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471.
A sharp variation of the near infrared photoluminescence intensity for spin-3/2 color centers in hexagonal (4H-, 6H-) and rhombic (15R-) SiC polytypes in the vicinity of level anticrossing (LAC) and cross-relaxation in an external magnetic field at room temperature are observed. This effect can be used for a purely all-optical sensing of the magnetic field with nanoscale spatial resolution. A distinctive feature of the LAC signal is a weak dependence on the magnetic field direction that allows monitoring of the LAC signals in the nonoriented systems, such as powder materials, without need to determine the nanocrystal orientation in the sensing measurements. Furthermore, an LAC-like signal is also observed for the spin color centers (NV centers) in diamond in low magnetic fields with only marginal dependence on the magnetic field direction. This effect is enabled to detect weak magnetic fields using nanodiamond samples in the form of disordered mixture. In addition, the optically detected magnetic resonance and LAC techniques are suggested to serve as a simple method to determine the local stress in nanodiamonds under ambient conditions.  相似文献   
472.
A novel efficient method for the synthesis of licochalcone C in good yield on up to 30 g scale was developed. The reaction sequence included relied on the directed ortho-metalation (DOM) of bis-O-MOM-protected resorcinol for the regioselective C-prenylation, followed by metalation-formylation, selective O-deprotection of a hydroxyl group located between the formyl and prenyl groups, its methylation, and aldol reaction with p-hydroxyacetophenone. Synthesis of structurally related retrochalcones, i.e., licoagrochalcones B, C, and D, was also proposed.  相似文献   
473.
474.
The formation of irradiation defects produced in a high voltage electron microscope (HVEM) has been studied in Ge and other semiconductor crystals in dependence on various thermal treatments and on covering of the specimen surface. It has been concluded that the defect formation depends — besides general features known for pure metals — also on the state of electrically neutral impurities. Besides, various interactions between dislocations and irradiation defects were observed.  相似文献   
475.
We prove continuity and Harnack's inequality for bounded solutions to elliptic equations of the type div | u | p 2 u + a ( x ) | u | q 2 u = 0 , a ( x ) 0 , | a ( x ) a ( y ) | A | x y | α μ ( | x y | ) , x y , div | u | p 2 u 1 + ln ( 1 + b ( x ) | u | ) = 0 , b ( x ) 0 , | b ( x ) b ( y ) | B | x y | μ ( | x y | ) , x y , div | u | p 2 u + c ( x ) | u | q 2 u 1 + ln ( 1 + | u | ) β = 0 , c ( x ) 0 , β 0 , | c ( x ) c ( y ) | C | x y | q p μ ( | x y | ) , x y , $$\begin{eqnarray*} \hspace*{13pc}&&{\rm div}{\left(|\nabla u|^{p-2}\,\nabla u+a(x)|\nabla u|^{q-2}\,\nabla u\right)}=0, \quad a(x)\ge 0,\\ &&\quad |a(x)-a(y)|\le A|x-y|^{\alpha }\mu (|x-y|), \quad x\ne y, \\ &&{\rm div}{\left(|\nabla u|^{p-2}\,\nabla u {\left[1+\ln (1+b(x)\, |\nabla u|) \right]} \right)}=0, \quad b(x)\ge 0, \\ &&\quad |b(x)-b(y)|\le B|x-y|\,\mu (|x-y|),\quad x\ne y,\\ &&{\rm div}{\left(|\nabla u|^{p-2}\,\nabla u+ c(x)|\nabla u|^{q-2}\,\nabla u {\left[1+\ln (1+|\nabla u|) \right]}^{\beta } \right)}=0,\\ &&c(x)\ge 0, \, \beta \ge 0, |c(x)-c(y)|\le C|x-y|^{q-p}\,\mu (|x-y|), \quad x\ne y, \end{eqnarray*}$$ under the precise choice of μ.   相似文献   
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