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Journal articles on the topic 'D-wave superconductor'

Author: Grafiati

Published: 6 September 2023

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1

LIAO, YAN-HUA, JIAN LI, and FENG WANG. "INTERFACE SCATTERING EFFECT ON JOSEPHSON CURRENT IN A d-WAVE SUPERCONDUCTOR/d-WAVE SUPERCONDUCTOR JUNCTION." Modern Physics Letters B 25, no. 02 (2011): 131–40. http://dx.doi.org/10.1142/s0217984911025547.

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By taking into account the interface scattering effect in a d-wave superconductor (S)/insulator layer (I)/d-wave superconductor (S) junction, the temperature dependence of the critical current and the current-phase relation are studied theoretically. It is found that both the barrier scattering and the roughness scattering at the interface always suppress the Andreev reflection and the current-phase relation is almost sinusoidal in the junction. The Josephson current strongly depends on the crystalline axis orientation of the d-wave superconductor in the junction. Some different phenomena appe

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2

Park, Mi-Ae, M. H. Lee, and Yong-Jihn Kim. "Impurity Scattering in a d-Wave Superconductor." Modern Physics Letters B 11, no. 16n17 (1997): 719–26. http://dx.doi.org/10.1142/s0217984997000888.

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The influence of (non-magnetic and magnetic) impurities on the transition temperature of a d-wave superconductor is studied anew within the framework of BCS theory. Pairing interaction decreases linearly with the impurity concentration. Accordingly T c suppression is proportional to the (potential or exchange) scattering rate, 1/τ, due to impurities. The initial slope versus 1/τ is found to depend on the superconductor contrary to Abrikosov–Gor'kov type theory. Near the critical impurity concentration T c drops abruptly to zero. Because the potential scattering rate is generally much larger th

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3

Morita, Y., M. Kohmoto, and K. Maki. "Aspects of a Single Vortex in d-Wave Superconductors." International Journal of Modern Physics B 12, no. 10 (1998): 989–1005. http://dx.doi.org/10.1142/s0217979298000557.

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Physical properties of a single vortex in d-wave superconductors are studied theoretically. After a brief review on a single vortex in "conventional" s-wave superconductors and the d-wave superconductivity underlying the hole-doped high-T c cuprates, we go on to study the quasiparticle spectrum around a single vortex in the high-T c superconductors. One of the characteristics of the high-T c superconductors is that they are close to the "quantum limit" (pFξ ~ O(1)). A new picture emerges of the quasiparticle spectrum. Instead of thousands of bound states in a "conventional" s-wave superconduct

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4

Cucolo, A. M., M. Cuoco, and C. Noce. "d-Wave Tunnel Junctions." International Journal of Modern Physics B 13, no. 09n10 (1999): 1295–99. http://dx.doi.org/10.1142/s0217979299001338.

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We study the tunneling spectra for superconductor-insulator-normal metal (S-I-N) tunnel junctions with an s -wave or a d -wave superconductor within the weak-coupling model. We deduce the temperature behavior of tunneling conductance and their peak positions as well as of the zero-bias conductance. The results obtained allow us to discriminate among the two singlet spin states.

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5

Belyavsky, V. I., V. V. Kapaev, and Yu V. Kopaev. "Topological d-wave superconductor." JETP Letters 96, no. 11 (2013): 724–29. http://dx.doi.org/10.1134/s002136401223004x.

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6

Popović, Zorica, Ljiljana Dobrosavljević-Grujić, and Radomir Zikic. "Quasiparticle Transport Properties of d-Wave Superconductor/Ferromagnet/d-Wave Superconductor Junctions." Journal of the Physical Society of Japan 82, no. 11 (2013): 114714. http://dx.doi.org/10.7566/jpsj.82.114714.

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7

Liao, Y. H., Z. C. Dong, Z. F. Yin, and H. Fu. "Josephson current in ferromagnetic d-wave superconductor/ferromagnetic d-wave superconductor junction." Physics Letters A 372, no. 8 (2008): 1327–32. http://dx.doi.org/10.1016/j.physleta.2007.09.031.

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8

Popović, Zorica, Predrag Miranović, and Radomir Zikic. "Zero Bias Conductance in d-Wave Superconductor/Ferromagnet/d-Wave Superconductor Trilayers." physica status solidi (b) 255, no. 6 (2018): 1700554. http://dx.doi.org/10.1002/pssb.201700554.

