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1.
Phys Rev Lett ; 123(3): 031302, 2019 Jul 19.
Artigo em Inglês | MEDLINE | ID: mdl-31386435

RESUMO

We present new constraints on the dark matter-induced annual modulation signal using 1.7 years of COSINE-100 data with a total exposure of 97.7 kg yr. The COSINE-100 experiment, consisting of 106 kg of NaI(Tl) target material, is designed to carry out a model-independent test of DAMA/LIBRA's claim of WIMP discovery by searching for the same annual modulation signal using the same NaI(Tl) target. The crystal data show a 2.7 cpd/kg/keV background rate on average in the 2-6 keV energy region of interest. Using a χ-squared minimization method we observe best fit values for modulation amplitude and phase of 0.0092±0.0067 cpd/kg/keV and 127.2±45.9 d, respectively.

2.
Phys Rev Lett ; 122(13): 131802, 2019 Apr 05.
Artigo em Inglês | MEDLINE | ID: mdl-31012610

RESUMO

A search for inelastic boosted dark matter (IBDM) using the COSINE-100 detector with 59.5 days of data is presented. This relativistic dark matter is theorized to interact with the target material through inelastic scattering with electrons, creating a heavier state that subsequently produces standard model particles, such as an electron-positron pair. In this study, we search for this electron-positron pair in coincidence with the initially scattered electron as a signature for an IBDM interaction. No excess over the predicted background event rate is observed. Therefore, we present limits on IBDM interactions under various hypotheses, one of which allows us to explore an area of the dark photon parameter space that has not yet been covered by other experiments. This is the first experimental search for IBDM using a terrestrial detector.

3.
Phys Rev Lett ; 122(13): 131301, 2019 Apr 05.
Artigo em Inglês | MEDLINE | ID: mdl-31012624

RESUMO

The scattering of dark matter (DM) particles with sub-GeV masses off nuclei is difficult to detect using liquid xenon-based DM search instruments because the energy transfer during nuclear recoils is smaller than the typical detector threshold. However, the tree-level DM-nucleus scattering diagram can be accompanied by simultaneous emission of a bremsstrahlung photon or a so-called "Migdal" electron. These provide an electron recoil component to the experimental signature at higher energies than the corresponding nuclear recoil. The presence of this signature allows liquid xenon detectors to use both the scintillation and the ionization signals in the analysis where the nuclear recoil signal would not be otherwise visible. We report constraints on spin-independent DM-nucleon scattering for DM particles with masses of 0.4-5 GeV/c^{2} using 1.4×10^{4} kg day of search exposure from the 2013 data from the Large Underground Xenon (LUX) experiment for four different classes of mediators. This analysis extends the reach of liquid xenon-based DM search instruments to lower DM masses than has been achieved previously.

4.
Eur Phys J C Part Fields ; 78(6): 490, 2018.
Artigo em Inglês | MEDLINE | ID: mdl-30956554

RESUMO

The COSINE-100 dark matter search experiment is an array of NaI(Tl) crystal detectors located in the Yangyang Underground Laboratory (Y2L). To understand measured backgrounds in the NaI(Tl) crystals we have performed Monte Carlo simulations using the Geant4 toolkit and developed background models for each crystal that consider contributions from both internal and external sources, including cosmogenic nuclides. The background models are based on comparisons of measurement data with Monte Carlo simulations that are guided by a campaign of material assays and are used to evaluate backgrounds and identify their sources. The average background level for the six crystals (70 kg total mass) that are studied is 3.5 counts/day/keV/kg in the (2-6) keV energy interval. The dominant contributors in this energy region are found to be 210 Pb and 3 H.

5.
Radiats Biol Radioecol ; 56(5): 494-502, 2016 Sep.
Artigo em Inglês, Russo | MEDLINE | ID: mdl-30703309

RESUMO

Inhibitors of the heat shock protein 90 (HSP90) activity are considered as potential radiosensitizers of tumors with a perspective of their application in radiotherapy. However, there are tumors and tumor cell lines whose radioresistance is not decreased after treatment with the HSP90 activity inhibitors; therefore, a predictive marker is needed, which would allow one to predict the response of target cells. As such a marker, herein it is proposed to use induction of the heat shock protein 70 (HSP70) that is an early cellular response to the HSP90 dysfunction and can easily be immunodetected. It follows from the data obtained that the radiosensitization of HSP90 inhibitor-treated cells occurs only when this treatment causes the prominent induction of HSP70 in them. Determination of this marker enables one: 1) to predict a possibility of radiosensitization of any cells by means of the HSP90 activity inhibitors, 2) to design the inhibitor concentration range upon which the radiosensitizing effect seems likely to occur, 3) to find whether this radiosensitization will be selective towards cancer cells.


Assuntos
Biomarcadores Tumorais/genética , Proteínas de Choque Térmico HSP70/genética , Proteínas de Choque Térmico HSP90/antagonistas & inibidores , Tolerância a Radiação/genética , Animais , Apoptose/efeitos dos fármacos , Proteínas de Choque Térmico HSP90/genética , Humanos , Células MCF-7 , Melanoma Experimental/genética , Melanoma Experimental/radioterapia , Camundongos , Tolerância a Radiação/efeitos da radiação , Radiossensibilizantes/farmacologia
6.
Phys Rev Lett ; 114(15): 151301, 2015 Apr 17.
Artigo em Inglês | MEDLINE | ID: mdl-25933303

RESUMO

We present an accurate model of the muon-induced background in the DAMA/LIBRA experiment. Our work challenges proposed mechanisms which seek to explain the observed DAMA signal modulation with muon-induced backgrounds. Muon generation and transport are performed using the MUSIC/MUSUN code, and subsequent interactions in the vicinity of the DAMA detector cavern are simulated with Geant4. We estimate the total muon-induced neutron flux in the detector cavern to be Φ(n)(ν)=1.0 × 10(-9) cm(-2) s(-1). We predict 3.49 × 10(-5) counts/day/kg/keV, which accounts for less than 0.3% of the DAMA signal modulation amplitude.

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