R.W. White
Los Alamos National Laboratory
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Featured researches published by R.W. White.
Cryogenics | 1966
J.D.G. Lindsay; R.W. White; R.D. Fowler
THE method of Schawlow and Devlin I is at present the most commonly used for the detection of superconductivity. This method employs the change in selfinductance of a solenoid when a sample located inside the coil becomes superconducting. In order to increase the sensitivity, the solenoid is made a part of a parallel resonant circuit that controls the frequency of an oscillator, and changes in frequency corresponding to small changes in inductance are measured on a frequency counter. The method requires no physical connections to the sample, and irregularly shaped samples may be used. Frequency stability of the oscillator is a problem, however, and, when the solenoid is in a cryogenic bath being cooled by pumping, the oscillator frequency changes--probably because bubbling of the liquid affects the dielectric material surrounding the solenoid. In the method to be described, pumping effects are reduced considerably by a balanced-bridge technique. Also, sensitivity is increased by utilizing both the inductance change and the change in coil loss 2 making it possible to detect superconductivity in less than 1 mg quantities of material. While both of these effects have been noted in the literature, 1-4 they have not previously been used simultaneously for the detection of superconductivity.
Physica D: Nonlinear Phenomena | 1971
H.H. Hill; J.D.G. Lindsay; R.W. White; L.B. Asprey; V.O. Struebing; B. T. Matthias
Abstract Small amounts of the metals Th, U, Np, PuI, and Am were dissolved individually into fcc La, and the superconducting transition temperatures T c of the alloys were measured and compared with that of La. Th decreased T c of La only very weakly, and U seemed to do likewise. Np and Pu depressed T c quite strongly, as does the anomalous rare-earth metal Ce. Am does not appear to possess a magnetic moment in La. The present data complement previous work on the 4f metals and illustrate some differences between the first few transactinium metals and their counterparts in the rare-earth series.
Solid State Communications | 1974
H.H. Hill; R.W. White; J.D.G. Lindsay; V.O. Struebing
Abstract Np and Pu were substituted for U in bcc γ-U alloys and the depression of Tc measured. By extrapolating the Np and Pu impurity concentrations to 100%, estimates were made for the maximum superconducting transition temperatures that may be expected for bcc γ-Np and ∈-Pu alloys.
Solid State Communications | 1973
R.W. White; J.D.G. Lindsay; R.D. Fowler
Determination of the uranium isotope effect on the superconducting transition temperature of U 6 Fe led to studies of the effects of stoichiometry on transition temperature. The isotope effect is T c ∝ M −0.37 .
Physical Review Letters | 1967
R.D. Fowler; J.D.G. Lindsay; R.W. White; H.H. Hill; B. T. Matthias
Physical Review Letters | 1965
R.D. Fowler; B. T. Matthias; L.B. Asprey; H.H. Hill; J.D.G. Lindsay; C.E. Olsen; R.W. White
Inorganic and Nuclear Chemistry Letters | 1971
L.B. Asprey; R.D. Fowler; J.D.G. Lindsay; R.W. White; Burris Cunningham
Cryogenics | 1966
J.D.G. Lindsay; R.W. White; R.D. Fowler
Cryogenics | 1966
J.D.G. Lindsay; R.W. White; R.D. Fowler
Cryogenics | 1966
J.D.G. Lindsay; R.W. White; R.D. Fowler