A Broadband/Resonant Approach to Axion Dark Matter Detection
暂无分享,去创建一个
[1] M. Tobar,et al. Axion Dark Matter Coupling to Resonant Photons via Magnetic Field. , 2015, Physical review letters.
[2] S. Lamoreaux,et al. Experimental Searches for the Axion and Axion-Like Particles , 2015, 1602.00039.
[3] C. Hill. Axion induced oscillating electric dipole moment of the electron , 2015, 1508.04083.
[4] J. Gamboa,et al. Parametric Resonance and Dark Matter Axion-Like Particles , 2015, 1506.02698.
[5] C. Hill. Axion induced oscillating electric dipole moments , 2015, 1504.01295.
[6] V. Flambaum,et al. Searching for dark matter and variation of fundamental constants with laser and maser interferometry. , 2014, Physical review letters.
[7] K. Irwin,et al. Radio for hidden-photon dark matter detection , 2014, 1411.7382.
[8] D. Budker,et al. Parity-violating interactions of cosmic fields with atoms, molecules, and nuclei: Concepts and calculations for laboratory searches and extracting limits , 2014, 1409.2564.
[9] S. Lamoreaux,et al. Future directions in the microwave cavity search for dark matter axions , 2014, 1405.3685.
[10] J. Read. The local dark matter density , 2014, 1404.1938.
[11] Jihn E. Kim,et al. Calculations of resonance enhancement factor in axion-search tube-experiments , 2014, 1403.1576.
[12] V. Flambaum,et al. Axion-induced effects in atoms, molecules, and nuclei: Parity nonconservation, anapole moments, electric dipole moments, and spin-gravity and spin-axion momentum couplings , 2013, 1312.6667.
[13] D. Tanner,et al. Proposal for axion dark matter detection using an LC circuit. , 2013, Physical review letters.
[14] Michael J. Pivovaroff,et al. Working Group Report: New Light Weakly Coupled Particles , 2013 .
[15] A. Lobanov,et al. WISPers from the Dark Side: Radio Probes of Axions and Hidden Photons , 2013, 1309.4170.
[16] Dmitry Budker,et al. Proposal for a Cosmic Axion Spin Precession Experiment (CASPEr) , 2013, 1306.6089.
[17] P. Graham,et al. New Observables for Direct Detection of Axion Dark Matter , 2013, 1306.6088.
[18] John Clarke,et al. Magnetic flux noise in dc SQUIDs: temperature and geometry dependence. , 2013, Physical review letters.
[19] M. J. Pivovaroff,et al. IAXO - The International Axion Observatory , 2013, 1302.3273.
[20] A. Lobanov,et al. Searching for WISPy Cold Dark Matter with a Dish Antenna , 2012, 1212.2970.
[21] O. Baker,et al. Prospects for searching axionlike particle dark matter with dipole, toroidal, and wiggler magnets , 2011, 1110.2180.
[22] P. Graham,et al. Axion dark matter detection with cold molecules , 2011, 1101.2691.
[23] D B Tanner,et al. SQUID-based microwave cavity search for dark-matter axions. , 2009, Physical review letters.
[24] S. K. Lee,et al. Calculation of magnetic field noise from high-permeability magnetic shields and conducting objects with simple geometry , 2007, 0709.2543.
[25] E. Witten,et al. Axions In String Theory , 2006, hep-th/0605206.
[26] John S George,et al. SQUID detected NMR in microtesla magnetic fields. , 2004, Journal of magnetic resonance (San Diego, Calif. 1997 : Print).
[27] Robert McDermott,et al. Microtesla MRI with a superconducting quantum interference device. , 2004, Proceedings of the National Academy of Sciences of the United States of America.
[28] L. Rosenberg,et al. Large-scale microwave cavity search for dark-matter axions , 2001 .
[29] J. Hutchison,et al. Gradiometer pick-up coil design for a low field SQUID-MRI system , 1999, Magnetic Resonance Materials in Physics, Biology and Medicine.
[30] R. Dolesi,et al. Thermal noise in a high Q cryogenic resonator , 1999 .
[31] Dietmar Drung,et al. Low‐noise high‐speed dc superconducting quantum interference device magnetometer with simplified feedback electronics , 1990 .
[32] P. Sikivie. Experimental Tests of the "INVISIBLE" Axion , 1983 .
[33] Laurence F Abbott,et al. A cosmological bound on the invisible axion , 1983 .
[34] Michael Dine,et al. The Not So Harmless Axion , 1983 .
[35] John Preskill,et al. Cosmology of the invisible axion , 1983 .
[36] Michael Dine,et al. A Simple Solution to the Strong CP Problem with a Harmless Axion , 1981 .
[37] A. Vainshtein,et al. Can Confinement Ensure Natural CP Invariance of Strong Interactions , 1980 .
[38] John Clarke,et al. Optimization of dc SQUID voltmeter and magnetometer circuits , 1979 .
[39] Jihn E. Kim. Weak Interaction Singlet and Strong CP Invariance , 1979 .
[40] F. Wilczek. Problem of Strong $P$ and $T$ Invariance in the Presence of Instantons , 1978 .
[41] S. Weinberg. A new light boson , 1978 .
[42] R. Peccei,et al. Constraints imposed by CP conservation in the presence of pseudoparticles , 1977 .
[43] R. Peccei,et al. CP Conservation in the Presence of Pseudoparticles , 1977 .
[44] H. Lübbig,et al. Current comparators with superconducting shields , 1974 .
[45] J. E. Zimmerman,et al. Sensitivity Enhancement of Superconducting Quantum Interference Devices through the Use of Fractional‐Turn Loops , 1971 .
[46] J. Hutchison,et al. Use of a DC SQUID receiver preamplifier in a low field MRI system , 1995, IEEE Transactions on Applied Superconductivity.
[47] A. R. Zhitnitskij. On possible suppression of the axion-hadron interactions , 1980 .
[48] A. Zhitnitsky. On Possible Suppression of the Axion Hadron Interactions. (In Russian) , 1980 .