Isha
Mutreja
a,
Nabil
Maalej
b,
Ajeet
Kaushik
cd,
Dhiraj
Kumar
*e and
Aamir
Raja
*f
aMinnesota Dental Research Center for Biomaterials and Biomechanics (MDRCBB), School of Dentistry, University of Minnesota, 515 Delaware St SE, Minneapolis, Minnesota 55455, USA. E-mail: imutreja@umn.edu
bDepartment of Physics, Khalifa University, Abu Dhabi, United Arab Emirates. E-mail: nabil.maalej@ku.ac.ae
cNanoBioTech Laboratory, Department of Environmental Engineering, Florida Polytechnic University, Lakeland, FL 33805, USA. E-mail: akaushik@floridapoly.edu
dSchool of Engineering, University of Petroleum and Energy Studies (UPES), Dehradun Uttarakhand, India
eDivision of Pediatric Dentistry, School of Dentistry, University of Minnesota, 515 Delaware St SE, Minneapolis, Minnesota 55455, USA. E-mail: kumard@umn.edu
fDepartment of Physics, Khalifa University, Abu Dhabi, United Arab Emirates. E-mail: aamir.raja@ku.ac.ae
First published on 17th August 2023
Spectral CT imaging (multi-energy detection) is a promising imaging technique that can benefit from the use of high atomic number (high-Z) based nanoparticles (NPs) as contrast agents. These NPs can improve image contrast and enable quantitative material reconstruction, potentially leading to more accurate diagnoses and better treatment planning. This article provides an overview of current research on the use of high-Z NPs for spectral CT imaging. This briefly covers the physicochemical properties and biocompatibility of eight high-Z elements: gadolinium, ytterbium, hafnium, tantalum, tungsten, rhenium, gold, and bismuth. This article also focuses on various in vitro, in vivo, and simulation studies that have investigated the potential advantages and limitations of using high-Z NPs as contrast agents for spectral CT imaging. In addition, the review also highlights the potential preclinical and clinical applications of high-Z NPs in cancer diagnosis, therapy, and cardiovascular disease. The emphasis has been on the key outcomes and limitations of prior studies and on identifying potential future research directions and applications for high-Z NPs and spectral photon-counting CT imaging. The article concludes by discussing advancements aimed at improving the efficacy and safety of high-Z NPs for clinical use, and potential future developments in the field.
During a CT scan, a poly energetic beam of X-rays is directed at the patient, and the X-ray tube rotates around the body. The detectors measure the intensity of the X-rays passing through the body from different angles. This information is then processed by a computer using advanced CT reconstruction algorithms. A detailed image of the internal structures or organs inside the body is created to provide a cross-sectional view of the body for diagnosis4 and interventional procedures such as image-guided biopsies and minimally invasive surgeries.5 CT imaging provides a quantitative 3D characterization of localized contrast to distinguish the different features of a living system. Modern developments in CT imaging techniques that improve speed, sensitivity/specificity, and resolution have significantly enhanced the ability of users to accurately diagnose, treat, and monitor disease response to treatment non-invasively in real-time. It is a powerful tool that goes beyond standard morphological assessments, such as size, shape, and structure, and visualizes multi-dimensional information in a preclinical setting (100 microns or greater voxel) to clinical setting (submillimeter to millimeter) with physiological and pathological significance that is otherwise challenging to decipher. Moreover, the use of nanoparticles in conjunction with spectral CT imaging has opened the door for potential translation to non-invasive molecular imaging at the human scale for the early detection of diseased cells.6–9
Spectral CT imaging relies on differentiating energy-dependent information from the CT X-ray scan in the form of linear absorption/attenuation coefficient of tissue, voxel material and/or other components; and concurrently characterizing the tissue and components. During the last two decades, spectral CT imaging has technologically advanced from dual-energy (dual-source or dual-detector, 1st generation) to multi-energy photon-counting (2nd generation).10 Dual-energy CT (DECT) technologies are advancements in CT imaging technology that have seen significant improvements since the early 2000s to overcome the limitations of traditional imaging technologies. The main principle is to provide a linear attenuation