倒易点阵 Reciprocal lattice
倒易点阵(英语:reciprocal lattice),又称倒(易)晶格、倒(易)格子,是物理学中描述空间波函数的傅立叶变换后的周期性的一种方法。相对于正晶格所描述的实空间周期性,倒晶格描述的是动量空间,亦可认为是k空间的周期性。根据位置和动量所满足的庞特里亚金对偶性,布拉菲晶格的倒晶格仍然是一种布拉菲晶格,而倒晶格的倒晶格就会变回原始晶格(正晶格)。
单词 | Dual lattice |
释义 |
Dual lattice
中文百科
倒易点阵 Reciprocal lattice(重定向自Dual lattice)
倒易点阵(英语:reciprocal lattice),又称倒(易)晶格、倒(易)格子,是物理学中描述空间波函数的傅立叶变换后的周期性的一种方法。相对于正晶格所描述的实空间周期性,倒晶格描述的是动量空间,亦可认为是k空间的周期性。根据位置和动量所满足的庞特里亚金对偶性,布拉菲晶格的倒晶格仍然是一种布拉菲晶格,而倒晶格的倒晶格就会变回原始晶格(正晶格)。
英语百科
Reciprocal lattice 倒易点阵(重定向自Dual lattice)
![]() ![]() ![]() ![]() In physics, the reciprocal lattice represents the Fourier transform of another lattice (usually a Bravais lattice). In normal usage, this first lattice (whose transform is represented by the reciprocal lattice) is usually a periodic spatial function in real-space and is also known as the direct lattice. While the direct lattice exists in real-space and is what one would commonly understand as a physical lattice, the reciprocal lattice exists in reciprocal space (also known as momentum space or less commonly K-space, due to the relationship between the Pontryagin duals momentum and position.) The reciprocal lattice of a reciprocal lattice, then, is the original direct lattice again, since the two lattices are Fourier Transforms of each other. |
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