About the radial Schrödinger quation

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Homework Help Overview

The discussion revolves around the radial Schrödinger equation, specifically the transformation of the equation into a different form using substitutions and derivatives. Participants are exploring the mathematical techniques involved in this transformation.

Discussion Character

  • Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants discuss the transformation of the radial Schrödinger equation into a second-order differential equation. There are attempts to differentiate and manipulate the equation using substitutions, with some participants questioning the steps taken and the implications of those transformations.

Discussion Status

The discussion is active, with participants providing guidance on differentiation and transformations. There are multiple interpretations being explored, particularly regarding the application of derivatives and the validity of the transformations. Some participants express confusion about the steps, indicating a collaborative effort to clarify the mathematical reasoning.

Contextual Notes

Participants note that the mathematical techniques are not well understood, referencing a specific book for context. There is an ongoing examination of assumptions and methods used in the problem-solving process.

Douasing
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Dear all,
I meet a difficult question as follows:

[itex]-\frac{1}{ρ^{2}}\frac{d}{dρ}(ρ^{2}\frac{dR_{l}}{dρ})+[\frac{l(l+1)}{ρ^{2}}+V(ρ)]R_{l}(ρ)=ER_{l}(ρ)[/itex] (1)

let [itex]x=ln(ρ)[/itex] and [itex]y=ρ^{1/2}R_{l}(ρ)[/itex] ,then

[itex]y^{''}=γy[/itex] (2)
[itex]γ=exp(2x)(V-E)+(l+\frac{1}{2})^{2}[/itex] (3)

What is the details from (1) to (2) and (3)?


Thank you in advance!

Paul
 
Last edited:
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Hi Paul! Welcome to PF! :smile:

(type "tex" instead of "itex" when you have tiny fractions! :wink:)
Douasing said:
Dear all,
I meet a difficult question as follows:

[tex]-\frac{1}{ρ^{2}}\frac{d}{dρ}\left(ρ^{2}\frac{dR_{l}}{dρ}\right)+ \left[\frac{l(l+1)}{ρ^{2}}+V(ρ)\right]R_{l}(ρ)=ER_{l}(ρ)[/tex] (1)

let [itex]x=ln(ρ)[/itex] and [itex]y=ρ^{1/2}R_{l}(ρ)[/itex] ,then

[itex]y^{''}=γy[/itex] (2)
[itex]γ=exp(2x)(V-E)+(l+\frac{1}{2})^{2}[/itex] (3)

What is the details from (1) to (2) and (3)?


Thank you in advance!

Paul
Put y = (√ρ)Rl(ρ), and differentiate twice …

show us what you get :wink:
 
tiny-tim said:
Hi Paul! Welcome to PF! :smile:

(type "tex" instead of "itex" when you have tiny fractions! :wink:)

Put y = (√ρ)Rl(ρ), and differentiate twice …

show us what you get :wink:




y''= -(1/4)ρ^(-3/2) R + ρ^(-1/2) R' + ρ^(1/2) R''

Am I right?
 
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Douasing said:
y''= -(1/4)ρ^(-3/2) R + ρ^(-1/2) R' + ρ^(1/2) R''

Am I right?

yes :smile:

hmm … that doesn't help at all :confused:

ohhhh … i think y'' means wrt x :redface:

try it with y = ex/2R(x) :wink:
 
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tiny-tim said:
yes :smile:

hmm … that doesn't help at all :confused:

ohhhh … i think y'' means wrt x :redface:

try it with y = ex/2R(x) :wink:

y''= [(1/4)R(x)+R'(x)+R''(x)]e^(x/2)

Is it right ?
 
By the way, The formulas above are in the book by L.T. Loucks (1967). But the mathematical techniques are not well understood by us,so I posted them here.
 
Hi Douasing! :smile:

(just got up :zzz:)
Douasing said:
y''= [(1/4)R(x)+R'(x)+R''(x)]e^(x/2)

Is it right ?

Yes!

ok, now put l(l+1) = (l + 1/2)2 - 1/4,

and use d/dρ = 1/ρ d/dx to rewrite

[itex]-\frac{1}{ρ^{2}}\left[\frac{d}{dρ}(ρ^{2}\frac{dR}{dρ})+l(l+1)R\right][/itex]
 
Hi,tiny-tim!

:smile:

tiny-tim said:
Hi Douasing! :smile:

(just got up :zzz:)


Yes!

ok, now put l(l+1) = (l + 1/2)2 - 1/4,

and use d/dρ = 1/ρ d/dx to rewrite

[itex]-\frac{1}{ρ^{2}}\left[\frac{d}{dρ}(ρ^{2}\frac{dR}{dρ})+l(l+1)R\right][/itex]


[tex]-\frac{1}{ρ^{2}}[\frac{1}{ρ}\frac{d}{dx}(ρ^{2}\frac{1}{ρ}\frac{dR}{dx})+(l+\frac{1}{2})^2R-\frac{1}{4}R][/tex]

:confused:
 
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why make it more difficult? :confused:

wouldn't it have been easier to differentiate the ρ2 wrt ρ first, before changing to d/dx ?
 
  • #10
tiny-tim said:
why make it more difficult? :confused:

wouldn't it have been easier to differentiate the ρ2 wrt ρ first, before changing to d/dx ?


ok, :)

[itex]-\frac{1}{ρ^{2}}\left[\frac{d}{dρ}(ρ^{2}\frac{dR}{dρ})+l(l+1)R\right][/itex]
[itex]= -\frac{1}{ρ^{2}}\left[2ρ\frac{dR}{dρ}+ρ^{2}\frac{d}{dρ}(\frac{dR}{dρ})+l(l+1)R\right][/itex]
[itex]= -\frac{1}{ρ^{2}}\left[2ρ+ρ\frac{d}{dx}(\frac{1}{ρ}\frac{dR}{dx})+(l+\frac{1}{2})^{2}R-\frac{1}{4}R\right][/itex]

and then ?
 
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  • #11
you've left out a dR/dρ

(and one of your minuses is wrong)
 
  • #12
Thanks for your kind reminding, now I copy them as follows:

(1) [tex]y^{''}=\left[\frac{1}{4}R+R^{'}+R^{''}\right]e^{\frac{x}{2}}[/tex]

(2) [tex]-\frac{1}{ρ^{2}}\left[2\frac{dR}{dx}+ρ\frac{d}{dx}(\frac{1}{ρ}\frac{dR}{dx})+(l+\frac{1}{2})^{2}R+\frac{1}{4}R\right][/tex]
 
Last edited:
  • #13
tiny-tim said:
Hi Douasing! :smile:

(just got up :zzz:)


Yes!

ok, now put l(l+1) = (l + 1/2)2 - 1/4,

and use d/dρ = 1/ρ d/dx to rewrite

[itex]-\frac{1}{ρ^{2}}\left[\frac{d}{dρ}(ρ^{2}\frac{dR}{dρ})+l(l+1)R\right][/itex]


Hi,tiny-tim,I finally got it. Thank you very much,especially for your patient with me.
:approve:
 

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