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dc.contributor.authorZanatta, Geancarlopt_BR
dc.contributor.authorGottfried, Carmem Juracy Silveirapt_BR
dc.contributor.authorSilva, Agmael Mendonçapt_BR
dc.contributor.authorCaetano, Ewerton Wagner Santospt_BR
dc.contributor.authorSales, Francisco Adilson Matospt_BR
dc.contributor.authorFreire, Valder Nogueirapt_BR
dc.date.accessioned2018-06-05T02:29:00Zpt_BR
dc.date.issued2014pt_BR
dc.identifier.issn0021-9606pt_BR
dc.identifier.urihttp://hdl.handle.net/10183/179089pt_BR
dc.description.abstractResults of optical absorption measurements are presented together with calculated structural, electronic, and optical properties for the anhydrous monoclinic L-asparagine crystal. Density functional theory (DFT) within the generalized gradient approximation (GGA) including dispersion effects (TS, Grimme) was employed to perform the calculations. The optical absorption measurements revealed that the anhydrous monoclinic L-asparagine crystal is a wide band gap material with 4.95 eV main gap energy. DFT-GGA+TS simulations, on the other hand, produced structural parameters in very good agreement with X-ray data. The lattice parameter differences a, b, c between theory and experiment were as small as 0.020, 0.051, and 0.022 Å, respectively. The calculated band gap energy is smaller than the experimental data by about 15%, with a 4.23 eV indirect band gap corresponding to Z→ and Z→β transitions. Three other indirect band gaps of 4.30 eV, 4.32 eV, and 4.36 eV are assigned to α3→ , α1→ , and α2→ transitions, respectively. -sol computations, on the other hand, predict a main band gap of 5.00 eV, just 50 meV above the experimental value. Electronic wavefunctions mainly originating from O 2p–carboxyl, C 2p–side chain, and C 2p–carboxyl orbitals contribute most significantly to the highest valence and lowest conduction energy bands, respectively. By varying the lattice parameters from their converged equilibrium values, we show that the unit cell is less stiff along the b direction than for the a and c directions. Effective mass calculations suggest that hole transport behavior is more anisotropic than electron transport, but the mass values allow for some charge mobility except along a direction perpendicular to the molecular layers of L-asparagine which form the crystal, so anhydrous monoclinic L-asparagine crystals could behave as wide gap semiconductors. Finally, the calculations point to a high degree oen
dc.format.mimetypeapplication/pdfpt_BR
dc.language.isoengpt_BR
dc.relation.ispartofThe journal of chemical physics. Lancaster. Vol. 140, no. 12 (Mar. 2014), 124511, [15 p.]pt_BR
dc.rightsOpen Accessen
dc.subjectÁcido aspárticopt_BR
dc.subjectAsparaginapt_BR
dc.titleL-Asparagine crystals with wide gap semiconductor features : optical absorption measurements and density functional theory computationspt_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb001068178pt_BR
dc.type.originEstrangeiropt_BR


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