{"id":26,"date":"2023-10-26T14:20:33","date_gmt":"2023-10-26T18:20:33","guid":{"rendered":"https:\/\/sites.bu.edu\/cheng\/?page_id=26"},"modified":"2025-11-12T15:31:12","modified_gmt":"2025-11-12T20:31:12","slug":"publications","status":"publish","type":"page","link":"https:\/\/sites.bu.edu\/cheng\/publications\/","title":{"rendered":"Publications"},"content":{"rendered":"<p><a href=\"https:\/\/scholar.google.com\/citations?user=055Ri_0AAAAJ&amp;hl=en\">Complete publication list<\/a><\/p>\n<p><strong>Selected journal publications:<\/strong><\/p>\n<p><span>Kim, B.K., Howard, A.C., Cheng, T.Y.\u00a0<\/span><i>et al.<\/i><span>\u00a0<strong>Mapping human cerebral blood flow with high-density, multi-channel speckle contrast optical spectroscopy<\/strong>.\u00a0<\/span><i>Commun Biol<\/i><span>\u00a0<\/span><b>8<\/b><span>, 1553 (2025). https:\/\/doi.org\/10.1038\/s42003-025-08915-x<\/span><\/p>\n<p style=\"text-align: left;\"><span><img loading=\"lazy\" src=\"\/cheng\/files\/2025\/11\/Screenshot-2025-11-12-152943-636x386.png\" alt=\"\" width=\"636\" height=\"386\" class=\"size-medium wp-image-245 alignleft\" srcset=\"https:\/\/sites.bu.edu\/cheng\/files\/2025\/11\/Screenshot-2025-11-12-152943-636x386.png 636w, https:\/\/sites.bu.edu\/cheng\/files\/2025\/11\/Screenshot-2025-11-12-152943.png 728w\" sizes=\"(max-width: 636px) 100vw, 636px\" \/>Recently, speckle contrast optical spectroscopy (SCOS) enabled non-invasive, high signal-to-noise-ratio (SNR) human cerebral blood flow (CBF) measurements, relevant for both neuroscience and clinical monitoring of diseases with CBF dysregulation. Single-channel SCOS measurements limit the information obtained to only one location on the head. In this work, we develop a multi-channel SCOS system to map spatial heterogeneity in CBF changes during human brain activation. Using a galvanometer, we temporally multiplex a free-space laser to 7 source fibers positioned at different locations on the head. Diffuse light collected from the tissue is captured by fiber bundles projecting to 17 complementary metal-oxide semiconductor (CMOS) cameras, resulting in 50 source-detector channels measuring optical density (OD) and relative CBF changes covering an area of 7.6\u2009cm by 6.6\u2009cm on the head. We validate the spatial specificity and stability of the system using a liquid flow phantom. We then measure brain activity during a word-color Stroop task in 15 subjects and obtain brain activation maps. The average signal changes in the channel showing the largest activation is 0.017 <\/span><span>in \u0394OD and 6.6% in CBF<\/span><\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p><span>Liu, B., Tang, R.P., Long, E.A., Yaqoob, Z., Simkulet, M.G., Postnov, D.D., Erdener, \u015e.E., Boas, D.A. and Cheng, X., 2025. <strong>Mapping of blood flow and slow speckle tissue dynamics using laser speckle contrast imaging<\/strong>.\u00a0<\/span><i>Biomedical Optics Express<\/i><span>,\u00a0<\/span><i>16<\/i><span>(9), pp.3712-3724.<\/span><\/p>\n<p><img loading=\"lazy\" src=\"\/cheng\/files\/2025\/09\/SSD.png\" alt=\"\" width=\"753\" height=\"516\" class=\"size-full wp-image-227 alignleft\" srcset=\"https:\/\/sites.bu.edu\/cheng\/files\/2025\/09\/SSD.png 753w, https:\/\/sites.bu.edu\/cheng\/files\/2025\/09\/SSD-636x436.png 636w\" sizes=\"(max-width: 753px) 100vw, 753px\" \/>Laser speckle contrast imaging (LSCI) is a wide-field optical technique commonly used to monitor cerebral blood flow (CBF). Recently, we have discovered that besides the fast-decorrelating signals from blood flow, LSCI can also detect slow-decorrelating signals associated with cellular activity. The ability to image these signals has significant implications for various research areas such