coefficient at two different energies. It can be achieved by using two different X-rays energies: one at low energy (typically 80 keV) and the other at high energy (typically 140 keV). However, the same can be achieved by using a single X-ray source with a dual-layer detection-based technique, which is widely used.10 One of the key advantages of DECT is its ability to perform material decomposition by combining two energy images to generate material density images. Material decomposition is a process in which different materials within the body are identified and separated based on their unique attenuation properties at different energy levels.11 DECT imaging is particularly useful for evaluating the brain, chest, abdomen, and pelvis, making it an important diagnostic tool for a range of conditions including cancer, trauma, and infection.12,13
Spectral photon-counting CT (SPCCT) is an innovative CT imaging technique that is considered to be the most advanced in the imaging field. This technique combines the use of conventional X-rays within the diagnostic energy range (30–140 keV). The SPCCT system incorporates specialized photon-counting detectors (PCDs) that are designed to measure and process the energy signatures of individual incoming photons as well as the signatures of specific atoms/elements – a process commonly referred to as the K-edge photoelectric effect. By utilizing the PCDs, the SPCCT system enables the acquisition of multiple energy-resolved images simultaneously, thereby significantly enhancing imaging capabilities. This approach provides valuable and detailed information about the composition of various elements.10,14–18 One of the main advantages of SPCCT is its ability to perform material identification and quantification of different materials based on their density, atomic composition, and energy-dependent attenuation. Unlike conventional CT or even DECT systems, SPCCT can effectively distinguish between different contrast agents with similar X-ray attenuation properties. Therefore, the development of new contrast agents that can generate distinctive spectral signatures is not only crucial for the further advancement of SPCCT, but the use of targeted contrast agents that bind to specific molecules or receptors can also provide information on the expression and distribution of site-specific targets, enabling the visualization of molecular and cellular processes.19 This can have significant clinical applications, such as in the detection and characterization of tumors and the assessment of therapeutic response.20,21
Moreover, SPCCT imaging improves traditional CT imaging by detecting and quantifying distinct K-edge energies of high-atomic-number (high-Z) elements in the targeted region.22 High-Z elements absorb X-rays more strongly than other elements commonly found in the body such as carbon, oxygen, nitrogen, and calcium. This leads to greater contrast between the high-Z elements and the surrounding tissues, including bone, making it easier to distinguish between different structures/organs/biological components in the body. These new K-edge or element energies of the selected elements are presented as colorized voxels against a standard X-ray background.23 The advantage of SPCCT over traditional CT imaging is its ability to isolate signals at the molecular level for molecular imaging. This property helps to overcome the relatively low inherent contrast within soft tissues.23,24 Consequently, SPCCT achieves better image contrast, higher spatial resolution, reduced radiation dose, and enhanced diagnostic accuracy, thereby reducing exposure to ionizing radiation.25–28
In general, high-Z NP studies for contrast agent development involve several important stages (Fig. 1A). First, the material for high-Z NPs and its synthesis technique must be selected with the desired properties such as shape, size, electrical, and optical properties in mind. It is also important that the NP surface be functionalized to achieve better targeting, better blood circulation, and biocompatibility. Surface modifications include covalent and non-covalent functionalization, encapsulation, and ligand exchange. After surface modification, the properties of the functionalized NP should also be characterized. The next stage is to test the high-Z nanoparticles in a phantom to determine if the NPs provide high contrast at sufficiently low concentrations to avoid toxicity. In vitro cell culture studies with healthy and cancer cells are required to verify cell targeting and determine cell