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131.
Specific features of photo and thermoluminescence of Tb ions in BaO-M2O3 (M=Ga, Al, In)-P2O5 glasses
S.V.G.V.A. Prasad 《Journal of luminescence》2007,127(2):637-644
BaO-P2O5 glasses mixed with the three metal oxides viz., Al2O3, Ga2O3 and In2O3 doped with Tb2O3 were prepared. The glasses were characterized by X-ray diffraction and differential thermal analysis. Optical absorption and photoluminescence spectra and thermoluminescence (TL) of these glasses have been studied. From the measured intensities of various absorption bands of these glasses, the Judd-Ofelt parameters Ω2, Ω4 and Ω6 have been evaluated and compared with those of other reported glass systems. The Judd-Ofelt theory could successfully be applied to characterize the absorption and luminescence spectra of these glasses. From this theory various radiative properties like transition probability A, branching ratio βr, the radiative lifetime τr and the emission cross-section σE for various emission levels of these glasses have been determined and reported. An attempt has also been made to throw some light on the relationship between the structural modifications and luminescence efficiencies of all the three glasses. The analysis of TL data indicate high non-radiative losses in In2O3 mixed glasses. 相似文献
132.
采用改进型Sagnac干涉光栅写入系统,利用532nm准带隙光曝光源和带+1/-1衍射级的相位掩模板,在两种不同直径的低损耗As_2S_3硫系玻璃光纤上刻写布喇格光栅,并研究曝光期间光栅的动态特性.实验表明,As_2S_3光纤布喇格光栅透射峰值随光纤直径的减小而增强;在曝光过程中,布喇格波长先是较快地向短波长方向移动,随着曝光时间的延长,布喇格波长缓慢地向长波长方向回复.曝光时间为800~1 000s时,在包层直径为140μm的As_2S_3光纤上获得质量良好的布喇格光栅光谱,其透射峰值可达-2.6dB,带宽为0.37nm.对As_2S_3硫系光纤纤芯的光敏性分析结果表明,折射率调制幅度和平均折射率变化随曝光时间分别可达到10-4和10-3数量级. 相似文献
133.
G. Schröder T. Knetter M.J. Alava H. Rieger 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,24(1):101-105
Random walk arguments and exact numerical computations are used to study one-dimensional random field chains. The ground state
structure is described with absorbing and non-absorbing random walk excursions. At low temperatures, the local magnetization
follows the ground state except at regions where a local random field fluctuation makes thermal excitations easier. This is
explained by the random walk picture, implying that the magnetization lengthscale is a product of the domain size and the
thermal excitation scale.
Received 16 October 2000 and Received in final form 7 June 2001 相似文献
134.
Lead scandium phosphate glasses (PbO-Sc2O3-P2O5) containing different concentrations of tungsten oxide (WO3) ranging from 0 to 5 mol% were prepared. A number of studies, viz. differential thermal analysis (DTA), infrared spectra, optical absorption, and electron spin resonance (ESR) spectra, have been carried out. The results of DTA indicated the highest glass forming ability for the glass containing 5 mol% of WO3. The results of spectroscopic studies have been analyzed in light of different oxidation states of tungsten ions. 相似文献
135.
This paper deals with the preparation and optical analysis of Er3+ (0.2 mol%) boro-fluoro-phosphate glasses in the following glass compositions:
-
Series A: 69.8 B2O3–10 P2O5–10(ZnO/CdO/TeO2)–10 AlF3
-
Series B: 69.8 B2O3–10 P2O5–10(ZnO/CdO/TeO2)–10 LiF
136.
The glass formation in the SiO2-rich region of the ternary oxide system Al2O3–ZrO2–SiO2 with MgO, CaO, and TiO2 as melting aids was analyzed. The crystallization of glasses with different content of TiO2 and phase evolution with the temperature was studied by X-ray diffraction, infrared, laser Raman spectroscopy and transmission electron microscopy. The use of TiO2 favored formation and crystallization of the glasses due to the decrease of the viscosity of melts and acting as a nucleating agent. The crystalline phase of t-ZrO2 was developed at temperatures as low as 880°C whereas in as prepared specimens without TiO2 its presence was not detected. For the specimens with TiO2, t-ZrO2 and mullite were the principal phases at 1000°C. TiO2 addition did not change the crystallization sequence but decreased the formation temperature of the crystalline phases. Most of Ti4+ ions entered into t-ZrO2 and only a small portion in mullite, but the surplus was detected in ZrTiO4. 相似文献
137.
C. Monthus T. Garel 《The European Physical Journal B - Condensed Matter and Complex Systems》2006,53(1):39-45
The directed polymer in a 1+3 dimensional
random medium is known to present a disorder-induced phase
transition. For a polymer of length L, the high temperature
phase is characterized by a diffusive behavior for the end-point
displacement R2 ∼L and by free-energy fluctuations of order
ΔF(L) ∼O(1). The low-temperature phase is characterized by
an anomalous wandering exponent R2/L ∼Lω and
by free-energy fluctuations of order ΔF(L) ∼Lω
where ω∼0.18. In this paper, we first study the scaling
behavior of various properties to localize the critical temperature
Tc. Our results concerning R2/L and ΔF(L) point towards
0.76 < Tc ≤T2=0.79, so our conclusion is that Tc is equal
or very close to the upper bound T2 derived by Derrida and
coworkers (T2 corresponds to the temperature above which the ratio
remains finite as L ↦
∞). We then present histograms for the free-energy, energy and
entropy over disorder samples. For T ≫Tc, the free-energy
distribution is found to be Gaussian. For T ≪Tc, the free-energy
distribution coincides with the ground state energy distribution, in
agreement with the zero-temperature fixed point picture. Moreover the
entropy fluctuations are of order ΔS ∼L1/2 and follow a
Gaussian distribution, in agreement with the droplet predictions,
where the free-energy term ΔF ∼Lω is a near
cancellation of energy and entropy contributions of order L1/2. 相似文献
138.
Replica field theory is used to study the n -dependent free energy of the Ising spin glass in a first order perturbative treatment. Large sample-to-sample deviations of the free energy from its quenched average prove to be Gaussian, independently of the special structure of the order parameter. The free energy difference between the replica symmetric and (infinite level) replica symmetry broken phases is studied in details: the line n(T) where it is zero coincides with the Almeida–Thouless line for d>8. The dimensional domain 6<d<8 is more complicated, and several scenarios are possible. 相似文献
139.
D. Okai R. Nagai G. Motoyama T. Fukami T. Yamasaki Y. Yokoyama H.M. Kimura A. Inoue 《Physica C: Superconductivity and its Applications》2010,470(20):1048-1051
The superconducting property of Zr(1−x)Cox (x = 10–50 at.%) alloys and a Zr55Co30Al15 bulk metallic glass fabricated using techniques of rapid solidification was investigated. The Zr55Co30Al15 alloy crystallized by heat treatment in a vacuum atmosphere exhibited superconductivity of Tc,on = 2.4 K. This was attributable to the superconducting property of a crystalline Zr–Co alloy precipitated in the Zr55Co30Al15 alloy. The Tc,on of the crystalline Zr(1−x)Cox alloy was sensitive to the Co content. The increase of Co content for the Zr(1−x)Cox alloy led to the decrease of Tc,on. The Zr(1−x)Cox alloy exhibited superconductivity of a maximum Tc,on = 3.9 K for the Zr80Co20 alloy with superconducting nanocrystal particles embedded in the amorphous matrix. 相似文献
140.