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19 protocols using uv 1800 double beam spectrophotometer

1

Photophysical Characterization of Novel Compounds

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All samples were prepared in HPLC grade acetonitrile with varying concentrations in the order of 10−4–10−6
m. Absorption spectra were recorded at room temperature using a Shimadzu UV‐1800 double‐beam spectrophotometer. Molar absorptivity determination was verified by linear least‐squares fit of values obtained from at least four independent solutions at varying concentrations with absorbance ranging from 6.05×10−5 to 2.07×10−5
m. PMMA‐doped films were prepared by spin‐coating the samples from a solution of 2‐methoxyethanol (HPLC grade) containing 5 % (w/w) of the desired sample. Steady‐state emission and excitation spectra and time‐resolved emission spectra of both CH3CN solutions and doped films were recorded at 298 K using an Edinburgh Instruments F980 device. Solid‐state PLQY measurements of thin‐films were performed in an integrating sphere under a nitrogen purge in a Hamamatsu C9920‐02 luminescence measurement system.33 See the Supporting Information for further details.
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2

Spectrophotometric Analysis of PDI

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The PDI (40 μM) was
dissolved in 500 μL of 10 mM potassium phosphate buffer, pH
6–8. The solution was transferred to a quartz cuvette with
a 1-cm light path, and the visible wavelengths between 400 and 700
nm were recorded using a UV-1800 double-beam spectrophotometer (Shimadzu
Scientific).
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3

Comprehensive Materials Characterization

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UV-Vis absorption spectra were measured using a Shimadzu UV-1800 double beam spectrophotometer. Steady-state emission and excitation spectra and time-resolved spectra were recorded at 298 K using an Edinburgh Instruments F980. The XPS analyses were carried out with a Kratos Axis Nova spectrometer using a monochromatic Al K(alpha) source (15 mA, 14 kV). The TEM/HRTEM images were recorded using Libra 200 MC operated at 200 kV. The FTIR spectra were obtained from a Nicolet 6700 FTIR spectrometer equipped with a smart iTR diamond horizontal attenuated total reflectance (ATR).
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4

Nanoparticle Drug Encapsulation Efficiency

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A definite weight of the nanoparticles (which theoretically contains the equivalent of 10 mg of drug) was dissolved in 100 mL solution of 0.1 N HCl. After continuous shaking for 10 minutes, the solution was filtered through a 0.2-µm membrane filter. The solution was appropriately diluted and the drug concentration was measured spectrophotometrically (Shimadzu UV-1800 double beam spectrophotometer, Kyoto, Japan) at a predetermined λmax of 234 nm.45 (link)–47 The actual drug content was determined from which the drug encapsulation efficiency % (EE%) was calculated using the following equation:41 (link),44 (link),48 (link)
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\begin{document}
$${\rm{EE \% = }}{{{\rm{Actual\,drug\,content}}} \over {{\rm{Theoretical\,drug\,content}}}}{\rm{ \times 100}}$$
\end{document}
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5

Yeast-based Glucose Uptake Assay

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A glucose uptake assay was performed using yeast cells according to the method of Cirillo et al. (1963) [75 (link)]. Commercial baker’s yeast suspended in distilled water was subjected to repeated centrifugation (3000 rpm for 5 min) until a clear supernatant was obtained, and 10% (v/v) of the suspension was prepared in distilled water. Various concentrations (50, 100, 150, and 200 μg/mL) of the plant extract were added to 1 mL of glucose solution (5 mM) and incubated together for 10 min at 37 °C. The reaction was started by adding 100 μL of the yeast suspension followed by vortexing and further incubation at 37 °C for 60 min. After the incubation, the tubes were centrifuged for 5 min at 3800 rpm, and the glucose was estimated using a spectrophotometer (Shimadzu UV1800 double-beam spectrophotometer) at 520 nm. Acarbose was used as the standard drug. All experiments were carried out in triplicate. The percentage increase in the glucose uptake by the yeast cells was calculated using the following formula: Glucose uptake %=Control O.D. Sample O.D.Control O.D.×100
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6

Fluorescence Spectroscopic Characterization

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Absorption studies were performed on a Shimadzu UV 1800 double beam spectrophotometer, using 10 mm path length of quartz cuvettes. A Horiba Jobin Yvon FluoroMax - 4 spectrofluorometer was used to measure emission and excitation spectra with 5 nm in band width. The steady state fluorescence anisotropy (rss) is defined as [23] rss=IVVGIVHIVV+2GIHH where Ivv and IVH are the fluorescence intensities and the subscript indicates the vertical (V) and horizontal (H) orientation of the excitation and emission polarizer. G is the instrumental correction factor. G=IHVIHH
The time-resolved fluorescence intensity decay profiles were collected using Horiba JobinYvon TCSPC Life Time System with FluoroHub single photon counting arrangement. Nano-LED of 280 nm (slit – 4) was used as excitation source. The pulse repetition rate was set at 1 MHz. The instrument response function was collected by using scattered medium, LUDOX AS40 colloidal silica. IBH software was used for the decay analysis. Decays were fitted to get a symmetrical distribution keeping χ2 value at 0.99 ≤ χ2 ≤ 1.2. The average lifetime was determined by using the following equation [23] , τavg=i=1nτiαi where τi is the lifetime of a component having amplitude αi.
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7

Comprehensive Spectroscopic Analysis of Samples

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The UV-vis absorption spectra were recorded with a UV-1800 double beam spectrophotometer (Shimadzu, Kyoto, Japan). The fluorescence measurements were recorded with an RF-5301PC spectrofluorometer (Shimadzu, Kyoto, Japan). The circular dichroism (CD) measurements were recorded on a JASCO J-1500CD spectrophotometer. FT-IR measurements were carried out on Avatar 360 E.S.P. FT-IR spectrometer (Thermo, Montral-Est, QC, Canada)
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8

Steady-State Fluorescence Spectroscopy

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UV–visible spectrophotometric experiments were recorded on a Shimadzu UV 1800 double beam spectrophotometer, using 10 mm quartz cuvettes. A Fluoromax-4 (Horiba Jobin Yvon, Germany) spectrofluorimeter was used to record the fluorescence spectra. Excitation and emission spectra were measured with 5 nm band width. Temperature control was achieved by circulating water through the jacketed cuvette holder from a refrigerated bath (Julabo, Germany). The steady state rss is defined as [23] , rss=IVVGIVHIVV+2GIVH where IVV and IVH are the fluorescence intensities and the subscript indicates the vertical (V) and horizontal (H) orientations of the excitation and emission polarizer. G is the instrumental correction factor, G=IHVIHH
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9

Spectrophotometric Quantification of Gels

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A predetermined amount of gels (10 mg) was mixed with 10 mL of methanol using a vortex mixer, followed by filtration through Whatman filter paper. A 1 mL portion of the filtrate was diluted with 4 mL of methanol. The resulting mixture was then filtered, and the absorbance was subsequently measured at a wavelength of 280 nm using a UV spectrophotometer (Shimadzu UV-1800 Double beam Spectrophotometer, Japan) [56 (link)].
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10

Spectrophotometric Analysis using UV 1800

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A UV 1800 double-beam spectrophotometer (Shimadzu, Japan) was used. It was operated with UVProbe software, version 2.34. UV scanning was performed at 2 nm bandwidth and 2800/min speed.
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