as ischemic stroke, as it enables longitudinal monitoring of both vascular and cellular dynamics, offering new biomarkers for tissue viability, injury progression, and therapeutic response. Here, we demonstrated that epi-illumination LSCI enables the mapping of both slow speckle dynamics (SSD) for evaluating cellular dynamics and traditional fast speckle dynamics (FSD) for evaluating CBF. We found that SSD signals are much more evident with epi-illumination than with conventional oblique illumination LSCI. Using mouse models of ischemic stroke, including both permanent and transient occlusion of the distal middle cerebral artery (dMCA), we demonstrated the system\u2019s ability to track stroke progression from minutes to days post-stroke. This study establishes a powerful, label-free imaging tool for investigating both cellular and vascular health during stroke core evolution.<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p><span>Howard, Alexander C., Byungchan Kim, Laura Carlton, Meryem A. Y\u00fccel, Bingxue Liu, David A. Boas, and Xiaojun Cheng. &#8220;<strong>Validation of the Linearity in Image Reconstruction Methods for Speckle Contrast Optical Tomography<\/strong>.&#8221;\u00a0<\/span><i>IEEE Journal of Selected Topics in Quantum Electronics<\/i><span>\u00a0(2025).<\/span><\/p>\n<p>This work demonstrates that linear methods, such as the general linear models developed for fNIRS, can be applied for SCOS\/SCOT data processing.<\/p>\n<p><span>Speckle contrast optical spectroscopy (SCOS) is an optical technique capable of measuring human cerebral blood flow and brain function non-invasively. Its tomographic extension, speckle contrast optical tomography (SCOT), can provide blood flow variation maps with measurements using overlapping source-detector channel pairs. Linearity is often assumed in most image reconstruction methods, but non-linearity could exist in the relations between measured signals and blood flow variations. We have constructed a forward model for SCOT using the Rytov approximation to solve the correlation diffusion equation and compared it with the first Born approximation as well as the more accurate, but computationally expensive Monte Carlo simulation approach. We have shown that the results obtained using the Rytov approximation are in good agreement with the Monte Carlo simulations, while the first Born approximation deviates from the other two methods for large blood flow variations. For instance, the first Born approximation breaks down at around 30% cerebral blood flow (CBF) changes within a volume of size\u00a0<\/span><svg class=\"gs_fsvg\" aria-label=\"60\\times 50 \\times 40\" width=\"87px\" height=\"11px\"><g transform=\"matrix(0.01600, 0.00000, 0.00000, 0.01600, 0.00000, 10.65600)\"><path transform=\"scale(0.48828, -0.48828)\" d=\"M 512 -45 Q 385 -45 300 22 T 168 197 T 104 423 T 86 662 Q 86 824 149 987 T 334 1257 T 625 1364 Q 695 1364 755 1337 T 850 1259 T 885 1135 Q 885 1093 856 1064 T 786 1036 Q 746 1036 717 1065 T 688 1135 Q 688 1175 717 1204 T 786 1233 H 797 Q 771 1270 723 1287 T 625 1305 Q 563 1305 510 1278 T 416 1205 T 346 1103 T 302 977 T 283 844 T 279 688 Q 315 772 381 825 T 530 879 Q 621 879 696 842 T 825 739 T 907 590 T 936 420 Q 936 300 882 191 T 732 19 T 512 -45 Z M 512 20 Q 591 20 639 56 T 709 151 T 737 271 T 743 420 Q 743 536 732 618 T 672 762 T 522 825 Q 439 825 385 769 T 307 627 T 283 463 Q 283 436 285 422 Q 285 419 284 417 T 283 412 Q 283 324 301 234 T 370 82 T 512 20 Z \"><\/path><path transform=\"matrix(0.48828, 0.00000, 0.00000, -0.48828, 500.00000, 0.00000)\" d=\"M 512 -45 Q 261 -45 170 161 T 80 653 Q 80 831 112 988 T 241 1254 T 512 1364 Q 647 1364 733 1298 T 864 1127 T 925 903 T 942 653 Q 942 477 909 323 T 782 62 T 