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9

HAN, QIANG. "VORTEX STATE IN f-WAVE SUPERCONDUCTORS." Modern Physics Letters B 21, no. 17 (2007): 1051–56. http://dx.doi.org/10.1142/s0217984907013377.

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Motivated by the controversy concerning the pairing symmetry of the superconducting sodium-doped cobalt oxide, we investigate the microscopic electronic structure of an f-wave superconductor in the vortex state by diagonalizing an effective Hamiltonian specified in the triangular lattice self-consistently. We find that the low-lying vortex core states are in essence extended for the nodal f-wave superconductors. In comparison, we find localized bound states in the vortex core of the fully-gapped (d + id')-wave superconductors.

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10

Jin Xia, Dong Zheng-Chao, Liang Zhi-Peng, and Zhong Chong-Gui. "Josephson effect in ferromagnetic d-wave superconductor/ferromagnet/ferromagnetic d-wave superconductor junctions." Acta Physica Sinica 62, no. 4 (2013): 047401. http://dx.doi.org/10.7498/aps.62.047401.

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11

Yan-Hua, Liao, Dong Zheng-Chao, Yin Zai-Feng, and Fu Hao. "Zeeman effects on Josephson current in d-wave superconductor/d-wave superconductor junctions." Chinese Physics B 17, no. 5 (2008): 1893–901. http://dx.doi.org/10.1088/1674-1056/17/5/058.

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12

Lin, Kai, Xiao-Mei Kuang, Wei-Liang Qian, Qiyuan Pan, and A. B. Pavan. "Analysis of s-wave, p-wave and d-wave holographic superconductors in Hořava–Lifshitz gravity." Modern Physics Letters A 33, no. 26 (2018): 1850147. http://dx.doi.org/10.1142/s021773231850147x.

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In this work, the s-wave, p-wave and d-wave holographic superconductors in the Hořava–Lifshitz gravity are investigated in the probe limit. For this approach, it is shown that the equations of motion for different wave states in Einstein gravity can be written as a unified form, and condensates take place in all three cases. This scheme is then generalized to Hořava–Lifshitz gravity, and a unified equation for multiple holographic states is obtained. Furthermore, the properties of the condensation and the optical conductivity are studied numerically. It is found that, in the case of Hořava–Lif

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13

LEE, C. Y. "dx2-y2-STATE OF HIGH TEMPERATURE SUPERCONDUCTORS WITH A SMALL ADMIXTURE OF dxy-STATE." Modern Physics Letters B 18, no. 12n13 (2004): 613–25. http://dx.doi.org/10.1142/s021798490400713x.

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It is well known that most of the high temperature superconductors (at least hole-type) are in d-wave state. But it is still an unsolved problem whether it is a pure d-wave state or one has some kind of mixed state. Among the candidates for an admixture, there are s- and d-wave states. Existing experiments could not resolve this issue. New possibilities for experimental resolution of this problem are opened via recent observation of the collective modes in UBe 13 (heavy fermion superconductor) by microwave impedance technique experiments and in Sr 2 RuO 4 (high temperature superconductor) by u

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14

Balents, Leon, Matthew P. A. Fisher, and Chetan Nayak. "Nodal Liquid Theory of the Pseudo-Gap Phase of High-Tc Superconductors." International Journal of Modern Physics B 12, no. 10 (1998): 1033–68. http://dx.doi.org/10.1142/s0217979298000570.

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We introduce and study the nodal liquid, a novel zero-temperature quantum phase obtained by quantum-disordering a d-wave superconductor. It has numerous remarkable properties which lead us to suggest it as an explanation of the pseudo-gap state in underdoped high-temperature superconductors. In the absence of impurities, these include power-law magnetic order, a T-linear spin susceptibility, nontrivial thermal conductivity, and two- and one-particle charge gaps, the latter evidenced, e.g. in transport and electron photoemission (which exhibits pronounced fourfold anisotropy inherited from the

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15

Popović, Zorica, Radomir Zikic, and Ljiljana Dobrosavljević-Grujić. "Orientation dependence of the Andreev transport in d-wave superconductor–ferromagnet–d-wave superconductor trilayers." Progress of Theoretical and Experimental Physics 2015, no. 10 (2015): 103I01. http://dx.doi.org/10.1093/ptep/ptv133.

