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Dive into the research topics where Östen Rapp is active.

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Featured researches published by Östen Rapp.


Solid State Communications | 1982

Evidence for correlation effects: −√T behaviour in the low temperature electrical resistance of disordered metals

Östen Rapp; S. M. Bhagat; H. Gudmundsson

Abstract It is found that the electrical resistance for several metal-metalloid amorphous alloys decreases with increasing temperature as −√ T from about 20 mK to several K. The form and magnitude of this temperature dependence is in agreement with recent predictions from interaction theories.


Solid State Communications | 1977

Measurements of the electrical resistivity of amorphous ferromagnets

Östen Rapp; S. M. Bhagat; Ch. Johannesson

Abstract The electrical resistivity of two amorphous ferromagnets is measured below 60K. There is a minimum in both cases below which the resistivity increases as Δϱ/ϱ ∼ − 1.9 × 10 −3 10 log T . Above the minima the resistivity is proportional to T2 which may be due to electron-electron scattering. The resistivity does not saturate down to at least 70 mK.


Solid State Communications | 1995

Superconducting fluctuations in the resistivity of Bi-based 2:2:2:3

Shunhui Han; Östen Rapp

Abstract The electrical resistance was measured for two sintered samples of Bi(Pb)SrCaCuO in the temperature region above the super-conducting transitions at about 110 K. The excess conductivity Δσ was analysed in the form ln Δσ = x ln (T − T c ) T c . Different choices of Tc are discussed. A consistent behaviour for both samples was found only with a careful construction of a mean field critical temperature. Two temperatures T ∗ and TG could then be identified for each sample. T ∗ corresponds to a transition from two to three dimensional fluctuations in the mean field region, characterized by exponents x1 = −1 and x 2 = − 1 2 respectively. At TG, about 0.6 K below T ∗ , there is a cross-over to a critical region with an exponent x3 of roughly −0.3. It is argued that the minor differences between the results for samples of different quality indicate that impurity effects probably do not influence the analysis.


Physica C-superconductivity and Its Applications | 1997

Excess conductivity in Y1−2xCaxTbxBa2Cu3O7−δ

Shun-Hui Han; P. Lundqvist; Östen Rapp

Abstract Superconducting fluctuations have been studied in zero magnetic field in sintered samples of Y 1−2x Ca x Tb x Ba 2 Cu 3 O 7−δ by electrical resistivity measurements for x=0, 0.025, and 0.05. The excess conductivity Δσ was analysed as a function of reduced temperature ϵ =ln(T/T c ) in the range −5 ϵ Δσ ∝ ϵ α of α 1 =−1, α 2 =−0.5 and α 3 ≈ −0.4 respectively.


Physica C-superconductivity and Its Applications | 1996

Neutron-diffraction studies and interatomic distances in CaPr doped NdBa2Cu3O7−δ

P. Lundqvist; C Tengroth; Östen Rapp; Roland Tellgren; Zsolt Hegedüs

Abstract Sintered samples of Nd 1−2 x Ca x Pr x Ba 2 Cu 3 O 7−δ with x = 0, 0.025, 0.050, and 0.10 have been studied by electrical-resistivity measurements, X-ray and neutron diffraction and from calculated bond-valence sums (BVS). Doping of equal amounts of CaPr suppresses a parabolic term in the decrease of the superconducting T c and results in a strong linear suppression of −d T c /d x = 206 K. This observation indicates a single-impurity effect and suggests that CaPr is a charge neutral doping in Nd-123. The c -axis length and cell volume decrease with doping and the Cu2O4 distance increases. BVS calculations suggest that T c in Pr doped 123 may be governed by small changes in interatomic distances and corresponding charge transfers, rather than a contribution from magnetic pair breaking as previously conjectured. Similar calculations of published data for oxygen-deficient Y-123 and Pr doped Y-123, show that the hole density in the planes →0 at about the concentration where T c vanishes. The average CuO 2 plane distance supports that Pr has valence +4 at low dopings. Results are discussed which suggest that the Pr valence at higher doping levels is +3.


Physica C-superconductivity and Its Applications | 1989

Structural, thermal and electrical studies of the Y1−2xCaxThxBa2Cu3O7−δ system with 0⩽x⩽0.20

Magnus Andersson; Zsolt Hegedüs; Mats Nygren; Östen Rapp

STRUCTURAL, THERMAL AND ELECTRICAL STUDIES OF THE Y1-2XCAXTHXBA2CU3O7-DELTA SYSTEM WITH 0 LESS-THAN-OR-EQUAL-TO 0.20


Journal of The Less Common Metals | 1978

New disordered superconductors

Östen Rapp; B Lindberg; H.S Chen; K.V Rao

Abstract We have measured the low temperature resistance of zirconium-based metallic glasses. Superconductivity is found in: Zr65Cu35, Tc = 2.0 K; Zr70Ni30, Tc = 2.9 K; and Zr70Co30, Tc = 3.3 K.


Physics Letters A | 1971

Low temperature specific heat measurements of ZrV2 and HfV2

Östen Rapp; L.J. Vieland

Abstract The C15 compounds ZrV 2 and HfV 2 show bulk superconductivity at 7.3 and 8.4 o K respectively, indicating a strong dependence of T c on the electron per atom number for C15 compounds. High electronic contributions to the specific heat are observed.


Solid State Communications | 1971

Superconductivity and electron-phonon interaction in TaV alloys

Östen Rapp

Abstract The electron-phonon coupling in TaV alloys is estimated from resistive measurements. It decreases rapidly with increasing V in Ta in qualitative agreement with the observed transition temperature, T c . A calculation of T c from the strong-coupling equation gives good agreement with observed values for a constant Coulomb pseudo-potential and one adjustable parameter.


Physica C-superconductivity and Its Applications | 2003

Fluctuation conductivity of polycrystalline Hg, Tl-1223

Shunhui Han; I. Bryntse; Johan Axnäs; B.R Zhao; Östen Rapp

Detailed resistivity measurements were made for polycrystalline Hg1-xTlxBa2Ca2Cu3O8+delta (x = 0 and 0.2) in zero field and above the superconducting T-c. The fluctuation conductivity Deltasigma is analyzed. With decreasing temperature two crossover temperatures could be identified for each sample; i.e. T* from two to three dimensional fluctuations in the mean field region (MFR), and T-G from the MFR to the critical region. All results are in agreement with the Lawrence-Doniach model. The c-axis coherence length and the interlayer coupling factor were obtained

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Magnus Andersson

Royal Institute of Technology

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Björn Lundqvist

Royal Institute of Technology

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W. Holm

Royal Institute of Technology

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Johan Axnäs

Royal Institute of Technology

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Yuri Eltsev

Royal Institute of Technology

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M. Rodmar

Royal Institute of Technology

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S. J. Poon

University of Virginia

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M. Ahlgren

Royal Institute of Technology

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A. Nordström

Royal Institute of Technology

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