Thermodynamics of SrO
Posted: Fri Apr 01, 2011 2:26 pm
Dear colleagues,
My problem is the following: I've calculated the thermal expansion coefficient of SrO in NaCl phase. The shape of its behaviour with increasing T is adequate, but all the values are by 4 order of magnitude larger than usual (10^-5).
My rf calcs. (phonon freqs. - wj) are in a very good agreement with experiments and previous DFT calcs. Room temperature S and Cv are also in a very good agreement with exp. data.
To calc. the thermal expansion coefficient I used an equation (14) given in PRB 50, 17054 : (1/3B0)*SUM(gj*Cvj). It depends on B0 (equilibrium bulk modulus), gj (Grueneisen parameters) and Cvj (phonon contribution to the constant volume specific heat). For B0 I got close to previous results (it doesn't influence the results much). I gave it in J/Bohr^3. For gj I got the values between 2 and -4 (I have soft modes in NaCl phase). For gj I did finite difference of ln's, with freqs given in Ha and volumes in Bohr^3. Later I tried with freqs in Hz, but I got the same values. Cvj I got from equations (4) and (5) in PRB 68, 224304 : Cvj = k*exp(hbar*wj/k*T)*(hbar*wj/k*T * 1/(exp(hbar*wj/k*T)-1))^2. Boltzmann constant I gave in J/K, hbar in Js, T in K and wj in Hz.
Just to mention, when one uses expression (16) from PRB 50, 17054 for Cvj and explicitly does the T derivation, one gets the same formula as in PRB 68, 224304, except that an equilibrium volume V0 appears in the denominator besides B0 (so, its (1/3B0V0)...). But in this case, I think that units in the expression do not give K^-1 needed for the thermal expansion coefficient. But even including the volume here, the results are still 2 orders of magnitude too large. I think volume should be not here.
When all is summed up, I get the above problem. I just cannot find the source of it. I would appreciate any thought, criticism and ideas on this issue and my way of doing it.
Thank you all in advance!
Yours,
Igor Lukacevic
My problem is the following: I've calculated the thermal expansion coefficient of SrO in NaCl phase. The shape of its behaviour with increasing T is adequate, but all the values are by 4 order of magnitude larger than usual (10^-5).
My rf calcs. (phonon freqs. - wj) are in a very good agreement with experiments and previous DFT calcs. Room temperature S and Cv are also in a very good agreement with exp. data.
To calc. the thermal expansion coefficient I used an equation (14) given in PRB 50, 17054 : (1/3B0)*SUM(gj*Cvj). It depends on B0 (equilibrium bulk modulus), gj (Grueneisen parameters) and Cvj (phonon contribution to the constant volume specific heat). For B0 I got close to previous results (it doesn't influence the results much). I gave it in J/Bohr^3. For gj I got the values between 2 and -4 (I have soft modes in NaCl phase). For gj I did finite difference of ln's, with freqs given in Ha and volumes in Bohr^3. Later I tried with freqs in Hz, but I got the same values. Cvj I got from equations (4) and (5) in PRB 68, 224304 : Cvj = k*exp(hbar*wj/k*T)*(hbar*wj/k*T * 1/(exp(hbar*wj/k*T)-1))^2. Boltzmann constant I gave in J/K, hbar in Js, T in K and wj in Hz.
Just to mention, when one uses expression (16) from PRB 50, 17054 for Cvj and explicitly does the T derivation, one gets the same formula as in PRB 68, 224304, except that an equilibrium volume V0 appears in the denominator besides B0 (so, its (1/3B0V0)...). But in this case, I think that units in the expression do not give K^-1 needed for the thermal expansion coefficient. But even including the volume here, the results are still 2 orders of magnitude too large. I think volume should be not here.
When all is summed up, I get the above problem. I just cannot find the source of it. I would appreciate any thought, criticism and ideas on this issue and my way of doing it.
Thank you all in advance!
Yours,
Igor Lukacevic