Portable optical resolution photoacoustic microscopy...

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Portable optical resolution photoacoustic microscopy (pORPAM) for human oral imaging TIAN JIN, 1 HENG GUO, 1 HUABEI JIANG, 1,2,3 BOWEN KE, 4 AND LEI XI 1,2, * 1 School of Physical Electronics, University of Electronic Science and Technology of China, Chengdu 610054, China 2 Center for Information in Biomedicine, University of Electronic Science and Technology of China, Chengdu 610054, China 3 Department of Medical Engineering, University of South Florida, Tampa, Florida 33620, USA 4 Laboratory of Anesthesiology and Critical Care Medicine, Translational Neuroscience Center, West China Hospital, Sichuan University, Chengdu 610040, China *Corresponding author: [email protected] Received 28 August 2017; revised 29 September 2017; accepted 2 October 2017; posted 3 October 2017 (Doc. ID 303243); published 25 October 2017 Optical resolution photoacoustic microscopy (ORPAM) represents one of the fastest evolving optical microscopic techniques. However, due to the bulky size and complicated system configuration of conventional ORPAM, it is largely limited to small animal experiments. In this Letter, we present the design and evaluation of a portable ORPAM with a high spatiotemporal resolution and a large field of view. In this system, we utilize a rotatory scanning mechanism instead of the conventional raster scanning to achieve translationless imaging of the probe/samples, mak- ing it accessible to the human oral lip and tongue. After phantom evaluation, we applied this system to monitor longitudinal neo-angiogenesis of tumor growth and, for the first time, to the best of our knowledge, image the oral vascular network of humans to show its potential in clinical detection of early-stage oral cancer. © 2017 Optical Society of America OCIS codes: (110.0180) Microscopy; (110.5120) Photoacoustic imaging; (170.6900) Three-dimensional microscopy. https://doi.org/10.1364/OL.42.004434 Oral cancer remains one of the common malignant tumors in the world [1,2]. Clinical investigations suggest that early diag- nosis and treatment will significantly improve the survival rate of patients. The classic diagnostic method for oral cancer is clinical observation, in which the physicians inspect the super- ficial tissues in the oral cavity using a stomatoscope and resect the suspicious tissues for pathological analysis [3]. However, clinical observation is subjective, lacks depth information, and highly depends on the experience of operators. Biological studies indicate that angiogenesis is one of the major symptoms during the early cancerization of tumor lesions. Optical imaging, which is extremely sensitive to hemoglobin changes, has been applied to various biological and clinical cancer studies [4,5]. Fluorescence spectroscopy and narrow- band imaging (NBI) have been proposed to clinically screen/diagnose oral cancers in the human oral cavity [6,7]. However, they suffer from limited penetration depth and lack of depth-resolving ability. Optical coherence tomography (OCT), a three-dimensional high-resolution imaging tech- nique, has been used to identify early-stage oral cancer lesions with the assistance of nanoparticles [8]. Nevertheless, OCT is sensitive to optical scattering properties, which are only tightly associated with morphological changes. Although OCT angi- ography is able to capture blood vessels using the flow contrast, it suffers from low temporal resolution, speckle noise, and lim- ited imaging depth. Laser speckle contrast imaging, capable of visualizing vasculatures, has the potential to be miniaturized and applied in oral inspection [9]. However, similar to NBI/ fluorescence imaging, it lacks depth information. Photoacoustic (PA) imaging, integrating rich optical con- trast, deep penetration depth, and high acoustic resolution in one modality, has been demonstrated in different biological and clinical studies [10,11]. Oraevesky and Fatakdawala uti- lized PA computed tomography and acoustic resolution PA microscopy, respectively, to detect oral tumor lesions using hamster-based tumor models [12,13]. Besides the limited res- olution, their systems are not suitable for clinical use. Currently, several encouraging approaches introduce water- immersed magnetic mirrors and graded-index lenses to achieve portable ORPAMs [14,15]. However, they have limited field of view (FOV), and the temporal resolution is not high enough to avoid the motion effect of hands, leading to potential deterio- rations in images. In this Letter, we report and evaluate a new portable optical resolution photoacoustic microscopy system (pORPAM) for human oral imaging. Compared with conven- tional ORPAMs, pORPAM enables translationless imaging of the samples/imaging interfaces, has a large FOV and depth of field (DOF), and provides access to the human oral cavity which is inaccessible to the existing ORPAMs. Figure 1 shows the layout of pORPAM. The 532 nm laser beam from a Q -switched pulsed laser (FQS-200-1-532, Elforlight Ltd.) has a 4 ns pulse duration and a maximum rep- etition rate of 20,000 Hz. Pulses, reshaped using an iris (GCM- 5702M, Daheng Optics Ltd.), pass through an optical spatial 4434 Vol. 42, No. 21 / November 1 2017 / Optics Letters Letter 0146-9592/17/214434-04 Journal © 2017 Optical Society of America

