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伪沃伊特峰形峰值参数估计的精度:一种通过混合参数控制实现高精度分析的新型优化方法。

Precision in Peak Parameter Estimation for the Pseudo-Voigt Profile: A Novel Optimization Approach for High-Precision Analysis via Mixing Parameter Control.

作者信息

Hagiwara Yuuki, Kuwatani Tatsu

机构信息

Research Institute for Marine Geodynamics, Japan Agency for Marine-Earth Science and Technology, Yokosuka 237-0061, Japan.

出版信息

ACS Meas Sci Au. 2025 Jun 17;5(4):497-510. doi: 10.1021/acsmeasuresciau.5c00030. eCollection 2025 Aug 20.

DOI:10.1021/acsmeasuresciau.5c00030
PMID:40861916
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC12371587/
Abstract

High-precision measurement of peak parameters such as intensity (), peak position (ω ), full width at half-maximum (Γ), and area () is pivotally important for advancing scientific research. Achieving high-precision requires elucidating the physical principles governing measurement precision and establishing guidelines for optimizing analytical conditions. Although the pseudo-Voigt profile is a widely used line-shape model, the underlying principles governing the precision of its parameter estimation remained unclear. For this study, we developed a model to quantify the parameter estimation precision under arbitrary conditions by integrating theoretical analysis, numerical calculations, and Monte Carlo simulations. Our quantification results indicate that when the mixing parameter (η) is fixed, the precision of , Γ, and is proportional to {Δ/Γ}, whereas the precision of ω is proportional to {ΓΔ/}, where Δ denotes the sampling interval. Furthermore, the analytical precision exhibits η-dependence: for and Γ, when the profile becomes more Lorentzian, the absolute value of the covariance between Γ and η as well as between and η increases, thereby degrading their estimation precision. This finding suggests that in addition to conventional methods such as improving the signal-to-noise ratio and reducing sampling interval, appropriately controlling η can be an effective strategy for optimizing precision. For instance, if broadening effects (e.g., instrumental or Doppler broadening) are deliberately introduced to tune η from 1 to 0, then this alone improves Γ estimation precision by a factor of 3.7, equivalent to a 14-fold increase in signal intensity. Furthermore, when the effect of increased Γ due to broadening is considered, even greater improvements in precision can be achieved. Overall, our model provides a foundational framework for research on peak parameter estimation. It serves as an alternative approach to error estimation when experimental evaluation is challenging and as a quantitative tool for assessing precision gain from instrument upgrades.

摘要

对诸如强度()、峰位(ω )、半高宽(Γ)和面积()等峰值参数进行高精度测量对推动科学研究至关重要。实现高精度需要阐明控制测量精度的物理原理,并建立优化分析条件的指导方针。尽管伪沃伊特轮廓是一种广泛使用的线形模型,但其参数估计精度的基本原理仍不清楚。在本研究中,我们通过整合理论分析、数值计算和蒙特卡罗模拟,开发了一个模型来量化任意条件下的参数估计精度。我们的量化结果表明,当混合参数(η)固定时,、Γ和的精度与{Δ/Γ}成正比,而ω 的精度与{ΓΔ/}成正比,其中Δ表示采样间隔。此外,分析精度表现出η依赖性:对于和Γ,当轮廓变得更接近洛伦兹分布时,Γ与η以及与η之间协方差的绝对值增加,从而降低它们的估计精度。这一发现表明,除了提高信噪比和减小采样间隔等传统方法外,适当控制η可以是优化精度的有效策略。例如,如果故意引入展宽效应(如仪器展宽或多普勒展宽)将η从1调整到0,那么仅此一项就能将Γ估计精度提高3.7倍,相当于信号强度增加14倍。此外,当考虑展宽导致的Γ增加的影响时,可以实现更高的精度提升。总体而言,我们的模型为峰值参数估计研究提供了一个基础框架。当实验评估具有挑战性时,它可作为误差估计的替代方法,并且作为评估仪器升级带来的精度提升的定量工具。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/b3af11468894/tg5c00030_0007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/41bbad7e30b0/tg5c00030_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/c5cc5bda6900/tg5c00030_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/2f9758d92288/tg5c00030_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/9d9b2c0d9ee6/tg5c00030_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/4797c6e40e91/tg5c00030_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/c5ee4f823f99/tg5c00030_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/b3af11468894/tg5c00030_0007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/41bbad7e30b0/tg5c00030_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/c5cc5bda6900/tg5c00030_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/2f9758d92288/tg5c00030_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/9d9b2c0d9ee6/tg5c00030_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/4797c6e40e91/tg5c00030_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/c5ee4f823f99/tg5c00030_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b216/12371587/b3af11468894/tg5c00030_0007.jpg

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