Partition function of classical oscillator with small anharmonic factor

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SUMMARY

The discussion focuses on calculating the partition function for a one-dimensional array of N oscillators with a frequency w and an anharmonic factor ax^4, where 0 < a << 1. The partition function is expressed as Z = (1/h) ∫ e^(-β(p²/2m + 1/2mw²x² + ax⁴)) dp dx. Participants provide insights on approximating the integrals and deriving expressions for energy E and heat capacity C_v, ultimately leading to C_v = Nk(1 - (6αk)/(m²w⁴)T). Key steps include performing the integrals and applying the small a approximation.

PREREQUISITES
  • Understanding of statistical mechanics concepts, particularly partition functions.
  • Familiarity with integrals involving exponential functions and Gaussian integrals.
  • Knowledge of thermodynamic derivatives, specifically E = -d ln Z/dβ and C_v = dE/dT.
  • Experience with perturbation theory in the context of anharmonic oscillators.
NEXT STEPS
  • Study the derivation of partition functions in statistical mechanics.
  • Learn about Gaussian integrals and their applications in physics.
  • Explore perturbation theory for anharmonic oscillators in greater detail.
  • Investigate the relationship between energy and heat capacity in thermodynamic systems.
USEFUL FOR

Students and researchers in physics, particularly those focusing on statistical mechanics, thermodynamics, and quantum mechanics, will benefit from this discussion.

castlemaster
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Homework Statement



Having a unidemsional array of N oscillators with same frequency w and with an anharmonic factor ax^4 where 0 < a << 1

Calculate, up to the first order of a, the partition function.

Homework Equations



For one oscillator

Z=\frac{1}{h}\int{e^{-\beta(p^2/2m+1/2mw^2x^2+ax^4)}dpdx}

The Attempt at a Solution



Tried to

Z=\frac{K&#039;}{h}\int{e^{\frac{-\beta*mw^2x^2}{2}(1+\frac{2a}{mw^2}x^2))}dpdx}

and I guess I can approximate (1+bx^2) to something ... but I know more or less the solution and I can't figure out how to reach it.
 
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<br /> Z=\frac{1}{h}\int{e^{-\beta(p^2/2m+1/2mw^2x^2+ax^4)}dpdx}<br />
<br /> =\frac{1}{h}\int{e^{-\beta(p^2/2m+1/2mw^2x^2)}e^{-\beta ax^4}dpdx}<br />
<br /> =\frac{1}{h}\int{e^{-\beta(p^2/2m+1/2mw^2x^2)} (1 -\beta ax^4 + \cdots) }dpdx}<br />

you should probably know how to calculate the last.
but here are some useful integrals

\int e^{-ax^2} = \sqrt{\pi/a}
\int x^2 e^{-ax^2} = \frac{1}{2} \sqrt{\frac{\pi}{a^3}}
\int x^4 e^{-ax^2} = \frac{3}{4} \sqrt{\frac{\pi}{a^5}}
 
good luck.
 
That's what I thought but part b of the problem say:

show that C_{v}=Nk(1-\frac{6*\alfa*k}{m^2w^4}T)

but
E=-\frac{d lnZ}{d\beta}
and
C_{v}=\frac{d E}{dT}

if I do all the integrals I get something like

ln Z=Nln(K_{1}\beta^{n})

and for the properties of the ln

ln Z=Nln(K_{1}) +Nnln(\beta)

and making the derivate over B will never give the Cv mentioned.

What I'm doing wrong?

Thanks for the answer
 
if I do

u=\frac{\beta mw^2x^2}{2}

then I get something like

\frac{1}{\beta mw^2}\int{e^{-u}e^{-\frac{4\alpha u^2}{\beta m^2w^4}}}

I think it approches what I need to end with, at least the variables are similar,

someone has a clue? maybe using the fact that the derivate of exp(ax^n) is nax^(n-1)exp(ax^n)

I'll appreciate any clue

thanks
 
i already told you how to do this.

step 1. do the math.
you end up with z = c_1 \beta^{-1} - a c_2 \beta^{-2}
for constants c1, and c2.

step 2. still do the math.
find E = - \frac{d \log z}{d\beta}, this will still have an a in
the denominator, drop it (using small a approximation)

step 3. do even more math.
find C_v = \frac{dE}{dT}

step 4. ?

step 5. profit.
 
You are right qbert,
I was just doing a stupid mistake everytime.

ln(a*b) = lna+lnb RIGHT
ln(a+b) = lna+lnb STUPID
ln(1+ax) aprox.= ax for a small

thanks for the patience
 

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