6,177 research outputs found

    Stress relaxation and mechanical properties of RL-1973 and PD-200-16 silicone resin sponge materials

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    Stress relaxation tests were conducted by loading specimens in double-lap shear to a preselected strain level and monitoring the decay of stress with time. The stress relaxation response characteristics were measured over a temperature range of 100 to 300 K and four strain levels. It is concluded that only a slight amount of stress relaxation was observed, and the stiffness increased approximately two orders of magnitude over the range of temperatures

    Exact solution of a 2d random Ising model

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    The model considered is a d=2 layered random Ising system on a square lattice with nearest neighbours interaction. It is assumed that all the vertical couplings are equal and take the positive value J while the horizontal couplings are quenched random variables which are equal in the same row but can take the two possible values J and J-K in different rows. The exact solution is obtained in the limit case of infinite K for any distribution of the horizontal couplings. The model which corresponds to this limit can be seen as an ordinary Ising system where the spins of some rows, chosen at random, are frozen in an antiferromagnetic order. No phase transition is found if the horizontal couplings are independent random variables while for correlated disorder one finds a low temperature phase with some glassy properties.Comment: 10 pages, Plain TeX, 3 ps figures, submitted to Europhys. Let

    An extreme ultraviolet spectrometer experiment for the Shuttle Get Away Special Program

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    An extreme ultraviolet (EUV) spectrometer experiment operated successfully during the STS-7 mission in an experiment to measure the global and diurnal variation of the EUV airglow. The spectrometer is an F 3.5 Wadsworth mount with mechanical collimator, a 75 x 75 mm grating, and a bare microchannel plate detector providing a spectral resolution of 7 X FWHM. Read-out of the signal is through discrete channels or resistive anode techniques. The experiment includes a microcomputer, 20 Mbit tape recorder, and a 28V, 40 Ahr silver-zinc battery. It is the first GAS payload to use an opening door. The spectrometer's 0.1 x 4.2 deg field of view is pointed vertically out of the shuttle bay. During the STS-7 flight data were acquired continuously for a period of 5 hours and 37 minutes, providing spectra of the 570 A to 850 A wavelength region of the airglow. Five diurnal cycles of the 584 A emission of neutral helium and the 834 A emission of ionized atomic oxygen were recorded. The experiment also recorded ion events and pressure pulses associated with thruster firings. The experiment is to fly again on Mission 41-F

    Localization transitions in non-Hermitian quantum mechanics

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    We study the localization transitions which arise in both one and two dimensions when quantum mechanical particles described by a random Schr\"odinger equation are subjected to a constant imaginary vector potential. A path-integral formulation relates the transition to flux lines depinned from columnar defects by a transverse magnetic field in superconductors. The theory predicts that the transverse Meissner effect is accompanied by stretched exponential relaxation of the field into the bulk and a diverging penetration depth at the transition.Comment: 4 pages (latex) with 3 figures (epsf) embedded in the text using the style file epsf.st

    Finite Temperature and Dynamical Properties of the Random Transverse-Field Ising Spin Chain

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    We study numerically the paramagnetic phase of the spin-1/2 random transverse-field Ising chain, using a mapping to non-interacting fermions. We extend our earlier work, Phys. Rev. 53, 8486 (1996), to finite temperatures and to dynamical properties. Our results are consistent with the idea that there are ``Griffiths-McCoy'' singularities in the paramagnetic phase described by a continuously varying exponent z(δ)z(\delta), where δ\delta measures the deviation from criticality. There are some discrepancies between the values of z(δ)z(\delta) obtained from different quantities, but this may be due to corrections to scaling. The average on-site time dependent correlation function decays with a power law in the paramagnetic phase, namely τ1/z(δ)\tau^{-1/z(\delta)}, where τ\tau is imaginary time. However, the typical value decays with a stretched exponential behavior, exp(cτ1/μ)\exp(-c\tau^{1/\mu}), where μ\mu may be related to z(δ)z(\delta). We also obtain results for the full probability distribution of time dependent correlation functions at different points in the paramagnetic phase.Comment: 10 pages, 14 postscript files included. The discussion of the typical time dependent correlation function has been greatly expanded. Other papers of APY are available on-line at http://schubert.ucsc.edu/pete

    Exact renormalization of the random transverse-field Ising spin chain in the strongly ordered and strongly disordered Griffiths phases

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    The real-space renormalization group (RG) treatment of random transverse-field Ising spin chains by Fisher ({\it Phys. Rev. B{\bf 51}, 6411 (1995)}) has been extended into the strongly ordered and strongly disordered Griffiths phases and asymptotically exact results are obtained. In the non-critical region the asymmetry of the renormalization of the couplings and the transverse fields is related to a non-linear quantum control parameter, Δ\Delta, which is a natural measure of the distance from the quantum critical point. Δ\Delta, which is found to stay invariant along the RG trajectories and has been expressed by the initial disorder distributions, stands in the singularity exponents of different physical quantities (magnetization, susceptibility, specific heat, etc), which are exactly calculated. In this way we have observed a weak-universality scenario: the Griffiths-McCoy singularities does not depend on the form of the disorder, provided the non-linear quantum control parameter has the same value. The exact scaling function of the magnetization with a small applied magnetic field is calculated and the critical point magnetization singularity is determined in a simple, direct way.Comment: 11 page