512 -45 Z M 512 8 Q 626 8 682 125 T 751 384 T 764 686 Q 764 840 751 970 T 682 1205 T 512 1311 Q 396 1311 340 1205 T 271 969 T 258 686 Q 258 572 263 471 T 293 262 T 370 81 T 512 8 Z \"><\/path><path transform=\"matrix(0.48828, 0.00000, 0.00000, -0.48828, 1222.22290, 0.00000)\" d=\"M 301 59 Q 301 75 311 88 L 737 512 L 311 938 Q 301 948 301 965 Q 301 980 313 993 T 342 1006 Q 356 1006 373 993 L 797 569 L 1219 993 Q 1236 1006 1249 1006 Q 1266 1006 1278 994 T 1290 965 Q 1290 948 1280 938 L 854 512 L 1280 88 Q 1290 75 1290 59 Q 1290 42 1278 30 T 1249 18 Q 1234 18 1219 33 L 797 455 L 373 33 Q 358 18 342 18 Q 325 18 313 31 T 301 59 Z \"><\/path><path transform=\"matrix(0.48828, 0.00000, 0.00000, -0.48828, 2222.22583, 0.00000)\" d=\"M 178 233 Q 199 173 242 124 T 345 47 T 469 20 Q 617 20 673 135 T 729 414 Q 729 485 726 533 T 713 627 Q 694 699 646 753 T 530 807 Q 461 807 411 786 T 331 737 T 276 678 T 246 645 H 223 Q 218 645 210 651 T 203 664 V 1348 Q 203 1353 209 1358 T 223 1364 H 229 Q 367 1298 522 1298 Q 674 1298 815 1364 H 821 Q 828 1364 834 1359 T 840 1348 V 1329 Q 840 1319 836 1319 Q 766 1226 660 1174 T 442 1122 Q 360 1122 274 1145 V 758 Q 342 813 395 836 T 532 860 Q 645 860 734 795 T 872 625 T 920 412 Q 920 289 859 184 T 695 17 T 469 -45 Q 368 -45 283 7 T 150 147 T 102 334 Q 102 380 132 409 T 207 438 Q 252 438 282 408 T 313 334 Q 313 290 282 259 T 207 229 Q 200 229 191 230 T 178 233 Z \"><\/path><path transform=\"matrix(0.48828, 0.00000, 0.00000, -0.48828, 2722.22583, 0.00000)\" d=\"M 512 -45 Q 261 -45 170 161 T 80 653 Q 80 831 112 988 T 241 1254 T 512 1364 Q 647 1364 733 1298 T 864 1127 T 925 903 T 942 653 Q 942 477 909 323 T 782 62 T 512 -45 Z M 512 8 Q 626 8 682 125 T 751 384 T 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d=\"M 512 -45 Q 261 -45 170 161 T 80 653 Q 80 831 112 988 T 241 1254 T 512 1364 Q 647 1364 733 1298 T 864 1127 T 925 903 T 942 653 Q 942 477 909 323 T 782 62 T 512 -45 Z M 512 8 Q 626 8 682 125 T 751 384 T 764 686 Q 764 840 751 970 T 682 1205 T 512 1311 Q 396 1311 340 1205 T 271 969 T 258 686 Q 258 572 263 471 T 293 262 T 370 81 T 512 8 Z \"><\/path><\/g><\/svg><span>\u00a0<\/span><svg class=\"gs_fsvg\" aria-label=\"mm^{3}\" width=\"34px\" height=\"13px\"><g transform=\"matrix(0.01600, 0.00000, 0.00000, 0.01600, 0.00000, 13.24307)\"><path transform=\"scale(0.48828, -0.48828)\" d=\"M 158 35 Q 158 47 160 53 L 313 664 Q 328 721 328 764 Q 328 852 268 852 Q 204 852 173 775 T 113 582 Q 113 576 107 572 T 96 569 H 72 Q 65 569 60 576 T 55 590 Q 77 679 97 741 T 161 854 T 270 905 Q 347 905 406 856 T 465 733 Q 526 813 608 859 T 782 905 Q 879 905 949 855 T 1020 715 Q 1083 804 1167 854 T 1352 905 Q 1458 905 1522 847 T 1587 684 Q 1587 600 1549 481 T 1456 215 Q 1427 144 1427 92 Q 1427 31 1475 31 Q 1555 31 1608 117 T 1683 301 Q 1689 313 1700 313 H 1724 Q 1732 313 1737 307 T 1743 295 Q 1743 293 1741 289 Q 1713 173 1643 75 T 1470 -23 Q 1398 -23 1347 26 T 1296 147 Q 1296 183 1313 227 Q 1371 381 1409 502 T 1448 715 Q 1448 772 1425 812 T 1348 852 Q 1236 852 1154 783 T 1012 602 Q 1008 582 1006 571 L 874 45 Q 867 17 842 -3 T 788 -23 Q 764 -23 745 -7 T 727 35 Q 727 47 729 53 L 860 575 Q 881 659 881 715 Q 881 772 857 812 T 778 852 Q 703 852 640 819 T 530 731 T 444 602 L 305 45 Q 298 17 273 -3 T 219 -23 Q 194 -23 176 -7 T 158 35 Z \"><\/path><g transform=\"translate(878.00000, 0.00000)\"><path transform=\"scale(0.48828, -0.48828)\" d=\"M 158 35 Q 158 47 160 53 L 313 664 Q 328 721 328 764 Q 328 852 268 852 Q 204 852 173 775 T 113 582 Q 113 576 107 572 T 96 569 H 72 Q 65 569 60 576 T 55 590 Q 77 679 97 741 T 161 854 T 270 905 Q 347 905 406 856 T 465 733 Q 526 813 608 859 T 782 905 Q 879 905 949 855 T 1020 715 Q 1083 804 1167 854 T 1352 905 Q 1458 905 1522 847 T 1587 684 Q 1587 600 