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16

Tanaka, Y., and S. Kashiwaya. "Theory of d.c. Josephson current in d-wave superconductor/normal metal/ d-wave superconductor junctions." Physica C: Superconductivity 282-287 (August 1997): 1855–56. http://dx.doi.org/10.1016/s0921-4534(97)01087-3.

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17

Blackstead, Howard A., and John D. Dow. "OCCURRENCE OF SPIN-FLUCTUATION PAIRING IN HIGH-TEMPERATURE SUPERCONDUCTORS." International Journal of Modern Physics B 13, no. 29n31 (1999): 3635–41. http://dx.doi.org/10.1142/s0217979299003581.

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The definitive property of a spin-fluctuation d-wave-pairing superconductor is that cuprate-plane Cu-site Ni is a weaker Cooper-pair-breaker than Zn on the same site. None of the major high-temperature superconductors, except possibly YBa 2 Cu 3 O x, exhibits this property experimentally.

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18

Ohkubo, M., G. Uehara, J. Beyer, et al. "Standard measurement method for normal state resistance and critical current of resistively shunted Josephson junctions." Superconductor Science and Technology 35, no. 4 (2022): 045002. http://dx.doi.org/10.1088/1361-6668/ac4f3b.

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Abstract An important parameter of Josephson junctions (JJs) is the product of normal state resistance (R n) and critical current (I c) for designing superconductor analogue devices or digital circuits. Determination of R n and I c from voltage–current (U–I) characteristic curves often faces difficulties; in particular I c is considerably reduced by intrinsic thermal or extrinsic electrical noises. Here, we propose a standard measurement method of R n and intrinsic critical current (I ci) for high-T c superconductor (HTS) grain boundary JJs operated in liquid nitrogen and low-T c superconducto

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19

Won, Hyekyung, and Kazumi Maki. "The antiparamagnon in D-wave superconductor." Physica C: Superconductivity 235-240 (December 1994): 1689–90. http://dx.doi.org/10.1016/0921-4534(94)92066-4.

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20

Kim, Wonkee, and C. S. Ting. "Ginzburg–Landau Equations for a d-Wave Superconductor with Paramagnetic Impurities." International Journal of Modern Physics B 12, no. 10 (1998): 1069–95. http://dx.doi.org/10.1142/s0217979298000582.

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Ginzburg–Landau (GL) equations for a d-wave superconductor with a repulsive s-wave interaction between electrons in the presence of paramagnetic impurities are microscopically derived based on the Born approximation. The diagrammatic relationships for the impurity-averaged product of Green's functions are algebraically established. The effect of paramagnetic impurities on the transition temperature and the London penetration depth are discussed. GL equations for a superconductor with both s-wave and d-wave pairing interactions are also examined. We show that the transition temperature for a su

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21

Guo, Hong, Fu-Wen Shu, Jing-He Chen, Hui Li, and Ze Yu. "A holographic model of d-wave superconductor vortices with Lifshitz scaling." International Journal of Modern Physics D 25, no. 02 (2016): 1650021. http://dx.doi.org/10.1142/s0218271816500218.

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We study analytically the [Formula: see text]-wave holographic superconductors with Lifshitz scaling in the presence of external magnetic field. The vortex lattice solutions of the model have also been obtained with different Lifshitz scaling. Our results imply that holographic [Formula: see text]-wave superconductor is indeed a type II one even for different Lifshitz scaling. This is the same as the conventional [Formula: see text]-wave superconductors in the Ginzburg–Landau (GL) theory. Our results also indicates that the dynamical exponent [Formula: see text] cannot affect the droplet solut

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22

Xiao-Wei, Li, and Dong Zheng-Chao. "Josephson Current in Superconductor-Ferromagnet/Insulator/d-Wave Superconductor Junctions." Communications in Theoretical Physics 43, no. 3 (2005): 551–55. http://dx.doi.org/10.1088/0253-6102/43/3/035.

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23

Won, Hyekyung, and Kazumi Maki. "D-wave superconductor as a model of high Tc superconductor." Physica B: Condensed Matter 194-196 (February 1994): 1459–60. http://dx.doi.org/10.1016/0921-4526(94)91229-7.

