物理学报
物理學報
물이학보
2013年
6期
385-392
,共8页
紧束缚模型%Zigzag型石墨烯纳米带%边缘态
緊束縳模型%Zigzag型石墨烯納米帶%邊緣態
긴속박모형%Zigzag형석묵희납미대%변연태
the tight-binding model%zigzag graphene nanoribbons%edge state
在紧束缚近似下,提出有限系统的Bloch定理方法,解析计算了Zigzag型石墨烯纳米带的电子态和能带.研究发现,其电子态有两类,分别是驻波态和边缘态;驻波态的波矢为实数,波函数是正弦函数形式;边缘态的波矢主要是虚数,实数部分为零或者π/2,波函数是双曲正弦函数形式. Zigzag型石墨烯纳米带的能带由驻波态能量和边缘态能量组成,我们推导了边缘态的关于无限长方向波矢和能量的精确取值范围.讨论了边缘态和驻波态的过渡点,发现两种电子态通过不同的方式在受限波矢趋于零时关于格点位置逼近线性关系.当受限方向也变成无限长时,可以得到与无限大石墨烯相同的能带关系.
在緊束縳近似下,提齣有限繫統的Bloch定理方法,解析計算瞭Zigzag型石墨烯納米帶的電子態和能帶.研究髮現,其電子態有兩類,分彆是駐波態和邊緣態;駐波態的波矢為實數,波函數是正絃函數形式;邊緣態的波矢主要是虛數,實數部分為零或者π/2,波函數是雙麯正絃函數形式. Zigzag型石墨烯納米帶的能帶由駐波態能量和邊緣態能量組成,我們推導瞭邊緣態的關于無限長方嚮波矢和能量的精確取值範圍.討論瞭邊緣態和駐波態的過渡點,髮現兩種電子態通過不同的方式在受限波矢趨于零時關于格點位置逼近線性關繫.噹受限方嚮也變成無限長時,可以得到與無限大石墨烯相同的能帶關繫.
재긴속박근사하,제출유한계통적Bloch정리방법,해석계산료Zigzag형석묵희납미대적전자태화능대.연구발현,기전자태유량류,분별시주파태화변연태;주파태적파시위실수,파함수시정현함수형식;변연태적파시주요시허수,실수부분위령혹자π/2,파함수시쌍곡정현함수형식. Zigzag형석묵희납미대적능대유주파태능량화변연태능량조성,아문추도료변연태적관우무한장방향파시화능량적정학취치범위.토론료변연태화주파태적과도점,발현량충전자태통과불동적방식재수한파시추우령시관우격점위치핍근선성관계.당수한방향야변성무한장시,가이득도여무한대석묵희상동적능대관계.
@@@@Based on the tight-binding model, the electronic state and band of zigzag graphene nanoribbons are given analytically by a new method. The results show that there are only two kinds electronic states, i.e., the standing wave state and edge state. For the standing wave state, the wave function is sine function and the vector is real;for the edge state, the wave function is hyperbolic sine function and the vector is complex, whose real part is 0 orπ/2. The energy band is composed of the energy of standing wave state and the energy of edge state. The accurate ranges of infinite direction wave vector and energy of the edge state are deduced. Then we discuss the transition point between the edge state and the standing wave state and find that the two kinds of electronic states tend to the linear relationship regarding the site of carbon lattice in different ways at the phase transition point. When the width of two restricted boundary goes to infinity, the result of the limited graphene tends to the infinite case.