Question on deriving Bessel's equation

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The discussion revolves around deriving Bessel's equation and the implications of setting coefficients in its series solution. The participant questions the assumption that C1 must equal zero, suggesting that setting C0 to zero could also be valid, which would alter the equation significantly. It is clarified that both choices lead to valid solutions, with the distinction affecting the series' terms. The normalization of C0 to a specific value is justified by the linearity of the equation, allowing for any convenient normalization in defining Bessel functions. Ultimately, the choice of coefficients influences the form of the solution but does not invalidate the underlying equation.
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\hbox { Bessel's equation of order p: }\;x^2y''+xy'+(x^2-p^2)y=0\;\hbox { and let}\;y=\sum_0^{\infty}C_nx^{n+r}
\Rightarrow\; \left[\sum_0^{\infty}C_k(k+r)(k+r-1)x^k+\sum_0^{\infty}C_k(k+r)x^k+\sum_2^{\infty} C_{k-2}x^k-p^2\sum_0^{\infty}C_kx^k\right]x^r\;=\;0
\Rightarrow\; x^r\left[(r^2-p^2)C_0+[(r+1)^2-p^2]C_1 x+\sum_2^{\infty}\left([(k+r)(k+r)-p^2]C_k+C_{k-2}\right)x^k\right]\;=\;0

According to the book, all the terms have to be zero for the equation to be zero.
(r^2-p^2)C_0=0\;\Rightarrow r=^+_-p
The book also say
[(r+1)^2-p^2]C_1=0\;\Rightarrow C_1=0\;\hbox { because from above, }\;r=^+_-p


My problem with this assumption ##C_1=0## is I can just as easy say ##(r+1)^2-p^2=0## and claim ##C_0=0##! This will change the whole equation of the Bessel's equation!

Why do I have to follow the book to let ##C_1=0## which result in all ##C_{2n+1}=0##? Is it just because it is simpler and more convenient this way?

Also, the book just said let ##C_0=\frac {1}{2^p\Gamma(1+p)}## without explaining why. Why?

I know it is for fitting the formula of:

J_p=\sum_0^{\infty} \frac{(-1)^k}{k! \Gamma(k+p+1)}\left(\frac {x}{2}\right)^{2k+p}

But can you just let ##C_0## to be anything?

Thanks
 
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yungman said:
\hbox { Bessel's equation of order p: }\;x^2y''+xy'+(x^2-p^2)y=0\;\hbox { and let}\;y=\sum_0^{\infty}C_nx^{n+r}
\Rightarrow\; \left[\sum_0^{\infty}C_k(k+r)(k+r-1)x^k+\sum_0^{\infty}C_k(k+r)x^k+\sum_2^{\infty} C_{k-2}x^k-p^2\sum_0^{\infty}C_kx^k\right]x^r\;=\;0
\Rightarrow\; x^r\left[(r^2-p^2)C_0+[(r+1)^2-p^2]C_1 x+\sum_2^{\infty}\left([(k+r)(k+r)-p^2]C_k+C_{k-2}\right)x^k\right]\;=\;0

According to the book, all the terms have to be zero for the equation to be zero.
(r^2-p^2)C_0=0\;\Rightarrow r=^+_-p
The book also say
[(r+1)^2-p^2]C_1=0\;\Rightarrow C_1=0\;\hbox { because from above, }\;r=^+_-p


My problem with this assumption ##C_1=0## is I can just as easy say ##(r+1)^2-p^2=0## and claim ##C_0=0##! This will change the whole equation of the Bessel's equation!

Why do I have to follow the book to let ##C_1=0## which result in all ##C_{2n+1}=0##? Is it just because it is simpler and more convenient this way?

You can make either choice. You will still find that the leading term in ##x^{k+r}## in the solution has degree ##p##. Choosing ##C_0\neq 0## makes ##r=p## and the sum over even powers ##k##, while choosing ##C_1\neq 0## makes ##r=p-1## and the sum over odd powers. In either case the series starts with ##x^p## and multiplies this by a polynomial in even powers. So the choice corresponds to shifting the definitions of ##k## and ##r## by ##\pm 1## in such a way that they cancel out in the complete solution.

Also, the book just said let ##C_0=\frac {1}{2^p\Gamma(1+p)}## without explaining why. Why?

I know it is for fitting the formula of:

J_p=\sum_0^{\infty} \frac{(-1)^k}{k! \Gamma(k+p+1)}\left(\frac {x}{2}\right)^{2k+p}

But can you just let ##C_0## to be anything?

Thanks

Yes, since the equation is linear, any multiple of a solution is still a solution. So we can choose any convenient normalization that we want when we define the Bessel functions.
 
Thanks for your answer.
 

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