1549 481 T 1456 215 Q 1427 144 1427 92 Q 1427 31 1475 31 Q 1555 31 1608 117 T 1683 301 Q 1689 313 1700 313 H 1724 Q 1732 313 1737 307 T 1743 295 Q 1743 293 1741 289 Q 1713 173 1643 75 T 1470 -23 Q 1398 -23 1347 26 T 1296 147 Q 1296 183 1313 227 Q 1371 381 1409 502 T 1448 715 Q 1448 772 1425 812 T 1348 852 Q 1236 852 1154 783 T 1012 602 Q 1008 582 1006 571 L 874 45 Q 867 17 842 -3 T 788 -23 Q 764 -23 745 -7 T 727 35 Q 727 47 729 53 L 860 575 Q 881 659 881 715 Q 881 772 857 812 T 778 852 Q 703 852 640 819 T 530 731 T 444 602 L 305 45 Q 298 17 273 -3 T 219 -23 Q 194 -23 176 -7 T 158 35 Z \"><\/path><g transform=\"translate(878.00000, -362.89200)\"><path transform=\"scale(0.34180, -0.34180)\" d=\"M 233 160 Q 268 114 324 85 T 443 44 T 571 33 Q 658 33 715 78 T 798 198 T 825 356 Q 825 442 798 515 T 713 634 T 569 680 H 418 Q 410 680 402 687 T 395 702 V 723 Q 395 732 402 738 T 418 745 L 547 754 Q 653 754 717 858 T 782 1077 Q 782 1173 725 1232 T 571 1292 Q 487 1292 413 1267 T 291 1188 Q 334 1188 363 1154 T 393 1077 Q 393 1033 362 1001 T 285 969 Q 238 969 206 1001 T 174 1077 Q 174 1172 235 1236 T 388 1330 T 571 1360 Q 664 1360 760 1329 T 922 1234 T 989 1077 Q 989 950 905 855 T 694 717 Q 785 698 867 649 T 1001 525 T 1053 356 Q 1053 236 981 145 T 798 7 T 571 -41 Q 463 -41 358 -8 T 182 98 T 111 279 Q 111 329 145 362 T 229 395 Q 261 395 287 380 T 330 338 T 346 279 Q 346 230 313 195 T 233 160 Z \"><\/path><\/g><\/g><\/g><\/svg><span>, therefore we recommend using the Rytov approximation above this threshold. We have shown that our defined blood flow index (BFi) measured in SCOT is linearly related to local CBF variations, thus the forward and inverse problems can be solved linearly using the sensitivity matrix approach. We have then demonstrated image reconstruction experimentally showing human brain activations using our recently developed high-density SCOS system. Our method guides experimental system design and data analysis for SCOT.<\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span>Cheng, Tom Y., Byungchan Kim, Bernhard B. Zimmermann, Mitchell B. Robinson, Marco Renna, Stefan A. Carp, Maria Angela Franceschini, David A. Boas, and Xiaojun Cheng. &#8220;<strong>Choosing a camera and optimizing system parameters for speckle contrast optical spectroscopy<\/strong>.&#8221;\u00a0<\/span><i>Scientific Reports<\/i><span>\u00a014, no. 1 (2024): 11915.<\/span><\/p>\n<p><span>\u00a0<img loading=\"lazy\" src=\"\/cheng\/files\/2024\/06\/Capture-1-582x636.png\" alt=\"\" width=\"200\" height=\"218\" class=\"alignleft wp-image-158\" srcset=\"https:\/\/sites.bu.edu\/cheng\/files\/2024\/06\/Capture-1-582x636.png 582w, https:\/\/sites.bu.edu\/cheng\/files\/2024\/06\/Capture-1.png 608w\" sizes=\"(max-width: 200px) 100vw, 200px\" \/>Speckle contrast optical spectroscopy (SCOS) is an emerging camera-based technique that can measure human cerebral blood flow (CBF) with high signal-to-noise ratio (SNR). At low photon flux levels typically encountered in human CBF measurements, camera noise and nonidealities could significantly impact SCOS measurement SNR and accuracy. Thus, a guide for characterizing, selecting, and optimizing a camera for SCOS measurements is crucial for the development of next-generation optical devices for monitoring human CBF and brain function. Here, we provide such a guide and illustrate it by evaluating three commercially available complementary metal\u2013oxide\u2013semiconductor cameras, considering a variety of factors including linearity, read noise, and quantization distortion. We show that some cameras that are well-suited for general intensity imaging could be challenged in accurately quantifying spatial contrast for SCOS. We then determine the optimal operating parameters for the preferred camera among the three and demonstrate measurement of human CBF with this selected low-cost camera. This work establishes a guideline for characterizing and selecting cameras as well as for determining optimal parameters for SCOS systems.