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One of the great features of JSP is its accessibility. There s no need to worry about complicated IDEs or compilers; you just save an HTML page with embedded Java, trigger it with your browser, and you are done. New Atlanta has made the installation and administration of its servlet engine similarly straightforward. It has done all the hard work of figuring out what needs to be done with each Web server and the configuration of the server is very simple. ServletExec (as well as ServletExec Debugger) is available for free as a development environment; only when you deploy you need to purchase a license. We ve introduced you to various vendors of the J2EE application servers. In the next section, we ll discuss how to avoid dependency on a particular vendor.

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fading standard deviation for various values of the correlation coef cient. For small values of the correlation coef cient, the impact of correlation is more accentuated for low values of the standard deviation. On the other hand, for larger values of the correlation coef cient, the increase in the amount of fading is equally important over the whole standard deviation range. 9.13.2.2 Outage Probability MRC The outage probability Pout of dual-branch MRC corresponds to the probability that MRC falls below a predetermined threshold th :

T3.1 File Management T3.2 Databases and Database Management Systems T3.3 Logical Data Organization T3.4 Creating Databases T3.5 Emerging Database Models T3.6 Data Warehouses T3.7 Database Management T3.8 An Emerging Technology: IP-based Storage T3.9 Data Storage Infrastructure and Management

We analyze Raman radiation with an IFS 66 Bruker interferometer with the FRA 106 Raman module. The optical conductance of an interferometer is given by Eq. 3.1-36: G = 2nF11Ro. The area at the beam splitter is FI = t.2n,with I' = 1.75 cm. The resolving power for the Raman line at D = (9398 992) = 8406 cm and at a bandwidth of A6 = 4 cm equals Ro = G1A3 = 2101. Thus:

BCP-null (for example, 1/2/1) BCP-dot1q (for example, 1/2/1:200 ) ATM (for example, 2/1/1:10/100 )

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1400 1450 1500 Raman shift (cm- )

(4.80)

(9.423)

1 1

we could not expect to directly observe different energy transitions with different angular distributions Rather, we can obtain unequal populations of the substates through the Boltzmann distribution of thermal energy when the sample is cooled to a temperature where kBT is small compared to the energy splitting The typical temperature to maintain nuclear orientation in an external magnetic eld is on the order of 10 mK Cooling small samples to such low temperatures is possible, but it requires special techniques such as 3He dilution refrigeration Example Problem Determine the temperature at which kBT is equal to the energy level splitting for the metastable state of 123Te at 2476 keV in an external magnetic eld of 40 tesla (T) Solution This state I 11 decays by (M4) IT to the ground state 1 with a half2 2 life of 1197 d.

The gyromagnetic ratio, or g factor, for this state is 01685: DEm gIBext mN kB T gIBext mN kB 0:1685 11 (4:0T) 5:05084 10 27 J=T 2 T 1:38066 10 23 J=K T T 1:4 10 3 K A much more common technique for observing angular correlations relies on detecting the direction of radiation from a process that feeds the excited state and then observing the angular distribution relative to that direction As indicated in Figure 97 this process could be a g-ray transition from a higher lying excited state, or it could be a b or a particle emitted by a parent nucleus The rst particle provides the reference axis, but it must also introduce an unequal population of the magnetic substates of the intermediate state in order for the second transition to have an anisotropic angular distribution.

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