Low temperature a.c. Susceptibility of amorphous holmium aluminosilicate (Al2O3)0.2(Ho2O3)0.2(SiO2)0.6. Frequency dependence of the spin freezing temperature

1979 ◽  
Vol 31 (3) ◽  
pp. 213-218 ◽  
Author(s):  
C. Chappert ◽  
P. Beauvillain ◽  
J.-P. Renard ◽  
K. Knorr
1974 ◽  
Vol 52 (12) ◽  
pp. 2539-2546 ◽  
Author(s):  
C. J. Andrews ◽  
M. K. Pomeroy ◽  
I. A. de la Roche

Seedlings of winter wheat (Triticum aestivwn cv. Rideau and Cappelle Desprez) grown on moist filter paper in petri plates in dark at low temperature increased in cold hardiness, as measured by changes in the LD50 temperatures. Rideau attained an LD50 temperature of −12 °C after 5 weeks, Cappelle Desprez, −6 °C. Exposure to light delayed the maximum hardiness by 2 weeks and increased it by 6 °C in both cultivars. Exposure to diurnal freezing temperature increased hardiness of both cultivars in the dark, and in light when excessive dehydration was prevented.Greater cold hardiness of plants of both cultivars was attained in soil in light at low temperature as compared with those in petri plates. Exposure of plants to diurnal freezing temperature maintained a higher level of hardiness after the maximum at 7 weeks than continuous low temperature without freezing. Diurnal freezing during active low temperature growth in petri plates or in soil increased hardiness of Rideau seedlings to an apparent maximum of −18 °C.


2011 ◽  
Vol 170 ◽  
pp. 276-281 ◽  
Author(s):  
Wen Long Wu ◽  
Alix McCollam ◽  
Ian P. Swainson ◽  
Stephen R. Julian

There is growing interest in a possible connection between incoherent metallic conduction and high temperature superconductivity, that is exemplified by the behaviour of the parent compounds of the new iron-pnictide high-temperature superconductors. We have recently discovered very incoherent behaviour in the non-superconducting arsenide, FeCrAs. This material shows a non-metallic resistivity that rises with decreasing temperature without saturation or a gap, over three decades of temperature, from 80 mK to 800 K. We briefly review this behaviour, and address the question of disorder: how to test for the presence of disorder in a system where the scattering rate inferred from the resistivity is highly abnormal, and how to produce single crystals with low levels of disorder. Our discussion will focus on magnetic properties. FeCrAs is a partly frustrated magnetic system with a Nèel temperature TN that depends on sample quality, a sample-dependent spin freezing temperature TF < TN, and magnetic hysteresis that depends strongly on preparation conditions due to ferromagnetic minority phases in disordered samples.


2013 ◽  
Vol 543 ◽  
pp. 507-510 ◽  
Author(s):  
Janis Jankovskis ◽  
Nikolajs Ponomarenko ◽  
Deniss Stepins

Complex permeability spectra of polycrystalline ferrites are analyzed on the basis of the model accounting for the effects of their grain size distribution (GSD). The model allows for explicit relation for absorption component. It shows, that by change of only one parameter (related with GSD) it is possible to turn from the relaxation to resonance character of spectrum, that spectra of ferrites, sintered at low temperature, tend to the most theoretical type - symmetrical one.


1999 ◽  
Vol 13 (09n10) ◽  
pp. 1235-1240
Author(s):  
M.-H. Julien ◽  
P. Carretta ◽  
F. Borsa ◽  
A. Rigamonti

139 La and 63 Cu NQR relaxation rates are used to obtain insights on the effects of itinerant holes on the magnetic in-plane correlation length, for x ≤ 0.04 in La 2-x Sr x CuO 4. For these concentrations, corresponding to spin-glass behavior at low temperature, evidence for the microsegregation of holes along stripes is presented. Preliminary relaxation results for an amount of Sr doping leading to superconductivity are also presented and discussed in terms of the crossover from the spin-glass to the underdoped superconducting regime: for x = 0.06 a slowing down of spin fluctuations is evidenced and superconductivity is found to coexist with spin-freezing.


2000 ◽  
Vol 69 (3) ◽  
pp. 888-894 ◽  
Author(s):  
Masafumi Ito ◽  
Yukio Yasui ◽  
Masaki Kanada ◽  
Hiroshi Harashina ◽  
Shunsuke Yoshii ◽  
...  

1999 ◽  
Vol 602 ◽  
Author(s):  
Y. Muraoka ◽  
H. Tabata ◽  
T. Kawai

AbstractA spin-glass state up to 210 K has been found in (Mg,Fe){Mg,Fe,Ti)2O4 spinel ferrite thin films formed on α-Al2O3(0001) substrates. The long-time relaxation of the magnetization in zero-field-cooled operation, which is characteristic feature of the spin-glass state, has been observed below 210 K. We have also achieved the change of magnetic state in the film from spin-glass to ferrimagnet over a wide temperature range below 160 K by means of light-irradiation. The amount of spin-melt on light-irradiation is calculated to be 41 % at 10 K and 26 % at 100 K.


Author(s):  
Lisa Fürtauer ◽  
Jakob Weiszmann ◽  
Wolfram Weckwerth ◽  
Thomas Nägele

Plants have evolved tightly regulated strategies to adapt and acclimate to a changing environment to ensure their survival. Various environmental factors affect plant distribution, growth and yield. Low temperature belongs to those abiotic factors which significantly constrain range boundaries of plant species. Exposing plants to low but non-freezing temperature induces a multigenic processes termed cold acclimation, which finally results in an increased freezing tolerance. Cold acclimation comprises reprogramming of the transcriptome, proteome and metabolome and affects communication and signaling between subcellular organelles. Reprogramming of the central carbohydrate metabolism plays a key role in cold acclimation. This review summarizes current knowledge about the role of carbohydrate metabolism in plant cold acclimation. A focus is laid on subcellular metabolic reprogramming, its thermodynamic constraints under low temperature and mathematical modelling of metabolism.


1972 ◽  
Vol 50 (9) ◽  
pp. 1965-1970 ◽  
Author(s):  
R. P. Pharis ◽  
H. Hellmers ◽  
E. Schuurmans

The daily course of photosynthesis (Ps) was determined for ponderosa pine (Pinus ponderosa Laws.) seedlings before and after their transfer from 23° to 11° or 3 °C and vice versa. Apparent Ps at 11 °C was greater than at 23 °C for up to 17 days after transfer. The increase was of the same order of magnitude as the decrease noted in dark respiration (Rs). Apparent Ps at 3 °C was little affected for the first 3 days after transfer, but declined to about 70% of pretreatment rate by day 10. If dark Rs at 3 °C is taken into account, actual Ps declined to about 50% of pretreatment rate by day 10. After this, the decline in Ps, with time, proceeds slowly. Recovery of Ps after transfer from the lower temperatures to 23 °C was rapid only if the length of time at the low temperature did not exceed 1 day. Return of apparent Ps to pretreatment rates was accomplished by day 7 for plants subjected to 17 days of 11 °C. Recovery of apparent Ps for plants subjected to 4 or more days of 3 °C reached 80% by day 7, and 90% by day 23. Dark Rs of plants brought from 3° to 23 °C was increased appreciably at first, this increase being of the same order of magnitude as the decrease in apparent Ps. Dark Rs then decreased with time at 23 °C, this decrease being correlated with an increase in apparent Ps. It is concluded that the initial chilling "injury," if any, occasioned by very low, but above freezing temperature, does not involve the physical or metabolic apparatus of Ps, but rather is associated with the respiratory apparatus as evidenced by increased rates of dark Rs during recovery at higher temperatures.


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