Band blue-shift

Silver particles in the 10()A > D > 20 A size domain having their absorption bands blue shifted from the plasmon band position in the bulk metal. 

The pyrano[3,2-c]xanthen-7-one exhibits the two absorption bands associated with a heteroatom at a peri position of the benzopyran nucleus. Pyrano[2,3-a]xanthen-12-one 44, in which the fusion of the chromone ring is reversed, shows an intense single band blue-shifted some 14 nm relative to 2,2-diphenyl-2//-naphtho[l,2-6]pyran [Xmax 403, 482 nm (PhMe)]. Both isomers are readily degraded <01HCA117>. It is noteworthy that 44 could not be... 

Mn(ni)-like Q band blue shifted by 4nm compared to the native Mn(III) one. When the reductive electrolysis is stopped (curve 3), there is a complete vanishing of the band at 688 nm to the detriment of the Mn(III)-like one at 729 nm. The Q band for the native Mn(III) film is reported for comparison (dashed curve). These observations may be explained by the formation of the doubly reduced superoxo intermediate (steps 1-3) that exhibits a Q band at 688 nm, while the formulated Mn(III)-superoxide adduct exhibits a Q band at 729 nm. When molecular oxygen was added to the reduced poly[Mn(II)-32] film in a DCM solution containing benzoic anhydride, with or without stopping the reductive electrolysis, it appears that there is a total restitution of the native film within 10 min, as it can be seen in... 

Figure 1 shows 77K absorption and fluorescence spectra of PSII RC suspended in the absence (A) or presence (B) of Triton X-100 in the buffer. Addition of small quantities of detergent causes significant changes in the spectra. The amplitude of the 680 nm absorption band decreases and the 673 nm band blue shifts to 670 nm (a small absorption shoulder at about 680 nm is also observed in PSII RC at 293K). The fluorescence intensity increases when Triton is added (fluorescence spectra are normalized in Fig. 1), and the main peak at 686 nm blue-shifts to 684 nm and broadens. Furthermore, the shoulder at 692 nm (not due to CP47 contamination) disappears. The CD spectra (Fig 1C) do not change qualitatively however, the amplitude of the 682 nm CD peak was... 

The robustness of the rhenium(i) diimine alkynyl systems and rich photophysical behavior have rendered them suitable as metalloligands for the synthesis of mixed-metal complexes. It is well-known that organometallic alkynes exhibit rich coordination chemistry with Cu(i), Ag(i) and Au(i) [214-218], however, photophysical properties of these r-coordinated compounds are rare. Recent work by Yam and coworkers has shown that luminescent mixed-metal alkynyl complexes could be synthesized by the metalloligand approach using the rhenium(i) diimine alkynyl complexes as the z -ligand. Reaction of the rhenium(i) diimine alkynyl complex [Re(bpy)(CO)3C=CPh] with [M(MeCN)4]PF6 in THF at room temperature in an inert atmosphere afforded mixed-metal Re(i)-Cu(i) or -Ag(i) alkynyl complexes (Scheme 10.31) [89]. Their photophysical properties have also been studied. These luminescent mixed-metal complexes were found to emit from their MLCT[d7i(Re) —> 7i (N N)] manifolds with emission bands blue-shifted relative to their mononuclear precursors (Table 10.5). This has been attributed to the stabilization of the dTi(Re) orbital as a consequence of the weaker t-donating ability of the alkynyl unit upon coordination to the d metal centers. 

Solvent Influence. Solvent nature has been found to influence absorption spectra, but fluorescence is substantiaHy less sensitive (9,58). Sensitivity to solvent media is one of the main characteristics of unsymmetrical dyes, especiaHy the merocyanines (59). Some dyes manifest positive solvatochromic effects (60) the band maximum is bathochromicaHy shifted as solvent polarity increases. Other dyes, eg, highly unsymmetrical ones, exhibit negative solvatochromicity, and the absorption band is blue-shifted on passing from nonpolar to highly polar solvent (59). In addition, solvents can lead to changes in intensity and shape of spectral bands (58). 

There have been very few examples of PTV derivatives substituted at the vinylene position. One example poly(2,5-thienylene-1,2-dimethoxy-ethenylene) 102 has been documented by Geise and co-workers and its synthesis is outlined in Scheme 1-32 [133]. Thiophene-2,5-dicarboxaldehyde 99 is polymerized using a benzoin condensation the polyacyloin precursor 100 was treated with base to obtain polydianion 101. Subsequent treatment with dimethyl sulfate affords 102, which is soluble in solvents such as chloroform, methanol, and DMF. The molar mass of the polymer obtained is rather low (M = 1010) and its band gap ( ,.=2.13 eV) is substantially blue-shifted relative to PTV itself. Despite the low effective conjugation, the material is reasonably conductive when doped with l2 (cr=0.4 S cm 1). 

Using a variety of transient and CW spectroscopies spanning the time domains from ps to ms, we have identified the dominant intrachain photoexcitations in C )-doped PPV films. These are spin-correlated polaron pairs, which are formed within picoseconds following exciton diffusion and subsequent dissociation at photoinduced PPV+/Cw> defect centers. We found that the higher-energy PA band of polaron pairs is blue-shifted by about 0.4 eV compared to that of isolated polarons in PPV. 

We have reported a simple, green, bench top, economical and environmentally benign room temperature synthesis of MSe (M=Cd or Zn) nanoparticles using starch, PVA and PVP as passivating agents. The whole process is a redox reaction with selenium acting as the oxidant and MSe as the reduction product. An entire "green" chemistry was explored in this synthetic procedure and it is reproducible. The optical spectroscopy showed that all the particles are blue shifted from the bulk band gap clearly due to quantum confinement. Starch capped CdSe nanoparticles showed the presence of monodispersed spherical... 

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