Spectrofluorometric studies. III. Ortho- and para-difluorobenzene

1968 ◽  
Vol 46 (20) ◽  
pp. 3177-3182 ◽  
Author(s):  
J. L. Durham ◽  
G. P. Semeluk ◽  
I. Unger

Spectrofluorometric techniques have been used to determine gas phase singlet and triplet yields in ortho- and para-difluorobenzene as a function of exciting wavelength and pressure. The importance of the "around the corner effect" in such measurements as the cause of large errors is briefly discussed.In the case of ortho-difluorobenzene, maxima in fluorescent yield are produced by the exciting wavelengths 2490, 2580, and 2700 Å; minima at 2540 and 2660 Å. Triplet yields, using the sensitized biacetyl emission technique, have been determined at 2500, 2580, 2660, and 2700 Å. The sums of the singlet and triplet yields at these wavelengths are 0.34, 0.52, 0.75, and 0.97 respectively.Para-difluorobenzene has the largest quantum yield of fluorescence of any fluorinated benzene yet examined. The fluorescent yield shows only one definite minimum at 2740 Å. Triplet yields have been determined at 2660, 2740, and 2760 Å. The sums of the singlet and triplet yields at these wavelengths are 0.5, 0.5, and 0.7 respectively.

2014 ◽  
Vol 118 (19) ◽  
pp. 10375-10383 ◽  
Author(s):  
A. M. P. Botas ◽  
R. A. S. Ferreira ◽  
R. N. Pereira ◽  
R. J. Anthony ◽  
T. Moura ◽  
...  

1965 ◽  
Vol 43 (6) ◽  
pp. 1714-1719 ◽  
Author(s):  
David L. Bunbury

The reaction of benzene and nitrogen dioxide to produce nitrobenzene has been studied in the liquid and gas phases, in the dark, and with irradiation by light of 439 mμ and of 366 mμ. The concentration of NO2 in the liquid was varied from 0.08 to 1.6 moles/1 and in the gas from 0.0035 to 0.053 moles/1. No nitrobenzene was produced under any conditions in the liquid phase. Nitrobenzene is produced in the gas phase at high NO2 concentrations with irradiation by 366 mμ light. The quantum yield is 0.2. At 439 mμ the quantum yield is not more than 0.02. There is a very small dark reaction. As the concentration of NO2 in the gas is reduced the yield of nitrobenzene falls off very rapidly and is zero at the lowest concentration used, both in dark and light.


1985 ◽  
Vol 30 (1) ◽  
pp. 1-11 ◽  
Author(s):  
Gerardo A. Argüello ◽  
Esther R. de Staricco ◽  
Eduardo H. Staricco

2003 ◽  
Vol 368 (3-4) ◽  
pp. 445-451 ◽  
Author(s):  
Alexander Hanf ◽  
Almuth Läuter ◽  
Hans-Robert Volpp

1985 ◽  
Vol 63 (1) ◽  
pp. 62-67 ◽  
Author(s):  
Hélène Deslauriers ◽  
Guy J. Collin

The photofragmentation of 2,3-dimethylbutene and 3,3-dimethylbutene has been studied at 147 and 184.9 nm in the gas phase. The main primary decomposition process at both wavelengths involves the rupture of a β(C—C) bond. The quantum yield for this process is higher than 0.7 at 147 nm and is probably even higher at 184.9 nm. All dimethallyl radicals formed at 147 nm in this process decompose at low pressure, but some of them isomerize from the α,β- to the α,α- structure (and vice versa) — via a 1,4-H transfer — before decomposition. At 184.9 nm, the same primary process is used to get a rough value for the lifetime of the photoexcited molecule, compared with the one made with RRKM calculations by assuming that all the photon energy resides in the vibrational framework of the fundamental electronic state. These lifetimes are about one nanosecond or less.


2011 ◽  
Vol 21 (21) ◽  
pp. 4041-4041 ◽  
Author(s):  
Rebecca J. Anthony ◽  
David J. Rowe ◽  
Matthias Stein ◽  
Jihua Yang ◽  
Uwe Kortshagen

2011 ◽  
Vol 21 (21) ◽  
pp. 4042-4046 ◽  
Author(s):  
Rebecca J. Anthony ◽  
David J. Rowe ◽  
Matthias Stein ◽  
Jihua Yang ◽  
Uwe Kortshagen

2006 ◽  
Vol 118 (4) ◽  
pp. 341-344 ◽  
Author(s):  
Manish Tak ◽  
Manabendra Chandra ◽  
Dulal Senapati ◽  
Puspendu K. Das
Keyword(s):  

1998 ◽  
Vol 52 (8) ◽  
pp. 1103-1110
Author(s):  
G. Kaindl ◽  
R. Weger ◽  
P. Bajons

A new method for the absolute determination of the quantum yield based on the trapping of fluorescence light within a cylinder is discussed. First the trapping probability of photons—which are emitted in transparent rods or fluid-filled tubes—is investigated theoretically. The studies are based on the extension of light governed by the laws of reflection and refraction. The effect of nonhomogeneous distribution of the centers of fluorescence light emission on the calculation procedures is taken into account. Then the adaptation of the theoretical results to a new practical method is shown. The quantum yield as a function of the exciting wavelength is determined in one experimental cycle. The discussion of the method is performed by measurements on fluorescein in aqueous solution. The results are compared to literature data. The conformity demonstrates the applicability of the new method.


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