David G. Cory’s research while affiliated with Institute for Quantum Computing and other places

What is this page?


This page lists works of an author who doesn't have a ResearchGate profile or hasn't added the works to their profile yet. It is automatically generated from public (personal) data to further our legitimate goal of comprehensive and accurate scientific recordkeeping. If you are this author and want this page removed, please let us know.

Publications (471)


Quantitative diagnosis of amyloid without Congo red staining using polarized light microscopy
  • Preprint
  • File available

February 2025

·

16 Reads

Owen Lailey

·

Maria Agustina Alais

·

Liuhe Wang

·

[...]

·

Jelena Mirkovic

Amyloidosis is a protein misfolding disease caused by the deposition of large, insoluble aggregates (amyloid fibrils) of protein in a tissue, which has been associated with various conditions, such as lymphoid disorders, Alzheimer's disease, diabetes mellitus type 2, chronic inflammatory processes, and cancers. Amyloid fibrils are commonly diagnosed by qualitative observation of green birefringence from Congo red stained biopsy tissue samples under polarized light, a technique that is limited by lack of specificity, dependence on subjective interpretation, and technical constraints. Studies emphasize the utility of quantitative polarized light microscopy (PLM) methodology to diagnose amyloid fibrils in Congo red stained tissues. However, while Congo red enhances the intrinsic birefringence of amyloid fibrillar structures, there are significant disadvantages such as the appearance of multiple non-green colors under polarized light and binding to other structures, which may result in misdiagnoses with Congo red dye and inconclusive explanations. In this work, we present an improved PLM methodology for quantitative detection of amyloid fibrils without requiring Congo red staining. We perform PLM measurements on four tissues: abdominal subcutaneous tissue biopsy, duodenal biopsy, thyroid biopsy, and breast biopsy, both with Congo red stain and H\&E stain, and through Fourier analysis quantify birefringence, birefringent axis orientation, dichroism, optical activity, and relative amyloid density. These results emphasize a quantitative analysis for amyloid diagnosis rooted in Fourier signal harmonics that does not require Congo red dye and paves the way for rapid, simple, and accurate diagnosis of amyloid fibrils.

Download

SANS interferometry with OAM states
a Pictorial depiction of the implemented SANS interferometry with orbital angular momentum (OAM) states. Ref. ²⁵ showed that a single array of fork-dislocation phase gratings prepares helical waves in the diffraction orders that carry well-defined OAM values and manifest doughnut-like intensity profiles. Here, to observe the transverse phase profile of these helical waves, we create a coherent superposition between ℓ and −ℓ OAM states. Note that we have neglected the higher order interference as the direct beam is orders of magnitude brighter than the diffraction orders. b The general idea behind the SANS interferometry technique is to observe the phase profile of a structured neutron beam with non-trivial propagation characteristics. We consider an incoming neutron with wave vector k0 and two arrays with periodicity a and separation distance d. The array of reference beams needs to spatially overlap the array of object beams in order to interfere with the camera. Therefore, the amplitude of the reference beams needs to diffract similarly to the object beams. One straightforward approach to achieve this is by ensuring that the phase profile of the reference beams ϕR(x, y) and the object beams ϕO(x, y) possess a matching carrier wave vector kx, complementary structured phase profiles f(x, y), and enforcing a translational shift Δx that ensures overlap (See Eq. (1)).
Neutron helical wave interference
The observed petal-structure signatures of neutron helical wave interference in the first diffraction orders as the pitch and yaw of the double-sided arrays of fork-dislocation phase-gratings were varied. a We find agreement for a simulation that considers a transverse coherence length of σ⊥ = 3 μm and translational offsets between the two arrays of xi = 0, yi = 800 nm. b The SANS image after incrementing the pitch by ≈0.6 mrad corresponds to an updated offset of xi = 0 nm, yi = 961 nm. c The profile following an additional increment in yaw by ≈0.5 mrad corresponding to xi = −135 nm, yi = 961 nm. In this proof of principle experiment, the poor visibility is mainly attributed to the wavelength spread, as depicted in Fig. 3.
Modeling the effects of experimental parameters on the petal-structure interference
The effect of array structure, distance between the reference and object elements, phase shift between the two interfering OAM states, and wavelength distribution on the petal-structure intensity profile produced in the first diffraction order by the double-sided arrays of fork-dislocation phase gratings. a Considering an ideal coherent and monochromatic neutron beam incident on object and reference elements with negligible distance between them, one would be able to resolve the interference pattern that is both indicative of the OAM interference and the two-dimensional array structure. b Removing the higher order frequencies corresponding to the two-dimensional array structure results in the OAM petal structure being emphasized. c Increasing the distance between the reference and object elements to the experimental value of 280 μm introduces a phase shift and propagation diffraction that manifests a winding structure in the interference pattern. d Adding to the object beams an additional OAM dependent π phase shift effectively rotates the petal pattern of c. e Increasing the wavelength distribution to the experimental Δλ/λ ≈ 0.13 smears the interference pattern of c.
Small-angle scattering interferometry with neutron orbital angular momentum states

