| Literature DB >> 31849205 |
Andy J Chen1, Kai-Chih Huang2,3, Selina Bopp4, Robert Summers4, Puting Dong2, Yimin Huang2, Cheng Zong2, Dyann Wirth4, Ji-Xin Cheng2,3,5.
Abstract
Hemozoin, the heme detoxification end product in malaria parasites during their growth in the red blood cells (RBCs), serves as an important marker for diagnosis and treatment target of malaria disease. However, the current method for hemozoin-targeted drug screening mainly relies on in vitro β-hematin inhibition assays, which may lead to false-positive events due to under-representation of the real hemozoin crystal. Quantitative in situ imaging of hemozoin is highly desired for high-throughput screening of antimalarial drugs and for elucidating the mechanisms of antimalarial drugs. We present transient absorption (TA) imaging as a high-speed single-cell analysis platform with chemical selectivity to hemozoin. We first demonstrated that TA microscopy is able to identify β-hematin, the artificial form of hemozoin, from the RBCs. We further utilized time-resolved TA imaging to in situ discern hemozoin from malaria-infected RBCs with optimized imaging conditions. Finally, we quantitatively analyzed the hemozoin amount in RBCs at different infection stages by single-shot TA imaging. These results highlight the potential of TA imaging for efficient antimalarial drug screening and drug mechanism investigation.Entities:
Keywords: chemical imaging; hemozoin; label-free imaging; malaria; transient absorption microscopy
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Year: 2019 PMID: 31849205 PMCID: PMC6916744 DOI: 10.1117/1.JBO.25.1.014507
Source DB: PubMed Journal: J Biomed Opt ISSN: 1083-3668 Impact factor: 3.170
Fig. 3Time-resolved TA imaging and phasor analysis differentiates hemozoin from hemoglobin in RBCs. (a) Raw TA images and decay curves of malaria-infected RBCs. Sample: RBCs infected with P. falciparum; ; laser power: 10 mW for each beam. Left panel: images at zero-time delay; scale bar: ; image display range: 0.02 to 0.5; RBC and hemozoin selected for generating decay curves were indicated with arrows. Right panel: raw TA decay curves of RBC and hemozoin; an area of about 100 pixels from both indicated objects were selected to plot the decay curves. The curves were smoothed by averaging among five nearby data points. (b) Mapping result retrieved from phasor analysis of data in (a). Left panel: retrieved images; red: RBC; green: hemozoin; scale bar: . Right panel: retrieved decay curves of hemozoin and RBCs; intensity was normalized to 1.0. (c) Phasor plot retrieved from phasor analysis of data in (a). Dots within red box: RBCs; dots within green box: hemozoin.
Fig. 1TA microscopy spectroscopically differentiates -hematin from hemoglobin in RBCs. (a) SEM image of synthesized -hematin. (b) Raman spectrum of -hematin: laser wavelength: 785 nm; laser power: 35 mW on the sample; dwell time: 10 s; objective: air; pinhole size: , grating: . (c) Time-resolved pump–probe images of -hematin and RBC mixture. Left panel: ; right panel: ; all images are at zero-time delay, dynamic range: 0.25 to 0.73; graphs are the decay curves of the -hematin and RBCs indicated by the arrows (green and red, respectively); laser power: 10 mW for each beam; pixel dwell time: ; water objective. (d) Phasor analysis outputs of the images in (c). (c)–(d) Left panel: ; right panel: . (c)–(d) Top panel: retrieved images from phasor analysis (-hematin is artificially colored green and RBCs in red); bottom panel: graphs are retrieved pump–probe spectra from phasor analysis.
Fig. 2Hemozoin TA signal dependence on excitation laser wavelength. (a) TA images of hemozoin using 680/1040 and as the pump/probe wavelengths, respectively. Sample: RBCs infected with P. falciparum 3D7 strain; laser power: 10 mW for each beam; scale bar: ; pixel dwell time: . Left panel: ; dynamic range: 0.1 to 1.8; right panel: ; dynamic range: 0.1 to 0.7. (b) SNR of TA signal using different pump wavelengths. Sample was a single hemozoin crystal from RBCs infected with P. falciparum 3D7. Probe beam wavelength: 1040 nm; laser power: 10 mW for each beam, pixel dwell time: ; SNR was calculated by first determining the intensity difference of a fixed area of hemozoin and an equal area of the RBC, then dividing the intensity difference by the standard deviation of the RBC.
Fig. 4Quantitative analysis of hemozoin in RBCs at different stages of malarial infection. (a) Representative single-shot TA images of infected RBCs. Sample: RBCs infected with P. falciparum 3D7 0, 12, 24, 36, and 48 h after invasion; since individual P. falciparum differs during synchronization and infection process, there is a range of 6 h at the beginning of synchronization, which expands to 12 h starting from 48 h after synchronization. Consequently, the time points were denoted as 0 to 6, 12 to 18, 24 to 30, 36 to 42 and 48 to 54 h; image was taken at zero-time delay; pump/probe: ; laser power: 30 mW for each beam; scale bar: ; pixel dwell time: ; (b) large area mapping of samples in (a). Images were artificially colored red; representative hemozoin crystals were indicated by arrows; scale bar: ; displaying ranges were adjusted to standardize the RBCs: 0 to 6 h = 0.03 to 0.23, 12 to 18 h = 0.02 to 0.2, 24 to 30 h = 0.01 to 0.34, 36 to 42 h = 0.03 to 0.48, 48 to 54 h = 0.03 to 0.23. (c) The graph of the number of hemozoin crystals at different time points after infection; crystal number was normalized to 1000 RBCs. (d) The graph of the size of hemozoin crystal at different time points after infection. Hemozoin crystal size was determined by applying a threshold to filter out RBC background and then the total number of pixels of the hemozoin is converted into square micrometers.