<\/span><\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p class=\"article-title\">Bingxue Liu, Dmitry Postnov, David A. Boas, and Xiaojun Cheng<strong>, <\/strong>2024.<strong> Dynamic light scattering and laser speckle contrast imaging of the brain: theory of the spatial and temporal statistics of speckle pattern evolution. <\/strong>Biomed. Opt. Express\u00a015(2), 579-593.<br \/>\n<span role=\"presentation\" dir=\"ltr\"><\/span><\/p>\n<p><img loading=\"lazy\" src=\"\/cheng\/files\/2024\/01\/Capture-636x517.jpg\" alt=\"\" width=\"547\" height=\"445\" class=\" wp-image-107 alignleft\" srcset=\"https:\/\/sites.bu.edu\/cheng\/files\/2024\/01\/Capture-636x517.jpg 636w, https:\/\/sites.bu.edu\/cheng\/files\/2024\/01\/Capture.jpg 714w\" sizes=\"(max-width: 547px) 100vw, 547px\" \/><\/p>\n<p>Dynamic light scattering (DLS) and laser speckle contrast imaging (LSCI) are closely related techniques that exploit the statistics of speckle patterns which can be utilized to measure cerebral blood flow (CBF). Conventionally, the temporal speckle intensity auto-correlation function is calculated in DLS, while the spatial speckle contrast is calculated in LSCI measurements. Due to the rapid development of CMOS detection technology with increased camera frame rates while still maintaining a large number of pixels, the ensemble or spatial average of the auto-correlation functions as well as the temporal contrast can be easily calculated and utilized to quantify CBF. Although many models have been established, a proper summary is still lacking to fully characterize DLS and LSCI measurements for spatial and temporal statistics, laser coherence properties, various motion types, etc. As a result, there are many instances where theoretical models are misused.\u00a0Therefore, we aim to provide a review of the speckle theory for both DLS and LSCI measurements with detailed derivations from first principles, taking into account non-ergodicity, spatial and temporal statistics of speckles, scatterer motion types, and laser coherence properties. From these calculations, we elaborate on the differences between spatial and temporal averaging for DLS and LSCI measurements that are typically ignored but can result in inaccurate measurements of blood flow. We also obtained in vivo mouse brain measurements using high frame rate CMOS cameras which have not been demonstrated before. This work provides a useful guide for choosing the correct model to analyze spatial and temporal speckle statistics in in vivo DLS and LSCI measurements.<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p><span>Kim, B., Zilpelwar, S., Sie, E.J., Marsili, F., Zimmermann, B., Boas, D.A. and Cheng, X., 2023. <strong>Measuring human cerebral blood flow and brain function with fiber-based speckle contrast optical spectroscopy system<\/strong>. <em>Communications Biology<\/em><\/span><span>, 6, 844.<\/span><\/p>\n<p><img loading=\"lazy\" src=\"\/cheng\/files\/2023\/10\/SCOS-636x310.png\" alt=\"\" width=\"636\" height=\"310\" class=\"alignleft wp-image-78 size-medium\" srcset=\"https:\/\/sites.bu.edu\/cheng\/files\/2023\/10\/SCOS-636x310.png 636w, https:\/\/sites.bu.edu\/cheng\/files\/2023\/10\/SCOS-1024x500.png 1024w, https:\/\/sites.bu.edu\/cheng\/files\/2023\/10\/SCOS-768x375.png 768w, https:\/\/sites.bu.edu\/cheng\/files\/2023\/10\/SCOS.png 1127w\" sizes=\"(max-width: 636px) 100vw, 636px\" \/><\/p>\n<p><span>Cerebral blood flow (CBF) is crucial for brain health. Speckle contrast