ALBERT

All Library Books, journals and Electronic Records Telegrafenberg

feed icon rss

Your email was sent successfully. Check your inbox.

An error occurred while sending the email. Please try again.

Proceed reservation?

Export
Filter
  • American Institute of Physics (AIP)  (16)
Collection
Publisher
Years
  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 5860-5861 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Measurements of the magnetization vector M of a polycrystalline (Ba,K)BiO3 sample turned in a fixed field H at 4.2 K show that the rotational behavior of MP, the penetrating vortex-flux component of M, depends sensitively on the magnetic state of the sample before rotation. For the field-cooled state at 240 Oe, the vortex lines represented by MP are seen to bifurcate into two groups, one of which rotates rigidly with the sample while the other is held by H and turns frictionally relative to the sample. This behavior, seen earlier in polycrystalline YBa2Cu3O7, is directly ascribable to a distribution in the strength of the vortex pinning forces. For the hysteretic state in which H is raised from a large negative value to +240 Oe, a vortex-flux bifurcation is again observed but with an important difference. The strongly pinned vortices (rotating rigidly) reflect the original negative polarity of H, whereas the weakly pinned vortices (turning frictionally) are those produced by the positive H. Hence, in this hysteretic state before rotation, there is a coexistence of vortices of opposing polarity.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 5879-5879 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetization-vector measurements were made at various temperatures on polycrystalline disks of YBa2Cu3O7 and (Ba,K)BiO3 as each was rotated about its axis in a fixed field H along the disk plane. For hysteretic starting states, the vortex flux density vector B is found to bifurcate into a BR component that rotates rigidly with the sample and a BF component that stays at a fixed angle (θF) relative to H, thus turning frictionally relative to the sample, as seen earlier. With increasing H, BR decreases and BF increases in size, indicating a distribution in the strength of the vortex pinning torques. After BR has vanished, the frictional angle θF decreases rapidly. Thus, the quantity Hμ sin θF (μ being the quantized vortex moment), which equals the average pinning torque (τp) on each vortex, does not remain constant but diminishes with increasing H. This decrease of τp is consistent with the collective pinning phenomenon known as vortex bundling. At fixed H, τp diminishes rapidly with increasing temperature, reaching very low values well below Tc. These results are compared with those derived from critical-state model interpretations of conventional hysteresis loop data. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 76 (1994), S. 6965-6965 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In the simple model proposed, repulsive intervortex forces are balanced by containing forces produced by the external field (H) and by frictional forces representing the effects of pinning on displaced vortices. For the field-cooled (FC) state, whose vortex density is presumably uniform, the empirical fact that the average flux density (B¯) in nearly equal to H yields an operational inverse-square dependence of the intervortex force on the intervortex spacing. For both the FC and zero-field-cooled (ZFC) states, expressions are derived for B¯ vs H (including the remanences at H=0) and for the profiles of B across the sample thickness. Calculations of these properties are compared with experiment and with the macroscopically related critical-state model, revealing again that the pinning forces are strongly dependent on H. The frictional interacting-vortex model is also used in deriving the critical current as a transport property of the FC and ZFC states.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 6343-6343 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Upon reversal of the external magnetic field H during any hysteretic cycling of a type-II superconductor in its vortex state, the rate at which the magnetic flux density B varies with H is typically seen to start from zero and then change gradually. Measurements have now been made of the time dependence of B (the vortex flux creep) at many fixed-H points on several hysteresis loops of a grain-oriented YBa2Cu3O7 sample at 4.2 K (with H and B along the c axis), and it is observed that the size of the logarithmic dB/dt drops abruptly to zero, before proceeding to change in sign, whenever H is reversed. This curious similarity between the hysteretic behavior of dB/dt at fixed H and that of the nearly instantaneously measured dB/dH can be understood qualitatively in terms of the vortex pinning. As rotational magnetization measurements have recently shown,1 the unpinning and repinning of moving vortices is manifested macroscopically as a frictional process. Thus, the reversal of vortex motion involves the reversal of frictional forces, during which the vortex population in the superconducting sample (which is proportional to B) does not change with time or field.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 5683-5685 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Applicability of the Preisach hysteresis model to superconductive hysteresis is tested on two types of materials using a vibrating sample magnetometer. The experiments are set up to check if the hysteresis displayed by the two samples satisfies the necessary and sufficient conditions for the applicability of the Preisach model. These conditions are wiping out of some field history by certain subsequent field extrema and congruency of minor hysteresis loops corresponding to the same field cycles, but having different histories. Observation of the measured minor hysteresis loops indicates that the two conditions are satisfied for the two samples tested. For this reason, it can be concluded that the Preisach model is a very accurate representation of superconductive hysteresis, at least for some superconducting materials.