viability at the required NPs concentration for contrast enhancement. Finally, animal studies are required to determine whether passive or active targeting of the NPs achieves sufficiently high concentration in the target tissue to achieve a perceivable contrast and to study the pharmacokinetics and toxicity of NPs contrast agents. Only after successful completion of the cell culture and in animal studies that the NPs testing can proceed to test in humans. Fig. 1B represents some sample images collected during research and clinical investigation using traditional (clockwise direction: FL, PAT, and US scans of tumors in mouse models, PET-CT scans of the human body, and MRI scans of mice showing different organs) and spectral photon-counting CT imaging technologies (clockwise direction: gold nanoparticles, yellow color in the lungs, gadolinium, green color – stomach and intestines, and iodine, red color – bladder and kidneys while soft tissue and bone in blue and white colors respectively – MARS bioimaging, mouse heart and surrounding tissue, Yb and Au nano colloid in blue and yellow in the mouse model, and AuNPs as yellow color in kidney and tumor in the mouse model – MARS bioimaging, and very first human wrist with a watch scan, & human ankle – MARS bioimaging).29–36
Fig. 1 Stages of development of high-Z NPs X-ray contrast agents. The stages include synthesis, characterization, surface modification of high-Z NPs followed by in phantom, in vitro, and in vivo testing/studies using small and large animal models (A). Representative image of research and clinical scans using traditional (clockwise direction: FL, PAT, and US scans of tumors in mouse models, PET-CT scan of human body, and MRI scan of mouse showing different organs) and advanced SPCCT technologies (clockwise direction: gold nanoparticles, yellow color in the lungs, gadolinium, green color – stomach and intestines, and iodine, red color – bladder and kidneys while soft tissue and bone in blue and white colors respectively-MARS bioimaging, mouse heart, and surrounding tissue, Yb and Au nano colloid in blue and yellow in the mouse model, and AuNPs as yellow color in kidney and tumor in mouse model-MARS bioimaging, and very first human wrist with a watch scan, & human ankle-MARS bioimaging) (B). Reproduced from ref. 29–36 with permission from American Chemical Society (copyright 2019), International Institute of Anticancer Research (copyright 2013), The Society of Nuclear Medicine and Molecular imaging (copyright 2019), Radiological Society of North America (copyright 2002), MARS bioimaging Ltd, New Zealand, and American Society of Chemistry (copyright 2022). |
However, the use of high-Z nanoparticles as contrast agents in imaging presents several challenges, including toxicity, rapid clearance, and retention in tissues. These challenges are especially important for clinical applications where high doses of the NP agent may be necessary to achieve sufficient contrast enhancement. Small NPs can be cleared quickly, which reduces the imaging sensitivity and limits the imaging time window. However, larger NPs may accumulate in organs such as the liver and spleen, which can cause tissue damage, inflammation, and other adverse effects.37,38 To overcome these challenges, it is essential to optimize the size, shape, surface coating, and dosing of the high-Z NPs before use in animals or humans.39 Additionally, high-Z NPs can be synthesized in optimal sizes, and shapes, and functionalized with biocompatible coatings to improve their retention in the body and reduce toxicity. With the optimization of these physico-chemical properties of nanoparticles, the cell-nanoparticle interaction can be controlled to guide the cellular or tissue uptake of nanoparticles by known mechanisms such as phagocytosis, clathrin-mediated endocytosis, caveolae-dependent endocytosis, micropinocytosis and others (diffusion, microinjection, and hole formation).40–48 For instance, biocompatible polymer coating has been shown to significantly reduce the toxicity of gold NPs.49,50 Therefore, in this review, we systematically collate the latest advances in the last decade, in which high-Z nanoparticulate systems have been used for contrast enhancement in DECT and SPCCT. This review focuses on covering studies focused on the utilization of high-Z NPs in in vitro, in vivo, and simulation research studies and delineates potential future developments. We also discussed the potential clinical benefits and limitations of using high-Z NPs as X-ray contrast agents.
