河南科学
河南科學
하남과학
HENAN SCIENCE
2014年
2期
153-162
,共10页
陈志远%吴涛%张全坤%谭亿平%胡永红
陳誌遠%吳濤%張全坤%譚億平%鬍永紅
진지원%오도%장전곤%담억평%호영홍
晶格动力学%次近邻原子间作用%色散关系%第一布里渊区%双原子正方晶格
晶格動力學%次近鄰原子間作用%色散關繫%第一佈裏淵區%雙原子正方晶格
정격동역학%차근린원자간작용%색산관계%제일포리연구%쌍원자정방정격
lattice dynamics%secondary neighbor coupling%dispersion relation%First Brillouin Zone%diatomic square lattice
利用晶格动力学理论推导了二维双原子正方晶格振动的色散关系表达式,得到第一布里渊区中沿Γ-X、Γ-M和X-M3种对称方向的声子色散曲线,每一对称方向有四支格波,即两支声学波和两支光学波。讨论了原子质量和次近邻原子间作用对色散关系的影响,结果表明:当两原子质量相等时,3个对称方向的声学波与光学波间无频隙;当两原子质量不等时,声学波与光学波间出现频隙。计及次近邻原子间作用,对Γ点声子频率的大小和简并不影响,两声学模频率为零、两光学模频率简并;对X点声子频率的简并也无影响,但相应频率增大;使M点声子频率的简并度降低,高频声学和光学声子的频率增大,而低频声学和光学声子的频率不变;沿Γ-X方向四支格波仍是非简并的,对应的频率增大,但都表现出色散性;沿Γ-M和X-M方向简并格波的简并度消失,除Γ-M方向低频声学支和光学支频率不变之外,其他格波声子的频率都增大,并且四支格波都表现出色散性。
利用晶格動力學理論推導瞭二維雙原子正方晶格振動的色散關繫錶達式,得到第一佈裏淵區中沿Γ-X、Γ-M和X-M3種對稱方嚮的聲子色散麯線,每一對稱方嚮有四支格波,即兩支聲學波和兩支光學波。討論瞭原子質量和次近鄰原子間作用對色散關繫的影響,結果錶明:噹兩原子質量相等時,3箇對稱方嚮的聲學波與光學波間無頻隙;噹兩原子質量不等時,聲學波與光學波間齣現頻隙。計及次近鄰原子間作用,對Γ點聲子頻率的大小和簡併不影響,兩聲學模頻率為零、兩光學模頻率簡併;對X點聲子頻率的簡併也無影響,但相應頻率增大;使M點聲子頻率的簡併度降低,高頻聲學和光學聲子的頻率增大,而低頻聲學和光學聲子的頻率不變;沿Γ-X方嚮四支格波仍是非簡併的,對應的頻率增大,但都錶現齣色散性;沿Γ-M和X-M方嚮簡併格波的簡併度消失,除Γ-M方嚮低頻聲學支和光學支頻率不變之外,其他格波聲子的頻率都增大,併且四支格波都錶現齣色散性。
이용정격동역학이론추도료이유쌍원자정방정격진동적색산관계표체식,득도제일포리연구중연Γ-X、Γ-M화X-M3충대칭방향적성자색산곡선,매일대칭방향유사지격파,즉량지성학파화량지광학파。토론료원자질량화차근린원자간작용대색산관계적영향,결과표명:당량원자질량상등시,3개대칭방향적성학파여광학파간무빈극;당량원자질량불등시,성학파여광학파간출현빈극。계급차근린원자간작용,대Γ점성자빈솔적대소화간병불영향,량성학모빈솔위령、량광학모빈솔간병;대X점성자빈솔적간병야무영향,단상응빈솔증대;사M점성자빈솔적간병도강저,고빈성학화광학성자적빈솔증대,이저빈성학화광학성자적빈솔불변;연Γ-X방향사지격파잉시비간병적,대응적빈솔증대,단도표현출색산성;연Γ-M화X-M방향간병격파적간병도소실,제Γ-M방향저빈성학지화광학지빈솔불변지외,기타격파성자적빈솔도증대,병차사지격파도표현출색산성。
Based on lattice dynamics,the expressions of dispersion relations were derived for two-dimensional diatomic square lattice,the curves of phonon dispersion alongΓ-X,Γ-M and X-M three symmetry directions were obtained in the First Brillouin Zone. There are four pieces of lattice waves in each direction,where two branches are acoustic waves and other two are optical waves. The effects of two atom masses and secondary neighbor coupling to the dispersion relations were discussed. The results show that,when two masses in the basis are same,there is no the frequency gap between acoustic branches and optical branches along three directions. As two masses are unequal, the frequency gap exists between acoustic branches and optical branches. In presence of secondary neighbor coupling,there are not effects to the value and degeneracy of the phonon frequencies atΓpoint,where both acoustic and optical modes are degenerate. Also,there are no effects to degeneracy of the phonon frequencies at X point, but the phonon frequencies are increased. The degree of degeneracy of the phonon frequencies is reduced at M point,and the frequencies of high frequency acoustic and optical phonon are increased,but the frequencies of low frequency acoustic and optical phonon keep unchanged. Four branches are still non-degenerate alongΓ-X direction, and the phonon frequencies are increased,but they display distinctly dispersion. The degree of degenerate branches is disappeared along Γ-M and X-M directions,except that the frequencies of low frequency acoustic and optical branches retain unchanged alongΓ-M,the others are increased,and four branches are show dispersion. The above results indicate that the dispersion relations are remarkably affected by the atom masses and secondary neighbor coupling.