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The upper critical field, $H_{c2}$, of Mg(B$_{1-x}$C$_x$)$_2$ has been measured in order to probe the maximum magnetic field range for superconductivity that can be attained by C doping. Carbon doped boron filaments are prepared by CVD…

The upper critical field ($H_{c2}$) in superconducting BaFe$_{2-x}$Ni$_{x}$As$_2$ single crystals has been determined by magnetotransport measurements down to 0.6 K over the whole superconducting dome with $0.065 \leqslant x \leqslant…

We report time-resolved measurements of the photoinduced change in reflectivity, Delta R, in the Bi2Sr2Ca(1-y)Dy(y)Cu2O(8+delta) (BSCCO) system of cuprate superconductors as a function of hole concentration. We find that the kinetics of…

Superconductivity · Physics 2007-05-23 N. Gedik , J. Orenstein , S. Ono , Yasushi Abe , Yoichi Ando

Scanning tunneling spectroscopy (STS) studies reveal long-range spatial homogeneity and predominantly $d_{x^2-y^2}$-pairing spectral characteristics in under- and optimally doped $\rm YBa_2Cu_3O_{7-\delta}$ superconductors, whereas STS on…

We present the investigation results of the in-plane \{rho}(T) resistivity tensor at the temperature range 0.4-40 K in magnetic fields up to 90kOe (H||c, J||ab) for electron-doped Nd{2-x}Ce{x}CuO{4+{\delta}} with different degree of…

To establish the doping-dependent phase diagram in alkali-metal doped C$_{60}$, we synthesize Rb-doped C$_{60}$ samples with different stoichiometries by using the improved wet-chemistry technique. The doping levels determined from the…

Superconductivity · Physics 2022-08-09 Li-Na Zong , Ren-Shu Wang , Di Peng , Xiao-Jia Chen

We report measurements of anamolously large dissipative conductivities in BiSrCaCuO(2212) at low temperatures. We have measured the complex conductivity of BSCCO thin films at 100-600 GHz as a function of doping from the underdoped to the…

Superconductivity · Physics 2009-10-31 J. Corson , R. Mallozzi , J. Orenstein , J. N. Eckstein , I. Bozovic

We have developed a simple and straightforward way to realize controlled post-doping towards 2D transition metal dichalcogenides (TMDs). The key idea is to use low-kinetic energy dopant beams and a high-flux chalcogen beam at the same time,…

The optical properties of optimally-doped Bi_2Sr_2CaCu_2O_{8+\delta} (Bi2212) have been measured normal to the edge planes [ac plane, bc plane, and (1\bar{1}0) plane], for light polarized parallel to nodal and anti-nodal (gap) directions,…

Superconductivity · Physics 2007-05-23 J. J. Tu , C. C. Homes , L. H. Greene , G. D. Gu , M. Strongin

To understand the link between doping and electronic properties in high temperature superconductors, we report first-principles calculations on the oxygen doping effect for the single layer cuprate HgBa$_2$CuO$_{4+\delta}$. The doping…

Superconductivity · Physics 2007-05-23 P. Süle , C. Ambrosch-Draxl , H. Auer , E. Y. Sherman

Within the kinetic energy driven superconducting mechanism, the magnetic nature of cuprate superconductors is discussed. It is shown that the superconducting state is controlled by both charge carrier gap function and quasiparticle coherent…

Superconductivity · Physics 2007-05-23 Shiping Feng , Tianxing Ma , Huaiming Guo

The London penetration depth was measured in single crystals of self-doped Na$_{1-\delta}$FeAs (from under - to optimal - doping, $T_c$ from 14 to 27 K) and electron-doped Na(Fe$_{1-x}$Co$_{x}$)As with $x$ ranging from undoped, $x=0$ to…

Superconductivity · Physics 2013-04-16 K. Cho , M. A. Tanatar , N. Spyrison , H. Kim , G. Tan , P. Dai , C. L. Zhang , R. Prozorov

We present a systematic study of the Hall conductance in Bi$_2$Sr$_2$CaCu$_2$O$_x$ (Bi2212) thin films over a large range of doping. We find that in a large part of the phase diagram the Hall coefficient changes sign as a function of…

Superconductivity · Physics 2023-04-07 Yuval Nitzav , Amit Kanigel

We report on infrared reflectivity measurements of the $ab$-plane response of superconducting Bi$_2$Sr$_2$CuO$_6$ single crystals. The frequency dependent conductivity has a maximum near 700 cm$^{-1}$ at room temperature, which shifts to…

Condensed Matter · Physics 2009-10-30 A. A. Tsvetkov , J. Schuetzmann , D. van der Marel

Understanding the origin of electron incoherence is the first step toward a theoretical description of the non-Fermi liquid behavior of the high-T$_{c}$ cuprate superconductors. Such electron incoherence manifests itself most evidently in…

Strongly Correlated Electrons · Physics 2024-01-02 Jianhua Yang , Tao Li

We discuss the irreversible magnetic properties of self-flux grown Ba(Fe1-xCox)2As2 single crystals for a wide range of concentrations covering the whole phase diagram from the underdoped to the overdoped regime, x=0.038, 0.047, 0.058,…

Superconductivity · Physics 2015-05-13 R. Prozorov , M. A. Tanatar , E. C. Blomberg , P. Prommapan , R. T. Gordon , N. Ni , S. L. Bud'ko , P. C. Canfield

We apply a recently-developed low-field technique to inductively measure the critical pair momentum $p_c$ in thin, underdoped films of Y$_{1-x}$Ca$_{x}$Ba$_{2}$Cu$_{3}$O$_{7-\delta}$ and Bi$_{2}$Sr$_{2}$CaCu$_{2}$O$_{8+\delta}$ reflecting a…

Superconductivity · Physics 2015-06-22 John Draskovic , Stanley Steers , Thomas McJunkin , Adam Ahmed , Thomas R. Lemberger

We present the c-axis optical conductivity $\sigma_{1c}(\omega, T)$ of underdoped ($x$ = 0.12) and optimally doped ($x$ = 0.15) LSCO from 4 meV to 1.8 eV obtained by a combination of reflectivity and transmission spectra. In addition to the…

Condensed Matter · Physics 2009-11-10 A. B. Kuzmenko , N. Tombros , H. J. A. Molegraaf , M. Grueninger , D. van der Marel , S. Uchida

We measured the terahertz (THz) complex conductivity of Ca doped YBa_{2}Cu_{3}O_{7-\delta} thin films in the frequency range of 0.1 to 3 THz (3 to 100 cm^{-1}) and at a temperature range of 20 to 300 K. The films were measured using both…

Superconductivity · Physics 2015-06-04 Nimrod Bachar , Eli Farber , Elena Zhukova , Boris Gorshunov , Michael Roth

We have studied the chemical potential shift in the high-temperature superconductor Bi$_2$Sr$_2$Ca$_{1-x}${\it R}$_{x}$Cu$_2$O$_{8+y}$ ({\it R} = Pr, Er), where the hole concentration is varied from 0.025 to 0.17 per Cu, by precise…

Superconductivity · Physics 2009-11-07 N. Harima , A. Fujimori , T. Sugaya , I. Terasaki