High-Z NPs have emerged as promising contrast agents for SPPCT imaging owing to their unique physical and chemical properties. In particular, they have been explored as promising contrast agents for DECT and SPCCT, advanced imaging modalities. These imaging technologies can enhance the contrast, and material composition of tissues by detecting and quantifying the distinct K-edge energies of high-Z elements in a targeted region. Many high-Z elements have been suggested as alternative elements for spectral CT imaging due to their ability to attenuate X-rays in the diagnostic energy range such as europium (Z = 63; K-edge = 48.5 keV), gadolinium (Z = 64; K-edge = 50.2 keV), terbium (Z = 65; K-edge = 52 keV), ytterbium (Z = 70; K-edge = 61.3 keV), hafnium (Z = 72; K-edge = 65.3 keV), tantalum (Z = 73; K-edge = 67.4 keV), tungsten (Z = 74; K-edge = 69.5 keV), rhenium (Z = 75; K-edge = 71.6 keV), gold (Z = 79; K-edge = 80.7 keV), and bismuth (Z = 83; K-edge = 90.5 keV). Fig. 2 shows the simulated mass attenuation coefficients of several high-Z NPs and their respective K-edges.49 Some of these high-Z NPs not only serve as contrast agents for imaging but also have therapeutic properties, allowing for targeted treatment of certain diseases or conditions. For example, gold nanoparticles have been investigated for their potential as both contrast agents and targeted drug delivery agents.53 By introducing high-Z NPs or hybrid high-Z NPs (mixed with Fe) at the disease site through passive or active targeting, the image contrast of targeted tissues can be enhanced, and the diagnostic accuracy of advanced and conventional imaging modalities can be improved.54–56
Fig. 2 Mass attenuation coefficients of several high-Z materials as a function of energy. Also showing a tungsten X-ray spectrum for 120 kVp tube peak voltage. Reproduced from ref. 51 with permission from by the authors, Licensee: Springer Nature, under the Creative Commons Attribution License, copyright 2018. The logarithmic mass attenuation coefficient emphasizes how the attenuation effect varies with energy and K-edge (B), reproduced from ref. 57 with permission from Elsevier B.V., copyright 2016. |
High-Z materials have K-edge energies within a diagnostic imaging energy range, where there are a reasonable number of photons above and below their K-edge (approximately 40–100 keV in a 120–140 kVp beam) as shown in Fig. 2A. Gold and bismuth have the highest Z and hence the highest attenuation coefficient at their respective K-edges. In an SPCCT system, the energy ranges of the photon-counting detectors can be adjusted to capture the sudden increase in X-ray attenuation of the elements.58 For instance, for a gold K-edge of 80.72 keV, setting an energy window immediately below and above the K-edge would result in a large difference in X-ray attenuation by high-Z NPs.59 Moreover, multi-energy windows provide users with the opportunity to set up energy windows in the low-energy photoelectric region. In general, the photoelectric and Compton effect are the primary mechanisms by which materials attenuate X-ray beams in the diagnostic energy range. Generally, in the photoelectric effect, a K-shell electron receives energy owing to a collision with a photon, which transfers its energy to the electron, leading to its ejection from its shell and traveling a short distance before its energy is lost. The photoelectric effect is scaled with Z3 for any given photon energy, which means that iodine (conventional contrast agent) is likely to produce 2.6- and 3.8-times smaller X-ray contrast than that of tantalum (Z = 73) and bismuth (Z = 83), respectively compared to iodine K-edge. However, the photoelectric effect is inversely proportional to the energy of the photon cubed (1/E3) and decreases as the energy increases. Consequently, tantalum and bismuth generate 8.1- and 20.2-times lower contrast respectively, compared to iodine due to their higher K-edge energy (Fig. 2B). This inverse relationship with energy could significantly negate the greater attenuation benefit from the high atomic number at higher energies. K-edge energy imaging can be used for the detection and differentiation of diverse elemental densities. Previous reports have demonstrated the effectiveness and potential application in quantitative measurements and differentiation of Ta and I during a phantom study using SPCCT.60 Such an analytical tool for region-of-interest (ROI) offers opportunities for diagnosing site-specific irregularities as a result of diseased tissue or blockage.
