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| We treat the core states fully relativistically and the valence states scalar relativistically and use angular momenta up to l=8 in the muffin-tin spheres for both the wave functions and charge density in the self-consistent cycles. The energy cutoff for the plane-wave expansion in the interstitial region between the muffin-tin spheres is taken to be 20.25 Ry, and the muffin-tin radii employed are RN=1.4 Bohr for N and RTa=2.47 Bohr for Ta, except for the N interstitials and the Ta3N5 phase where, due to the smaller N-Ta distances,we used RTa=2.10 bohr and RTa=2.2 bohr, respectively.In the calculation of energy differences, we took care to use exactly the same plane-wave cutoff and muffin-tin radii and, as close as possible, k-point samplings. |
» 搶金幣啦!回帖就可以得到:
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木蟲(chóng) (著名寫(xiě)手)
| 我們對(duì)核心國(guó)家完全relativistically和價(jià)州relativistically和使用角momenta標(biāo)量,muffin-tin,我是8年來(lái)的領(lǐng)域和裝藥密度波函數(shù)在自洽場(chǎng)周期。 截止的能量為給飛機(jī)波浪擴(kuò)張的球體muffin-tin間質(zhì)間部位就被當(dāng)作是當(dāng)代20.25,采用muffin-tin半徑的RN代碼= 1.4波爾氮之= 247波爾為助教,除了N interstitials和Ta3N5的階段,在這個(gè)階段中,由于距離,我們使用小N-Ta等= 2.10波爾之= 220波爾,分別。在計(jì)算照顧能量不同,我們使用相同的給飛機(jī)波浪修剪和muffin-tin半徑,盡可能近的地方,k-point取樣。 |
金蟲(chóng) (小有名氣)
| 我們將核心狀態(tài)與價(jià)態(tài)標(biāo)量視為完全相對(duì)性的,為了讓波動(dòng)函數(shù)和電荷密度達(dá)到自洽周期,使糕模球體的角動(dòng)量達(dá)到l=8。平面波展開(kāi)法在糕模球體達(dá)到20.25Ry和糕模半徑N被設(shè)為RN=1.4波爾、Ta設(shè)為Rta=2.47波爾之間的間質(zhì)期能量中斷,間隙的N和Ta3N5階段,由于需要較小的N-Ta距離,我們分別設(shè)RTA=2.10波爾和Rta=2.2波爾。對(duì)于能源偏差的計(jì)算,應(yīng)注意精確的使用平面波切斷和糕模半徑并盡可能的接近抽樣的彈性極限。 |
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