Can we use this approximation for k_D<<k_F?

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Petar Mali
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For [tex]k_D<<k_F[/tex]

[tex]|\frac{\hbar^2k^2_F}{2m}-\frac{\hbar^2k^2}{2m}|\approx \frac{\hbar^2k_F}{m}|k_F-k|[/tex]

Where [tex]k[/tex] goes from [tex]k-k_D[/tex] to [tex]k+k_D[/tex]

[tex]k_F[/tex] - Fermi wave vector
[tex]k_D[/tex] - Debay wave vector
 
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I suppose you mean [itex]k[/itex] goes between [itex]k_F+k_D[/itex] and [itex]k_F-k_D[/itex]?

Yes it is valid. Let's denote [itex]k=k_F+\delta k[/itex], then

[tex] |\frac{\hbar^2k_F^2}{2m}-\frac{\hbar^2k^2}{2m}|=|\frac{\hbar^2k_F\delta k}{m}+\frac{\hbar^2 \delta k^2}{2m}|[/tex]

since [itex]\delta k<k_D\ll k_F[/itex] we can neglect the last term (quadratic in [itex]\delta k[/itex] and get

[tex] |\frac{\hbar^2k_F\delta k}{m}|=\frac{\hbar^2k_F}{m}|k_F-k|<br /> [/itex][/tex]
 
Thanks a lot! :) Yes from [tex]k_F-k_D[/tex] to [tex]k_F+k_D[/tex].

I think that you have just a little mistake

You must write like

[tex] <br /> |\frac{\hbar^2k_F^2}{2m}-\frac{\hbar^2k^2}{2m}|=|-\frac{\hbar^2k_F\delta k}{m}-\frac{\hbar^2 \delta k^2}{2m}|<br /> [/tex]

To get [tex]C|k_F-k|[/tex] or in case you wrote you will get

[tex]C|k-k_F|[/tex]

You helped me a lot!
 
Petar Mali said:
Thanks a lot! :) Yes from [tex]k_F-k_D[/tex] to [tex]k_F+k_D[/tex].

I think that you have just a little mistake

You must write like

[tex] <br /> |\frac{\hbar^2k_F^2}{2m}-\frac{\hbar^2k^2}{2m}|=|-\frac{\hbar^2k_F\delta k}{m}-\frac{\hbar^2 \delta k^2}{2m}|<br /> [/tex]

To get [tex]C|k_F-k|[/tex] or in case you wrote you will get

[tex]C|k-k_F|[/tex]

I assumed that [itex]|\ldots |[/itex] meant taking the absolute value. If this is so then overall signs do not matter.

Anyway, You're welcome.
 
Yes! My mistake!