<p>Broadband oxide-based photodetectors have attracted considerable attention owing to their stability, low cost, and potential for optoelectronic applications. In this work, a SnO<InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>/Co<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>4</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>/Si n-p-n heterojunction photodetector was fabricated using chemically synthesized Co<InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>4</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> and SnO<InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> nanostructures. The novelty of this work lies in the development of a SnO<InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>/Co<InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>4</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>/Si n-p-n heterojunction that combines n-type SnO<InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> and p-type Co<InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>4</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> to promote efficient carrier separation and broadband visible-infrared photodetection. The X-ray diffraction patterns confirmed that the Co<InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>4</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> nanoparticles possessed a cubic spinel structure, whereas SnO<InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> exhibited a tetragonal crystal system, with crystallite sizes of 29 and 27 nm, respectively. SEM observations revealed rod-like Co<InlineEquation ID="IEq22"> <EquationSource Format="TEX">\(_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq23"> <EquationSource Format="TEX">\(_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>4</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> agglomerates together with uniformly distributed SnO<InlineEquation ID="IEq24"> <EquationSource Format="TEX">\(_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> nanoparticles, confirming the successful formation of the oxide layers. UV–Vis spectroscopy revealed optical band gaps of 2.70 and 3.75 eV for Co<InlineEquation ID="IEq25"> <EquationSource Format="TEX">\(_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq26"> <EquationSource Format="TEX">\(_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>4</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> and SnO<InlineEquation ID="IEq27"> <EquationSource Format="TEX">\(_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>, respectively, which are larger than those of the corresponding bulk materials, confirming successful nanostructure formation. FTIR spectra showed O-H, C=O, and C-H bands in addition to the characteristic Co-O/O-Co-O and Sn-O-Sn vibrational modes. The current–voltage (I-V) characteristics of the SnO<InlineEquation ID="IEq28"> <EquationSource Format="TEX">\(_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>/Co<InlineEquation ID="IEq29"> <EquationSource Format="TEX">\(_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq30"> <EquationSource Format="TEX">\(_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>4</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>/Si heterojunction were evaluated under dark and illuminated conditions in both forward and reverse bias. The fabricated photodetector exhibited responsivities of 0.27 and 0.56 A/W in the visible and infrared regions, respectively. The external quantum efficiency and specific detectivity followed the same trend as the spectral responsivity, reaching 75.62% and 3.92 10<InlineEquation ID="IEq31"> <EquationSource Format="TEX">\(^{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>12</mn> </mmultiscripts> </math></EquationSource> </InlineEquation> Jones at 450 nm, respectively. At longer wavelengths, enhanced absorption in the silicon substrate increased these values to 82.06% and 8.04 <InlineEquation ID="IEq32"> <EquationSource Format="TEX">\(\times \)</EquationSource> <EquationSource Format="MATHML"><math> <mo>×</mo> </math></EquationSource> </InlineEquation> 10<InlineEquation ID="IEq33"> <EquationSource Format="TEX">\(^{12}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>12</mn> </mmultiscripts> </math></EquationSource> </InlineEquation> Jones, respectively, at 850 nm. The enhanced photodetection performance is attributed to the effective SnO<InlineEquation ID="IEq34"> <EquationSource Format="TEX">\(_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>/Co<InlineEquation ID="IEq35"> <EquationSource Format="TEX">\(_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq36"> <EquationSource Format="TEX">\(_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>4</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> heterointerface, which promotes carrier separation and transport. These findings demonstrate that the proposed SnO<InlineEquation ID="IEq37"> <EquationSource Format="TEX">\(_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>/Co<InlineEquation ID="IEq38"> <EquationSource Format="TEX">\(_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq39"> <EquationSource Format="TEX">\(_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>4</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>/Si heterojunction is a promising candidate for broadband visible-infrared optoelectronic applications.</p>

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Fabrication of photodetector (SnO\(_{2}\)/Co\(_{3}\)O\(_{4}\)/Si) for Vis-IR detection by chemical method

  • Rawaa Yaseen Taha,
  • Wedian K. Abad,
  • Mohammed Jassim Mohammed Ali,
  • Ahmed N. Abd

摘要

Broadband oxide-based photodetectors have attracted considerable attention owing to their stability, low cost, and potential for optoelectronic applications. In this work, a SnO \(_{2}\) 2 /Co \(_{3}\) 3 O \(_{4}\) 4 /Si n-p-n heterojunction photodetector was fabricated using chemically synthesized Co \(_{3}\) 3 O \(_{4}\) 4 and SnO \(_{2}\) 2 nanostructures. The novelty of this work lies in the development of a SnO \(_{2}\) 2 /Co \(_{3}\) 3 O \(_{4}\) 4 /Si n-p-n heterojunction that combines n-type SnO \(_{2}\) 2 and p-type Co \(_{3}\) 3 O \(_{4}\) 4 to promote efficient carrier separation and broadband visible-infrared photodetection. The X-ray diffraction patterns confirmed that the Co \(_{3}\) 3 O \(_{4}\) 4 nanoparticles possessed a cubic spinel structure, whereas SnO \(_{2}\) 2 exhibited a tetragonal crystal system, with crystallite sizes of 29 and 27 nm, respectively. SEM observations revealed rod-like Co \(_{3}\) 3 O \(_{4}\) 4 agglomerates together with uniformly distributed SnO \(_{2}\) 2 nanoparticles, confirming the successful formation of the oxide layers. UV–Vis spectroscopy revealed optical band gaps of 2.70 and 3.75 eV for Co \(_{3}\) 3 O \(_{4}\) 4 and SnO \(_{2}\) 2 , respectively, which are larger than those of the corresponding bulk materials, confirming successful nanostructure formation. FTIR spectra showed O-H, C=O, and C-H bands in addition to the characteristic Co-O/O-Co-O and Sn-O-Sn vibrational modes. The current–voltage (I-V) characteristics of the SnO \(_{2}\) 2 /Co \(_{3}\) 3 O \(_{4}\) 4 /Si heterojunction were evaluated under dark and illuminated conditions in both forward and reverse bias. The fabricated photodetector exhibited responsivities of 0.27 and 0.56 A/W in the visible and infrared regions, respectively. The external quantum efficiency and specific detectivity followed the same trend as the spectral responsivity, reaching 75.62% and 3.92 10 \(^{12}\) 12 Jones at 450 nm, respectively. At longer wavelengths, enhanced absorption in the silicon substrate increased these values to 82.06% and 8.04 \(\times \) × 10 \(^{12}\) 12 Jones, respectively, at 850 nm. The enhanced photodetection performance is attributed to the effective SnO \(_{2}\) 2 /Co \(_{3}\) 3 O \(_{4}\) 4 heterointerface, which promotes carrier separation and transport. These findings demonstrate that the proposed SnO \(_{2}\) 2 /Co \(_{3}\) 3 O \(_{4}\) 4 /Si heterojunction is a promising candidate for broadband visible-infrared optoelectronic applications.