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首页> 外文期刊>Physical review letters >Erratum: Low Frequency Raman Scattering from Acoustic Phonons Confined in ZnO Nanoparticles [Phys. Rev. Lett. 97, 085502 (2006)]
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Erratum: Low Frequency Raman Scattering from Acoustic Phonons Confined in ZnO Nanoparticles [Phys. Rev. Lett. 97, 085502 (2006)]

机译:勘误:局限在ZnO纳米粒子中的声子的低频拉曼散射[Phys。牧师97,085502(2006)]

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摘要

Our recent Letter contained a few errors. (i) The eigenvalue equations for the spheroidal modes of the homogenous elastic body [Eq. (3) of our Letter] should read as follows: 2{η~2+(l-1)(l+2)[ηj_(l+1)(η)/j_l(η)-(l+1)]}ξj_(l+1)(ξ)/j_l(ξ)-η~4/2+(l-1)(2l+1)η~2+[η~2-2l(l-1)(l+2)]ηj_(l+1)(η)/j_l(η)=0 for (l>0) and tan(ξ)(1-η~2/4)-ξ=0 for(l=0). (ii) The theoretical Raman mode frequencies were calculated using Eqs. (7), (8) which were not derived from Eq. (4) as was erroneously written in the Letter. These equations were reported by Tanaka et al. [1] and are essentially the same for ZnO as for CdS since the ratio of the longitudinal and the transverse sound velocities in CdS is the same as that in ZnO. [The longitudinal and the transverse sound velocities for ZnO are 6365 m/s (v_l) and 2735 m/s (v_t), respectively, and the ratio (v_l/v_t) is 2.32 [2] and for CdS this ratio is 2.28 due to v_l being 4247 m/s and v_t = 1859 m/s [1].]
机译:我们最近的信中包含一些错误。 (i)均质弹性体球状模态的特征值方程我们的信中的(3)应该如下:2 {η〜2 +(l-1)(l + 2)[ηj_(l + 1)(η)/ j_l(η)-(l + 1)] }ξj_(l + 1)(ξ)/ j_l(ξ)-η〜4/2 +(l-1)(2l + 1)η〜2 + [η〜2-2l(l-1)(l + 2)]对于(l> 0),ηj_(l + 1)(η)/ j_l(η)= 0,对于(l = 0),tan(ξ)(1-η〜2/4)-ξ= 0。 (ii)使用等式计算理论拉曼模式频率。 (7),(8)并非源自方程(4)错误地写在信中。这些方程式由Tanaka等报道。 [1] ZnO与CdS基本相同,因为CdS中的纵向声速和横向声速之比与ZnO中的相同。 [ZnO的纵向和横向声速分别为6365 m / s(v_1)和2735 m / s(v_t),比率(v_1 / v_t)为2.32 [2],而对于CdS,该比率为2.28。 v_l为4247 m / s,v_t = 1859 m / s [1]。]

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