Method of intrinsic spectral analysis and applications thereof
11680902 · 2023-06-20
Assignee
Inventors
Cpc classification
G01N21/6428
PHYSICS
G01N2015/1402
PHYSICS
International classification
Abstract
A library of known intrinsic spectra is provided to identify at least one known material in a sample of interest. The library includes individual intrinsic spectra channels defined by the assignment of intrinsic spectra of at least one known material, and combinations thereof, so that the assigned intrinsic spectra of each intrinsic spectra channel is correlated to at least one known material. The at least one known material is identified in the sample of interest when intrinsic spectra obtained from the sample of interest is matched to an assigned intrinsic spectra of an intrinsic spectra channel of the library of known intrinsic spectra.
Claims
1. A method of creating a library of known intrinsic spectra of known materials, said method comprising: obtaining intrinsic spectra of each known material of a plurality of known materials; generating a known intrinsic spectrum of totality by adding together the intrinsic spectra of each known material; individually subtracting the intrinsic spectra of said each know material, and all combinations thereof, from the intrinsic spectrum of totality to obtain a plurality of individual composite known intrinsic spectra resulting from said individual subtractions; and assigning the intrinsic spectra of each known material, the known intrinsic spectrum of totality and the plurality of individual composite known intrinsic spectra to define individual intrinsic spectra channels of said library of known intrinsic spectra, wherein the assigned intrinsic spectra of each intrinsic spectra channel is correlated to at least one known material of said plurality of known materials.
2. The method according to claim 1, wherein the intrinsic spectra of each known material is determined by adding at respective wavelengths the intensities of intrinsic absorption spectra and intrinsic emission spectra of said known material.
3. The method according to claim 2, wherein said intrinsic absorption spectra is obtained by multiplying by minus one (−1) the intensities of intrinsic excitation spectra of said known material.
4. The method according to claim 1, wherein said library of known intrinsic spectra further includes an intrinsic spectral channel corresponding to unknown intrinsic spectra.
5. The method according to claim 1, wherein said at least one known material comprises a fluorescent labeling material.
6. The method according to claim 5, wherein said individual intrinsic spectral channels represents fluorescence channels defined by a shape of known intrinsic spectra of said at least one known fluorescent labeling material.
7. The method according to claim 1, wherein the intrinsic spectra of at least one known material is determined directly from the at least one known material by means of intrinsic spectrometry instrumentation.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1) Further features and advantages of the invention will become apparent from the following detailed description taken in conjunction with the accompanying figures showing illustrative embodiments of the invention, in which:
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(13) Throughout the figures, the same reference numbers and characters, unless otherwise stated, are used to denote like elements, components, portions or features of the illustrated embodiments. The subject invention will be described in detail in conjunction with the accompanying figures, in view of the illustrative embodiments.
DETAILED DESCRIPTION OF THE INVENTION
(14) Recently, a new Intrinsic Hyper-Spectral Flow Cytometer has been proposed that does not use narrow band filters and dichroic mirrors to define its fluorescence channels. Rather, this new instrument generates intrinsic spectra of the individual cells, as described in U.S. Pat. No. 10,670,512 B1, incorporated herein by reference in its entirety. The analysis of intrinsic spectra obtained from a cell sample labeled with multiple fluorochromes starts with a physical de-convolution of the cell spectra where the irrelevant illumination, i.e., the illumination not absorbed by the cell, is eliminated, revealing the intrinsic spectrum of the cell. These intrinsic spectra contain the intrinsic absorption and emission components of each of the fluorochromes. This process is described in the U.S. Pat. Nos. 9,435,687, 10,670,512, and U.S. application Ser. No. 16/888,660, incorporated herein by reference in their entirety.
(15) Briefly explained, an instrument is calibrated. Each analyte passing through the excitation beam is correlated with its focused and defocused/diffused spectral data and processed by subtracting the defocused/diffused spectrum from the focused spectrum. The resulting spectra are averaged pixel by pixel across the wavelength range of the excitation energy to yield the Average Residual Spectrum (ARS) at the specific instrument settings. The ARS is then added back into each of the defocused/diffused spectra and the adjusted defocused/diffused set of spectra are subtracted from the focused spectra of each analyte, respectively. This process produces a Zero Order Spectrum (ZOS) for the analyte that has a zero value across its entire excitation wavelength range validating that the instrument is calibrated and ready to collect intrinsic spectral data. Without changing the instrument settings, the analyte of interest is run and the ARS from the calibration step is added to the spectra of each analyte of the defocused/diffused data stream. These adjusted defocused/diffused spectra are then subtracted from the corresponding focused spectra of each analyte. This procedure generates the intrinsic spectra of the analytes that contains both the absorption and fluorescence spectral components across the excitation wavelength range.
(16) Thus, the elimination of the irrelevant illumination is accomplished by either subtracting the defocused or the translucent/diffused spectrum from the illumination focused on the fluidic stream. Accordingly, the present invention validates and applies the de-convolution methodology that defines the fluorescence channels to which the intrinsic spectrum of each cell is matched.
