2012
DOI: 10.1063/1.3684548
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Deep ultraviolet and visible crystalloluminescence of sodium chloride

Abstract: A protocol has been developed for production of intense crystalloluminescence (XTL) from sodium chloride in aqueous solution by selective doping with transition metal salts (Ag(+), Cu(2+), and Dy(3+)). The method was used to record complete, fully dispersed deep UV-visible (200-650 nm) XTL spectra of sodium chloride for the first time. The results show conclusively that the emissions are due to dopant cations in the NaCl lattice, with no evidence for emission directly from NaCl, e.g., by triboluminescence resu… Show more

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Cited by 14 publications
(16 citation statements)
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References 34 publications
(60 reference statements)
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“…The free monomer ions are in a very different electric environment than those in metastable clusters or the crystal, indicating a gradual coordination transformation from fully hydrated free monomer ions, to partially hydrated metastable clusters, and then to the fully dehydrated crystal. The Cl − ion average potential increases almost linearly from free ions → clusters → bulk crystal, with a difference in an average potential of ⟨V(Cl − )⟩ 4 3 − ⟨V(Cl − )⟩ free ion = + 240 mV = +5.52 kcal/mol. In contrast, the Na + ion average potential decreases starting from the free ions to the clusters; however, it must reach a minimum and then increase to reach the bulk crystal limit, with a difference in an average potential of ⟨V(Na + )⟩ 4 3 − ⟨V(Na + )⟩ free ion = − 110 mV = −2.53 kcal/mol.…”
Section: ■ Resultsmentioning
confidence: 99%
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“…The free monomer ions are in a very different electric environment than those in metastable clusters or the crystal, indicating a gradual coordination transformation from fully hydrated free monomer ions, to partially hydrated metastable clusters, and then to the fully dehydrated crystal. The Cl − ion average potential increases almost linearly from free ions → clusters → bulk crystal, with a difference in an average potential of ⟨V(Cl − )⟩ 4 3 − ⟨V(Cl − )⟩ free ion = + 240 mV = +5.52 kcal/mol. In contrast, the Na + ion average potential decreases starting from the free ions to the clusters; however, it must reach a minimum and then increase to reach the bulk crystal limit, with a difference in an average potential of ⟨V(Na + )⟩ 4 3 − ⟨V(Na + )⟩ free ion = − 110 mV = −2.53 kcal/mol.…”
Section: ■ Resultsmentioning
confidence: 99%
“…The Cl − ion average potential increases almost linearly from free ions → clusters → bulk crystal, with a difference in an average potential of ⟨V(Cl − )⟩ 4 3 − ⟨V(Cl − )⟩ free ion = + 240 mV = +5.52 kcal/mol. In contrast, the Na + ion average potential decreases starting from the free ions to the clusters; however, it must reach a minimum and then increase to reach the bulk crystal limit, with a difference in an average potential of ⟨V(Na + )⟩ 4 3 − ⟨V(Na + )⟩ free ion = − 110 mV = −2.53 kcal/mol. For comparison, we also show the average interior ion potentials for the bulk crystal to indicate how much the ions' potentials change between the free ions, metastable clusters, and when they are within the interior of a bulk crystal.…”
Section: ■ Resultsmentioning
confidence: 99%
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“…Similarly, the crushing of such ordinary materials such as white crystalline sugar will induce flashes of luminescence [ 11 , 12 ], because bonds are disrupted and the energy is partially dissipated as light. That chemical bonds play important roles in the luminescent properties of certain solids is further exemplified by the fact that photons may equally be produced during crystallization processes [ 13 , 14 ] in which atoms take their place at certain positions in the crystal lattice and bonds are formed. This form of luminescence is aptly called crystalloluminescence.…”
Section: Introductionmentioning
confidence: 99%