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Portable optical resolution photoacousticmicroscopy (pORPAM) for human oral imagingTIAN JIN,1 HENG GUO,1 HUABEI JIANG,1,2,3 BOWEN KE,4 AND LEI XI1,2,*1School of Physical Electronics, University of Electronic Science and Technology of China, Chengdu 610054, China2Center for Information in Biomedicine, University of Electronic Science and Technology of China, Chengdu 610054, China3Department of Medical Engineering, University of South Florida, Tampa, Florida 33620, USA4Laboratory of Anesthesiology and Critical Care Medicine, Translational Neuroscience Center, West China Hospital, Sichuan University,Chengdu 610040, China*Corresponding author: [email protected]

Received 28 August 2017; revised 29 September 2017; accepted 2 October 2017; posted 3 October 2017 (Doc. ID 303243);published 25 October 2017

Optical resolution photoacoustic microscopy (ORPAM)represents one of the fastest evolving optical microscopictechniques. However, due to the bulky size and complicatedsystem configuration of conventional ORPAM, it is largelylimited to small animal experiments. In this Letter, wepresent the design and evaluation of a portable ORPAMwith a high spatiotemporal resolution and a large fieldof view. In this system, we utilize a rotatory scanningmechanism instead of the conventional raster scanning toachieve translationless imaging of the probe/samples, mak-ing it accessible to the human oral lip and tongue. Afterphantom evaluation, we applied this system to monitorlongitudinal neo-angiogenesis of tumor growth and, forthe first time, to the best of our knowledge, image the oralvascular network of humans to show its potential in clinicaldetection of early-stage oral cancer. © 2017 Optical Societyof America

OCIS codes: (110.0180) Microscopy; (110.5120) Photoacoustic

imaging; (170.6900) Three-dimensional microscopy.

https://doi.org/10.1364/OL.42.004434

Oral cancer remains one of the common malignant tumors inthe world [1,2]. Clinical investigations suggest that early diag-nosis and treatment will significantly improve the survival rateof patients. The classic diagnostic method for oral cancer isclinical observation, in which the physicians inspect the super-ficial tissues in the oral cavity using a stomatoscope and resectthe suspicious tissues for pathological analysis [3]. However,clinical observation is subjective, lacks depth information,and highly depends on the experience of operators.Biological studies indicate that angiogenesis is one of the majorsymptoms during the early cancerization of tumor lesions.Optical imaging, which is extremely sensitive to hemoglobinchanges, has been applied to various biological and clinicalcancer studies [4,5]. Fluorescence spectroscopy and narrow-band imaging (NBI) have been proposed to clinically

screen/diagnose oral cancers in the human oral cavity [6,7].However, they suffer from limited penetration depth and lackof depth-resolving ability. Optical coherence tomography(OCT), a three-dimensional high-resolution imaging tech-nique, has been used to identify early-stage oral cancer lesionswith the assistance of nanoparticles [8]. Nevertheless, OCT issensitive to optical scattering properties, which are only tightlyassociated with morphological changes. Although OCT angi-ography is able to capture blood vessels using the flow contrast,it suffers from low temporal resolution, speckle noise, and lim-ited imaging depth. Laser speckle contrast imaging, capable ofvisualizing vasculatures, has the potential to be miniaturizedand applied in oral inspection [9]. However, similar to NBI/fluorescence imaging, it lacks depth information.

