2001
DOI: 10.1103/physrevb.64.100505
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Superconducting gap anisotropy ofLuNi2B2Cthin films from microwave surface impedance measurements

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Cited by 16 publications
(9 citation statements)
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“…Rather, we observe that while |F (q 11 )|/H does indeed lie above |F (q 10 )|/H, other higher order form factors fall in between these two limiting curves. This is not surprising when one keeps in mind that LuNi 2 B 2 C, as well as the other members of the rare earth nickelborocarbide superconductors, posseses a significant in-plane anisotropy [60][61][62][63][64][65][66][67][68][69][70]. While it would be straightforward to incorporate an in-plane penetration depth anisotropy into the models discussed above, a model independent analysis of the data is desirable.…”
Section: Vortex Lattice Form Factormentioning
confidence: 99%
“…Rather, we observe that while |F (q 11 )|/H does indeed lie above |F (q 10 )|/H, other higher order form factors fall in between these two limiting curves. This is not surprising when one keeps in mind that LuNi 2 B 2 C, as well as the other members of the rare earth nickelborocarbide superconductors, posseses a significant in-plane anisotropy [60][61][62][63][64][65][66][67][68][69][70]. While it would be straightforward to incorporate an in-plane penetration depth anisotropy into the models discussed above, a model independent analysis of the data is desirable.…”
Section: Vortex Lattice Form Factormentioning
confidence: 99%
“…It is well known that LuNi 2 B 2 C, as well as the other members of the rare-earth nickelborocarbide superconductors, posseses a significant in-plane anisotropy. [9][10][11][12][13][14][15][16][17][18][19][20] The fourfold, in-plane anisotropy manifests itself most strongly in the experimental data in Fig. 4, when comparing the ͓110͔ and ͓100͔ crystalline directions, corresponding to the ͑10͒ and ͑11͒ VL reflections.…”
Section: Higher Order Form Factors ͦF(q Hk )ͦmentioning
confidence: 99%
“…To correlate the above structural properties with the low energy excitations, we have carried out l ab ðTÞ measurements in the range 1.5 K-T c using different techniques: (i) a single coil-mutual inductance technique at 4 MHz [6]; (ii) a microstrip resonator with fundamental quasi-TEM mode at 1.44 GHz [7]; (iii) a sapphire loaded cylindrical resonator operating in the TE 011 mode at 19.8 GHz [8].…”
Section: Resultsmentioning
confidence: 99%