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 70 (1991), S. 5733-5735 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetization-vector measurements at 77 K on a field-cooled sample rotated by angle θ relative to fixed field H reveal that MP, the penetrating vortex-flux component of the magnetization, undergoes some extraordinary changes at H≈30 Oe. As θ is raised above 180°, MP decreases in size to a very small minimum while its direction shifts rapidly, and these changes repeat as θ is then lowered below 180°. This behavior, which evolves systematically with H, was observed earlier for the same sample at 4.2 K but at much higher H (∼800 Oe) and is readily ascribed to a broad distribution in strength of the vortex pinning forces. Due to this distribution, the vortex lines bifurcate into two groups, one of which rotates rigidly with the sample while the other is held by H and turns frictionally relative to the sample.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 7
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: For this cubic pseudobinary compound, the bifurcation of the magnetization (M) vs temperature for warming and cooling in low fields (after zero-field cooling) indicates a spin-glass freezing point (Tg) of ∼20 K. Isotherms of M vs cooling field show zero spontaneous moments down to 4.2 K but an initial susceptibility that almost diverges below Tg〈sbxs〉. From rotational measurements of M as a vector in a fixed field (H) at 4.2 K, the anisotropy field produced by field cooling (HK) is found to turn rigidly with the sample for H below ∼1 kOe. At higher H, HK rotates up to some angle relative to H and then stays fixed as the sample continues to turn, thus exhibiting a frictional rotation relative to the sample. Nevertheless, HK remains sizeable in magnitude (∼12 kOe). Comparisons are made with analogous results for isostructural (Tb, Y) Ag, where spin-glass order coexists with antiferromagnetism, as well as for various prototypal spin-glass alloys.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 4527-4529 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A polycrystalline superconducting thin-disk sample was rotated in a fixed field (H) at 4.2 K, and the vector magnitude and orientation of the total magnetization (M) were measured as the sample-rotation angle (θ) was slowly cycled between 0° and 360°. The measured M was decomposed into a penetrating (vortex) flux component Mp that rotates rigidly with the sample at very small θ and a diamagnetic (shielding) component Md that stays antiparallel to H. As θ is raised, Mp deviates from rigid rotation, and the deviations are very different for the zero-field-cooled (ZFC) and field-cooled (FC) states at the same H, indicating different distributions in the strengths of the initial pinning forces. However, Md is exactly the same for both states and closely equals χ0H, where χ0 is the low-H (ZFC) diamagnetic susceptibility. At still higher θ, Mp rotates up to some critical angle relative to H, where it remains as the sample continues to turn. This frictional motion of Mp relative to the sample presumably derives from a sequential hopping of vortices between pinning centers.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 5261-5261 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: As nonmagnetic yttrium is substituted for terbium, TbAg changes from a conventional antiferromagnet into a complex magnetic system with components of both commensurate and incommensurate spin structures and bulk magnetic properties typical of spin-glass behavior for x≤0.5. We have carried out neutron diffraction experiments on polycrystalline samples with x=0.15, 0.5, and 1.0 to complement our earlier studies for x=0.3.1 For x=0.5, the system orders at T≈58 K into the mixed structure observed for x=0.3, but with a much sharper (1/2 1/2 0) peak. On cooling below 40 K the incommensurate peaks almost disappear, remaining only as low-intensity shoulders of the commensurate peak at the lowest temperature measured (T=4 K). Hysteresis is observed in the relative intensity of the two components of the structure between 45 and 55 K. For x=0.15, the system orders at T≈18 K into the two-component structure, but with an approximately constant intensity ratio and no evidence of hysteresis, similar to the behavior found for x=0.3. Thus, as the Tb concentration decreases, the relative stability of the commensurate and incommensurate structures appears to change. This balance between competing magnetic structures will be related to the spin-glass properties observed in this system.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 5961-5963 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: This cubic pseudobinary compound with antiferromagnetic order and spin-glass properties below Tg (36 K) was studied by magnetization-vector measurements on a field-cooled (FC) polycrystalline sample disk rotated in various fixed fields (H). At 4.2 K, the FC-induced anisotropy field HK is seen to turn rigidly with the sample for all rotation angles (θ≤180°) even at H=15 kOe, and since the rotational magnetization follows HK very closely, it is deduced that HK 〉100 kOe. At 20 K, HK turns rigidly, but only below a threshold field, above which HK rotates up to some critical angle relative to H, where it remains as the sample continues to turn. Thus HK rotates frictionally relative to the sample. Nevertheless, it is found that its magnitude continues to exceed 100 kOe.
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
    BibTip Others were also interested in ...
Close ⊗
This website uses cookies and the analysis tool Matomo. More information can be found here...