Abstract:Precision radio-frequency measurements of the magnetic susceptibility using the tunnel diode resonator (TDR) technique are used to study the delicate effects in magnetic and superconducting materials. High resolution (in ppb range) measurements are particularly important for studies of the London and Campbell penetration depths in a superconductor and for the investigation of magnetic transitions in (anti)ferromagnets. Due to the small rf magnetic-excitation in a mOe range, the TDR is especially useful at low-… Show more
“…The variation of the rf magnetic penetration depth λ m was measured in a dilution refrigerator by using a TDO technique [35] (for review, see Refs. [36,37]).…”
Magnetic penetration depth, λ m , was measured as a function of temperature and magnetic field in single crystals of low carrier density superconductor YPtBi by using a tunnel-diode oscillator technique. Measurements in zero DC magnetic field yield London penetration depth, λ L (T ), but in the applied field the signal includes the Campbell penetration depth, λ C (T ), which is the characteristic length of the attenuation of small excitation field, H AC , into the Abrikosov vortex lattice due to its elasticity. Whereas the magnetic field dependent λ C exhibit λ C ∼ B p with p = 1/2 in most of the conventional and unconventional superconductors, we found that p ≈ 0.23 1/2 in YPtBi due to rapid suppression of the pinning strength. From the measured λ C (T, H ), the critical current density is j c ≈ 40 A/cm 2 at 75 mK. This is orders of magnitude lower than that of conventional superconductors of comparable T c .
“…The variation of the rf magnetic penetration depth λ m was measured in a dilution refrigerator by using a TDO technique [35] (for review, see Refs. [36,37]).…”
Magnetic penetration depth, λ m , was measured as a function of temperature and magnetic field in single crystals of low carrier density superconductor YPtBi by using a tunnel-diode oscillator technique. Measurements in zero DC magnetic field yield London penetration depth, λ L (T ), but in the applied field the signal includes the Campbell penetration depth, λ C (T ), which is the characteristic length of the attenuation of small excitation field, H AC , into the Abrikosov vortex lattice due to its elasticity. Whereas the magnetic field dependent λ C exhibit λ C ∼ B p with p = 1/2 in most of the conventional and unconventional superconductors, we found that p ≈ 0.23 1/2 in YPtBi due to rapid suppression of the pinning strength. From the measured λ C (T, H ), the critical current density is j c ≈ 40 A/cm 2 at 75 mK. This is orders of magnitude lower than that of conventional superconductors of comparable T c .
“…The variation of the radio-frequency (rf) magnetic penetration depth ∆λ m was measured in a dilution refrigerator by using a tunnel diode oscillator (TDO) technique [35] (for review, see Ref. [36,37]).…”
Magnetic penetration depth, λm, was measured as a function of temperature and magnetic field in single crystals of low carrier density superconductor YPtBi by using a tunnel-diode oscillator technique. Measurements in zero DC magnetic field yield London penetration depth, λL (T ), but in the applied field the signal includes the Campbell penetration depth, λC (T ), which is the characteristic length of the attenuation of small excitation field, Hac, into the Abrikosov vortex lattice due to its elasticity. Whereas the magnetic field dependent λC exhibit λC ∼ B p with p = 1/2 in most of the conventional and unconventional superconductors, we found that p ≈ 0.23 1/2 in YPtBi due to rapid suppression of the pinning strength. From the measured λC (T, H), the critical current density is jc ≈ 40 A/cm 2 at 75 mK. This is orders of magnitude lower than that of conventional superconductors of comparable Tc. Since the pinning centers (lattice defects) and vortex structure are not expected to be much different in YPtBi, this observation is direct evidence of the low density of the Cooper pairs because jc ∝ ns.
“…Please see reviews [34,35,36] for the detailed description of the principles of the TDR technique used in the present work, and Ref. [37] for the technical discussion of the implementation of the TDR in a dilution refrigerator, which was used in our experiments in this work.…”
Section: Methodsmentioning
confidence: 99%
“…Essentially, the tunnel diode compensates for the losses and, when the impedances properly match, triggers spontaneous self-oscillations at f 0 . It is possible to maintain this state with minimal external noise and excellent stability, provided that the circuit itself is well stabilized and shielded [37,38]. The outstanding sensitivity of the technique comes from the fact that it operates in the frequency domain (similar to microwave cavity perturbation technique and NMR), but without the need to scan the frequency (or field) in search for the resonance, which is an added benefit.…”
MHz) AC magnetic susceptibility, χ AC , of Dy 2 Ti 2 O 7 was measured using self-oscillating tunnel-diode resonator. Measurements were made with the excitation AC field parallel to the superimposed DC magnetic field up 5 T in a wide temperature range from 50 mK to 100 K. At 14.6 MHz a known broad peak of χ AC (T ) from kHz -range audiofrequency measurements around 15 K for both [111] and [110] directions shifts to 45 K, continuing the Arrhenius activated behavior with the same activation energy barrier of Ea ≈ 230 K. Magnetic field dependence of χ AC along [111] reproduces previously reported low-temperature two-in-two-out to three-in-oneout spin configuration transition at about 1 T, and an intermediate phase between 1 and 1.5 T. The boundaries of the intermediate phase show reasonable overlap with the literature data and connect at a critical endpoint of the first order transition line, suggesting that these low-temperature features are frequency independent. An unusual upturn of magnetic susceptibility at T → 0 was observed in magnetic fields between 1.5 T and 2 T for both magnetic field directions, before fully polarized configuration sets in above 2 T.
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