1) parabolic quantum dot
抛物量子点
1.
Influence of temperature on the properties of the strong-coupling magnetopolaron in a parabolic quantum dot;
温度对抛物量子点中强耦合磁极化子性质的影响
2.
The properties of a bound polaron in a parabolic quantum dot with weak electron-LO-phonon coupling under a Coulomb field are studied.
研究了库仑场中抛物量子点中束缚极化子的性质。
2) parabolic quantum well
抛物量子阱
1.
The binding energy of a bound polaron in a finite parabolic quantum well is studied theoretically by a fractional-dimensional variational method.
采用分维变分方法讨论了有限深抛物量子阱中束缚极化子的束缚能,得到了束缚能随阱宽的变化关系,并给出了声子对束缚能的贡献随阱宽的变化曲线。
2.
In the adiabatic approximation,the ground states energy of the electron in the parabolic quantum well structures was studied under an external magnetic filed.
采用变分法,研究了外界磁场对抛物量子阱中基态能量的影响,并给出抛物量子阱CaN/AlxCa1-xN中的数值结果。
3.
The polarization potential,the ground state energy and the energy shift of the bound polaron in a parabolic quantum well(PQW) are discussed.
利用变分法研究了抛物量子阱中束缚极化子的极化势、基态能量和能量移动,讨论了抛物量子阱中体纵光学(LO)声子和界面纵光学(IO)声子的影响。
3) parabolic quantum wire
抛物量子线
1.
With the Tokudas improved linear combination operators and the Lagrange multiplier and the variational method,the strong-coupling megnetopolaron effective mass m~* and the mean number N of optical phonon in a parabolic quantum wire were investigated.
采用改进的线性组合算符法、Lagrange乘子和变分法,在考虑电子与LO声子相互作用情况下,计算了抛物量子线中强耦合磁极化子的有效质量m 和光学声子平均数N。
4) semi-parabolic quantum well
半抛物量子阱
1.
The influence of the depolarization effect on the third-harmonic generation spectrum in an asymmetric semi-parabolic quantum well is studied.
在半抛物量子阱中,给出三次谐波产生的数值结果。
2.
By adopting the methods of displacement harmonic oscillation and numerical calculation, the structures of the energy levels of the bound states in a semi-parabolic quantum well with an applied electric field is studied.
采用位移谐振子与数值求解相结合的方法,研究和讨论了施加电场的半抛物量子阱中束缚态的能级结构,得到了体系的本征能量与本征函数的表达式。
5) semiparabolic quantum well(QW)
半抛物量子阱(QW)
6) parabolic point
抛物点
补充资料：抛物点
抛物点
parabolic point
抛物点「弹门场拉c，宙戒;，I即丽0洲叨c~功~] 正则曲面上使密切抛物面(osculatillg PaJ冠比】。id)退化为抛物柱面(Ix班泣伙走c cyUnder)的点，在抛物点处，〕.画标线(Dupin jndiG孟trix)是一对平行直线，Ga璐曲率(Ga哎curvatu化)等于零，一个主曲率(principalc一ture)消失，以及第二基本形式(~d山ndamental扬rm)的系数满足下列方程 LN一MZ二0. 瓜.从.Q次叭oB撰【补注】
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参考词条