Photoacoustic (PA) imaging, integrating rich optical con-trast, deep penetration depth, and high acoustic resolutionin one modality, has been demonstrated in different biologicaland clinical studies [10,11]. Oraevesky and Fatakdawala uti-lized PA computed tomography and acoustic resolution PAmicroscopy, respectively, to detect oral tumor lesions usinghamster-based tumor models [12,13]. Besides the limited res-olution, their systems are not suitable for clinical use.Currently, several encouraging approaches introduce water-immersed magnetic mirrors and graded-index lenses to achieveportable ORPAMs [14,15]. However, they have limited field ofview (FOV), and the temporal resolution is not high enough toavoid the motion effect of hands, leading to potential deterio-rations in images. In this Letter, we report and evaluate a newportable optical resolution photoacoustic microscopy system(pORPAM) for human oral imaging. Compared with conven-tional ORPAMs, pORPAM enables translationless imaging ofthe samples/imaging interfaces, has a large FOV and depth offield (DOF), and provides access to the human oral cavitywhich is inaccessible to the existing ORPAMs.

Figure 1 shows the layout of pORPAM. The 532 nm laserbeam from a Q-switched pulsed laser (FQS-200-1-532,Elforlight Ltd.) has a 4 ns pulse duration and a maximum rep-etition rate of 20,000 Hz. Pulses, reshaped using an iris (GCM-5702M, Daheng Optics Ltd.), pass through an optical spatial

4434 Vol. 42, No. 21 / November 1 2017 / Optics Letters Letter

0146-9592/17/214434-04 Journal © 2017 Optical Society of America

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filter system (KT310/M, Thorlabs Inc.) to form a clean, spa-tially uniform, Gussian beam, enter into a single-mode fiberassisted with a free-space to fiber coupler (APFC-5T-FC,Zolix Instruments Ltd.), and are collimated via a fiber collima-tor (F220FC-532, Thorlabs Inc.). A fast photodiode (PD818-BB-21, Newport Corp.) records partial pulse energy reflectedby a beam splitter (BS025, Thorlabs Inc.) to remove the fluc-tuation of laser pulses. The transmission beam is delivered intoa two-dimensional galvanometric scanner (GVS002, ThorlabsInc.) and scanned on the back surface of the imaging lens.The scanner is driven by a multifunctional data acquisitioncard (PCI-6731, National Instruments). A motorized rotator(RSA-100, Zolix Inc.) equipped with a customized acceleratinggear group with a ratio of 1:4 is used to rotate a cylindricallyfocused transducer (V324-SU, Olympus IMS), which has afocal length of 38 mm, a center frequency of 15 MHz, anda larger active area of 12.7 mm. The PA signals are amplifiedby ∼39 dB using an amplifier (5073PR, Olympus IMS) anddigitized by a data acquisition card (NI-5124, NationalInstruments, TX) at a sampling rate of 200 MS/s.

In pORPAM, we utilize a rotary scanning mechanism, in-stead of conventional raster scanning [16]. Briefly, the acousticfocal line of a cylindrically focused transducer is adjusted to beconfocal with the optical imaging plane, and the focused laserspot starts to scan in line from the left edge to the right edge ofacoustic focal line to form a B-scan. After one optical line scan,both the acoustic focal line and the optical scan line rotateclockwise with a given angle. To cover the entire imaging area,the acoustic focal line and optical scan line need to rotatemultiple times with a total scanning angle of 180°. MultipleB-scans are used to form a volumetric image.

Before in vivo animal and human experiments, we usedphantoms to calibrate and evaluate the performance of thissystem. First, we calibrated the inhomogeneous sensitivityover the entire imaging area in three steps: (1) due to the inho-mogeneous sampling pattern of the scanning mechanism,weighting factors calculated based on the number of scansin each pixel were used to remove the non-uniformity ofthe reconstructed images; (2) owing to the uneven detection

sensitivity of the cylindrically focused ultrasound transducerin the focal line, the response was experimentally derived toeliminate the inhomogeneous sensitivity in the imaging area;(3) the fluctuation of the photon intensity of each pulse wasmeasured by a photodiode and used to calibrate each originalPA signal. Figure 2(a) shows the imaging result of a black tapewithout calibration. Figure 2(b) presents the black tape imageafter calibrations which make the imaging area much morehomogeneous.

In order to evaluate the resolutions and signal-to-noise ratios(SNRs) of the system, tissue mimicking background phantomswere prepared. Agarose, intralipid, and India ink were mixed tosimulate normal tissues with an optical absorption coefficient of0.01 mm−1 and a reduced scattering coefficient of 1.0 mm−1.After the mixture was solidified, we vertically inserted a sharpblade into the phantom and tilted it with an angle of 15° tosimulate an ideal edge in different depths. The sharp edgeof the blade was imaged by pORPAM to estimate the lateralresolutions, axial resolutions, and PA amplitudes in depths. Inthe experiments, there were 1400 A-lines with an interval of5 μm in a B-scan, and 1800 B-scans with a 0.1° in a volumeimage.

