Title: Axion detection via superfluid 3He ferromagnetic phase and quantum measurement techniques
A<sc>bstract</sc> We propose to use the nuclear spin excitation in the ferromagnetic A1phase of the superfluid3He for the axion dark matter detection. This approach is striking in that it is sensitive to the axion-nucleon coupling, one of the most important features of the QCD axion introduced to solve the strong CP problem. We review a quantum mechanical description of the nuclear spin excitation and apply it to the estimation of the axion-induced spin excitation rate. We also describe a possible detection method of the spin excitation in detail and show that the combination of the squeezing of the final state with the Josephson parametric amplifier and the homodyne measurement can enhance the sensitivity. It turns out that this approach gives good sensitivity to the axion dark matter with the mass of$$ \mathcal{O} $$ (1) μeV depending on the size of the external magnetic field. We estimate the parameters of experimental setups, e.g., the detector volume and the amplitude of squeezing, required to reach the QCD axion parameter space. more »« less
Kalsi, Amandeep Kaur; Kamon, Teruki; Kim, Seulgi; Lee, Jason_S H; Rathjens, Denis; Roh, Youn Jung; Thompson, Adrian; Watson, Ian James
(, Journal of High Energy Physics)
JHEP
(Ed.)
A<sc>bstract</sc> A minimal non-thermal dark matter model that can explain both the existence of dark matter and the baryon asymmetry in the universe is studied. It requires two color-triplet, iso-singlet scalars with$$ \mathcal{O}\left(\textrm{TeV}\right) $$ masses and a singlet Majorana fermion with a mass of$$ \mathcal{O}\left(\textrm{GeV}\right) $$ . The fermion becomes stable and can play the role of the dark matter candidate. We consider the fermion to interact with a top quark via the exchange of QCD-charged scalar fields coupled dominantly to third generation fermions. The signature of a single top quark production associated with a bottom quark and large missing transverse momentum opens up the possibility to search for this type of model at the LHC in a way complementary to existing monotop searches.
Fosbinder-Elkins, H.; Kim, Y.; Dargert, J.; Harkness, M.; Geraci, A. A.; Levenson-Falk, E.; Mumford, S.; Fang, A.; Kapitulnik, A.; Matlashov, A.; et al
(, Quantum Science and Technology)
Abstract The QCD axion is a particle postulated to exist since the 1970s to explain the strong-CP problem in particle physics. It could also account for all of the observed dark matter in the Universe. The axion resonant interaction detection experiment (ARIADNE) intends to detect the QCD axion by sensing the fictitious ‘magnetic field’ created by its coupling to spin. Short-range axion-mediated interactions can occur between a sample of laser-polarized3He nuclear spins and an unpolarized source-mass sprocket. The experiment must be sensitive to magnetic fields below the 10−19T level to achieve its design sensitivity, necessitating tight control of the experiment’s magnetic environment. We describe a method for controlling three aspects of that environment which would otherwise limit the experimental sensitivity. Firstly, a system of superconducting magnetic shielding is described to screen ordinary magnetic noise from the sample volume at the 108level, which should be sufficient to reduce the contribution of Johnson noise in the sprocket-shaped source mass, expected to be at the 10−12T level, to below the threshold for signal detection. Secondly, a method for reducing magnetic field gradients within the sample up to 102times is described, using a simple and cost-effective design geometry. Thirdly, a novel coil design is introduced which allows the generation of fields similar to those produced by Helmholtz coils in regions directly abutting superconducting boundaries. This method allows the nuclear Larmor frequency of the sample to be tuned to match the axion field modulation frequency set by the sprocket rotation. Finally, we experimentally investigate the magnetic shielding factor of sputtered thin-film superconducting niobium on quartz substrates for various geometries and film thicknesses relevant for the ARIADNE axion experiment using SQUID magnetometry. The methods may be generally useful for magnetic field control near superconducting boundaries in other experiments where similar considerations apply.
Dror, Jeff A; Sandick, Pearl; Haghi, Barmak_Shams Es; Yang, Fengwei
(, Journal of High Energy Physics)
A<sc>bstract</sc> Cosmologically stable, light particles that came into thermal contact with the Standard Model in the early universe may persist today as a form of hot dark matter. For relics with masses in the eV range, their role in structure formation depends critically on their mass. We trace the evolution of such hot relics and derive their density profiles around cold dark matter halos, introducing a framework for theirindirect detection. Applying this framework to axions — a natural candidate for a particle that can reach thermal equilibrium with the Standard Model in the early universe and capable of decaying into two photons — we establish stringent limits on the axion-photon couplinggaγusing current observations of dwarf galaxies, the Milky Way halo, and galaxy clusters. Our results set new bounds on hot axions in the$$ \mathcal{O}\left(1-10\right) $$ eV range.
