Informatics & Technology

A new computational approach to Digital Holographic Microscopy

Digital Holographic Microscopy offers a unique way for researchers to precisely examine the 3D topography of microscopic objects. However, until now the capabilities of this technique have been limited by complications involving the complex computational method used. The Optical Imaging Research Laboratory at the University of Memphis, led by Dr Ana Doblas, and collaborators have constructed algorithms which can automatically reconstruct 3D topography without any user expertise. Their work could offer new opportunities for using the technique in research areas ranging from materials physics to biomedical imaging.

 

Researchers have a wealth of techniques at their disposal for recording images of objects under a microscope. By measuring how light is shifted, scattered, and absorbed by samples, they can often determine the 3D topologies of microscopic objects in precise levels of detail. However, these techniques are not always entirely suitable for imaging transparent objects, such as living cells or artificial crystals. Without any way for researchers to determine the precise positions of the features contained within these samples, their results are likely to be less reliable.

This problem has now created an incentive to develop techniques which can directly create 3D digital images of entire transparent objects. To do this, researchers can use ‘Digital Holographic Microscopy’ (DHM) – through which a uniform laser beam is first split into an ‘object’ and a ‘reference’ beam. As it interacts with the transparent sample, the object beam is then scattered to varying degrees, depending on the depth to which it penetrated into the sample. Finally, these scattered wavefronts are collected by a microscope lens, and merged with the reference beam. Based on its unique pattern, a computer can then calculate a transparent, 3D image of the object using a specialised reconstruction algorithm.

Fig. 1: The panels are: (a) True complex (amplitude and phase) distributions of the simulated object. (b) Hologram and its Fourier transform using a reference slightly tilted. (c) The Fourier transform of the demodulated components provided by the estimated phase shift of our approach. (d) The Fourier transform of the d1 demodulated components by spatial filtering of D3 and estimated phase image via inverse filtering D1 after compensating the interference angle. The quantitative phase image obtained from the demodulated component d+1. The true phase steps was Δφ’ = 60, and the estimated Reduced Phase was 60.003 deg. The mean square error between the true and the estimated phase images is 1.56×10-6. Note that, using simulated data, the accuracy of the estimated phase is higher using 3 images than 2 images. But, maybe this difference is insignificant within the experimental noise.

From these digital reconstructions, researchers can precisely analyse the 3D structures contained within transparent microscopic objects. Currently, however, the quality and accuracy of the digital reconstructions are highly dependent on the computational approach and the user’s expertise in selecting the correct parameters, introducing an unavoidable source of human error. So far, this shortcoming has limited the application of DHM in cutting-edge studies, including materials physics and biomedical imaging. A new computational DHM reconstruction method must be proposed before DHM can become more widely adopted.

Overlapping orders
When a simple laser beam passes through a diffraction grating, and the resulting interference pattern is projected onto a screen, a bright peak in light intensity will appear in the centre of the pattern, where the beam would have shone if the grating were not there. However, other pairs of brightness peaks will also appear at regular intervals to either side of this central spot, whose widths, intensities, and spacings will vary both with the light’s wavelength and the spacing between gaps in the grating. Subsequently, peak pairs at successively larger distances from the centre are described as having progressively higher ‘orders’ of diffraction.

Although the random speckled patterns recorded by DHM are far more complex than single laser beams, they still abide by the same physical laws. This means that any peaks in brightness will be surrounded by three detectable orders of diffraction. Since microscopic target objects such as cells and crystal structures can have complex, arbitrary shapes, the paths taken by the light scattered off them will vary widely and unpredictably. Ultimately, this leads to substantial difficulties when interpreting their resulting interference patterns.

“The angle between the reference and object waves entails the possibility to operate under three different DHM architectures: in-line, slightly off-axis, or off-axis”, explains Dr Ana Doblas, principal investigator of the Optical Imaging Research Laboratory at the University of Memphis. “In slightly off-axis and in-line DHM systems, the three diffraction orders that compose the hologram spectrum are overlapped.” Without any way of knowing the extent to which this overlapping occurs, it is impossible for algorithms to reconstruct images effectively. So far, accounting for this problem has required a cumbersome set of techniques.

Fig. 2: The panels are: (a) True complex (amplitude and phase) distributions of the simulated object. (b) Hologram and its Fourier transform using a reference slightly tilted. (c) The Fourier transform of the demodulated components provided by the estimated phase shift of our approach. (d) The quantitative phase image obtained from the demodulated component d+1. The true phase steps were Δφ2’ = 60 and Δφ3’ = 180 degrees, respectively. The estimated Reduced Phase: Δφ2’ = ϕ1 – ϕ2 = 1.0472 rad = 60.00014 deg and Δφ3’ = ϕ1 – ϕ3 = 3.1416 rad = 180.0004209 deg. The values of the mean-square-error between the true object phase and the retrieved one is 5.5339e-16, almost null.