December 2024

·

75 Reads

·

1 Citation

Methods to prepare and characterize neutron helical waves carrying orbital angular momentum (OAM) were recently demonstrated at small-angle neutron scattering (SANS) facilities. These methods enable access to the neutron orbital degree of freedom which provides new avenues of exploration in fundamental science experiments as well as in material characterization applications. However, it remains a challenge to recover phase profiles from SANS measurements. We introduce and demonstrate a novel neutron interferometry technique for extracting phase information that is typically lost in SANS measurements. An array of reference beams, with complementary structured phase profiles, are put into a coherent superposition with the array of object beams, thereby manifesting the phase information in the far-field intensity profile. We demonstrate this by resolving petal-structure signatures of helical wave interference for the first time: an implementation of the long-sought recovery of phase information from small-angle scattering measurements.


Efficiently Characterizing the Quantum Information Flow, Loss, and Recovery in the Central Spin System

December 2024

·

9 Reads

Understanding the flow, loss, and recovery of the information between a system and its environment is essential for advancing quantum technologies. The central spin system serves as a useful model for a single qubit, offering valuable insights into how quantum systems can be manipulated and protected from decoherence. This work uses the stimulated echo experiment to track the information flow between the central spin and its environment, providing a direct measure of the sensitivity of system/environment correlations to environmental dynamics. The extent of mixing and the growth of correlations are quantified through autocorrelation functions of the noise and environmental dynamics, which also enable the estimation of nested commutators between the system/environment and environmental Hamiltonians. Complementary decoupling experiments offer a straightforward measure of the strength of the system Hamiltonians. The approach is experimentally demonstrated on a spin system.


Thermal state structure in the Tavis--Cummings model and rapid simulations in mesoscopic quantum ensembles

December 2024

·

8 Reads

Hybrid quantum systems consisting of a collection of N spin-1/2 particles uniformly interacting with an electromagnetic field, such as one confined in a cavity, are important for the development of quantum information processors and will be useful for metrology, as well as tests of collective behavior. Such systems are often modeled by the Tavis-Cummings model and having an accurate understanding of the thermal behaviors of this system is needed to understand the behavior of them in realistic environments. We quantitatively show in this work that the Dicke subspace approximation is at times invoked too readily, in specific we show that there is a temperature above which the degeneracies in the system become dominant and the Dicke subspace is minimally populated. This transition occurs at a lower temperature than priorly considered. When in such a temperature regime, the key constants of the motion are the total excitation count between the spin system and cavity and the collective angular momentum of the spin system. These enable perturbative expansions for thermal properties in terms of the energy shifts of dressed states, called Lamb shifts herein. These enable efficient numeric methods for obtaining certain parameters that scale as O(N)O(\sqrt{N}), and is thus highly efficient. These provide methods for approximating, and bounding, properties of these systems as well as characterizing the dominant population regions, including under perturbative noise. In the regime of stronger spin-spin coupling the perturbations outweigh the expansion series terms and inefficient methods likely are needed to be employed, removing the computational efficiency of simulating such systems. The results in this work can also be used for related systems such as coupled-cavity arrays, cavity mediated coupling of collective spin ensembles, and collective spin systems.