optical spectroscopy (SCOS) is a technique that has been recently developed to measure CBF, but the use of SCOS to measure human brain function at large source-detector separations with comparable or greater sensitivity to cerebral rather than extracerebral blood flow has not been demonstrated. We describe a fiber-based SCOS system capable of measuring human brain activation-induced CBF changes at 33\u2009mm source-detector separations using CMOS detectors. The system implements a pulsing strategy to improve the photon flux and uses a data processing pipeline to improve measurement accuracy. We show that SCOS outperforms the current leading optical modality for measuring CBF, i.e. diffuse correlation spectroscopy (DCS), achieving more than 10x SNR improvement at a similar financial cost. Fiber-based SCOS provides an alternative approach to functional neuroimaging for cognitive neuroscience and health science applications.<\/span><\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p><span>Liu, B., Shah, S., K\u00fcreli, G., Devor, A., Boas, D.A. and Cheng, X., 2023. <strong>Measurements of slow tissue dynamics with short-separation speckle contrast optical spectrosco<\/strong>py. <\/span><i>Biomedical Optics Express<\/i><span>,\u00a0<\/span><i>14<\/i><span>(9), pp.4790-4799.<\/span><\/p>\n<p><img loading=\"lazy\" src=\"\/cheng\/files\/2023\/10\/Mouse_SCOS.png\" alt=\"\" width=\"400\" height=\"321\" class=\"wp-image-82 alignleft\" \/><\/p>\n<p>Laser speckle contrast imaging (LSCI) measures 2D maps of cerebral blood flow (CBF) in small animal brains such as mice.<br \/>\nThe contrast measured in LSCI also includes the static and slow-varying components that contain information about brain tissue dynamics. But these components are less studied as compared to the fast dynamics of CBF. In traditional wide-field LSCI, the contrast measured in the tissue is largely contaminated by neighboring blood vessels, which reduces the sensitivity to these static and slow components. Our goal is to enhance the sensitivity of the contrast to static and slow tissue dynamics and test models to quantify the characteristics of these components. To achieve this, we have developed a short-separation speckle contrast optical spectroscopy (ss-SCOS) system by implementing point illumination and point detection using multi-mode fiber arrays to enhance the static and slow components in speckle contrast measurements as compared to traditional wide-field LSCI (WF-LSCI). We observed larger fractions of the static and slow components when measured in the tissue using ss-SCOS than in traditional LSCI for the same animal and region of interest. We have also established models to obtain the fractions of the static and slow components and quantify the decorrelation time constants of the intensity auto-correlation function for both fast blood flow and slower tissue dynamics.<br \/>\nUsing ss-SCOS, we demonstrate the variations of fast and slow brain dynamics in animals before and post-stroke, as well as within an hour post-euthanasia. This technique establishes the foundation to measure brain tissue dynamics other than CBF such as intracellular motility.<\/p>\n<p>&nbsp;<\/p>\n<p><span>Zilpelwar, S., Sie, E.J., Postnov, D., Chen, A.I., Zimmermann, B., Marsili, F., Boas, D.A. and Cheng, X., 2022. <strong>Model of dynamic speckle evolution for evaluating laser speckle contrast measurements of tissue dynamics<\/strong>.\u00a0<\/span><i>Biomedical Optics Express<\/i><span>,\u00a0<\/span><i>13<\/i><span>(12), pp.6533-6549.