Moreover, a few studies have also indicated that elements with Z numbers in the range of 63–73 can be considered optimal for enhancing spectral X-ray contrast efficiency, while higher Z elements may decrease photon counts sensed by the detectors and increase the crosstalk between bone and other surrounding soft tissues.2,51,61 In addition to the X-ray attention of high-Z NPs, other properties need to be considered, that includes biocompatibility, non-toxicity, ease of synthesis and tuning of sizes and shapes, ease of surface functionalization for cell targeting, favorable pharmacokinetics, and low cost.51
Fig. 3 Important properties of AuNPs (tunable size and shape) (A), ease of surface functionalization (B), reproduced from ref. 62 with permission by the authors, Licensee: MDPI, Basel, Switzerland, under the Creative Commons Attribution License, copyright 2018, and SPCCT imaging of different concentrations of gold and AuNP-herceptin binding to HER2-positive breast cancer cells (SKBR3) (C), reproduced from ref. 63 with permission by the authors, Licensee: John Wiley & Sons and Hindawi Publishing Corporation, under the Creative Commons Attribution License, copyright 2018. |
The literature provides strong evidence that AuNPs smaller than 100 nm have been favored for different clinical applications, especially cancer cell targeting, imaging, and therapy in humans and animals.62 This influx of AuNPs has been linked to biocompatibility, nontoxicity, and longer blood or lymphatic circulation times.64 In a recent in vitro study, the MARS SPCCT scanner was used to show the selective uptake of monoclonal antibody (trastuzumab or rituximab)-conjugated AuNPs (40 nm) by cancer cells in vitro. For this, SKBR3 and Raji lymphoma cancer cells with trastuzumab-AuNPs and rituximab-AuNPs, respectively after which the cells were collected in Eppendorf tubes which were fixed in a PMMA phantom holder. The study exploited the tendency of trastuzumab (Herceptin) to bind with HER2-positive breast cancer cells (SKBR3) and rituximab to bind to the CD20 antigen of B-cell lymphomas. The authors reported AuNP-trastuzumab uptake in SKBR3 cells and AuNP-rituximab uptake in Raji cells (Fig. 3C) as detected and imaged by MARS SPCCT. They demonstrated the potential application of SPCCT in molecular imaging, which allows the detection and quantification of functionalized AuNP uptake by cancer cells in vitro.63,65
Several reports confirm the size-dependent uptake of NPs by cancer cells. In this context, a study described higher uptake of 18 and 80 nm “as prepared” AuNPs in ovarian cancer cells (OVCAR5 and SKOV3), and selective targeting of ovarian cancer in an in vivo model using LHRH peptide-conjugated (PEG-peptide mixed monolayer) AuNPs.66,67 Another study also showed the accumulation of 15 nm AuNPs at the periphery of Lewis lung carcinoma implanted in mice. These studies highlight the importance of SPCCT for the detection and quantification of AuNPs in cancerous cells and tissues both in vitro and in vivo.65 In another study, AuNPs functionalized with an anti-plasma membrane heat-shock protein antibody were used for in vitro cell culture and in vivo imaging in mice. They showed that functionalized AuNPs accumulated in the plasma of tumor cells but not in normal cells. Spectral CT imaging and histological studies confirmed the selective accumulation of functionalized AuNPs in different tumor mouse models64 (Fig. 4A).
Fig. 4 Tumor detection in tumor-bearing mice using spectral photon-counting CT. Functionalized AuNPs were located in the tumor periphery and were highly dispersed in the tumor center (A), reproduced from ref. 64 with permission by the authors, Licensee: MDPI, Basel, Switzerland, under the Creative Commons Attribution License, copyright 2020. Darkfield microscopy showing PEG-AuNP and RGD-AuNP targeting of endothelial in vitro for 1 mg mL−1 and 6 mg mL−1 of gold (B), reproduced from ref. 68 with permission from Ivyspring International Publisher, copyright 2018, and SPCCT fused images of atherosclerotic rabbit aorta 2 days after injection of AuNPs and iodine (Iomeprol, 400 mg mL−1) as contrast agents (C), reproduced from ref. 59 with permission from Radiological Society of North America, copyright 2021. |
One study used DECT to quantify the accumulation of iodine, bare AuNPs, and RGD peptide-functionalized AuNPs (25 nm) to enhance the radiation therapy tumor dose in mice. Human umbilical vein endothelial cells (HUVECs) were exposed to AuNPs in an in vitro experiment. Darkfield microscopy showed an increased accumulation of AuNPs in HUVECs, especially when labeled with the RGD peptide (Fig. 4B). They quantified the effect of AuNPs on radiation-induced tumor vascular disruption. DECT allowed for the measurement of AuNP accumulation and assessment of vascular permeability.68 In yet another study, DECT was employed to measure the concentration of AuNPs functionalized with folic acid (FA-AuNP) in human nasopharyngeal cancer cells. NPs (15 nm in size) were synthesized, and different concentrations (0.25–2 mg mL−1) were placed in the phantom for imaging at 80 and 140 kVp. KB cells incubated with FA-AuNPs under different concentrations were detected and quantified by DECT. The study reported that FA-AuNPs are suitable candidate for targeted DECT imaging of nasopharyngeal cancer cells.69 In another study, Cormode et al. investigated SPCCT imaging of AuNPs functionalized with high-density lipoprotein (Au-HDL). The AuNP formulation was used for the characterization of macrophage burden, calcification, and atherosclerotic plaque in apo E-KO mice and in a phantom. SPCCT with a 3 mm-thick cadmium telluride detector was used to acquire images for six energy windows (0–25, 25–34, 34–51, 51–80, 80–91, and 91–110 keV).70 Material decomposition (MD) using the maximum likelihood method was used to detect gold and iodine. Phenomena such as photoelectric and Compton effects allowed the differentiation of Au-HDL, iodine, and calcium phosphate in the phantoms. During the in vivo study, accumulation of Au-HDL was detected in the aortas of atherosclerotic mice. This demonstrates that SPCCT imaging of Au-HDL can be used to detect macrophages in atherosclerosis.70