Figure 1. Target stimuli (top) with Nf=7, 12, 17 and 22 with ω=1.9, 3.8, 5.8 and 7.7 Hz, respectively, as viewed through an ideal polariser. Enface projection of the entoptic pattern with a central obstruction with radius RT and Nf=7 azimuthal fringes onto the retina (bottom)
Summary of interocular differences
Central obstruction radius RT for the various SL-based entoptic images with visible fringe numbers Nf=7, 12, 17, and 22 for the dominant and non-dominant eyes (DE & NDE)
Eye dominance and testing order effects in the circularly-oriented macular pigment optical density measurements that rely on the perception of structured light-based stimuli

November 2024

·

13 Reads

Psychophysical discrimination of structured light (SL) stimuli may be useful in screening for various macular disorders, including degenerative macular diseases. The circularly-oriented macular pigment optical density (coMPOD), calculated from the discrimination performance of SL-induced entoptic phenomena, may reveal a novel functional biomarker of macular health. In this study, we investigated the potential influence of eye dominance and testing order effects on SL-based stimulus perception, factors that potentially influence the sensitivity of screening tests based on SL technology. A total of 28 participants (aged 18-38 years) were selected for the study after undergoing a comprehensive eye examination. A psychophysical task was performed where various SL-based entoptic images with multiple azimuthal fringes rotating with a specific temporal frequency were projected onto the participants' retinas. By occluding the central areas of entoptic images, we measured the retinal eccentricity (R) of the perceivable area of the stimuli. The slope of the coMPOD profile (a-value) was calculated for each participant using a spatiotemporal sensitivity model that takes into account the perceptual threshold measurements of structured light stimuli with varying spatial densities and temporal frequencies. The Pearson correlation coefficient between eye dominance and testing order effects was r=0.8 (p<0.01p<0.01). The Bland-Altman plots for both factors indicated zero bias. The results indicate repeatable measurements for both eyes, implying minimal impact from eye dominance and testing order on SL-based stimulus perception. The results provide a foundation for future studies exploring the clinical utility of SL tools in eye health.


Figure 1. The Haidinger's brush pattern that is observed when a healthy person views polarized blue light. The orientation of the brush follows the orientation of the light's polarization direction (shown in red). Figure taken from Ref. [5].
Figure 2. Examples of phase and polarization profiles of structured light stimuli (left column) and the corresponding entoptic profiles that a participant with a healthy macula would observe (right column). Figure adapted from Ref [9].
Structured Light in Vision Science Applications

October 2024

·

45 Reads

The European Physical Journal Conferences

The dichroic macular pigment in the eye acts as a natural radial polarization filter and enables humans to directly perceive polarization-related entoptic phenomena. Linearly polarized blue light induces a subtle bowtie-like pattern known as Haidinger’s brush in the central point of vision. The clarity and shape of this perceived pattern are directly linked to the health of the macula, rendering Haidinger’s brush a potential diagnostic marker in research on early-stage age-related macular degeneration (AMD) and central field visual dysfunction. However, due to the faint nature of this signal, integrating the perception of Haidinger’s brush into modern clinical methods remains a challenge. Here we review some advances in techniques to increase the strength of the perceived signal by employing polarization coupled orbital angular momentum states. We successfully achieved the creation of stimuli with higher numbers of azimuthal fringes, enabling the perception and discrimination of Pancharatnam-Berry phases, measuring the visual angle of entoptic phenomena, retinal imaging using structured light, and the creation of radially varying entoptic stimuli. Our current studies are focusing on applying the structured light methods that we developed to subjects that suffer from ocular diseases such as AMD.


Fig. 1. Experimental setup using neutron SPP [12] shown on the left placed in path I of interferometer and the phase generated by SPP measured by 2D detector (false-color image on the right corresponds to SPP with topology equal to 3). By placing linear phase gradient (wedge) in path one the holography image could be generated as shown in [13].
Structured neutron waves and neutron holography

October 2024

·

38 Reads

The European Physical Journal Conferences

The development of advanced spintronics materials necessitates novel characterization tools with the ability to analyze nanometer-scale spin textures. Neutrons, with their angstrom-sized wavelengths, electric neutrality, and controllable spin states, are uniquely suited for this task. Recent research has prioritized expanding the capabilities of the “neutron toolbox” to effectively characterize emerging materials. This involves the development of holographic and tomographic techniques for 3D characterization of bulk spin textures, alongside methods for creating structured neutron beams with specific spin-orbit states like helical and skyrmion configurations. Here we provide a concise overview of these advancements, exploring their potential future applications.


