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Second harmonic generation in generalized Thue-Morse ferroelectric superlattices

机译:广义Thue-Morse铁电超晶格中的二次谐波生成

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In this paper the second harmonic generation (SHG) in generalized Thue-Morse (GTM(m, n)) ferroelectric superlattices is studied. Under the small-signal approximation, the SHG spectra in both real and reciprocal spaces are investigated. It is found that: (1) only when the structure parameters l, l(A), and l(B) are all chosen to be proper, can SHG in GTM(m, n) ferroelectric superlattices be generated; (2) for Family A of generalized Thue-Morse, GTM(m, 1) ferroelectric systems, with the increase of parameter m, the intense peaks of SHG concentrate on the long wavelength 1.4-1.5 mu m (the fundamental beam (FB) wavelength is within 0.8-1.5 mu m), but for Family B of generalized Thue-Morse, GTM(1, n) ferroelectric superlattices, with the increase of parameter n, the intense peaks of SHG concentrate on the middle wavelength 1.1-1.2 mu m; and (3) for GTM(m, 1) ferroelectric superlattices, the bigger the m, the stronger the relative integral intensity (RII) of SHG would be, but for GTM(1, n) ferroelectric systems, the bigger the n, the weaker the RII of SHG would be.
机译:本文研究了广义Thue-Morse(GTM(m,n))铁电超晶格中的二次谐波(SHG)。在小信号近似下,研究了实空间和倒数空间中的SHG谱。发现:(1)只有当结构参数l,l(A)和l(B)都被选择为适当时,才能生成GTM(m,n)铁电超晶格中的SHG; (2)对于广义Thue-Morse GTM(m,1)铁电系统的族A,随着参数m的增加,SHG的强峰集中在1.4-1.5μm长波长(基波(FB))上波长在0.8-1.5μm之内),但是对于广义Thue-Morse族B,GTM(1,n)铁电超晶格,随着参数n的增加,SHG的强峰集中在中间波长1.1-1.2μm m; (3)对于GTM(m,1)铁电超晶格,m越大,SHG的相对积分强度(RII)越强,但是对于GTM(1,n)铁电系统,n越大,则SHG的RII会更弱。

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