Acharya, S; Adamová, D; Adler, A; Aglieri_Rinella, G; Agnello, M; Agrawal, N; Ahammed, Z; Ahmad, S; Ahn, S U; Ahuja, I; et al
(, Journal of High Energy Physics)
A<sc>bstract</sc> Measurements of inclusive charged-particle jet production in pp and p-Pb collisions at center-of-mass energy per nucleon-nucleon collision$$ \sqrt{s_{\textrm{NN}}} $$ = 5.02 TeV and the corresponding nuclear modification factor$$ {R}_{\textrm{pPb}}^{\textrm{ch}\ \textrm{jet}} $$ are presented, using data collected with the ALICE detector at the LHC. Jets are reconstructed in the central rapidity region |ηjet|<0.5 from charged particles using the anti-kTalgorithm with resolution parametersR= 0.2, 0.3, and 0.4. ThepT-differential inclusive production cross section of charged-particle jets, as well as the corresponding cross section ratios, are reported for pp and p-Pb collisions in the transverse momentum range 10<$$ {p}_{\textrm{T},\textrm{jet}}^{\textrm{ch}} $$ <140 GeV/cand 10<$$ {p}_{\textrm{T},\textrm{jet}}^{\textrm{ch}} $$ <160 GeV/c, respectively, together with the nuclear modification factor$$ {R}_{\textrm{pPb}}^{\textrm{ch}\ \textrm{jet}} $$ in the range 10<$$ {p}_{\textrm{T},\textrm{jet}}^{\textrm{ch}} $$ <140 GeV/c. The analysis extends thepTrange of the previously-reported charged-particle jet measurements by the ALICE Collaboration. The nuclear modification factor is found to be consistent with one and independent of the jet resolution parameter with the improved precision of this study, indicating that the possible influence of cold nuclear matter effects on the production cross section of charged-particle jets in p-Pb collisions at$$ \sqrt{s_{\textrm{NN}}} $$ = 5.02 TeV is smaller than the current precision. The obtained results are in agreement with other minimum bias jet measurements available for RHIC and LHC energies, and are well reproduced by the NLO perturbative QCD Powhegcalculations with parton shower provided by Pythia8 as well as by Jetscapesimulations.
Gong, Ruotian; Du, Xinyi; Janzen, Eli; Liu, Vincent; Liu, Zhongyuan; He, Guanghui; Ye, Bingtian; Li, Tongcang; Yao, Norman Y; Edgar, James H; et al
(, Nature Communications)
Abstract Spin defects in van der Waals materials offer a promising platform for advancing quantum technologies. Here, we propose and demonstrate a powerful technique based on isotope engineering of host materials to significantly enhance the coherence properties of embedded spin defects. Focusing on the recently-discovered negatively charged boron vacancy center ($${{{{{{{{\rm{V}}}}}}}}}_{{{{{{{{\rm{B}}}}}}}}}^{-}$$ ) in hexagonal boron nitride (hBN), we grow isotopically purified h10B15N crystals. Compared to$${{{{{{{{\rm{V}}}}}}}}}_{{{{{{{{\rm{B}}}}}}}}}^{-}$$ in hBN with the natural distribution of isotopes, we observe substantially narrower and less crowded$${{{{{{{{\rm{V}}}}}}}}}_{{{{{{{{\rm{B}}}}}}}}}^{-}$$ spin transitions as well as extended coherence timeT2and relaxation timeT1. For quantum sensing,$${{{{{{{{\rm{V}}}}}}}}}_{{{{{{{{\rm{B}}}}}}}}}^{-}$$ centers in our h10B15N samples exhibit a factor of 4 (2) enhancement in DC (AC) magnetic field sensitivity. For additional quantum resources, the individual addressability of the$${{{{{{{{\rm{V}}}}}}}}}_{{{{{{{{\rm{B}}}}}}}}}^{-}$$ hyperfine levels enables the dynamical polarization and coherent control of the three nearest-neighbor15N nuclear spins. Our results demonstrate the power of isotope engineering for enhancing the properties of quantum spin defects in hBN, and can be readily extended to improving spin qubits in a broad family of van der Waals materials.
Chigusa, So, Kondo, Dan, Murayama, Hitoshi, Okabe, Risshin, and Sudo, Hiroyuki. Axion detection via superfluid 3He ferromagnetic phase and quantum measurement techniques. Retrieved from https://par.nsf.gov/biblio/10635152. Journal of High Energy Physics 2024.9 Web. doi:10.1007/JHEP09(2024)191.
Chigusa, So, Kondo, Dan, Murayama, Hitoshi, Okabe, Risshin, & Sudo, Hiroyuki. Axion detection via superfluid 3He ferromagnetic phase and quantum measurement techniques. Journal of High Energy Physics, 2024 (9). Retrieved from https://par.nsf.gov/biblio/10635152. https://doi.org/10.1007/JHEP09(2024)191
Chigusa, So, Kondo, Dan, Murayama, Hitoshi, Okabe, Risshin, and Sudo, Hiroyuki.
"Axion detection via superfluid 3He ferromagnetic phase and quantum measurement techniques". Journal of High Energy Physics 2024 (9). Country unknown/Code not available: Springer. https://doi.org/10.1007/JHEP09(2024)191.https://par.nsf.gov/biblio/10635152.
@article{osti_10635152,
place = {Country unknown/Code not available},
title = {Axion detection via superfluid 3He ferromagnetic phase and quantum measurement techniques},
url = {https://par.nsf.gov/biblio/10635152},
DOI = {10.1007/JHEP09(2024)191},
abstractNote = {A<sc>bstract</sc> We propose to use the nuclear spin excitation in the ferromagnetic A1phase of the superfluid3He for the axion dark matter detection. This approach is striking in that it is sensitive to the axion-nucleon coupling, one of the most important features of the QCD axion introduced to solve the strong CP problem. We review a quantum mechanical description of the nuclear spin excitation and apply it to the estimation of the axion-induced spin excitation rate. We also describe a possible detection method of the spin excitation in detail and show that the combination of the squeezing of the final state with the Josephson parametric amplifier and the homodyne measurement can enhance the sensitivity. It turns out that this approach gives good sensitivity to the axion dark matter with the mass of$$ \mathcal{O} $$O(1) μeV depending on the size of the external magnetic field. We estimate the parameters of experimental setups, e.g., the detector volume and the amplitude of squeezing, required to reach the QCD axion parameter space.},
journal = {Journal of High Energy Physics},
volume = {2024},
number = {9},
publisher = {Springer},
author = {Chigusa, So and Kondo, Dan and Murayama, Hitoshi and Okabe, Risshin and Sudo, Hiroyuki},
}
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