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24

Dong, Zhengchao. "Zeeman effects on d-wave superconductor and tunneling spectrum in normal-metal/d-wave superconductor tunnel junction." Science in China Series G: Physics, Mechanics and Astronomy 49, no. 5 (2006): 597–605. http://dx.doi.org/10.1007/s11433-006-0597-y.

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25

Pang, Guiming, Michael Smidman, Jinglei Zhang, et al. "Fully gapped d-wave superconductivity in CeCu2Si2." Proceedings of the National Academy of Sciences 115, no. 21 (2018): 5343–47. http://dx.doi.org/10.1073/pnas.1720291115.

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The nature of the pairing symmetry of the first heavy fermion superconductor CeCu2Si2 has recently become the subject of controversy. While CeCu2Si2 was generally believed to be a d-wave superconductor, recent low-temperature specific heat measurements showed evidence for fully gapped superconductivity, contrary to the nodal behavior inferred from earlier results. Here, we report London penetration depth measurements, which also reveal fully gapped behavior at very low temperatures. To explain these seemingly conflicting results, we propose a fully gapped d+d band-mixing pairing state for CeCu

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26

Leroux, Maxime, Vivek Mishra, Jacob P. C. Ruff, et al. "Disorder raises the critical temperature of a cuprate superconductor." Proceedings of the National Academy of Sciences 116, no. 22 (2019): 10691–97. http://dx.doi.org/10.1073/pnas.1817134116.

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With the discovery of charge-density waves (CDWs) in most members of the cuprate high-temperature superconductors, the interplay between superconductivity and CDWs has become a key point in the debate on the origin of high-temperature superconductivity. Some experiments in cuprates point toward a CDW state competing with superconductivity, but others raise the possibility of a CDW-superconductivity intertwined order or more elusive pair-density waves (PDWs). Here, we have used proton irradiation to induce disorder in crystals of La1.875Ba0.125CuO4 and observed a striking 50% increase of Tc, ac

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27

Caixeiro, E. S., E. V. L. de Mello, and A. Troper. "Calculations for an inhomogeneous d-wave superconductor." Physica C: Superconductivity 459, no. 1-2 (2007): 37–42. http://dx.doi.org/10.1016/j.physc.2007.04.219.

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28

Maki, Kazumi, Nils Schopohl, and Hyekyung Won. "D-wave superconductor in high magnetic fields." Physica B: Condensed Matter 204, no. 1-4 (1995): 214–21. http://dx.doi.org/10.1016/0921-4526(94)00266-x.

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29

Han, Jung Hoon. "Tunneling Spectra of Inhomogeneous d-Wave Superconductor." International Journal of Modern Physics B 17, no. 18n20 (2003): 3484–92. http://dx.doi.org/10.1142/s0217979203021253.

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The tunneling spectrum of an inhomogeneous d-wave superconductor is discussed in the framework of self-consistent slave-boson mean-field theory. Distinct from the usual BCS-type mean-field theory, an electron is now described using both fermionic and bosonic degree of freedom. We show that one can define two types of tunneling spectra in this theory, which also corresponds to two ways of calibrating the STM spectra. In good agreement with the experimental observation, we show that one type of tunneling spectrum remains inhomogeneous while the other type shows a remarkable degree of homogeneity

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30

Millo, Oded, and Gad Koren. "What can Andreev bound states tell us about superconductors?" Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 376, no. 2125 (2018): 20140143. http://dx.doi.org/10.1098/rsta.2014.0143.

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Zero-energy Andreev bound states, which manifest themselves in the tunnelling spectra as zero-bias conductance peaks (ZBCPs), are abundant at interfaces between superconductors and other materials and on the nodal surface of high-temperature superconductors. In this review, we focus on the information such excitations can provide on the properties of superconductor systems. First, a general introduction to the physics of Andreev bound states in superconductor/normal metal interfaces is given with a particular emphasis on why they appear at zero energy in d -wave superconductors. Then, specific

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31

Verma, Sanjeev K., Anushri Gupta, Anita Kumari та B. D. Indu. "Superconducting gap anisotropy and d-wave pairing in YBa2Cu3O7−δ". International Journal of Modern Physics B 32, № 04 (2018): 1850035. http://dx.doi.org/10.1142/s0217979218500352.