Figures 2(c) and 2(d) present the lateral and axial resolutionsat the focal plane, in which the lateral resolution was calculatedby deriving the line spread functions from the edge spreadfunctions of the blade edge, and the axial resolutions was esti-mated through the full width at half-maximum of theGaussian-fitted axial profiles. The lateral and axial resolutionsare 10.4 and 90 μm, respectively. As we expected, in Fig. 2(e),with the increase of the imaging depth, the lateral resolutiondeteriorates. However, no obvious deterioration of axial

Fig. 1. Illustration of the system configuration and closeup view ofthe imaging head. BS, beam splitter; PD, photodiode; Obj, objective;P, pinhole; L, convex lens; GVS, galvanometer scanner; SMF, single-mode fiber; CG, cover glass; IL, imaging lens; US, ultrasound wave;LB, laser beam.

Fig. 2. Evaluation of system performance. pOPRPAM imaging of ablack tape (a) before and (b) after calibrations. Experimental evalu-ation of (c) lateral resolution and (d) axial resolution. Amplitudesof PA (e) signals and (f ) resolutions in different depths.

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resolution is observed. Figure 2(f ) presents the amplitude of PAsignals in different depths. Due to the scattering properties ofthe tissue-mimicking phantom, the SNR becomes worse.

In addition to phantom experiments, pORPAM was furtherperformed for longitudinal monitoring of angiogenesis in amouse tumor model to show the clinical feasibility in earlydiagnosis of oral lesions. Mouse LS174T cell line was used(ATCC, VA, USA).

The cells were cultured at 37°C and 5% CO2 in a humidi-fied incubator in Dulbecco’s Modified Eagle’s Medium supple-mented with 10% fetal bovine serum and antibiotics. About1 × 106 cells were implanted into mammary fat pads of 10BALB/C nu/nu mice (4 ∼ 6 weeks). Mice were sacrificed afterthe completion of experiments. All the procedures have beenapproved by the University of Electronic Science andTechnology of China (UESTC).

Figure 3 presents the kinetics of vascular development in anaturally growing tumor. pORPAM started to capture the vol-ume of blood vessels on the tumor surface when the tumor wasvisible, and continued to monitor the vascular developmentevery 24 h until the tumor size reached 1 cm in diameter.At day 1, there were a few large blood vessels surrounding

the tumor and countable small blood vessels on the tumor sur-face. From day 2, as the tumor developed, numerous newbornvessels split from host vessels appeared to starve for feedingnutrition. The formation of newborn vessels began from theboundary of the tumor, and spread to the tumor center withan increased vascular density. Quantitative analyses of imageentropy revealing the texture chaos of vasculatures [17], bloodvolume representing the total number of blood vessels, and vas-cular density in the tumor area are presented in Figs. 3(b)–3(e),respectively. The irregular appearance of numerous newbornblood vessels caused a slow increase of entropy, blood volume,and vascular density from day 1 to day 4. Starting from day 5,the changes became steep, which was consistent with the cal-culated tumor volumes in Fig. 3(e). This result suggests thatpORPAM has sufficient resolution and DOF to visualize an-giogenesis during the early cancerization of tumors.

One of the major challenges for ORPAMs is the lack of aproper clinical application, which prevents its clinical transla-tion. It is known that there are ultra-high dense vascular net-works in the oral cavity. Structural and functional changes ofvasculatures in the oral cavity are tightly associated with earlycancerization of oral lesions. To show the clinical feasibility of

