Ananalytical solution of the master equation for two qubits-field system in the dispersive reservoir are investigated, the qubits are initially in werner states. Under the influence of the damping we investigate the quantum correlation in a two-qubit based on measurement-induced disturbance (MID). We compare MID and entanglement measured by negativity and illustrate their different characteristics. We find the effect of damping on MID is weaker than negativity. Negativity will experience a sudden transition but this will not happen for MID.

Ananalytical solution of the master equation for two qubits-field system in the dispersive reservoir are investigated, the qubits are initially in werner states. Under the influence of the damping we investigate the quantum correlation in a two-qubit based on measurement-induced disturbance (MID). We compare MID and entanglement measured by negativity and illustrate their different characteristics. We find the effect of damping on MID is weaker than negativity. Negativity will experience a sudden transition but this will not happen for MID.

Ananalytical solution of the master equation for two qubits-field system in the dispersive reservoir are investigated, the qubits are initially in werner states. Under the influence of the damping we investigate the quantum correlation in a two-qubit based on measurement-induced disturbance (MID). We compare MID and entanglement measured by negativity and illustrate their different characteristics. We find the effect of damping on MID is weaker than negativity. Negativity will experience a sudden transition but this will not happen for MID.

The effect of anodization parameters, e.g. anodizing voltage, anodizing current, duration time, electrolyte temperature, electrolyte type and concentration, on the volume expansion of anodized Al, Al-1wt%Si and Al-1%Cu thin films have been studied. The volume expansion factor of anodic porous alumina is found to vary from 1.32 to 2.08, depending on the anodizing voltage, anodizing current density and electrolyte type. The electrolyte temperature and impurity type have slight effect on the volume expansion factor. The relation between the pore density of porous alumina and the anodizing voltage is found to follow the relation NP=9.4×1010exp(-0.042V). In addition, the current efficiency during the anodization was determined to be about 83%.

Tin dioxide(SnO2) nanoparticlesweresynthesizedbyaconventionalprecipitation methodusingthereactionbetweentinchloridepentahydrateandammoniasolutions. The obtainedpowderswerecalcinedatvariedtemperaturesfrom300to1050 1C, and then characterizedbyusingthermogravimetricanalysis,differentialthermalanalysisand Fourier transformationinfraredspectroscopy.Theaveragecrystallitesize,determinedby x-ray diffraction,wasfoundtobeintherangeof3.45–23.5 nm.Theanalysisexhibiteda tetragonalphase.Theactivationenergyofcrystalgrowthwascalculatedandfoundtobe 12.12kJ/mol.Themicrostructureofnanoparticleswasexaminedbyhighresolution transmission electronmicroscopy.OpticalpropertieswereinvestigatedbyaUV–vis absorptionspectrophotometer.Thecalculatedopticalbandgapliesbetween4.75–4.25eV as aresultofincreasingthecalcinationtemperaturesandcrystallitesize.

Tin dioxide(SnO2) nanoparticlesweresynthesizedbyaconventionalprecipitation methodusingthereactionbetweentinchloridepentahydrateandammoniasolutions. The obtainedpowderswerecalcinedatvariedtemperaturesfrom300to1050 1C, and then characterizedbyusingthermogravimetricanalysis,differentialthermalanalysisand Fourier transformationinfraredspectroscopy.Theaveragecrystallitesize,determinedby x-ray diffraction,wasfoundtobeintherangeof3.45–23.5 nm.Theanalysisexhibiteda tetragonalphase.Theactivationenergyofcrystalgrowthwascalculatedandfoundtobe 12.12kJ/mol.Themicrostructureofnanoparticleswasexaminedbyhighresolution transmission electronmicroscopy.OpticalpropertieswereinvestigatedbyaUV–vis absorptionspectrophotometer.Thecalculatedopticalbandgapliesbetween4.75–4.25eV as aresultofincreasingthecalcinationtemperaturesandcrystallitesize.

Tin dioxide(SnO2) nanoparticlesweresynthesizedbyaconventionalprecipitation methodusingthereactionbetweentinchloridepentahydrateandammoniasolutions. The obtainedpowderswerecalcinedatvariedtemperaturesfrom300to1050 1C, and then characterizedbyusingthermogravimetricanalysis,differentialthermalanalysisand Fourier transformationinfraredspectroscopy.Theaveragecrystallitesize,determinedby x-ray diffraction,wasfoundtobeintherangeof3.45–23.5 nm.Theanalysisexhibiteda tetragonalphase.Theactivationenergyofcrystalgrowthwascalculatedandfoundtobe 12.12kJ/mol.Themicrostructureofnanoparticleswasexaminedbyhighresolution transmission electronmicroscopy.OpticalpropertieswereinvestigatedbyaUV–vis absorptionspectrophotometer.Thecalculatedopticalbandgapliesbetween4.75–4.25eV as aresultofincreasingthecalcinationtemperaturesandcrystallitesize.

The binding of antitumor flavonoids, namely 3- hydroxyflavone (3HF) and hesperidin (Hesp) with dsDNA was investigated in the absence and presence of Cu(II) using cyclic voltammetry and square wave voltammetry at the hanging mercury drop electrode. The reduction currents of 3HF, 3HF-Cu complex, and the 3HF-β-cyclodextrin inclusion complex decreased after intercalation into dsDNA. The intercalation of Hesp into dsDNA is weak. dsDNA is reduced at a potential of −1.48 V overlaying the reduction of Hesp. In contrast, in the presence of Cu(II), the interaction of Hesp with dsDNA leads to a much stronger intercalation. The binding constants of the flavonoid-Cu complex with dsDNA were evaluated and calibration graphs for the determination of dsDNAwere obtained fromthe decrease in the peak current in the cyclic voltammograms of 3HF in the presence of dsDNA. The proposed method exhibited good recovery and reproducibility for indirect determination of dsDNA.