    Five-Year Growth of Rock Lichens in a Low-Arctic Mountain Environment, Northern Labrador

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    In 1978, three lichen growth stations were established for Rhizocarpon section Rhizocarpon species and one for Alectoria miniscula in the Cirque Mountain area of the Torngat mountains. Five years later, in 1983, the lichens were remeasured. The five-year growth represented by the change in the theoretical diameter is very variable, between 0.10 and 0.54 mm per year. These rates are larger than expected and exceed rates previously determined for an eastern Arctic area, the Northern Cumberland Peninsula of Baffin Island, by more than 3 to more than 20 times. Similar rates are known for 'great period' growth outside Arctic regions. If the growth rates represent long-term growth, the ages of recessional moraines in the Torngat Mountains should be recalculated. Moraines formerly described as Late Wisconsin to mid-Holocene may be of Neoglacial age. Variability of growth rates from one individual to another precludes using these data for constructing growth curves which may be used, even locally, in lichenometric dating.En 1978, on a établi quatre sites de croissance du lichen dans la région du mont du Cirque dans les monts Torngat: trois sites des espèces Rhizocarpon de la section Rhizocarpon et un site de Alectoria miniscula. Cinq ans plus tard, en 1983, on a mesuré de nouveau les lichens pour constater que le diamètre moyen, qui témoigne de la croissance, a crû de manière très variable, soit de 0,10 à 0,54 mm par année. Ces taux de croissance sont plus élevés que prévu puisqu'ils dépassent de 3 à 20 fois les taux déjà mesurés dans le nord de la péninsule de Cumberland, île de Baffin. De tels taux de croissance du lichen s'apparentent davantage à ceux que l'on a observé dans les régions non arctiques au cours de sa période dite de grande croissance. Si ces taux s'appliquent à de longues périodes, il faudrait réévaluer la date de dépôt des moraines de récession dans les monts Torngat. Les moraines, que l'on croit dater de la période s'étendant du Wisconsinien supérieur à l'Holocène moyen, pourraient en fait dater du néoglaciaire. Toutefois, les variations observées entre les taux de croissance ne permettent pas d'utiliser ces données, même à l'échelle locale, pour tracer des courbes de croissance qui serviraient à établir des datations lichénométriques.1978 wurden im Cirque-Mountain-Gebiet der Torngat mountains vier Stationen zur Beobachtung des Flechten-Wachstums eingerichtet : drei Stationen fur Rhizocarpon-Arten der Sektion Rhizocarpon und eine Station fur Alectoria miniscula. Fùnf Jahre spâter, 1983, wurden die Flechten wieder gemessen. Der Fùnfjahreswuchs, der sich im Wechsel des durchschnittlichen Durchmessers ablesen IaBt, ist sehr unterschiedlich, zwischen 0.10 und 0.54 mm pro Jahr. Dièse Wachstumsraten sind grôfîer als erwartet und gehen ùber die zuvor fur ein ôstliches arktisches Gebiet, die Nord-Cumberland HaIbinsel der lnsel Baffin, bestimmten Raten mehr als dreifach bis zu mehr als zwanzigfach hinaus. Àhnliche Wachstumsraten sind fur die "groBe Periode" des Flechten-Wachstums auBerhalb der arktischen Gebiete bekannt. Wenn die Wachstumsraten Langzeit-Wachstum reprâsentieren, mûfite das Alter der Rùckzugs-Morànen in den Torngat-Bergen neu berechnet werden. Morànen, die zuvor dem spàten Wisconsin bis mittleren Holozân zugeschrieben wurden, kônnten aus der Neoglazialzeit stammen. Die Variationen der Wachstumsraten von einer Person zur anderen schlieBen eine Nutzung dieser Daten zum Aufbau von Wachstumskurven aus, welche, selbst lokal, zur Datierung auf der Basis der Flechten benutzt werden kônnten

    Griffiths-McCoy singularities in random quantum spin chains: Exact results through renormalization

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    The Ma-Dasgupta-Hu renormalization group (RG) scheme is used to study singular quantities in the Griffiths phase of random quantum spin chains. For the random transverse-field Ising spin chain we have extended Fisher's analytical solution to the off-critical region and calculated the dynamical exponent exactly. Concerning other random chains we argue by scaling considerations that the RG method generally becomes asymptotically exact for large times, both at the critical point and in the whole Griffiths phase. This statement is checked via numerical calculations on the random Heisenberg and quantum Potts models by the density matrix renormalization group method.Comment: 4 pages RevTeX, 2 figures include

    Influence of rare regions on magnetic quantum phase transitions

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    The effects of quenched disorder on the critical properties of itinerant quantum magnets are considered. Particular attention is paid to locally ordered rare regions that are formed in the presence of quenched disorder even when the bulk system is still in the nonmagnetic phase. It is shown that these local moments or instantons destroy the previously found critical fixed point in the case of antiferromagnets. In the case of itinerant ferromagnets, the critical behavior is unaffected by the rare regions due to an effective long-range interaction between the order parameter fluctuations.Comment: 4 pp., REVTe
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