(17) Construction of an Intrinsic Fluorescence Channel Library
(18) In general, the analysis of intrinsic spectra is based on comparison of the intrinsic spectra of a sample of interest to an intrinsic spectrum in a library of known spectra that are obtained directly from intrinsic spectrometry instrumentation from the known material of interest, as explained in U.S. Pat. Nos. 9,435,687, 10,670,512, and U.S. application Ser. No. 16/888,660, incorporated herein in their entirety by reference. Alternatively, as will be explained below, the intrinsic spectrum in a library of known spectra can be generated by intrinsic spectral construction through the composite/addition of the intrinsic components, e.g., absorption, excitation, emission, as determined by classical spectrometry instrumentation. It is also envisioned that a combination of both methods can be used together to construct the library of known spectra, where some of the known spectra is determined directly via intrinsic spectrometry instrumentation and other known spectra is determined via the composite/addition of the intrinsic components, as will be explained below.
(19) By definition, the unique fluorescent absorption and emission components of a dye are intrinsic since they do not contain any of the irrelevant spectral components of the illumination. The first step in creating an intrinsic fluorescence channel library requires the generation of the intrinsic spectrum of each fluorochrome from their absorption and emission components. The intrinsic spectrum of each fluorochrome is generated by adding the intensities of the respective absorption and emission components across the entire wavelength range of the illumination, as shown in
(20) The fluorescence channels representing each intrinsic spectrum of the single and combined fluorochrome labels are equivalent to those normally defined by narrow band pass filters and represented as the axes of two-dimensional dot plots shown in
IS(FITC)=[IS(FITC)+IS(PE)]−IS(PE) (1)
IS(PE)=[IS(FITC)+IS(PE)]−IS(FITC) (2)
(21) The traditional dot plot format for immunophenotyping works only up to three fluorochromes. The number of 2D dot plots can become overwhelming and confusing especially attempting to represent multi-dimensional dot plots.
(22) This situation may be represented mathematically by the equation that describes combinations:
Number of combinations=(n!/r!(n−r)!) (2)
(23) where: n is the number of fluorochromes, and r is the number of fluorochromes taken in combination per dot plot.
(24) For example, if there are three fluorochromes used, the number of 2D dot plots required are:
Number of 2D Dot Plots=3!/2!(3−2)!=(3×2×1)/(2×1)×(1)=6/2=3
(25) However, if there are ten fluorochromes are present, then the number of 2D dot plots required are:
Number of 2D Dot Plots=10!/2!(10−2)!=(10×9)/(2×1)=90/2=45
(26) Application of Intrinsic Fluorescence Channel Library
(27) As the demand increased for poly-chromatic immunophenotyping, automated software-implemented solutions to manage multi-dimensional color compensation were required. With the implementation of multi lasers and dozens of dyes, such immunophenotyping strategy was impractical. Ten fluorochromes generates forty-five 2D dot plots, a situation which is not trivial in terms of gating and re-gating to isolate specific sub-populations of cells. This traditional dot plot approach would require generating an additional larger number of difficult to visualize 3D and higher dimensionality dot plots that represent cell populations that bind combination of three or more different fluorescence labels.
(28) However, the present invention solves these problems following returning principles of data management. The basic analytical data required for immunophenotyping: (1) isolation of cell populations (2) report the number of cells in each analyzed population (3) report fluorescence intensity distribution of cell populations of interest
(29) The use of intrinsic spectra according to the present invention to define fluorescence channels provides a simple solution to obtaining these data.
(30) For example, consider a library of fluorescence channels for ten fluorochromes that for practical purposes, is limited to cells that bind four or less different fluorochrome labeled antibodies that would generate the following channels plus one channel for unlabeled cell populations:
(31) TABLE-US-00001 TABLE 1 Number of Intrinsic Fluorescence Channels 10!/1!(10-1)! 10 10!/2!(10-2)! 45 10!/3!(10-3)! 120 10!/4!(10-4)! 210 Unlabeled 1 Total 386
(32) To employ the de-convolution methodology of fluorescing cells according to the invention, a complete library of known intrinsic fluorescence channels is pre-determined and are stored in the instrument's computer. Alternatively, the complete library of known intrinsic fluorescence channels is stored remotely from the instrument.
(33) In accordance to a preferred embodiment in flow cytometry, as the cells pass through the interrogation point, the intrinsic spectrum of each cell is compared to the whole intrinsic spectrum, with respect to the wavelength positions of maxima, minima and profile, i.e., shape, of the intrinsic spectra in the library of known intrinsic spectra that is defining a particular fluorescence channel. Each labelled cell is assigned to its matching fluorescence channel. The number of cells that fall within each of the single and multiple intrinsic fluorochrome channels is directly determined without the use of error prone subjective gates. Antibody binding capacity (ABC) of each cell population can be represented by an intensity histogram of each intrinsic fluorescence channel, respectively.
