![3.4 非對(duì)稱的非晶態(tài)物質(zhì)穆斯堡爾譜的擬合法<sup>[18]</sup>](https://imgs.zsbeike.com/imgs/E/E03020/e03020.0166.6[15f4535ad36f].png)
 由于非對(duì)稱的非晶態(tài)物質(zhì)的穆斯堡爾譜存在著超精細(xì)場(chǎng)Hhf,四極分裂ΔEQ和同質(zhì)異能移位δ。假定,如果電場(chǎng)梯度軸向不對(duì)稱(η=0),則某個(gè)Hhf的亞譜的峰位為式中αK和βK為Hhf和ΔEQ對(duì)譜線峰位的影響系數(shù)。a,b,c和d四個(gè)常數(shù)的大小和正負(fù)決定 (共 308 字) [閱讀本文] >>
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![3.4 非對(duì)稱的非晶態(tài)物質(zhì)穆斯堡爾譜的擬合法<sup>[18]</sup>](https://imgs.zsbeike.com/imgs/E/E03020/e03020.0166.6[15f4535ad36f].png)
 由于非對(duì)稱的非晶態(tài)物質(zhì)的穆斯堡爾譜存在著超精細(xì)場(chǎng)Hhf,四極分裂ΔEQ和同質(zhì)異能移位δ。假定,如果電場(chǎng)梯度軸向不對(duì)稱(η=0),則某個(gè)Hhf的亞譜的峰位為式中αK和βK為Hhf和ΔEQ對(duì)譜線峰位的影響系數(shù)。a,b,c和d四個(gè)常數(shù)的大小和正負(fù)決定 (共 308 字) [閱讀本文] >>
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