FIG. 1. Interferometer crystals. Hera, the largest LLL crystal, is approximately 10 cm × 10 cm in size. Talos, the subject of this work, is the smallest.
FIG. 2. Neutrons entering the interferometer are split via the first diffracting blade (S) into two paths. The paths are again diffracted by a mirror blade (M). Lastly, the two paths interfere in an analyzer crystal (A). Any differences between the paths modulates the intensities I O and I H measured at the detectors. By rotating a phase flag by an angle δ one can vary I O and I H . Normally, the distances L 1,2 are significantly long enough such that the I 1 and I 4 beams escape the interferometer without striking the analyzer crystal. This is not the case for the interferometer Talos. Here neutron absorbing cadmium (Cd) sheets are placed behind the analyzer crystal to eliminate I 1 and I 4 from reaching the detectors.
FIG. 3. Interferograms of the maximum contrast observed in the I O beam for the initial and final stage of fabrication. The (•) symbols represent the I O intensity for the initial (final) stage. Lines are fits to the data using Eq. (4) and the uncertainties shown are purely statistical. See the text for a description the techniques used at each fabrication stage.
FIG. 8. Contrast maps of Talos. The color scale is the same throughout. (a) stage 0; an early contrast map of the interferometer. (b) stage 1; following a 5-minute acid etch. (c) stage 3; after the results in (b) the faces of the interferometer were refabricated and the crystal was annealed. Contrast decreased and a sweet spot appeared. (d) stage 12; high contrast as restored after re-fabricating the crystal surfaces. No data were taken at coordinate Z = 18 mm for (d).
FIG. 9. Phase maps of Talos for the same cases shown in Fig. 8. The color scale is the same throughout. White pixels in (a) and (c) correspond to areas of low contrast where φ uncertainties are greater or equal than ±20 • and have been omitted. No data were taken at coordinate Z = 18 mm for (d). In (c), a modulus of 2π is crossed in the middle.
Achieving a near-ideal silicon crystal neutron interferometer using submicrometer fabrication techniques

October 2024

·

32 Reads

Physical Review Research

Perfect-crystal neutron interferometry, which is analogous to Mach-Zehnder interferometry, uses Bragg diffraction to form interfering neutron paths. The measured phase shifts can be used to probe many types of interactions whether it be nuclear, electromagnetic, gravitational, or topological in nature. For a perfect-crystal interferometer to preserve coherence, the crystal must possess a high degree of dimensional tolerance as well as being relatively defect-free with minimal internal stresses. In the past, perfect-crystal neutron interferometers have been produced by a two-step process. First, a resin diamond wheel would be used to remove excess material and shape the interferometer. Afterword, the crystal would be etched to remove surface defects and elevate strains. This process has had limitations in terms of repeatability and in maximizing the final contrast, or fringe visibility, of the interferometer. We have tested various fabrication and post-fabrication techniques on a single perfect-crystal neutron interferometer and measured the interferometer's performance at each step. Here we report a robust, nonetching fabrication process with high final contrast. For the interferometer used in this work, we achieved contrasts of greater than 90% several times and ultimately finished with an interferometer that has 92% contrast and a uniform phase distribution. Published by the American Physical Society 2024


Robust Micro-Macro Entangled States

October 2024

·

3 Reads

Bipartite entangled states between a qubit and macroscopically distinct states of a mesoscopic system, known as micro-macro entangled states, are emerging resources for quantum information processing. One main challenge in generating such states in the lab is their fragility to environmental noise. We analyze this fragility in detail for single particle noise by identifying what factors play a role in the robustness and quantifying their effect. There is a trade-off between the macroscopicity of a micro-macro entangled state and the robustness of its bipartite entanglement to environmental noise. We identify symmetric micro-macro entangled states as the most robust states to single particle noise. We show that the robustness of bipartite entanglement of such states to single particle noise decreases as the second order of macroscopicity, which identifies a regime where the bipartite entangled state is both robust and macroscopic. Our result is a step towards retaining quantum characteristics on large scales and experimental realization of micro-macro entangled spin states and their use for connecting separated qubits. Moreover, it advances our understanding of quantum to classical transition.


