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Different changes of E F with gate voltage for different graphene layers could result in different carrier density changes with gate voltage, so are the changes of the quantum capacitance with gate voltage.
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This fact is explained by a change of the quantum-well bottom caused by the external electrical field.
The second one is that edge doping changes the symmetry of the quantum well and forbidden optical transitions for the rectangular structure become now allowed.
One is to change the size of the quantum dots, based on the quantum confinement effect.
Uniaxial strain changes the density of states and hence changes the quantum capacitance CQ of the channel which is directly proportional to the density of states.
The changes in the quantum yield of electron transport (φEo) in the grape leaves during heat stress are shown in Figure 3C.
The changes in the quantum yield of photochemical energy conversion in PSII (ΦPSII) (Fig. 8d), the quantum yield of regulated non-photochemical energy loss in PSII (NPQ) (Fig. 8e), and the quantum yield of non-regulated, non-photochemical energy loss in PSII (NO) (Fig. 8f) were quite similar in L693 and L661.
In addition, the carbon nanofibers can provide sufficient room to accommodate the huge volume changes of Cr2O3 quantum nanodots during cycling, and also enhance the electronic conductivity and ion diffusion rate as well as granting a good free-standing matrix.
The decrease in the ratio of the height to base diameter (approximately 48 nm) should result in a change in the quantum confinement of electrons and holes from a three-dimensional confinement to a quasi-one-dimensional strong confinement in the height direction.
This change increased the quantum yield of the probes in the Zn2+-free state such that they no longer exhibit a fluorescent response to Zn2+ binding.
In this paper, we intend to study the optical absorption coefficients and refractive index changes of a quantum wire with a parallelogram cross section.
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