2000
DOI: 10.1103/physrevb.61.689
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Nonequilibrium microwave emission due to tunnel injection of quasiparticles into a high-TcBi2

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Cited by 23 publications
(15 citation statements)
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“…1,2 Much effort has been made to stimulate powerful radiations, first using artificial Josephson junction arrays [3][4][5][6][7][8][9][10][11] and later on Josephson junctions inherent in cuprate high-T c superconductors of layered structures. [12][13][14][15][16][17][18][19][20][21][22][23][24][25][26] The latter have obvious advantages since the junctions are homogeneous at the atomic scale guaranteed by the high quality of single crystals, and the superconductivity gap is large, typically of tens of meV, which in principle permits the frequency to cover the whole range of the terahertz ͑THz͒ band, a very useful regime of EM waves still lacking of compact solid-state generators. 27,28 An experimental breakthrough was achieved in 2007.…”
Section: Introductionmentioning
confidence: 99%
“…1,2 Much effort has been made to stimulate powerful radiations, first using artificial Josephson junction arrays [3][4][5][6][7][8][9][10][11] and later on Josephson junctions inherent in cuprate high-T c superconductors of layered structures. [12][13][14][15][16][17][18][19][20][21][22][23][24][25][26] The latter have obvious advantages since the junctions are homogeneous at the atomic scale guaranteed by the high quality of single crystals, and the superconductivity gap is large, typically of tens of meV, which in principle permits the frequency to cover the whole range of the terahertz ͑THz͒ band, a very useful regime of EM waves still lacking of compact solid-state generators. 27,28 An experimental breakthrough was achieved in 2007.…”
Section: Introductionmentioning
confidence: 99%
“…1 The Josephson current flowing along the c axis interacts with the electromagnetic field inside the insulating dielectric layers, producing Josephson plasma waves ͑JPWs͒. [1][2][3][4][5][6][7][8][9][10][11][12] In other words, the layered structure of superconductors favors the propagation of electromagnetic waves. A challenge is to excite 13 and to control 14,15 electromagnetic waves in Bi 2 Sr 2 CaCu 2 O 8+␦ ͑BSCCO͒ samples because of their subterahertz and terahertz frequency range, 11,16 which is still hardly reachable for both electronic and optical devices.…”
Section: Introductionmentioning
confidence: 99%
“…It should be noted that the nonlinearity of the coupled sine-Gordon equation is still retained in the equation for P s l , Eq. (24). With this approximation, we can calculate A 1…”
Section: Solutionsmentioning
confidence: 99%
“…[13,14,15,16,17,18,19] In spite of these works, it is still lack of clear evidence of coherent radiation. Radiation from BSCCO with injection of quasiparticles has been reported [20,21,22,23,24]. Alternatively, the terahertz radiation without a magnetic field has also been attempted [25,26,27,28,29].…”
Section: Introductionmentioning
confidence: 99%