FIG. 2. Example of a 2-up/1-down staircase protocol. The reversal points are marked with black points and crosses for clarity, and the change in the obstruction size with each trial is noted in each region. 10 pixels on the Spatial Light Modulator is around 0.45 • retinal eccentricity. After 14 staircase reversals or 90 trials, the arithmetic mean of the final six reversals (marked by black points) is taken to be the participant's threshold radius (blue dashed line) for the given stimulus.
FIG. 3. The average of the retinal eccentricity threshold results for the five different stimuli presented in this study: (N = 3, ω = 1.9 Hz), (N = 8, ω = 3.8 Hz), (N = 11, ω = 5 Hz), (N = 13, ω = 5.8 Hz), (N = 18, ω = 7.7 Hz). Also shown are the averages of threshold radii obtained through fitting the coMPOD Model for individual participants. The Pearson χ 2 fit statistic comparing the coMPOD model and the data is approximately 0.06, indicating a good fit.
FIG. 4. The obtained coMPOD parameter for each individual participant. The average a was found to be a = 0.08 • ± 0.02 • . Shown in dashed lines are ±1 standard deviation. Error bars on each data point denote an approximate 99.9% confidence interval.
Characterizing the circularly-oriented macular pigment using spatiotemporal sensitivity to structured light entoptic phenomena

September 2024

·

55 Reads

The macular pigment (MP) in the radially-oriented Henle fibers that surround the foveola enables the ability to perceive the orientation of polarized blue light through an entoptic phenomena known as the Haidinger's brush. The MP has been linked to eye diseases and central field dysfunctions, most notably age-related macular degeneration (AMD), a globally leading cause of irreversible blindness. Recent integration of structured light techniques into vision science has allowed for the development of more selective and versatile entoptic probes of eye health that provide interpretable thresholds. For example, it enabled the use of variable spatial frequencies and arbitrary obstructions in the presented stimuli. Additionally, it expanded the 2{\deg} retinal eccentricity extent of the Haidinger's brush to 5{\deg} for a similar class of fringe-based stimuli. In this work, we develop a spatiotemporal sensitivity model that maps perceptual thresholds of entoptic phenomenon to the underlying MP structure that supports its perception. We therefore selectively characterize the circularly-oriented macular pigment optical density (coMPOD) rather than total MPOD as typically measured, providing an additional quantification of macular health. A study was performed where the retinal eccentricity thresholds were measured for five structured light stimuli with unique spatiotemporal frequencies. The results from fifteen healthy young participants indicate that the coMPOD is inversely proportional to retinal eccentricity in the range of 1.5{\deg} to 5.5{\deg}. Good agreement between the model and the collected data is found with a Pearson χ2\chi^2 fit statistic of 0.06. The presented techniques can be applied in novel early diagnostic tests for a variety of diseases related to macular degeneration such as AMD, macular telangiectasia, and pathological myopia.


Citations (45)


... The Moiré effect [24], an optical phenomenon that occurs when two repetitive patterns or patterns with slightly different frequencies (such as grids or sinusoidal patterns) are overlaid at an angle or slightly displaced, has found applications in various fields including metrology [25], encryption [26][27][28], imaging [29,30], phase singularities [31] , neutron interferometry [32][33][34], photonics and optoelectronics [35][36][37]. Moreover, FSI can also be implemented by utilizing sinusoidal structured illumination patterns [38][39][40]. ...

Reference:

Moiré encryption and decryption in Fourier single-pixel imaging
Phase and contrast moiré signatures in two-dimensional cone beam interferometry

Physical Review Research

... These unique abruptly autofocusing characteristics allow their maximum intensity to increase dramatically at the focal point [5]. Recently, the production and manipulation of Fermion Airy beams have attracted considerable attention, particularly with respect to phenomena specific to electrons [10] and neutron [11]. Given the parallels between light waves and electronic de Broglie waves, both electron vortex beams [12], electron Airy beams [13,14] and electron Bessel beams [15] have been experimentally generated using holographic phase plates. ...

Generation of neutron Airy beams

... The Moiré effect [24], an optical phenomenon that occurs when two repetitive patterns or patterns with slightly different frequencies (such as grids or sinusoidal patterns) are overlaid at an angle or slightly displaced, has found applications in various fields including metrology [25], encryption [26][27][28], imaging [29,30], phase singularities [31] , neutron interferometry [32][33][34], photonics and optoelectronics [35][36][37]. Moreover, FSI can also be implemented by utilizing sinusoidal structured illumination patterns [38][39][40]. ...