An in vivo study used PEG-conjugated AuNPs to quantify macrophage burden in atherosclerotic plaque after intravenous injection of 3.5 mL kg−1 AuNP-PEG (stock −65 mg mL−1) in a rabbit model. AuNP-PEG K-edge imaging allowed plaque image enhancement. The results were confirmed by histological examination, transmission electron microscopy, inductively coupled plasma analysis, and optical emission spectrometry. Fig. 4C shows the SPCCT image of the rabbit aorta where AuNPs (yellow) accumulated in the plaque and iodine as an additional contrast agent (red). This illustrated the ability of SPCCT to image AuNP accumulation in atherosclerotic plaques. Detection and quantification of the Au concentration in the macrophage burden in atherosclerotic plaques are possible with SPCCT.59 Si-Mohamed has also employed the PEGylated-AuNPs in conjunction with SPCCT to investigate the biodistribution of gold (a high-Z material) as well as molecular imaging of mononuclear phagocyte system (MPS) in a rabbit model.71 Another study reported the use of SPCCT to visualize Au-labeled macrophages extracted from the bone marrow and implanted these cells as therapeutic cells in 21 rats with brain damage. This study showed the feasibility of using AuNP-labeled macrophages for two weeks after implantation in clinically stimulated brain injury. This shows that unlike the short-lived positron emitters used in PET imaging, AuNPs can be imaged for a much longer period using SPCCT.72 Wan et al. used silica coated AuNPs further functionalized with DNA Transfectin 3000 as a potential cellular probe for tracking stem cells in bone regeneration using DECT. The study suggested that DECT imaging with AuNPs–SiO2 allowed accurate and noninvasive tracking of stem cells in an in vivo model. This study was scoped for the potential new possibilities of stem cell-mediated bone regeneration. Additionally, gold nanoparticles were found to be minimally toxic and did not adversely affect stem cells or surrounding tissues.73
Cormode et al. used a spectral CT to investigate the feasibility of simultaneously imaging and quantifying PEG-coated AuNPs and iodine contrast agents in a phantom and in vivo in New Zealand white rabbits. They concluded that SPCCT allows the simultaneous imaging and quantification of AuNPs and iodine as contrast agents in vivo.74 Si Mohamed et al. used Au, gadolinium, and iodine-based contrast agents at concentrations that yielded the same HU of 280. Contrary to conventional CT, they showed that SPCCT allowed differentiation between contrast agents in a phantom study using material recognition methods.25 Dong et al. studied the effect of the size (4–152 nm) of AuNPs capped with 5 kDa m-PEG as an image contrast agent using two conventional clinical CT scanners, two micro-CTs, and an SPCCT. They reported that at the same concentrations (0–10 mg mL−1) in a phantom, there was no significant difference in image contrast owing to size variability. However, the HU values increased linearly with concentration for all sizes. In addition, the study concluded that 15 nm or smaller AuNP-mPEG had a longer circulation time in six mice injected with an NPs dose of 500 mg kg−1. Larger NPs accumulate in the liver and spleen.75 Zambrano-Rodrigues et al. used dual energy micro-CT to image AuNPs and iodine as contrast agents to enhance the myelogram in the rat (sample size −18). They used commercially available iodine-based (Iomeron® 400 and Fenestra® VC) and AuNP-based (AuroVist™ 15 nm, Nanoprobes) contrast agents. They obtained a better contrast-to-noise ratio (CNR) using single-energy time subtraction with Iomeron as a contrast agent. However, this study also showed the potential application of AuNPs as contrast agents to obtain high-resolution myelograms with micro-CT.76
Sadeghian et al. conducted an MC simulation study to simulate the SPCCT imaging of gold, silver, and bismuth 50 nm NP and iodine at concentrations of 2, 4, and 8 mg mL−1 in a water-filled cylindrical phantom. The simulation indicated that high-Z NPs had a higher CNR than iodine.77 Jo et al. used the Monte Carlo method to simulate SPCCT imaging and DECT for three-material decomposition (lipid, iodine, and gold nanoparticles) to identify vulnerable plaques in the coronary artery. The proposed technique analyzes the composition of plaques by quantifying the number of lipids and calcification. They modeled a coronary artery (3 mm diameter tube) filled with iodine contrast, AuNPs, or lipids. They found that the technique had good sensitivity and specificity for identifying the three materials. This study suggests that this new technique has the potential to detect the accumulation of AuNPs in plaques in the presence of lipid and iodine contrasts in the lumen. This has the potential clinical application to improve the diagnosis and management of coronary artery disease.78Table 1 captures a summary of AuNP studies performed since 2014 with a focus on the size and shape of the nanoparticles, nanoparticle size, targeting agent, the type of study (in phantom, in vitro, in vivo, or simulation), and the application.