Struggles with phase-shifting
In wave terminology, two waves with the same frequency are said to be ‘phase shifted’ if their points of highest and lowest amplitude are misaligned as they propagate. If two such waves are propagating together, they will destructively interfere with each other to reduce the light intensity seen by an observer – to an extent which depends on just how out of phase they are. On microscopic scales, comparable to the wavelengths of visible light, this principle can be exploited to determine precise distances.

If Dr Doblas’ techniques become more widely adopted, they could greatly improve the applicability of advanced microscopy.

Through the technique of Phase-Shifting DHM (PS-DHM), images with different phase shifts can be created alongside the main image. From these resulting ‘phase maps’, reconstruction algorithms can better calculate distances from the camera to different parts of the target object – enabling more accurate 3D images. To an extent, PS-DHM allows researchers to mitigate the effects of overlapping diffraction orders, but the approach comes with its own limitations. “Phase-shifting techniques are needed to recover complex object information, imposing the need for multiple hologram recordings”, Dr Doblas describes. “Conventional PS-DHM methods require the accurate knowledge of the phase shifts between the recorded holograms. However, experimentally such accuracy is frequently arduous, leading to the use of inexact values of the phase shift which produce distorted and unreliable phase maps.”

Digital Holographic Microscopy (DHM)

In turn, image reconstruction algorithms are provided with a less reliable basis, leading to less accurate images and, subsequently, limiting the practicality of PS-DHM in the lab. Through their research, Dr Doblas and her collaborators aim to minimise the number of recordings needed and to develop a more advanced set of algorithms to ease the use of PS-DHM for inexperienced users.

Incorporating blind algorithms
In a 2020 study, the research group describes a basis for algorithms which take a more trial-and-error approach to phase shifting. These programs first take in mathematical approximations of hologram interference patterns, then make blind, repeated attempts to accurately recover the information they contain until their outcomes can no longer be improved. This significantly reduces the number of phase-shifted holograms required for the process. “As an alternative of conventional PS-DHM algorithms, blind phase-shifting algorithms do not need the accurate knowledge of phase shifts”, Dr Doblas explains. “We present two phase-shifting algorithms for accurate quantitative phase images in PS-DHM. The proposed methods operate with at most three phase-shifted holograms.”

Through their latest experiments, Dr Doblas’ team has now clearly demonstrated four distinct advantages of their algorithms, compared with previous approaches to PS-DHM. Firstly, they can work effectively with a minimal number of recorded holograms since they don’t require an accurate knowledge of phase shifts. Secondly, they produce a minimal error in calculated phase shifts, approaching just 0.005%. Thirdly, the algorithms produce the maximum possible correlation between the phase shift of each image, and the phase of the actual image received after processing. Finally, they require significantly lower processing time compared with previous approaches.

Bringing DHM to the lab
Thanks to these numerous benefits, Dr Doblas and her collaborators now hope to extend their approach to holograms of complex microscopic systems which move and change shape over time. “The hallmarks of our methods are accuracy, and reduced acquisition and processing times leading to a PS-DHM system more suitable for dynamic imaging, as is the case of live cell imaging and colloidal systems”, she concludes.

If Dr Doblas’ techniques become more widely adopted, they could greatly improve the applicability of an advanced microscopy technique which has, until recently, been viewed as impractical by many researchers. Ultimately, they could soon improve research opportunities for groups ranging from physicists studying the intricate crystal structures of advanced artificial materials to biologists imaging the time-varying behaviours of microscopic living systems.

Personal Response

What advantages could be offered through your approach to PS-DHM when compared with more conventional microscopy techniques?

Advantages include the reduced number of acquisition images, resulting in a more suitable approach for dynamic samples, as well as an automatic approach without prior knowledge of the user. The latter would allow researchers to investigate the samples without knowledge in DHM, leading to a commercial prototype.

This feature article was created with the approval of the research team featured. This is a collaborative production, supported by those featured to aid free of charge, global distribution.

Want to read more articles like this?

Sign up to our mailing list and read about the topics that matter to you the most.
Sign Up!

Leave a Reply

Your email address will not be published. Required fields are marked *

Thank you for expressing interest in joining our mailing list and community. Below you can select how you’d like us to interact with you and we’ll keep you updated with our latest content.

You can change your preferences or unsubscribe by clicking the unsubscribe link in the footer of any email you receive from us, or by contacting us at audience@researchoutreach.org at any time and if you have any questions about how we handle your data, please review our privacy agreement.

Would you like to learn more about our services?

We use MailChimp as our marketing automation platform. By clicking below to submit this form, you acknowledge that the information you provide will be transferred to MailChimp for processing in accordance with their Privacy Policy and Terms.

Subscribe to our FREE PUBLICATION