About the radial Schrödinger quation

In summary, the conversation discusses a difficult question involving equations (1), (2), and (3). The participants use various mathematical techniques and substitutions to solve the problem, ultimately arriving at the rewritten form of equation (1) using d/dρ = 1/ρ d/dx. They also discuss the importance of differentiating and rewriting equations accurately.
  • #1
Douasing
41
0
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
 
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  • #2
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:
 
  • #3
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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  • #4
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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  • #5
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 ?
 
  • #6
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.
 
  • #7
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]
 
  • #8
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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  • #9
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]
 
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  • #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:
 

FAQ: About the radial Schrödinger quation

What is the radial Schrödinger equation?

The radial Schrödinger equation is a mathematical equation that describes the behavior of quantum particles, such as electrons, in terms of their position and energy. It is a fundamental equation in quantum mechanics and is used to solve for the probability of finding a particle in a particular region of space.

Why is the radial Schrödinger equation important?

The radial Schrödinger equation is important because it allows us to understand how quantum particles behave and interact. It is used in many areas of physics, including atomic and molecular physics, condensed matter physics, and nuclear physics.

What are the variables in the radial Schrödinger equation?

The variables in the radial Schrödinger equation include the radial coordinate (r), the angular momentum quantum number (l), the energy of the particle (E), and the potential energy function (V). These variables vary depending on the specific system being studied.

How is the radial Schrödinger equation solved?

The radial Schrödinger equation is solved using various mathematical techniques, such as separation of variables, perturbation theory, and numerical methods. The specific method used depends on the complexity of the system and the desired level of accuracy.

What are the applications of the radial Schrödinger equation?

The radial Schrödinger equation is used in many areas of physics, including quantum mechanics, atomic and molecular physics, nuclear physics, and condensed matter physics. It is also used in chemistry and materials science to understand the properties and behavior of atoms and molecules. Additionally, it has applications in technology, such as in the design of electronic devices and quantum computers.

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