Constraints on low-mass, relic dark matter candidates from a surface-operated SuperCDMS single-charge sensitive detector
Constraints on low-mass, relic dark matter candidates from a surface-operated SuperCDMS single-charge sensitive detector
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DOI:
10.1103/physrevd.102.091101
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发表时间:
2020-05
影响因子:
5
通讯作者:
D. Amaral;T. Aralis;T. Aramaki;I. Arnquist;E. Azadbakht;S. Banik;D. Barker;C. Bathurst;D. Bauer;L. V. S. Bezerra-L. V. S.-Bezerra-1432230453;R. Bhattacharyya;T. Binder;M. Bowles;P. Brink;R. Bunker;B. Cabrera;R. Calkins;R. Cameron;C. Cartaro;D. Cerdeño;Y.-Y. Chang-Y.;R. Chen;N. Chott;J. Cooley;H. Coombes;J. Corbett;P. Cushman;F. De Brienne;M. L. di Vacri;M. Diamond;E. Fascione;E. Figueroa-Feliciano;C. Fink;K. Fouts;M. Fritts;G. Gerbier;R. Germond;M. Ghaith;S. Golwala;H. R. Harris;N. Herbert;B. Hines;M. Hollister;Z. Hong;E. Hoppe;L. Hsu;M. Huber;V. Iyer;D. Jardin;A. Jastram;M. Kelsey;A. Kubik;N. Kurinsky;R. Lawrence;A. Li;B. Loer;E. Lopez Asamar;P. Lukens;D. MacDonell;D. Macfarlane;R. Mahapatra;V. Mandic;N. Mast;A. Mayer;É. Michaud;E. Michielin;N. Mirabolfathi;B. Mohanty;J. Morales Mendoza;S. Nagorny;J. Nelson;H. Neog;V. Novati;J. Orrell;S. Oser;W. Page;P. Pakarha;R. Partridge;R. Podviianiuk;F. Ponce;S. Poudel;M. Pyle;W. Rau;E. Reid;R. Ren;T. Reynolds;A. Roberts;A. Robinson;H. Rogers;T. Saab;B. Sadoulet;J. Sander;A. Sattari;R. Schnee;S. Scorza;B. Serfass;D. Sincavage;C. Stanford;M. Stein;J. Street;D. Toback;R. Underwood;S. Verma;A. Villano;B. von Krosigk;S. Watkins;L. Wills;J. S. Wilson-J. S.-Wilson-2109103973;M. Wilson;J. Winchell;D. Wright;S. Yellin;B. Young;T. Yu;E. Zhang;H. G. Zhang-H. G.-Zhang-2125674700;X. Zhao;L. Zheng
中科院分区:
文献类型:
--
作者:
D. Amaral;T. Aralis;T. Aramaki;I. Arnquist;E. Azadbakht;S. Banik;D. Barker;C. Bathurst;D. Bauer;L. V. S. Bezerra-L. V. S.-Bezerra-1432230453;R. Bhattacharyya;T. Binder;M. Bowles;P. Brink;R. Bunker;B. Cabrera;R. Calkins;R. Cameron;C. Cartaro;D. Cerdeño;Y.-Y. Chang-Y.;R. Chen;N. Chott;J. Cooley;H. Coombes;J. Corbett;P. Cushman;F. De Brienne;M. L. di Vacri;M. Diamond;E. Fascione;E. Figueroa-Feliciano;C. Fink;K. Fouts;M. Fritts;G. Gerbier;R. Germond;M. Ghaith;S. Golwala;H. R. Harris;N. Herbert;B. Hines;M. Hollister;Z. Hong;E. Hoppe;L. Hsu;M. Huber;V. Iyer;D. Jardin;A. Jastram;M. Kelsey;A. Kubik;N. Kurinsky;R. Lawrence;A. Li;B. Loer;E. Lopez Asamar;P. Lukens;D. MacDonell;D. Macfarlane;R. Mahapatra;V. Mandic;N. Mast;A. Mayer;É. Michaud;E. Michielin;N. Mirabolfathi;B. Mohanty;J. Morales Mendoza;S. Nagorny;J. Nelson;H. Neog;V. Novati;J. Orrell;S. Oser;W. Page;P. Pakarha;R. Partridge;R. Podviianiuk;F. Ponce;S. Poudel;M. Pyle;W. Rau;E. Reid;R. Ren;T. Reynolds;A. Roberts;A. Robinson;H. Rogers;T. Saab;B. Sadoulet;J. Sander;A. Sattari;R. Schnee;S. Scorza;B. Serfass;D. Sincavage;C. Stanford;M. Stein;J. Street;D. Toback;R. Underwood;S. Verma;A. Villano;B. von Krosigk;S. Watkins;L. Wills;J. S. Wilson-J. S.-Wilson-2109103973;M. Wilson;J. Winchell;D. Wright;S. Yellin;B. Young;T. Yu;E. Zhang;H. G. Zhang-H. G.-Zhang-2125674700;X. Zhao;L. Zheng
This article presents an analysis and the resulting limits on light dark matter inelastically scattering off of electrons, and on dark photon and axion-like particle absorption, using a second-generation SuperCDMS high-voltage eV-resolution detector. The 0.93 gram Si detector achieved a 3 eV phonon energy resolution; for a detector bias of 100 V, this corresponds to a charge resolution of 3% of a single electron-hole pair. The energy spectrum is reported from a blind analysis with 1.2 gram-days of exposure acquired in an above-ground laboratory. With charge carrier trapping and impact ionization effects incorporated into the dark matter signal models, the dark matter-electron cross section $\bar{\sigma}_{e}$ is constrained for dark matter masses from 0.5--$10^{4} $MeV$/c^{2}$; in the mass range from 1.2--50 eV$/c^{2}$ the dark photon kinetic mixing parameter $\varepsilon$ and the axioelectric coupling constant $g_{ae}$ are constrained. The minimum 90% confidence-level upper limits within the above mentioned mass ranges are $\bar{\sigma}_{e}\,=\,8.7\times10^{-34}$ cm$^{2}$, $\varepsilon\,=\,3.3\times10^{-14}$, and $g_{ae}\,=\,1.0\times10^{-9}$.