A new method for direct determination of the recoilless fraction using a single room-temperature Mössbauer measurement of a two-foil absorber

2002 ◽  
Vol 54 (4) ◽  
pp. 256-259 ◽  
Author(s):  
Monica Sorescu
2002 ◽  
Vol 721 ◽  
Author(s):  
Monica Sorescu

AbstractWe propose a two-lattice method for direct determination of the recoilless fraction using a single room-temperature transmission Mössbauer measurement. The method is first demonstrated for the case of iron and metallic glass two-foil system and is next generalized for the case of physical mixtures of two powders. We further apply this method to determine the recoilless fraction of hematite and magnetite particles. Finally, we provide direct measurement of the recoilless fraction in nanohematite and nanomagnetite with an average particle size of 19 nm.


1999 ◽  
Vol 33 (5) ◽  
pp. 807-813 ◽  
Author(s):  
Tanya Bangthanh To ◽  
D. Kirk Nordstrom ◽  
Kirkwood M. Cunningham ◽  
James W. Ball ◽  
R. Blaine McCleskey

1989 ◽  
Vol 227 ◽  
pp. 319-324 ◽  
Author(s):  
A. Cepeda-Saez ◽  
M.L. Vazquez ◽  
L. Sargi ◽  
P. Prognon ◽  
G. Mahuzier ◽  
...  

2000 ◽  
Vol 46 (3) ◽  
pp. 379-384 ◽  
Author(s):  
Michael Landt

Abstract Background: Leptin, a hormone produced primarily by adipose tissue, is known to be present in serum as both monomeric (free) and higher molecular mass (bound) forms, but little is known about the nature of the bound forms or physiological variation in binding capacity. Methods: A new method to quantify the free and bound forms was developed, based on HPLC separation and RIA quantification in chromatography fractions. Reanalysis of specimens after addition of exogenous leptin allowed direct determination of leptin-binding capacity and the degree of saturation of leptin-binding capacity. Results: HPLC chromatography fractionated serum leptin into both the free form and as a broad peak of 59–130 kDa. Several experiments were conducted to validate the new method. The concentrations of bound leptin in serum were 0.45–3.94 μg/L, and they increased as total leptin (reflecting adiposity) increased in 24 lean and obese volunteers. Leptin was readily dissociated from the bound fraction by competition from exogenous leptin. Rechromatography of the bound fraction led to dissociation of leptin, which was promoted by warming the sera before chromatography. Leptin-binding capacity was 1.8–5.3 μg/L; binding capacity was nearly constant over a range of total leptin concentrations of 2–10 μg/L, and slowly increased at higher total leptin concentrations. Saturation of binding capacity was low (15%) at very low total leptin concentrations (<5 μg/L), but rose quickly to a plateau near 80% at higher total leptin concentrations. Conclusions: The new method facilitates measurement of free and bound fractions of serum leptin, and is the first method measuring leptin-binding capacity. These experiments demonstrate that the concentration of bound leptin and leptin-binding capacity vary physiologically, with binding/binding capacity increasing with adiposity. Except in very lean individuals, binding capacity is nearly completely saturated.


1987 ◽  
Vol 109 ◽  
Author(s):  
Hisao Uchiki ◽  
Takayoshi Kobayashi

ABSTRACTWe propose a new method for the determination of the electro-optic constant. Third-order nonlinear susceptibility (X(3)(-ω;ω,0, 0)) of polycarbonate films doped with 4-diethylamino-4′-nitrostilbene molecules was determined between 550 and 800 nm at room temperature by using this method. X(3)(-ω;ω0, 0) is (5-4i) × 10-12 esu at 600 nm.


2011 ◽  
Vol 694 ◽  
pp. 184-188 ◽  
Author(s):  
Kao Wen Zhou ◽  
Zi Qiao Zhang ◽  
Li Jing Xing ◽  
Xin Li ◽  
Chun Xue Fu

A new sensor based on cataluminescence (CTL) produced on the surface of nanosized TiW3Cr2O14 was demonstrated for direct determination of ammonia in air. Trace ammonia was firstly absorbed on active carbon at room temperature to concentrate, then desorbed at 105°C to determine. The sensor showed high selectivity to ammonia at wavelength of 540 nm, satisfying activity at temperature of 275°C and good stability at air carrier flow rate of 115 ml/min. The linear range of CTL intensity versus concentration of ammonia was 1.0~50 mg/m3 (γ=0.9990), and the detection limit (3σ) was 0.5 mg/m3. The recovery of artificial sample was 97.45%—102.73% by this method. There was no response to benzene, SO2, CO and formaldehyde, and insignificant response to ethanol. This gas sensor allows on-line monitoring of ammonia in air.


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