<\/span><\/p>\n<p><img loading=\"lazy\" src=\"\/cheng\/files\/2023\/10\/DSM-636x615.png\" alt=\"\" width=\"448\" height=\"434\" class=\"alignleft wp-image-84\" srcset=\"https:\/\/sites.bu.edu\/cheng\/files\/2023\/10\/DSM-636x615.png 636w, https:\/\/sites.bu.edu\/cheng\/files\/2023\/10\/DSM.png 681w\" sizes=\"(max-width: 448px) 100vw, 448px\" \/><\/p>\n<p>We introduce a dynamic speckle model (DSM) to simulate the temporal evolution of fully developed speckle patterns arising from the interference of scattered light reemitted from dynamic tissue. Using this numerical tool, the performance of laser speckle contrast imaging (LSCI) or speckle contrast optical spectroscopy (SCOS) systems which quantify tissue dynamics using the spatial contrast of the speckle patterns with a certain camera exposure time is evaluated. We have investigated noise sources arising from the fundamental speckle statistics due to the finite sampling of the speckle patterns as well as those induced by experimental measurement conditions including shot noise, camera dark, and read noise, and calibrated the parameters of an analytical noise model initially developed in the fundamental or shot noise regime that quantifies the performance of SCOS systems using the number of independent observables (NIO). Our analysis is particularly focused on the low photon flux regime relevant for human brain measurements, where the impact of shot noise and camera read noise can become significant. Our numerical model is also validated experimentally using a novel fiber-based SCOS (fb-SCOS) system for a dynamic sample. We have found that the signal-to-noise ratio (SNR) of fb-SCOS measurements plateaus at a camera exposure time which marks the regime where shot and fundamental noise dominate over camera read noise. For a fixed total measurement time, there exists an optimized camera exposure time if temporal averaging is utilized to improve SNR. For a certain camera exposure time, photon flux value, and camera noise properties, there exists an optimized speckle-to-pixel size ratio (s\/p) at which SNR is maximized. Our work provides the design principles for any LSCI or SCOS systems given the detected photon flux and properties of the instruments, which will guide the way for the experimental development of a high-quality, low-cost fb-SCOS system that monitors human brain blood flow and functions in the future.<\/p>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Complete publication list Selected journal publications: Kim, B.K., Howard, A.C., Cheng, T.Y.\u00a0et al.\u00a0Mapping human cerebral blood flow with high-density, multi-channel speckle contrast optical spectroscopy.\u00a0Commun Biol\u00a08, 1553 (2025). https:\/\/doi.org\/10.1038\/s42003-025-08915-x Recently, speckle contrast optical spectroscopy (SCOS) enabled non-invasive, high signal-to-noise-ratio (SNR) human cerebral blood flow (CBF) measurements, relevant for both neuroscience and clinical monitoring of diseases with [&hellip;]<\/p>\n","protected":false},"author":14271,"featured_media":0,"parent":0,"menu_order":3,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"_links":{"self":[{"href":"https:\/\/sites.bu.edu\/cheng\/wp-json\/wp\/v2\/pages\/26"}],"collection":[{"href":"https:\/\/sites.bu.edu\/cheng\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/sites.bu.edu\/cheng\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/sites.bu.edu\/cheng\/wp-json\/wp\/v2\/users\/14271"}],"replies":[{"embeddable":true,"href":"https:\/\/sites.bu.edu\/cheng\/wp-json\/wp\/v2\/comments?post=26"}],"version-history":[{"count":20,"href":"https:\/\/sites.bu.edu\/cheng\/wp-json\/wp\/v2\/pages\/26\/revisions"}],"predecessor-version":[{"id":246,"href":"https:\/\/sites.bu.edu\/cheng\/wp-json\/wp\/v2\/pages\/26\/revisions\/246"}],"wp:attachment":[{"href":"https:\/\/sites.bu.edu\/cheng\/wp-json\/wp\/v2\/media?parent=26"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}