Fig. 3. In vivomaximum amplitude projection (MAP) images of vascular development and quantitative analysis of image entropy, vascular density,blood volume, and tumor volume in a LS174T tumor. (a) On the appearance of the tumor as indicated by the dashed orange circle in day 1, majorvessels in the injection site became discontinued and split into a number of small blood vessels which grew into the tumor and around the boundary.In the steady development of the tumor (day 1 to day 4), large vessels close to the boundary and on the tumor surface disappeared (indicated by whitearrows and dashed circles in day 3), and more and more small blood vessels came out to fulfill the abnormal nutrition requirement of tumor cells.During the fast growth period of the tumor (day 5 to day 8), the vasculature network became extremely dense, and the partial tumor cells started todie leading to necrosis, as indicated by white circles in day 7 and 8. (b) Image entropy is used to reveal the texture chaos of the vascular network. Withthe growth of newborn blood vessels, the vasculatures become messy leading to the increase of image entropy. The entropy increases with a steadyvelocity from day 1 to day 4, and in a steep way from day 5. (c) Vascular density in the tumor area increases from day 1 to day 3, keeps flat from day 3to day 5, and reaches the peak value at day 7. There is no obvious increase of vascular density from day 7 to day 8 due to two reasons: (1) the imagingarea is not large enough to cover the entire tumor; (2) there is partial tumor tissue necrosis, as indicated by white circles in Fig. 3. (d) Changes of theblood volume which represent the total number of blood vessels in the tumor site confirm that there are numerous newborn blood vessels with thegrowth of the tumor. (e) Calculated tumor volumes according to the formula of width2 × length × 0.5. Scale bar: 1 mm.

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pORPAM in oral vascular imaging, we imaged the tongues andlips of three male volunteers. All volunteers wore the protectionglass to avoid potential laser exposure to the eyes. The lips andtongues were attached to the imaging interface via drinkablewater. After the experiments, dentists continued to examinethe imaged area for seven days, and no abnormal symptomwas observed. We have obtained consents from all the volun-teers participating in the experiments. Figures 4(a) and 4(b)present typical maximum amplitude projection (MAP) imagesof the lip and tongue vascular network, from which we clearlysee ultra-dense vasculatures. The corresponding volume render-ing of the vascular network in Fig. 4(b) is shown in Fig. 4(c).Visualization 1 shows sequential cross-sectional slices at differ-ent depths. Three representative cross-sectional slices at 0.1,0.3, and 0.5 mm beneath the lip surface are presented inFig. 4(d). Within 0.1 mm volume under the surface, as indi-cated by the dashed yellow circle and yellow arrows in Fig. 4(d),a considerable amount of capillary loops was located whichwould bend and twist at the early stage of oral cancers [18].

For animal and human studies, the energy of laser pulsesafter the scan lens was measured to be 80 nJ. Considering thatthe size of the optical focus is 10.4 μm, the photon density inthe focal plane is calculated as 95 mJ∕cm2 in water. In the invivo experiments, the focal plane was adjusted to be ∼500 μmunder the tissue surface. Due to the high optical scatteringproperty of the biological tissue, the photon density in the im-aging plane is much lower than the American NationalStandards Institute safety limit of 22 mJ∕cm2.

In summary, we report the first human oral imaging studyusing a new portable ORPAM system. The system utilizes arotary scanning mechanism which enables translationless imag-ing of the sample/interface and provides a large FOV. The port-able configuration makes it accessible to human oral imaging.Through animal studies, we demonstrate that pORPAM is

capable of monitoring angiogenetic development which is vitalto identify the early-stage oral cancers. The volumetric visuali-zation of vascular networks in the human lip and tongue provesthe clinical feasibility of pORPAM in oral cancer detection.Before the clinical translation of pORPAM, we need to opti-mize the system and do further improvements. The imagingspeed is primarily limited by the laser repetition rate. Ourcurrent laser is able to emit 20,000 pulses per second, whichlasts 35 s for a typical volumetric image. An ultrafast nano-second pulsed laser with a maximum repetition rate of1,500,000 Hz is commercially available, and could significantlyaccelerate the imaging speed to 2 volumes per second. In ad-dition, the size can be further reduced by using a two-phasestepper motor, instead of a current motorized rotator.Furthermore, the imaging interface needs a special designfor uneven regions in the oral cavity such as palate and gum.

Funding. National Natural Science Foundation of China(NSFC) (61528401, 61775028, 81571722); StateInternational Collaboration Program, Department of Scienceand Technology of Sichuan Province (2016HH0019);University of Electronic Science and Technology of China(UESTC) (A03012023601011).

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Fig. 4. In vivo pORPAM imaging of oral vasculature in volunteers.(a) pORPAM image of the bottom surface of a human tongue.(b) MAP image of the vascular networks in a human lip.(c) Volume rendering of the vascular networks in a human lip.(d) Three representative slices at different depths of 0.1, 0.3, and0.5 mm under the lip surface. Scale bars: 1 mm.

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