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The third transition X* is attributed to generic charged exciton, as it does not show polarisation dependence due to the lack of exchange interaction [29].
Open image in new window Figure 2 The DWR per unit length versus DW width for different values of exchange interaction strength.
Therefore, the magnification of exchange interaction between μ6-C and (μ2-S 3in the complex [Re12CS17 CN 6]8−should result in its ionization and reduction in the distances between {Re6} subunits.
Exciton (X) and biexciton (XX) transitions are clearly identified as each of them is comprised of two linearly polarised and energetically distant components - the result of exchange interaction between electron and hole in a low rotational symmetry QD.
Differentiating W e by s, we find the force of exchange interaction of VBL per unit length: {F}_e=frac{16 A}{varLambda sqrt{Q}} exp left(- s/varLambda right).
Borders are divisive, but borders also unite us -- they are points of exchange, interaction and creativity.
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The nature and magnitude of exchange interactions are further corroborated by density functional calculations.
A theoretical framework based on modified Brillouin function which considers the effects of exchange interactions, ferromagnetic domains, elastic dipoles, dispersed particles, and defect within the sample was elaborated.
Almost identical values of dTCA/dP = +4.7 ÷ +5.9 K GPa−1 point to a normalized steepness of a dependence of exchange interactions on interatomic distances.
The appearance of the α-Fe2O3 phases will induce the additional unidirectional anisotropy energy due to the existence of exchange interactions between Fe core and α-Fe2O3 shell at the interface, and thus, the coercivity increases significantly than that of the pure Fe due to the spin drag effect for the unpinned uncompensated spin at the interface [30].
At the same time, averaging of exchange interactions over such a fine grain size, which is much lower than the characteristic exchange length for Co (≈25 45 nm), precludes the display of local magnetocrystalline easy axes, thereby leading to low switching fields.
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