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A sharp absorption edge located at 320 nm can be observed for FTO glass.
The extended conformation gives rise to a sharp absorption band at 338 nm.
Since the PFs polymers show a sharp absorption peak λmax ~ 385 390 nm of the π π* electronic transition [18].
A sharp absorption band at 275, 277 and 280 nm is observed, respectively, for samples a, b and c.
A sharp absorption band at 280, 283, and 288 nm is observed for samples a, b, and c, respectively.
A sharp absorption band at 276 and 272 nm is observed respectively for samples a and b.
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This phenomenon gives rise in the simplest case to a paramagnetic-resonance absorption spectrum consisting of a single sharp absorption line.
The EPR spectra of the ancient samples showed a characteristic sharp absorption centered at g =2.0037 without a hyperfine structure, and have been identified as those of carbon radicals.
The EPR spectra of 40hTH applied with SOD solution at various experimental conditions were shown in Figure 2. The EPR spectra of the samples showed a characteristic sharp absorption centered at g =2.0037 without a hyperfine structure, and have been identified as those of carbon radicals [3].
In the IR spectrum of TNCB, corresponding to the stretching vibrational mode of C Cl bond, a strong sharp absorption band is noticed at ~718 cm−1, which is absent in the carbon bonded anionic sigma complexes 1 to 3 clearly denotes that there is removal of chlorine atom during the formation of them.
A relatively sharp absorption around 405 nm was observed just after excitation, which nearly disappeared within 100 fs, and was replaced by a broad absorption with a maximum at 460 nm.
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