D. E. Moncton
Massachusetts Institute of Technology
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Featured researches published by D. E. Moncton.
Physical Review Letters | 1987
D. Vaknin; S. K. Sinha; D. E. Moncton; D. C. Johnston; John M. Newsam; Cyrus R. Safinya; H. E. King
Powder neutron diffraction studies of undoped
Solid State Communications | 1980
J.P. Remeika; G. P. Espinosa; A.S. Cooper; H. Barz; J.M. Rowell; D.B. McWhan; J.M. Vandenberg; D. E. Moncton; Z. Fisk; L.D. Woolf; H.C. Hamaker; M. B. Maple; G. Shirane; W. Thomlinson
{\mathrm{La}}_{2}
Physics Today | 1982
Ronald Pindak; D. E. Moncton
Physica A-statistical Mechanics and Its Applications | 1986
Jacob Bohr; Doon Gibbs; D. E. Moncton; K.L. D'Amico
{\mathrm{CuO}}_{4\mathrm{\ensuremath{-}}\mathrm{y}}
Physical Review Letters | 2012
W. Graves; Franz X. Kärtner; D. E. Moncton; P. Piot
have revealed new superlattice peaks below \ensuremath{\sim}220 K. The absence of corresponding x-ray superlattice lines and an observed susceptibility anomaly near 220 K suggest the occurrence of antiferromagnetism. From the magnetic peak intensities we deduce a structure consisting of ferromagnetic sheets of Cu spins alternating along the [100] orthorhombic axis, with the spins aligned along the [001] orthorhombic axis, The low-temperature magnetic moment is approximately 0.5
Solid State Communications | 1978
Jeffrey W. Lynn; D. E. Moncton; W. Thomlinson; G. Shirane; R.N. Shelton
{\mathrm{\ensuremath{\mu}}}_{\mathrm{B}}
Physica B-condensed Matter | 1989
Jakob Bohr; Doon Gibbs; J. D. Axe; D. E. Moncton; K.L. D'Amico; C.F. Majkrzak; J. Kwo; M. Hong; C. L. Chien; J. Jensen
/(Cu atom). The tetragonal-orthorhombic transition at 505 K has also been studied.
European Physical Journal B | 1987
E. D. Specht; A. Mak; C. J. Peters; Mark Sutton; R. J. Birgeneau; K.L. D'Amico; D. E. Moncton; S. E. Nagler; P. M. Horn
Abstract A new family of rare earth-rhodium-tin intermetallic compounds, with the representative formula (RE)Rh x Sn y , has been synthesized in single crystal form. The compounds containing the heavier rare earths are superconducting and those with the lighter rare earths are generally magnetic. The compound ErRh 1.1 Sn 3.6 exhibits reentrant superconductivity with T c = 0.97 K and T m = 0.57 K as determined from ac magnetic susceptibility measurements. The synthesis and X-ray characterization of the series are described and the results of electrical resistivity, upper critical magnetic field, magnetic susceptibility, specific heat and neutron scattering measurements on the Er compound are given.
Physical Review Special Topics-accelerators and Beams | 2014
W. Graves; J. Bessuille; P. Brown; Sergio Carbajo; V. Dolgashev; Kyung-Han Hong; E. Ihloff; Boris Khaykovich; Hua Lin; Krishna Murari; Emilio A. Nanni; Giacomo Resta; S. Tantawi; Luis E. Zapata; Franz X. Kärtner; D. E. Moncton
Nearly all the microscopically small devices that are contributing to the “microtechnological” revolution are composed of thin layers of materials. Such devices are nearly two‐dimensional, and many of the questions concerning the ultimate possibilities and limitations of the technology will require investigation of the physical processes in two dimensions. Similarly, questions that arise in such diverse fields as surface physics, membrane biology and catalytic chemistry involve two‐dimensional phenomena. At least as important as these practical questions is simple intellectural curiously: How does Nature behave in a world of limited dimensionality?
Journal of Applied Physics | 1979
D. E. Moncton
The analysis of data obtained in magnetic X-ray scattering experiments on rare earth metals, particularly holmium, has led to a phenomenological model for one-dimensional spatially propagating magnetic structures. Based on the concept of spin slips or discommensurations, this model explains the observed lock-in transitions in the magnetic spirals of the rare earths in terms of simple commensurate structures. Further, the anomalous intensities of previously observed higher harmonic magnetic satellites, as well as the qualitative behavior of the magnetic wave vector in the presence of a magnetic field, are understood directly within the spin slip description. We discuss how the presence of spin slips in the magnetic structure can lead to modulations of the crystal lattice as demonstrated by a recent magnetic X-ray study of holmium.