How Is Equation 15.5.7 Derived in Schaum's Outline of Quantum Mechanics?

jhon
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in Schaum's Outline of Theory and Problems of Quantum Mechanics

how did they got eq 15.5.7

qpnns5.jpg
 
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Did you try using the relation

\sin[x]=\frac{\exp[ix]-\exp[-ix]}{2i}

in Equation 15.5.6 and expanding to see what you get? It looks like you should get the result they obtain if you work at it using that relation.
 
the second eq II ?? it's equale zero why??
 
If you have expanded Equation 15.5.6 using the substitution given, try separating the resulting equation into the real and imaginary components. It looks to me like Equation I in 15.5.7 is the imaginary part and Equation II of 15.5.7 is the real part after substituting for \sin[x].
 
I don't think that the two parts of 15.5.7 are the real and imaginary parts of 15.5.6, but rather they result from the fact that e^{ikr} and e^{-ikr} are orthogonal functions of r, and hence the relation \alpha e^{ikr}+\beta e^{-ikr}=0[/itex] can only be true for all r if \alpha=\beta=0.
 
jdwood983 and gabbagabbahey thanks for help
 
To solve this, I first used the units to work out that a= m* a/m, i.e. t=z/λ. This would allow you to determine the time duration within an interval section by section and then add this to the previous ones to obtain the age of the respective layer. However, this would require a constant thickness per year for each interval. However, since this is most likely not the case, my next consideration was that the age must be the integral of a 1/λ(z) function, which I cannot model.
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