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Irradiance gain

A schematic presentation of an optical concentrator is given in Fig. 2.3. The shape of the system can be arbitrary, as well as its mechanism of focusing. The important factor of the system is its concentration ratio, defined as a ratio between the input (collector) area and the exit area. In an ideal concentration system, this ratio should be equal to the ratio of incident optical flux to the exit flux. In a real system, possible absorption losses (for instance in metal parts) will have to be deducted. Thus the concentration ratio of a light concentrator can be defined either as the geometric concentration ratio C, the ratio of the entry aperture area (AcoUector) to the exit aperture area (Aexit), or as the irradiance gain C the ratio of the irra-diance on the collector (fr ) to that on the entry aperture (Ir ). The two concentration terms are related by the fraction of total incident power entering the module that reaches the concentrator exit aperture. [Pg.47]

Disadvantages. The magic angle must be extremely stable and accurately set. The spiiming speed must show good stability over the duration of the experiment. The probe needs to be accurately tuned and careful correction for irradiation and detection variations with frequency, and baseline effects are necessary. The gain... [Pg.1485]

One of the first applications of this technique was to the enrichment of and "B isotopes, present as 18.7 and 81.3 per cent, respectively, in natural abundance. Boron trichloride, BCI3, dissociates when irradiated with a pulsed CO2 laser in the 3g vibrational band at 958 cm (vj is an e vibration of the planar, D j, molecule). One of the products of dissociation was detected by reaction with O2 to form BO which then produced chemiluminescence (emission of radiation as a result of energy gained by chemical reaction) in the visible region due to A U — fluorescence. Irradiation in the 3g band of BCls or "BCI3 resulted in °BO or BO chemiluminescence. The fluorescence of °BO is easily resolved from that of "BO. [Pg.376]

Although photochemical cycloadditions have gained acceptance in synthetic chemistry, most such reactions are limited to a relatively small scale. The use of a 1000-watt street lamp permits the irradiation of up to 1 mol of substrate in less time than 0.2 mol can be irradiated with the conventional 450-watt lamps. Thus, under optimum conditions, the submitters were able to add ethylene to 3-methylcyclohexenone on a 20-g scale in 48 hr (801) with a 450-watt lamp with the apparatus described here 94 g of this enone was condensed with ethylene in 8 hr (91%). [Pg.122]

Among the various radiation-induced modifications, the EB-processing of polymers has gained special importance as it requires less energy, is simple, fast, and versatile in application. The overall properties of EB-irradiated polymeric materials are also improved compared to those induced by other ionizing radiation. [Pg.906]

The cycloreversion experiments showed a clean Tf=T-DNA to T/T-DNA transformation. No by-products were detected, which supports the idea that DNA may be more stable towards reduction compared to oxidation. Even heating the irradiated DNA with piperidine furnished no other DNA strands other then the repaired strands, showing that base labile sites - indicative for DNA damage - are not formed in the reductive regime. The quantum yield of the intra-DNA repair reaction was therefore calculated based on the assumption that the irradiation of the flavin-Tf=T-DNA strands induces a clean intramolecular excess electron transfer driven cycloreversion. The quantum yield was found to be around 0=0.005, which is high for a photoreaction in DNA. A first insight into how DNA is able to mediate the excess electron transfer was gained with the double strands 11 and 12 in which an additional A T base pair compared to 7 and 8 separates the dimer and the flavin unit. [Pg.207]

Theory tells us that the maximum gain in proton signal intensity is 50%, but normally we are dealing with changes of only a few per cent, and the magnitude of these is dependent on the distance between the irradiated proton(s) and the observed ones the effect is too small to be visible when this distance exceeds about 5 A. [Pg.17]

Spectroscopic evidence (44,45) has been adduced for the formation of electron-gain centres upon y-irradiation of the binuclear carbonyls Mn2(C0)lo and Re2(C0)lo. A study (45) of a single crystal of irradiated Mn2(CO)10 has shown that the radical anion contains two equivalent 55Mn nuclei whose hyperfine tensors lie 118 apart. This has led to the suggestion that the anion radical contains a bridging CO and that its correct formulation is Mn2(C0)9 . The observation of a bridged Mn2(C0)9 species in u.v.-photolyzed material lends some support to this hypothesis (46). [Pg.184]

To ensure complete conversion for all examples of a 21-member library, irradiation times of 30-60 min were used (Scheme 7.39), employing a multi-vessel rotor system for parallel microwave-assisted synthesis (see Fig. 3.7). The results were confirmed by on-bead FTIR analysis, accurate weight-gain measurements of washed and dried resins, and post-cleavage analysis of the prepared enones. [Pg.323]

Fig. 9.17o). Ions in both these levels are further excited by an ESA mechanism to gain energy from the irradiating 785-nm radiation. Those in the 4In/2 energy level are excited to the 4F3 /2, 5/2 doublet ... [Pg.422]

The gratings can also be made in situ by holographic irradiation as was demonstrated for low molecular stilbenes in a polystyrene matrix [197]. Here, the spatial modulation of gain dominates over the refractive index modulation in its contribution to optical feedback. The principles of holographic irradiation will be described in Section VIII, which discusses photosensitive materials. [Pg.140]

One of the exciting areas that has gained importance over the recent decade is the photochemical cyclization of non-conjugated dienes in the presence of species that can act as templates. One such species that has been used is copper(I) salts. The earliest example of the use of copper salts in the intramolecular photocycloaddition of non-conjugated dienes is that described for cycloocta-1,5-diene. When this is irradiated in the presence... [Pg.270]


See other pages where Irradiance gain is mentioned: [Pg.506]    [Pg.1443]    [Pg.291]    [Pg.318]    [Pg.51]    [Pg.254]    [Pg.913]    [Pg.153]    [Pg.79]    [Pg.188]    [Pg.281]    [Pg.913]    [Pg.184]    [Pg.429]    [Pg.13]    [Pg.149]    [Pg.110]    [Pg.110]    [Pg.173]    [Pg.174]    [Pg.370]    [Pg.180]    [Pg.184]    [Pg.363]    [Pg.38]    [Pg.372]    [Pg.249]    [Pg.110]    [Pg.172]    [Pg.18]    [Pg.138]    [Pg.568]    [Pg.88]    [Pg.530]    [Pg.39]    [Pg.135]    [Pg.231]    [Pg.132]   
See also in sourсe #XX -- [ Pg.47 ]




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