Add to ORKGWe present specific-heat C measurements of a high-quality polycrystal of UBe_(13) for 0.2≤T≤1.2 K and 0≤H≤80 kG. Field-sweep data, C(H) at fixed T, reveal two broad peaks in the superconducting state for T<0.6 K. The low-field feature occurs at H≊20 kG, independent of temperature. Conventional temperature scans, C(T) at fixed H, presumably smear this feature beyond recognition
Electrical-resistivity, magnetic-susceptibility, and specific-heat data reveal that UBe13 is superco...
We report on measurements of the low-temperature specific heat Cp(T, B) of the unconventional superc...
We report on measurements of the low-temperature specific heat Cp(T, B) of the unconventional superc...
We present specific-heat C measurements of high-purity polycrystals of U_(1-x)Th_xBe_(13) for 0≤x≤0....
We present specific-heat C measurements of high-purity polycrystals of U_(1-x)Th_xBe_(13) for 0≤x≤0....
We present magnetic field-temperature (H-T) phase diagrams of the double transitions of superconduct...
We present magnetic field-temperature (H-T) phase diagrams of the double transitions of superconduct...
We have measured the specific heat, C, of single-crystal UPt_3 in the superconducting regime as a fu...
We present magnetic field-temperature (H-T) phase diagrams of the double transitions of superconduct...
We have measured the specific heat, C, of single-crystal UPt_3 in the superconducting regime as a fu...
We have measured the specific heat, C, of single-crystal UPt_3 in the superconducting regime as a fu...
We have measured the specific heat of pure and thoriated (3.3% thorium) UBe13 in the temperature int...
We measure the specific heat C under pressure of high purity polycrystals of the heavy fermion super...
Low-temperature measurements (200 mK≲T≲18 K) of the specific heat C(T) of polycrystalline UBe13 show...
Low-temperature measurements (200 mK≲T≲18 K) of the specific heat C(T) of polycrystalline UBe13 show...
Electrical-resistivity, magnetic-susceptibility, and specific-heat data reveal that UBe13 is superco...
We report on measurements of the low-temperature specific heat Cp(T, B) of the unconventional superc...
We report on measurements of the low-temperature specific heat Cp(T, B) of the unconventional superc...
We present specific-heat C measurements of high-purity polycrystals of U_(1-x)Th_xBe_(13) for 0≤x≤0....
We present specific-heat C measurements of high-purity polycrystals of U_(1-x)Th_xBe_(13) for 0≤x≤0....
We present magnetic field-temperature (H-T) phase diagrams of the double transitions of superconduct...
We present magnetic field-temperature (H-T) phase diagrams of the double transitions of superconduct...
We have measured the specific heat, C, of single-crystal UPt_3 in the superconducting regime as a fu...
We present magnetic field-temperature (H-T) phase diagrams of the double transitions of superconduct...
We have measured the specific heat, C, of single-crystal UPt_3 in the superconducting regime as a fu...
We have measured the specific heat, C, of single-crystal UPt_3 in the superconducting regime as a fu...
We have measured the specific heat of pure and thoriated (3.3% thorium) UBe13 in the temperature int...
We measure the specific heat C under pressure of high purity polycrystals of the heavy fermion super...
Low-temperature measurements (200 mK≲T≲18 K) of the specific heat C(T) of polycrystalline UBe13 show...
Low-temperature measurements (200 mK≲T≲18 K) of the specific heat C(T) of polycrystalline UBe13 show...
Electrical-resistivity, magnetic-susceptibility, and specific-heat data reveal that UBe13 is superco...
We report on measurements of the low-temperature specific heat Cp(T, B) of the unconventional superc...
We report on measurements of the low-temperature specific heat Cp(T, B) of the unconventional superc...