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Considering Born–Mayer–Huggins potential as a most suitable potential to study the dynamical properties of high-temperature superconductors (HTS), the many-body quantum dynamics to obtain phonon Green’s functions has been developed via a Hamiltonian that incorporates the contributions of harmonic electron and phonon fields, phonon field anharmonicities, defects and electron–phonon interactions without considering BCS structure. This enables one to develop the quasiparticle renormalized frequency dispersion in the representative high-temperature cuprate superconductor YBa2Cu3O[Formula: see text

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32

SAMOKHIN, K. V., and B. MITROVIĆ. "CLASSICAL PHASE FLUCTUATIONS IN d-WAVE SUPERCONDUCTORS." Modern Physics Letters B 19, no. 21 (2005): 991–1009. http://dx.doi.org/10.1142/s0217984905009067.

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We study the effects of low-energy nodal quasiparticles on the classical phase fluctuations in a two-dimensional d-wave superconductor. The singularities of the phase-only action at T→0 are removed in the presence of disorder, which justifies using an extended classical XY-model to describe phase fluctuations at low temperatures.

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33

Ummarino, G. A., R. S. Gonnelli, C. Bravi, and Masumi Inoue. "Pair Symmetry and Degree of Gap Depression at S-I Interfaces in HTS Josephson Junctions." International Journal of Modern Physics B 13, no. 09n10 (1999): 1301–6. http://dx.doi.org/10.1142/s021797929900134x.

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A new possible indirect way of testing pair symmetry in high-Tc superconductors has been set up. The degree of intrinsic gap depression at Superconductor-Insulator [S-I] interfaces required to match Ic(T)Rn(T) data in HTS Josephson junctions depends on the pair symmetry of the material itself, so that an higher fraction of d-wave symmetry for the order parameter requires less gap depression, while an higher fraction of s-wave corresponds to a larger degree of gap depression. In order to obtain a general reference value for the intrinsic amount of gap depression at S-I interfaces the de Gennes

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34

Sun, Ye, and Kazumi Maki. "Comparison between d-wave superconductor with nonmagnetic impurities and s-wave superconductor with magnetic impurities." Physica B: Condensed Matter 230-232 (February 1997): 942–44. http://dx.doi.org/10.1016/s0921-4526(96)00699-0.

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35

Zhu, Jian-Xin, Z. D. Wang, and H. X. Tang. "Bound states and Josephson current in mesoscopics-wave superconductor–normal-metal–d-wave superconductor junctions." Physical Review B 54, no. 10 (1996): 7354–59. http://dx.doi.org/10.1103/physrevb.54.7354.

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36

Lv, Bo, and Wei Guo. "The spin pairing symmetry of d-wave superconductor indicated by tunneling spectroscopy." International Journal of Modern Physics B 31, no. 25 (2017): 1745017. http://dx.doi.org/10.1142/s0217979217450175.

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Andreev reflection on the interface of ferromagnet/superconductor ([Formula: see text]) junction provides a tool for exhibiting the spin pairing symmetry in superconductors. The triplet tunneling in [Formula: see text]-wave [Formula: see text] junction observed in recent experiments revived a fundamental interest: the pairing mechanism of the superconducting cuprate. Here we show that in a doped cuprate, the effective spin coupling between the doped holes on the O sites yields a symmetric bound pair state [Formula: see text] with quantum numbers [Formula: see text], [Formula: see text] in the

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37

Donini, Andrea, Víctor Enguita-Vileta, Fabian Esser, and Veronica Sanz. "Generalising Holographic Superconductors." Advances in High Energy Physics 2022 (June 17, 2022): 1–19. http://dx.doi.org/10.1155/2022/1785050.

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In this paper we propose a generalised holographic framework to describe superconductors. We first unify the description of s-, p-, and d-wave superconductors in a way that can be easily promoted to higher spin. Using a semianalytical procedure to compute the superconductor properties, we are able to further generalise the geometric description of the hologram beyond the AdS-Schwarzschild Black Hole paradigm and propose a set of higher-dimensional metrics which exhibit the same universal behaviour. We then apply this generalised description to study the properties of the condensate and the sca

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38

Sugiyama, T., and T. Ohmi. "Paramagnetically Limited Critical Field of d-Wave Superconductor." Progress of Theoretical Physics 89, no. 4 (1993): 787–91. http://dx.doi.org/10.1143/ptp/89.4.787.

