acts as a "portal" to a new Dark Sector of particles in Nature, not charged under known interactions. In this work we present the results of the $Z'$ search performed by the NA64-$e$ experiment at CERN SPS, that collected $\sim 9\times10^{11}$ 100 GeV electrons impinging on an active thick target. Despite the suppressed $Z'$ production yield with an electron beam, NA64-$e$ provides the first accelerator-based results excluding the $g-2$ preferred band of the $Z'$ parameter space in the 1 keV $ < m_{Z'} \lesssim 2$ MeV range, in complementarity with the limits recently obtained by the NA64-$μ$ experiment with a muon beam.
title First constraints on the $L_μ-L_τ$ explanation of the muon $g-2$ anomaly from NA64-$e$ at CERN
topic High Energy Physics - Experiment
High Energy Physics - Phenomenology
url https://arxiv.org/abs/2404.06982