Abstract

A shift-invariant variational autoencoder (shift-VAE) is developed as an unsupervised method for the analysis of spectral data in the presence of shifts along the parameter axis, disentangling the physically-relevant shifts from other latent variables. Using synthetic data sets, we show that the shift-VAE latent variables closely match the ground truth parameters. The shift VAE is extended towards the analysis of band-excitation piezoresponse force microscopy data, disentangling the resonance frequency shifts from the peak shape parameters in a model-free unsupervised manner. The extensions of this approach towards denoising of data and model-free dimensionality reduction in imaging and spectroscopic data are further demonstrated. This approach is universal and can also be extended to analysis of x-ray diffraction, photoluminescence, Raman spectra, and other data sets.

Highlights

  • A shift-invariant variational autoencoder is developed as an unsupervised method for the analysis of spectral data in the presence of shifts along the parameter axis, disentangling the physically-relevant shifts from other latent variables

  • The response curve is fitted by a simple harmonic oscillator (SHO) model, and the derived response amplitude, resonance frequency, and quality factor are visualized as a function of spatial coordinates or control parameters such as voltage and time in complex spectroscopies

  • Of interest is the development of unsupervised machine learning methods capable of analysis of band excitation (BE) data, and extendable to other similar data sets such as those emerging in X-Ray scattering, mass-spectrometry, or optical and Raman spectroscopies

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Summary

Introduction

A shift-invariant variational autoencoder (shift-VAE) is developed as an unsupervised method for the analysis of spectral data in the presence of shifts along the parameter axis, disentangling the physically-relevant shifts from other latent variables. A heat map in Figure 2e shows the number of components required to represent the data as a function of the maximum noise level and maximum shift μ0.

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