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TABLE VII. NEUTRON RADIATION OF OPTICAL FIBER

in unknown title
by unknown authors

Table 2. Radiative transitions for O

in Radiation Modeling With Direct Simulation Monte Carlo
by Ann B. Carlson, H. A. Hassan 1991
Cited by 1

Table 2. Radiative transitions for O

in Radiation Modeling with Direct Simulation Monte Carlo. AIAA Paper 91-1409
by Ann B. Carlson, H. A. Hassan 1991
Cited by 1

Table 3. Radiative transitions for N

in Radiation Modeling with Direct Simulation Monte Carlo. AIAA Paper 91-1409
by Ann B. Carlson, H. A. Hassan 1991
Cited by 1

Table 1 The radiation and optical parameters of the excimer laser Laser

in
by Alfons Vervaet, Sam Siau, Johan De Baets, Boniface Manirambona 2005
"... In PAGE 3: ...The excimer wavelength of 248 nm is commonly used because it is strongly absorbed by most materials. The radiation and optical parameters of the excimer laser are presented in Table1 . From this table we see that this laser has a pulse energy density of 150 mJ/cm2 at a maximal repetition rate of 200 Hz.... ..."

TABLE IV. DATABASE OF RADIATION EFFECTS ON MULTIMODE OPTICAL FIBERS

in unknown title
by unknown authors

TABLE V. DATABASE OF RADIATION EFFECTS ON SINGLE MODE OPTICAL FIBERS

in unknown title
by unknown authors

TABLE VI. DATABASE OF RADIATION EFFECTS ON POLARIZATION MAINTAINING OPTICAL FIBERS

in unknown title
by unknown authors

Table 1. Interstellar Ultraviolet Radiation Fields ( gt; 912 A)

in J., in Press (1996)
by Structure Of, B. T. Draine, Frank Bertoldi 20
"... In PAGE 7: ...4 Habing (1968) estimated the intensity of interstellar starlight at = 1000 A to be u = 4 10?14 erg cm?3. We will consider various radiation elds u , and will characterize the intensity of each at 1000 A, relative to Habing apos;s estimate, by the dimensionless factor [ u ]1000 A 4 10?14 erg cm?3 : (20) In Table1 we list spectral forms which have been considered by various workers. For each spectrum we list the photon ux in the 1110 ? 912 A interval, F 1110 A Z 912 A h?1 u d ; (21) the logarithmic derivative d ln u =d ln evaluated at 1000 A, and the color temperature Tcolor, the temperature of a blackbody having the same logarithmic derivative at 1000 A.... In PAGE 8: ... This radiation eld was employed by van Dishoeck amp; Black (1986) in their modelling of di use clouds, and by Black amp; van Dishoeck (1987) in their models of photodissociation fronts. As seen in Table1 , this spectrum is somewhat harder than eq. (23).... In PAGE 8: ...5 Pumping rates and dissociation rates for optically-thin H2 in various rotation-vibration states are given in Table 2 for the radiation elds (24) and (23). Also given in Table1 is the probability pdiss(v; J) that photoexcitation out of level X(v; J) will be followed by dissociation, and the probability hpret(v; J)i that photoexcitation out of X(v; J) will be followed by direct spontaneous decay back to the original level X(v; J). Since there are many possible UV transitions possible out of any given level X(v; J), both pdiss and hpreti depend on the shape of the illuminating spectrum, but Table 2 shows that for unshielded H2 the changes in hpdissi or pret are typically only a few percent when the shape of the radiation eld is changed.... In PAGE 41: ... Their models had IUV = 300 which (cf. Table1 ) corresponds to 670 { a factor of 7.5 weaker than the = 5000 favored here.... ..."

Table 1: devices and radiation dose/fluence

in Neutron, proton and gamma radiation effects in candidate InGaAs p-i-n photodiodes for the CMS tracker optical links
by Troska Blackett Laboratory, J. Troska, K. Gill, R. Grabit, F. Vasey
"... In PAGE 3: ... The optical sub-assembly is then mounted in a hermetically sealed, ceramic 8-pin Dual In-Line (DIL) package. Table1 outlines the number of devices irradiated and the fluence/dose received by each device. p-i-n silicon submount fibre... In PAGE 4: ... The average energy of the neutrons was 6MeV. The neutron fluence was measured by activated foil dosimetry (using 4mm diameter Ni foils) with the different fluences given in Table1 . The absolute accuracy is ~15% due to a systematic uncertainty in the activation cross-sections, but fluence measurements are typically reproducible to within a few percent.... ..."
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