Nonlinear optical response of LiClK (n = 1–6) superalkali clusters.

The geometrical structures, stabilities, electronic properties and nonlinear optical response of the halogen doped bimetallic LiClK (n = 1–6) clusters were studied within the density functional theory. Based on the dissociation energy, second order energy difference and GH-L (HOMO-LUMO gap), the LiC...

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Publicado en:Zeitschrift für Naturforschung Section A: A Journal of Physical Sciences Vol. 79; no. 2; pp. 101 - 116
Autores principales: Şentürk, Şükrü, Ekincioğlu, Yavuz, Doğan, Ümit
Formato: Artículo
Publicado: De Gruyter Feb2024
Materias:
Acceso en línea:Ver este registro en EBSCOhost
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      dt: Feb2024
      vid: 79
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      pub: De Gruyter
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        175445339
        10.1515/zna-2023-0177
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      tig:
        atl: Nonlinear optical response of LiClK (n = 1–6) superalkali clusters.
      aug:
        au:
          Şentürk, Şükrü
          Ekincioğlu, Yavuz
          Doğan, Ümit
        affil:
          Department of Physics, Dumlupınar University, 43100, Kütahya, Türkiye
          Department of Opticianry, Bayburt University, 69000, Bayburt, Türkiye
      su:
        Excess electrons
        Density functional theory
        Ionization energy
        Molecular polarizability
      sug:
        subj:
          Excess electrons
          Density functional theory
          Ionization energy
          Molecular polarizability
      keyword:
        electronic structure
        nonlinear optical response
        stability
        superalkali
      ab: The geometrical structures, stabilities, electronic properties and nonlinear optical response of the halogen doped bimetallic LiClK (n = 1–6) clusters were studied within the density functional theory. Based on the dissociation energy, second order energy difference and GH-L (HOMO-LUMO gap), the LiClK (n = 2, 4, 6) clusters are more stable. According to their ionization energies, the clusters can be classified as a superalkali. From the NBO analysis, the clusters are excess electron systems. The obtained first static hyperpolarizability (β) values are in the range of 1.56 × 10 − 4.33 × 10 au while the second static hyperpolarizability vary within 2.47 × 10 au to 13.9 × 10 au for the LiClK (n = 1–6) superalkalis that are slightly higher than the nonlinear optical response of halogen doped monometallic clusters. More importantly, the LiClK is transparent in the deep UV region (λ < 300 nm) among the superalkalis indicating that the LiClK superalkali can be a candidate structure as new member of NLO materials.
      pubtype: Academic Journal
      doctype: Article
      src: R
    language: English
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          year: 2024
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