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39

Chesca, B. "SQUID-Based Investigation of D-Wave Superconductor Junctions." Sensor Letters 7, no. 3 (2009): 263–65. http://dx.doi.org/10.1166/sl.2009.1039.

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40

Afsaneh, E., and H. Yavari. "Critical current of a granular d-wave superconductor." Solid State Communications 152, no. 21 (2012): 1933–38. http://dx.doi.org/10.1016/j.ssc.2012.07.007.

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41

Hajati, Y., S. Vosoughi nia, and G. Rashedi. "Tunneling transport in d-wave superconductor-silicene junction." Superlattices and Microstructures 102 (February 2017): 202–11. http://dx.doi.org/10.1016/j.spmi.2016.11.067.

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42

Won, Hyekyung, and Kazumi Maki. "Antiparamagnon and NMR in a d-wave superconductor." Physica B: Condensed Matter 206-207 (February 1995): 664–66. http://dx.doi.org/10.1016/0921-4526(94)00550-f.

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43

Arberg, P., M. Mansor, and J. P. Carbotte. "Penetration depth for a 2D D-wave superconductor." Solid State Communications 86, no. 10 (1993): 671–73. http://dx.doi.org/10.1016/0038-1098(93)90837-d.

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44

Jiang, C., and J. P. Carbotte. "Raman profile in superconductor with d-wave symmetry." Solid State Communications 95, no. 9 (1995): 643–45. http://dx.doi.org/10.1016/0038-1098(95)00047-x.

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45

Balatsky, A. V., Ar Abanov, and Jian-Xin Zhu. "Inelastic tunneling spectroscopy in a d-wave superconductor." Physica C: Superconductivity 408-410 (August 2004): 246–47. http://dx.doi.org/10.1016/j.physc.2004.02.134.

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46

Vali, R., and Mehran Vali. "Conductance properties of topological insulator based ferromagnetic insulator/d-wave superconductor and normal metal/ferromagnetic insulator/d-wave superconductor junctions." Journal of Applied Physics 112, no. 8 (2012): 083911. http://dx.doi.org/10.1063/1.4759250.

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47

Zagoskin, Alexandre M. "The half-periodic Josephson effect in an s-wave superconductor - normal-metal - d-wave superconductor junction." Journal of Physics: Condensed Matter 9, no. 31 (1997): L419—L426. http://dx.doi.org/10.1088/0953-8984/9/31/001.

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48

Dong, Z. C. "Zeeman effects on d-wave superconductor and the coherent tunneling spectrum in normal-metal/d-wave superconductor/normal-metal tunnel junctions." Solid State Communications 142, no. 10 (2007): 577–82. http://dx.doi.org/10.1016/j.ssc.2007.04.002.

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49

Zheng, Guo-Qing. "Extended Quasiparticle States Outside the Vortex Cores in a d-Wave Superconductor." International Journal of Modern Physics B 17, no. 18n20 (2003): 3509–12. http://dx.doi.org/10.1142/s0217979203021307.

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We a describe a measurement of the spin Knight shift (Ks) around the middle point between two vortices as a function of magnetic field (H) up to 28 T in a high-Tc superconductor TlSr 2 CaCu 2 O 6.8. At low temperatures, Ks increases substantially with increasing field, which indicates that the quasiparticle states with an ungapped spectrum are extended outside the vortex cores in a d-wave superconductor. The density of such states is found to be [Formula: see text], with N0 being the normal-state density of states and Hc2 being the upper critical field.

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50

Ong, Tzen, Piers Coleman, and Jörg Schmalian. "Concealed d-wave pairs in the s± condensate of iron-based superconductors." Proceedings of the National Academy of Sciences 113, no. 20 (2016): 5486–91. http://dx.doi.org/10.1073/pnas.1523064113.

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A central question in iron-based superconductivity is the mechanism by which the paired electrons minimize their strong mutual Coulomb repulsion. In most unconventional superconductors, Coulomb repulsion is minimized through the formation of higher angular momentum Cooper pairs, with Fermi surface nodes in the pair wavefunction. The apparent absence of such nodes in the iron-based superconductors has led to a belief they form an s-wave (s±) singlet state, which changes sign between the electron and hole pockets. However, the multiorbital nature of these systems opens an alternative possibility

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