<p>Designing photonic devices that can manipulate and process light without altering the fabrication process is a longstanding challenge and crucial for many practical photonics applications. In particular, the reconfigurable photonic crystal (PhC) consists of a periodic array of dielectric, which adds additional freedom to tune the flow of light by strongly confining the light field. Herein, we numerically design and optimize a one-dimensional defect photonic crystal (1-D DPhC) and demonstrate a tunable absorption in the visible wavelength. The <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\hbox {Sb}_2\hbox {S}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Sb</mtext> <mn>2</mn> </msub> <msub> <mtext>S</mtext> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>, a wide-band gap phase change material, is employed as a defect layer to tune the photonic bandgap and defect mode optical properties. A maximum change in absorption of 31% is achieved at 626&#xa0;nm when the 10&#xa0;nm <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\hbox {Sb}_2\hbox {S}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Sb</mtext> <mn>2</mn> </msub> <msub> <mtext>S</mtext> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> defect layer switches its structure from an amorphous to a crystalline state in the PhC, corresponding to a resonance with a <i>Q</i>-factor of approximately 12,518. Moreover, the defect mode absorption exhibits a pronounced redshift of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\Delta \lambda = 150\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Δ</mi> <mi>λ</mi> <mo>=</mo> <mn>150</mn> </mrow> </math></EquationSource> </InlineEquation>&#xa0;nm from the visible to the near-infrared region as the defect layer thickness increases from 5 to 70&#xa0;nm, highlighting the potential for tuning photonic responses across a broad spectral range. The optimized <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\hbox {Sb}_2\hbox {S}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Sb</mtext> <mn>2</mn> </msub> <msub> <mtext>S</mtext> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>-based 1-D DPhC structure is polarization-independent and shows a blue shift of <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\Delta \lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Δ</mi> <mi>λ</mi> </mrow> </math></EquationSource> </InlineEquation> = 75 nm in an angle rotation of <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(60^\circ \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mn>60</mn> <mo>∘</mo> </msup> </math></EquationSource> </InlineEquation>. The temperature-dependent optical properties of <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\hbox {Sb}_2\hbox {S}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Sb</mtext> <mn>2</mn> </msub> <msub> <mtext>S</mtext> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> during its amorphous-to-crystalline phase transition reveal a strong correlation between refractive index changes and enhanced absorption, demonstrating the robustness and adaptability of this PhC design for applications in tunable in-chip optical devices.</p>

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Defect-engineered \(\hbox {Sb}_2\hbox {S}_3\) Layer in one-dimensional photonic crystals for wavelength-tunable absorption

  • Anas Ittepadan,
  • Jitendra Kumar Behera,
  • Chittaranjan Nayak

摘要

Designing photonic devices that can manipulate and process light without altering the fabrication process is a longstanding challenge and crucial for many practical photonics applications. In particular, the reconfigurable photonic crystal (PhC) consists of a periodic array of dielectric, which adds additional freedom to tune the flow of light by strongly confining the light field. Herein, we numerically design and optimize a one-dimensional defect photonic crystal (1-D DPhC) and demonstrate a tunable absorption in the visible wavelength. The \(\hbox {Sb}_2\hbox {S}_3\) Sb 2 S 3 , a wide-band gap phase change material, is employed as a defect layer to tune the photonic bandgap and defect mode optical properties. A maximum change in absorption of 31% is achieved at 626 nm when the 10 nm \(\hbox {Sb}_2\hbox {S}_3\) Sb 2 S 3 defect layer switches its structure from an amorphous to a crystalline state in the PhC, corresponding to a resonance with a Q-factor of approximately 12,518. Moreover, the defect mode absorption exhibits a pronounced redshift of \(\Delta \lambda = 150\) Δ λ = 150  nm from the visible to the near-infrared region as the defect layer thickness increases from 5 to 70 nm, highlighting the potential for tuning photonic responses across a broad spectral range. The optimized \(\hbox {Sb}_2\hbox {S}_3\) Sb 2 S 3 -based 1-D DPhC structure is polarization-independent and shows a blue shift of \(\Delta \lambda \) Δ λ = 75 nm in an angle rotation of \(60^\circ \) 60 . The temperature-dependent optical properties of \(\hbox {Sb}_2\hbox {S}_3\) Sb 2 S 3 during its amorphous-to-crystalline phase transition reveal a strong correlation between refractive index changes and enhanced absorption, demonstrating the robustness and adaptability of this PhC design for applications in tunable in-chip optical devices.