Cone beam neutron interferometry: From modeling to applications

Physical Review Research

... Standard methods, such as Haidinger's brush (HB), have been limited in effectiveness due to weak signals, low contrast, restricted stimulus flexibility, and a narrow visual extent [2][3][4][5][6]. Using structured light (SL) techniques, light can be engineered to have distinct spatial polarisation states that elicit rich entoptic patterns and mitigate these limitations [7][8][9]. Notably, SL-induced entoptic phenomena with azimuthal fringes Nf ≥ 11 can be observed beyond the foveal region, extending up to ≈ 5° retinal eccentricity RT [7] compared to HB with RT ≈ 2° [1,2,4,6]. SL-based stimulus perception has the potential to be used as a diagnostic tool [3,10,11] for detecting early functional signs of macular degenerative diseases such as age-related macular degeneration (AMD) [12][13][14], type 2 macular telangiectasia (MacTel) [15][16][17], and pathologic myopia [18][19][20]. ...

Psychophysical discrimination of radially varying polarization-based entoptic phenomena
  • Citing Article
  • January 2024

Physical Review Applied

... Standard methods, such as Haidinger's brush (HB), have been limited in effectiveness due to weak signals, low contrast, restricted stimulus flexibility, and a narrow visual extent [2][3][4][5][6]. Using structured light (SL) techniques, light can be engineered to have distinct spatial polarisation states that elicit rich entoptic patterns and mitigate these limitations [7][8][9]. Notably, SL-induced entoptic phenomena with azimuthal fringes Nf ≥ 11 can be observed beyond the foveal region, extending up to ≈ 5° retinal eccentricity RT [7] compared to HB with RT ≈ 2° [1,2,4,6]. SL-based stimulus perception has the potential to be used as a diagnostic tool [3,10,11] for detecting early functional signs of macular degenerative diseases such as age-related macular degeneration (AMD) [12][13][14], type 2 macular telangiectasia (MacTel) [15][16][17], and pathologic myopia [18][19][20]. ...

Measuring the visual angle of polarization-related entoptic phenomena using structured light

... However, in many situations and for practical considerations, one does not require a full description of the quantum degrees of freedom of the mediating fields. Examples of these setups are the spin-coupling in electron pair resonance [1,2], nuclear magnetic resonance [3], among others. In general, effective non-relativistic direct-coupling theories are often used everywhere. ...

Electron spin resonance spectroscopy using a Nb superconducting resonator
  • Citing Article
  • November 2023

... The Hamiltonian is expressed in a letter format to show the division between the four standard spin-1 operators, S x/y , and "twisted" spin-1 operators, S ′ x/y = i[S y/x , S 2 z ], resulting from moving into the interaction frame of the internal Hamiltonian [30,31]. It is the presence of all four of these operators that allows for access to transition-selective control in the absence of an applied static magnetic field. ...

Optimal control theory techniques for nitrogen vacancy ensembles in single crystal diamond

Quantum Information Processing

... Studying the impact of eye testing order aids in identifying sources of variability and determining the technique's reliability and consistency [34][35][36]. The assessment of SL-based stimulus perception in a monocular context [3,[7][8][9][10][11]25,37] raises the possibility that the observer may exhibit task learning from one test to the next. Thus, it is important to ascertain potential learning effects. ...

Psychophysical and image-based characterization of macular pigment using structured light

Journal of Vision

... Phase information is sacrificed in detection since the far-field neutron intensity profile is proportional to the square modulus of the Fourier transform of the outgoing wave function. Recent work, inspired by computed tomography methods, examined phase recovery by employing multi-angle SANS measurements 16,17 . ...

Three-dimensional neutron far-field tomography of a bulk skyrmion lattice

Nature Physics

... Optical beams with transverse, position-dependent polarisation demonstrate a wide range of geometric, topological and singular features [1]. For instance, such a 2D polarisation pattern displays polarisation singularities, actively studied for over 40 years [2][3][4][5][6][7][8][9][10][11][12][13][14], notably C points of right-or left-handed circular polarisation, at which the polarisation azimuth and vibration phase are singular, and L lines of linear polarisation * Author to whom any correspondence should be addressed. ...

Roadmap on structured waves