The identity of dark matter has been a mystery in astronomy, cosmology, and particle theory for about a century. We present the first dark matter search with a high-dispersion spectrograph by using WINERED at the 6.5 m Magellan Clay telescope to measure the photons from the dark matter decays. The dwarf spheroidal galaxies (dSphs) Leo V and Tucana II are observed by utilizing an object-sky-object nodding observation technique. Employing zero consistent flux data after the sky subtraction and performing Doppler shift analysis for further background subtraction, we have established one of the most stringent limits to date on dark matter lifetime in the mass range of 1.8-2.7 eV. The conservative bound is translated to the photon coupling, g_{ϕγγ} for axionlike par ticles around g_{ϕγγ}≲(2-3)×10^{-11} GeV^{-1} (10^{-10} GeV^{-1}) for the case that ultrafaint dSphs have the Navarro-Frenk-White (generalized Hernquist) dark matter profile.
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http://dx.doi.org/10.1103/PhysRevLett.134.051004 | DOI Listing |
Water Res
March 2025
Division of Applied Microbiology, Department of Chemistry, Lund University, SE-221 00 Lund, Sweden; Division of Water Resources Engineering, Department of Building and Environmental Technology, Lund University, SE-221 00 Lund, Sweden.
Slow sand filters (SSFs) for drinking water production are habitats for diverse microbes from multiple domains of life, which are integral to the ability of SSFs to purify water. While cultivation-independent analyses of the prokaryotic communities of SSFs have provided valuable insights, little attention has been paid to fungi inhabiting SSFs. This study characterized the fungal communities in the sand biofilm of one established, one inoculated and one non-inoculated SSF.
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February 2025
Institute of High Energy Physics, Key Laboratory of Particle Astrophysics & Experimental Physics Division & Computing Center, Chinese Academy of Sciences, 100049 Beijing, China.
The diffuse Galactic gamma-ray emission is a very important tool used to study the propagation and interaction of cosmic rays in the Milky Way. In this Letter, we report the measurements of the diffuse emission from the Galactic plane-covering Galactic longitudes from 15° to 235° and latitudes from -5° to +5°, in an energy range of 1 to 25 TeV-made with the Water Cherenkov Detector Array (WCDA) of the Large High Altitude Air Shower Observatory. After the sky regions of known sources are masked, the diffuse emission is detected with 24.
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February 2025
King's College London, Theoretical Particle Physics and Cosmology, Strand, London, WC2R 2LS, United Kingdom.
Laboratory experiments have the capacity to detect the QCD axion in the next decade, and precisely measure its mass, if it composes the majority of the dark matter. In type IIB string theory on Calabi-Yau threefolds in the geometric regime, the QCD axion mass, m_{a}, is strongly correlated with the topological Hodge number h^{1,1}. We compute m_{a} in a scan of 185965 compactifications of type IIB string theory on toric hypersurface Calabi-Yau threefolds.
View Article and Find Full Text PDFPhys Rev Lett
February 2025
Utrecht University, Institute for Theoretical Physics, Princetonplein 5, 3584 CC, Utrecht, Netherlands.
Our standard model of the Universe predicts the distribution of dark matter to 1% at the scales needed for upcoming experiments, yet our predictions for how the luminous matter-which has interactions besides gravity-is distributed remain highly uncertain. Understanding how much gas and stars there are in the Universe and where they preferentially live is challenging, and the uncertainty affects how well we can understand the cosmological model itself. For example, it compromises our ability to tell apart different models for dark energy, the mysterious force driving the accelerated expansion of the Universe.
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February 2025
Harvard-MIT Center for Ultracold Atoms, Cambridge, Massachusetts 02138, USA.
We report a magneto-optical trap of strontium monohydroxide (SrOH) containing 2000(600) molecules at a temperature of 1.2(3) mK. The lifetime is 91(9) ms, which is limited by decay to optically unaddressed vibrational states.
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