We present magnetic field-temperature (H-T) phase diagrams of the double transitions of superconducting U_(1-x)Th_xBe_(13) with x=0.030 and x=0.022. For both samples increasing the applied magnetic field moves the two transitions to lower temperature while decreasing their separation in temperature. For the x=0.030 sample, the transitions remain distinct for T>100 mK. For x=0.022, however, the two transitions appear to merge near H=20 kOe acid T=350 mK, analogous to the situation in the related heavy fermion superconductor UPt_3
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....
Evidence is presented for the coexistence of two superconducting order parameters in U0.97Th0.03Be13...
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 present specific-heat C measurements of a high-quality polycrystal of UBe_(13) for 0.2≤T≤1.2 K an...
I discuss recent experiments on the heavy fermion superconductor U_(1-x) Th_xBe_(13), with an emphas...
I discuss recent experiments on the heavy fermion superconductor U_(1-x) Th_xBe_(13), with an emphas...
We present measurements of the upper critical magnetic field Hc2(T) determined from the dc magnetiza...
We present measurements of the upper critical magnetic field Hc2(T) determined from the dc magnetiza...
We present measurements of the upper critical magnetic field Hc2(T) determined from the dc magnetiza...
We measure the specific heat C under pressure of high purity polycrystals of the heavy fermion super...
A phase diagram is proposed for the different superconducting states in U1-xThxBe13. It suggests tha...
A phase diagram is proposed for the different superconducting states in U1-xThxBe13. It suggests tha...
Measurements of specific heat cp(T) and thermal conductivity λ(T) give a detailed picture of the Tc(...
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....
Evidence is presented for the coexistence of two superconducting order parameters in U0.97Th0.03Be13...
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 present specific-heat C measurements of a high-quality polycrystal of UBe_(13) for 0.2≤T≤1.2 K an...
I discuss recent experiments on the heavy fermion superconductor U_(1-x) Th_xBe_(13), with an emphas...
I discuss recent experiments on the heavy fermion superconductor U_(1-x) Th_xBe_(13), with an emphas...
We present measurements of the upper critical magnetic field Hc2(T) determined from the dc magnetiza...
We present measurements of the upper critical magnetic field Hc2(T) determined from the dc magnetiza...
We present measurements of the upper critical magnetic field Hc2(T) determined from the dc magnetiza...
We measure the specific heat C under pressure of high purity polycrystals of the heavy fermion super...
A phase diagram is proposed for the different superconducting states in U1-xThxBe13. It suggests tha...
A phase diagram is proposed for the different superconducting states in U1-xThxBe13. It suggests tha...
Measurements of specific heat cp(T) and thermal conductivity λ(T) give a detailed picture of the Tc(...
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....
Evidence is presented for the coexistence of two superconducting order parameters in U0.97Th0.03Be13...