2017
DOI: 10.1016/j.electacta.2017.05.051
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SPR effect of AgNPs decorated TiO 2 in DSSC using TPMPI in the electrolyte: Approach towards low light trapping

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Cited by 21 publications
(4 citation statements)
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“…[ 56 ] The τ 1 and τ 2 are generally used to further evaluate the electron transition efficiency in DSSCs. [ 57 ] One computed τ 1 and τ 2 via these formulas [ 58 ] τ1badbreak=1.499fabse12$$\begin{equation}{\tau }_1 = \frac{{1.499}}{{{f}_{{\rm{abs}}}e_1^2}}\end{equation}$$ τ2badbreak=2πε0meh2c3e4E2f$$\begin{equation}{\tau }_2 = \frac{{2\pi {\varepsilon }_0{m}_{\rm{e}}{h}^2{c}^3}}{{{e}^4{E}^2f}}\end{equation}$$where f abs represents the excited‐state oscillator strength and e 1 depicts the excitation energy; e , m e , ɛ 0 , and h represent the elementary charge, electronic quality, vacuum dielectric coefficient, and Planck constant, respectively; E and f represent the emitted energy and oscillator strength, and c is the light speed. The corresponding data are indicated in Table 3 , and the values of τ 2 are in the following order: HJL‐1 (4.392 ns) > HJL‐3 (4.157 ns) > HJL‐2 (3.758 ns); thus, HJL‐1 and HJL‐3 have higher fluorescence efficiency.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…[ 56 ] The τ 1 and τ 2 are generally used to further evaluate the electron transition efficiency in DSSCs. [ 57 ] One computed τ 1 and τ 2 via these formulas [ 58 ] τ1badbreak=1.499fabse12$$\begin{equation}{\tau }_1 = \frac{{1.499}}{{{f}_{{\rm{abs}}}e_1^2}}\end{equation}$$ τ2badbreak=2πε0meh2c3e4E2f$$\begin{equation}{\tau }_2 = \frac{{2\pi {\varepsilon }_0{m}_{\rm{e}}{h}^2{c}^3}}{{{e}^4{E}^2f}}\end{equation}$$where f abs represents the excited‐state oscillator strength and e 1 depicts the excitation energy; e , m e , ɛ 0 , and h represent the elementary charge, electronic quality, vacuum dielectric coefficient, and Planck constant, respectively; E and f represent the emitted energy and oscillator strength, and c is the light speed. The corresponding data are indicated in Table 3 , and the values of τ 2 are in the following order: HJL‐1 (4.392 ns) > HJL‐3 (4.157 ns) > HJL‐2 (3.758 ns); thus, HJL‐1 and HJL‐3 have higher fluorescence efficiency.…”
Section: Resultsmentioning
confidence: 99%
“…[56] The 𝜏 1 and 𝜏 2 are generally used to further evaluate the electron transition efficiency in DSSCs. [57] One computed 𝜏 1 and 𝜏 2 via these formulas [58] 𝜏 1 = 1.499…”
Section: The Properties Of Absorption and Fluorescencementioning
confidence: 99%
“…Silver (Ag) is an exquisite metal that can be catalytic, nontoxic, and cost-effective and that possesses good thermal and electrical conductivity. In addition, doping Ag is one of the methods for enhancing its chemical and electrical properties and is often used to enhance DSSC performance [26][27][28][29]. In this investigation, a TiO 2 -film-making experiment was conducted in which TiO 2 that was immersed into dye DN-F05 mixed with Ag.…”
Section: Preparation and Manufacture Of Tio2 Pastementioning
confidence: 99%
“…In conclusion, the R 1 and R 2 are the interface impedances that represent the photo-generated electron degree of difficulty to recombine with the holes in the electrolyte. The suppression of electron recombination greatly reduces the electronic loss of DSSC [8,37], and this was the reason for the increase in fill factor, and thus the photovoltaic efficiency can be enhanced [38]. The highest efficiency is observed under an intensity of 30 mW/cm 2 .…”
Section: Performance Of the Dssc Under Different Illuminationsmentioning
confidence: 99%