scholarly journals Evidence for mirror dark matter from the CDMS low energy electron recoil spectrum

2009 ◽  
Vol 80 (9) ◽  
Author(s):  
R. Foot
Keyword(s):  
Dark Matter ◽  
Low Energy ◽  
Energy Electron ◽  
Electron Recoil ◽  
Low Energy Electron ◽  
Recoil Spectrum

scholarly journals Analysis of the low-energy electron-recoil spectrum of the CDMS experiment

2010 ◽  
Vol 81 (4) ◽  
Author(s):  
Z. Ahmed ◽  
D. S. Akerib ◽  
S. Arrenberg ◽  
C. N. Bailey ◽  
D. Balakishiyeva ◽  
...  
Keyword(s):  
Low Energy ◽  
Energy Electron ◽  
Electron Recoil ◽  
Low Energy Electron ◽  
Recoil Spectrum

scholarly journals Collider constraints on a dark matter interpretation of the XENON1T excess

2020 ◽  
Vol 80 (11) ◽  
Author(s):  
R. Primulando ◽  
J. Julio ◽  
P. Uttayarat
Keyword(s):  
Dark Matter ◽  
Fast Moving ◽  
New Physics ◽  
Low Energy ◽  
Energy Electron ◽  
Electron Interaction ◽  
Vector Particle ◽  
Electron Recoil ◽  
Low Energy Electron ◽  
Production Mechanisms

AbstractIn light of the excess in the low-energy electron recoil events reported by XENON1T, many new physics scenarios have been proposed as a possible origin of the excess. One possible explanation is that the excess is a result of a fast moving dark matter (DM), with velocity $$v\sim $$ v ∼ 0.05–0.20 and mass between 1 MeV and 10 GeV, scattering off an electron. Assuming the fast moving DM-electron interaction is mediated by a vector particle, we derive collider constraints on the said DM-electron interaction. The bounds on DM-electron coupling is then used to constrain possible production mechanisms of the fast moving DM. We find that the preferred mass of the vector mediator is relatively light ($$\lesssim $$ ≲ 1 GeV) and the coupling of the vector to the electron is much smaller than the coupling to the fast moving DM.

scholarly journals Low energy electron and nuclear recoil thresholds in the DRIFT-II negative ion TPC for dark matter searches

2009 ◽  
Vol 4 (04) ◽  
pp. P04014-P04014 ◽  
Author(s):  
S Burgos ◽  
E Daw ◽  
J Forbes ◽  
C Ghag ◽  
M Gold ◽  
...  
Keyword(s):  
Dark Matter ◽  
Low Energy ◽  
Energy Electron ◽  
Nuclear Recoil ◽  
Negative Ion ◽  
Low Energy Electron

scholarly journals GaAs as a Bright Cryogenic Scintillator for the Detection of Low-Energy Electron Recoils From MeV/c2 Dark Matter

2019 ◽  
Vol 66 (11) ◽  
pp. 2333-2337 ◽  
Author(s):  
S. Vasiukov ◽  
F. Chiossi ◽  
C. Braggio ◽  
G. Carugno ◽  
F. Moretti ◽  
...  
Keyword(s):  
Dark Matter ◽  
Low Energy ◽  
Energy Electron ◽  
Low Energy Electron

scholarly journals MIMAC low energy electron-recoil discrimination measured with fast neutrons

2016 ◽  
Vol 11 (08) ◽  
pp. P08011-P08011 ◽  
Author(s):  
Q. Riffard ◽  
D. Santos ◽  
O. Guillaudin ◽  
G. Bosson ◽  
O. Bourrion ◽  
...  
Keyword(s):  
Low Energy ◽  
Energy Electron ◽  
Fast Neutrons ◽  
Electron Recoil ◽  
Low Energy Electron ◽  
Recoil Discrimination

Performance Evaluation of a Novel Type of Low-Energy Electron Microscope

1990 ◽  
Vol 48 (1) ◽  
pp. 354-355
Author(s):  
Bertholdand Senftinger ◽  
Helmut Liebl
Keyword(s):  
Electron Microscope ◽  
High Resolution ◽  
Field Strength ◽  
Numerical Aperture ◽  
Low Energy ◽  
Energy Electron ◽  
High Resolution Imaging ◽  
Lens System ◽  
Resolution Imaging ◽  
Low Energy Electron

During the last few years the investigation of clean and adsorbate-covered solid surfaces as well as thin-film growth and molecular dynamics have given rise to a constant demand for high-resolution imaging microscopy with reflected and diffracted low energy electrons as well as photo-electrons. A recent successful implementation of a UHV low-energy electron microscope by Bauer and Telieps encouraged us to construct such a low energy electron microscope (LEEM) for high-resolution imaging incorporating several novel design features, which is described more detailed elsewhere.The constraint of high field strength at the surface required to keep the aberrations caused by the accelerating field small and high UV photon intensity to get an improved signal-to-noise ratio for photoemission led to the design of a tetrode emission lens system capable of also focusing the UV light at the surface through an integrated Schwarzschild-type objective. Fig. 1 shows an axial section of the emission lens in the LEEM with sample (28) and part of the sample holder (29). The integrated mirror objective (50a, 50b) is used for visual in situ microscopic observation of the sample as well as for UV illumination. The electron optical components and the sample with accelerating field followed by an einzel lens form a tetrode system. In order to keep the field strength high, the sample is separated from the first element of the einzel lens by only 1.6 mm. With a numerical aperture of 0.5 for the Schwarzschild objective the orifice in the first element of the einzel lens has to be about 3.0 mm in diameter. Considering the much smaller distance to the sample one can expect intense distortions of the accelerating field in front of the sample. Because the achievable lateral resolution depends mainly on the quality of the first imaging step, careful investigation of the aberrations caused by the emission lens system had to be done in order to avoid sacrificing high lateral resolution for larger numerical aperture.

Low-Energy-Electron-Diffraction Structural Studies of (100) Cleavage Surfaces of In4Se3 Layered Crystals

2014 ◽  
Vol 59 (6) ◽  
pp. 612-621 ◽  
Author(s):  
P.V. Galiy ◽  
◽  
Ya.B. Losovyj ◽  
T.M. Nenchuk ◽  
I.R. Yarovets’ ◽  
...  
Keyword(s):  
Electron Diffraction ◽  
Low Energy ◽  
Energy Electron ◽  
Structural Studies ◽  
Low Energy Electron Diffraction ◽  
Layered Crystals ◽  
Low Energy Electron
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