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141.
142.
Roy Mathias 《Numerische Mathematik》1992,63(1):213-226
LetM
n
denote the space ofn×n matrices. GivenX, ZM
n
define
相似文献
143.
144.
145.
D. Ghosh J. Roy M. Basu A. Bhattacharjee T. Guhathakurta K. Sengupta 《Czechoslovak Journal of Physics》1982,32(11):1221-1224
This paper presents an extensive study on the dependence of the mean number of the fast fragment of the target nucleus n
g on the incident beam energy in proton-nucleus interaction in emulsion in the range 6·2E
0400 GeV/c. It has been observed that n
g decreases in the range 6·2E
0200 GeV/c, then increases and attains an approximately steady value up to 400 GeV/c. It is very difficult to explain this behaviour with the help of the existing nuclear production models.The author would like to thank Prof A. J. Herz (CERN), Prof. K. D. Tolostov (Dubna, U.S.S.R.), Prof. P. L. Jain (State University of New York, U.S.A.), Prof. G. Giacomelly (Italy) for kindly supplying the exposed emulsion plates. 相似文献
146.
Abstract. The respiration rates and respiratory control ratios of isolated bean mitochondria have been measured following exposure to 0, 150, 300 and 900 J/m
147.
D. Ravichandran K. Yamakawa A.S. Bhalla R. Roy 《Journal of Sol-Gel Science and Technology》1997,9(1):95-101
Phase pure powder and thin films of the novel ferroelectric materials SrBi2Ta2O9 (SBT) have been prepared using the organic precursors. The xero-gel formed was dried and characterized using TGA and DTA
to determine the organic burn out and crystallization temperature of SBT. Powder X-ray diffraction was used systematically
to check the crystallinity of SBT. Phase pure SBT powder was formed as low as 650°C and thin films at 600°C in comparison
to other earlier reported work. SEM micrographs show a grain size of ≈0.1 μm and show crack free films with a film thickness
of 2 μm. 相似文献
148.
The development of a sensitive and specific method of determining individually the five tetraalkyllead compounds normally present in ambient air is described. The method is based on collection of the analytes on a porous polymer using a prefilter to destroy ozone and prevent decomposition of the sample during collection and storage. Two-stage thermal desorption, separation by gas chromatography and detection by modified flame atomic absorption spectrometry gives detection limits (3σ) of ca. 0.25 ng Pb m?3 for tetramethyllead and 0.37 ng Pb m?3 for tetraethyllead in an air sample of 80 dm3 collected over a 3–24 h period. Environmental sampling by this method in paralle with a wet chemical (iodine monochloride) method was used to validate the method. During the comparative study, higher organic lead levels were consistently found by the iodine monochloride method; it is postulated that this indicates the presence of vapour-phase tri-(or di)-alkyllead in excess of 1 ng Pb m?3 in rural air. The versatility of the method is demonstrated by the results of atmospheric sampling at two locations, one rural and one at the kerbside in a city centre. 相似文献
149.
The polyamines putrescine, cadaverine, spermine and spermidine were separated and quantified by micellar electrokinetic chromatography (MEKC) with laser-induced fluorescence detection. The derivatization reagent, 1-pyrenebutanoic acid succinimidyl ester (PSE), allowed for the selective detection of the polyamines at 490 nm. Multiple labeling of the polyamines with PSE allows the formation of intramolecular excimers that emit at longer wavelengths (450-520 nm) than mono-labeled analytes (360-420 nm). Optimal separation of the labeled polyamines was achieved using a separation buffer consisting of 10 mM phosphate pH 7.2, 30 mM cholate, and 30% acetonitrile. Using these conditions, the four polyamines were separated in under 10 min. Limits of detection for putrescine, cadaverine, spermine and spermidine were 6, 5, 15 and 13 nM, respectively. These are superior or comparable to those previously reported in the literature using fluorescence detection. 相似文献
150.
Thermal noise in Hg0.795Cd0.205Te detectors is estimated for large biasing fields at a lattice temperature of 77 K, by computing the correlation functions of the velocity fluctuations with the Monte Carlo technique. The noise temperature for current components transverse to the field is almost independent of the field, but that corresponding to the parallel component increases by a factor of about 1.3 at 50 V/cm and by a factor of 3.0 at 300V/cm. The thermal noise voltage for a detector of 85 resistance increases from 0.6nV/Hz1/2 at low biasing fields to about 3nV/Hz1/2 at a field of 300 V/cm. The noise power is also found to remain constant up to about 75 GHz, and it decreases thereafter by a factor of 0.25 for doubling of the frequency. 相似文献
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