Continuous solid solutions were isolated within the system A
ICd
1-xM
IxPO
4(A
I=Li, Na; M
II=Mn, Co) for 0≤x≤1. The steady decrease of the lattice parameters and unit cell volume within the solid solution domains was ascribed to the substitution of Cd
2+ cations by smaller size M
2+ ions (M=Mn, Co) as the composition progresses between x=0 and x=1. The investigation of the luminescence of Mn(II) has evidenced two large emission bands peaking at circa 576-580nm and 693-710nm for the analyzed compounds LiCd
1-xMn
xPO
4(0≤x≤0.7) under the excitation radiation with λ
exc=438nm. In this system, a small red shift seems to appear for both emission bands when a higher excitation energy is used (λ
exc=325nm). In the case of LiZn
1-xMn
xPO
4(0≤x≤0.2), only one luminescence band was recorded within a narrower range 550-556nm for λ
exc=488nm and at ca. 562nm under λ
exc=325nm. For the composition analysed in the system NaCd
1-xMn
xPO
4(x=0.05), the emission bands were found at 624.5nm and 616.4nm under excitation wavelengths equal to 488 and 325nm respectively. The luminescence of Mn
2+ ions in all investigated phases was attributed to the same electronic transition
4T
1g(
4G)
6A
1g(
6S) which is very sensitive to the crystal filed strength as evidenced by Tanabe-Sugano energy diagram. Indeed as the solid solution progresses in the case of LiCd
1-xMn
xPO
4 for example (0≤x≤1), the size of the cavities hosting Mn
2+ ions is consequently changing. As a matter of fact, the mean manganese-oxygen distance is expected to vary between the values corresponding to the mean bond length of the divalent cation in LiCdPO
4(<Cd-0>=2.298Å) and LiMnPO
4(<Mn-O>=2.201Å) respectively. The resulting change of the crystal field around Mn(II) may explain why the emission is observed in the green region for low values of x while it shifts to the red domain for compositions close to LiMnPO
4(x>0.5). The correlation between the modification of the wavelength of Mn
2+ luminescence bands and the crystal field strength inherent to the variation of the chemical composition is therefore established. A model for the distribution of the divalent cations within the lattice along the solid solutions was also proposed.
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