东南大学学报(自然科学版)
東南大學學報(自然科學版)
동남대학학보(자연과학판)
JOURNAL OF SOUTHEAST UNIVERSITY
2009年
5期
1028-1032
,共5页
王家佳%陈爱华%李瑜璞%于金%吴三械
王傢佳%陳愛華%李瑜璞%于金%吳三械
왕가가%진애화%리유박%우금%오삼계
钒%压致相变%第一性原理%相变压力%电子结构
釩%壓緻相變%第一性原理%相變壓力%電子結構
범%압치상변%제일성원리%상변압력%전자결구
vanadium%pressure-induced phase transition%first principles%phase transition pressure%electronic structure
利用投影缀加波方法对金属钒加压至400 GPa左右的结构相变过程进行了第一性原理研究. 计算了相变中的热力学转变压力和失稳转变压力, 并对相变前后的电子性质进行了研究. 结果表明: 钒在低压下为体心立方结构, 随着压力增大转变为菱方结构, 压力继续增大最后又重新转变为体心立方结构. 热力学计算得到的BCC→rh~u(α>109.47°)→rh~l(α<109.47°)→BCC三次转变压力分别为27,104和310 GPa. 利用剪切弹性常数C44计算得到的2次失稳压力分别为52和255 GPa. 能带计算表明, 在加压过程中高对称点Γ处靠近费米能级的能带由低压下的非电子占据态变为高压下的占据态, 而费米能级以上的电子态密度计算可见明显的s,p-d带间电子迁移现象.
利用投影綴加波方法對金屬釩加壓至400 GPa左右的結構相變過程進行瞭第一性原理研究. 計算瞭相變中的熱力學轉變壓力和失穩轉變壓力, 併對相變前後的電子性質進行瞭研究. 結果錶明: 釩在低壓下為體心立方結構, 隨著壓力增大轉變為蔆方結構, 壓力繼續增大最後又重新轉變為體心立方結構. 熱力學計算得到的BCC→rh~u(α>109.47°)→rh~l(α<109.47°)→BCC三次轉變壓力分彆為27,104和310 GPa. 利用剪切彈性常數C44計算得到的2次失穩壓力分彆為52和255 GPa. 能帶計算錶明, 在加壓過程中高對稱點Γ處靠近費米能級的能帶由低壓下的非電子佔據態變為高壓下的佔據態, 而費米能級以上的電子態密度計算可見明顯的s,p-d帶間電子遷移現象.
이용투영철가파방법대금속범가압지400 GPa좌우적결구상변과정진행료제일성원리연구. 계산료상변중적열역학전변압력화실은전변압력, 병대상변전후적전자성질진행료연구. 결과표명: 범재저압하위체심립방결구, 수착압력증대전변위릉방결구, 압력계속증대최후우중신전변위체심립방결구. 열역학계산득도적BCC→rh~u(α>109.47°)→rh~l(α<109.47°)→BCC삼차전변압력분별위27,104화310 GPa. 이용전절탄성상수C44계산득도적2차실은압력분별위52화255 GPa. 능대계산표명, 재가압과정중고대칭점Γ처고근비미능급적능대유저압하적비전자점거태변위고압하적점거태, 이비미능급이상적전자태밀도계산가견명현적s,p-d대간전자천이현상.
Recent experiment revealed a new structural phase transition in vanadium at high pressure. Here the whole phase transition process under pressure up to 400 GPa was investigated from first principles calculation with projector augmented wave (PAW) method. The results show that body -centered cubic (BCC) vanadium firstly makes a transition to rhombohedral(rh) structure under pressure, and with increasing pressure, it transforms back to BCC again. Three thermodynamic phase transition pressures of BCC→rh~u(α > 109. 47°) →rh~1( α < 109. 47°) →BCC are 27, 104 and 310 GPa, respectively. Two instability pressures obtained by calculation of shear elastic constant C_(44) at different pressures are 52 and 255 GPa. Electronic properties calculation reveals that bands near Γ point gradually move below the Fermi level and become occupied condition. Calculation of decomposed density of states at Fermi level presents obvious s, p-d electrons transition among bands.