(34) This methodology provides precisely defined fluorescence channels for the intrinsic flow cytometer libraries because the individual contributions of intrinsic components of the spectra are determined by the excitation and emission components determined by spectrofluorometers. The intrinsic components of each fluorochrome can be combined into its respective spectrum. By combining the intrinsic spectra of the fluorochromes in an assay, all the intrinsic spectra added, generates the intrinsic spectrum of totality for the assay. By de-convoluting the intrinsic spectrum of totality, a library of known intrinsic spectra can be produced that represent all of fluorescence channels representing the individual fluorochromes, as well as, any combination of fluorochrome labeled cell populations, thereof.
(35) Although in accordance to a preferred embodiment, these methodologies were developed for intrinsic flow cytometers, they are not limited to this instrumentation. It should be noted that intrinsic flow cytometry presents the most well-defined application considering the small number of fluorochromes used in any assay, and whose intrinsic spectra can easily be generated since all of their intrinsic components, excitation (absorption) and emission are easily determined with a spectrofluorometer.
(36) In the case of Intrinsic Imaging instruments, i.e., cameras, that produce intrinsic spectra associated with each pixel of a field of view, many of the contributing intrinsic spectra may be unknown, so identification of all the materials in an image may not be feasible. However, the de-convolute methodology of the present invention provides a powerful tool to positively determine the presence or absence of the specific materials of intrinsic spectra. The intrinsic spectra of the library can be compared to the intrinsic spectrum associated with each pixel of an multi-spectral or hyper-spectral image to determine the spatial location and associations of these known materials in the image. These locations can, for example, be presented in an isolation display by assigning an intensity value of zero to all pixels in the image that do not have a match with intrinsic spectra in the Library. The resulting image of matching pixels appear as they do in the original image, but on a black background. Alternatively, the intensity value of the matching pixels can be increased by an appropriate factor, e.g., a factor of 2 to 10 times, to have the known material or materials clearly stand out in the image.
(37) It is to be understood, that according to another embodiment of the present invention, the library of known intrinsic spectra can also comprise of a single intrinsic spectral channel assigned to the intrinsic spectra of at least one known material of interest.
EXAMPLES
(38) In these examples, excitation and emission spectra wavelength range covered UV to near IR (300-949 nm). The data was obtained from a ThermoFisher SpectraViewer (thermofisher.com). The excitation spectra were converted to absorption spectra by multiplying the excitation intensities by minus one (−1). Both the absorption and emission spectra met the criteria of being intrinsic spectral components since they were devoid of irrelevant illumination spectral components.
Example 1: De-Convolution Methodology of Intrinsic Spectral Components
(39) Since an intrinsic fluorescence spectrum contains only spectral components that are generated from absorption of illumination energy, it follows that an intrinsic spectrum is the sum of intrinsic spectral components, specifically, absorption and emission. Therefore, adding the absorption and emission spectral components of a fluorochrome will produce the intrinsic fluorescence spectrum of the fluorochrome, as illustrated with fluorescein in
Example 2: De-Convolution Methodology of Intrinsic Spectra
(40) Similar to Example 1, intrinsic spectra can be added together to form composite intrinsic spectra. For example, the Intrinsic Spectra of Totality comprised of FITC, PE and Percp-Cy5.5 can be formed by adding the intrinsic spectrum of each fluorochrome together, as illustrated in
Example 3: Construction of a Simple Intrinsic Fluorescence Channels Library
(41) A library of fluorescence reference channels was created for FITC, PE and Percp-Cy5.5. These three intrinsic spectra, as generated in Example 1, are then added together to form an Intrinsic Spectrum of Totality. This intrinsic spectrum of totality was then de-convoluted to create the three double-labeled fluorescence channels that represent the other combinations of possible fluorescence binding to cells in this assay, as illustrated in
Example 4: Simulation of an Intrinsic Spectral Analysis Report of a Multi Fluorochrome Labeled Blood
(42) Health human blood is stained with FITC-CD3 and PE-CD4 and Percp-Cy5.5-CD8 antibodies. The intrinsic flow cytometer detects the intrinsic spectrum of each cell that passes through the fluorescence detection system. The intrinsic spectrum of each cell is matched with one of the intrinsic fluorescence channels in the Library of Known Intrinsic Fluorescence Channels previously generated in Example 3. Each matched cell, along with its intensity, is assigned to its respective fluorescence channel. The analysis reports the number of cells in each channel and a plotted of their intensity as a simple histogram, as illustrated in
Example 5: Simulation of the De-Convolution Methodology Applied to Imaging
(43) An intrinsic hyper-spectral image is obtained of a field of view that is suspected of containing several specific known materials. The intrinsic image is generated by removing the irrelevant illumination as described in U.S. Pat. No. 10,652,484 or U.S. application Ser. No. 16/888,660, incorporated herein in their entirety by reference. This is accomplished by taking a focused image of the field of view, as seen in
(44) Although the present invention has been described herein with reference to the foregoing exemplary embodiment, this embodiment does not serve to limit the scope of the present invention. Accordingly, those skilled in the art to which the present invention pertains will appreciate that various modifications are possible, without departing from the technical spirit of the present invention.