NP (size (nm)) | Functionalization | Study type | Application | Ref. |
---|---|---|---|---|
Au (3.1) | HDL | In phantom and in mice aorta | Detect macrophages in atherosclerosis | 70 |
Au (12.5) | PEG coating | In phantom and New Zealand rabbits with atherosclerotic plaque | Quantify macrophage burden in atherosclerotic plaque | 59 |
Au (50), Ag (50), Bi (50) | None | In phantom | Monte Carlo simulation to measure contrast | 79 |
Au (45 ± 15) | Anti-plasm membrane heat shock protein antibody | In vitro cell culture and in mice | Functionalized AuNP targeting of cancer cells | 64 |
Au (22) | 11-Mercaptoundecanoic acid | In phantom, in cell culture | AuNP used to label implanted microphages in damaged rat brain | 72 |
Au (15) | Folic acid | Cell culture | Au–FA targeted nasopharyngeal cancer cells | 69 |
Au (4–152) | m-PEG | In phantom and in mice aorta | Contrast depends on concentration does not size of NP | 75 |
Au (18) | None | In phantom | Color imaging of Au, Gd, and iodine when they give the same HU. | 25 |
Au (18, 40, 60, 80) | None | In phantom, in cell culture, and in mice | In vitro and in vivo targeting and imaging of cancer cells | 65 |
Au (40) | Herceptin | In phantom, in cell culture | In vitro and in vivo imaging of cancer cells | 63 |
Au (25) | RGD peptide | In cell culture and in mice | Targeting of endothelial cells and assessment of vascular permeability | 68 |
Au (12) | PEG | In phantom and in vivo rabbits | Quantification of AuNP and iodine contrast agents in vivo | 74 |
Au (12.5) | PEG | In vivo | Quantification and biodistribution of NPs in vivo | 71 |
Au (20) | Silica and DNA transferrin 3000 | In vitro and in vivo rabbits | In vitro and in vivo targeting bone marrow stem cells using AuNP–SiO2 with DNA transferrin 3000 | 73 |
Kochebina et al. used SPCCT and SPECT to image and quantify GdNPs in phantom studies. GdNPs were labeled with gamma-emitting84 In for SPECT imaging using a Philips Healthcare System. A prototype with maximum likelihood material decomposition methods with 0.25 mm spatial resolution in all directions was used. The study concluded that GdNP detection and quantification are possible with SPCCT and SPECT; however, SPCCT does not require radiolabeling while preserving the sample scan time compared to SPECT.85 A study by Badea et al. systematically investigated the preclinical efficacy of Gd and iodine-based liposomal nanostructures as contrast agents for cancer imaging. They also imaged mice administered with liposomal iodine (145 nm size and 0.2 g Gd kg−1) and liposomal GdNPs (270 nm, 0.2 g Gd kg−1). They demonstrated that DECT allows simultaneous qualitative and quantitative analysis of iodine and Gd-based contrast agents. To satisfy the dose limit of detectability and to keep the signal-to-noise ratio (CNR) at a minimum, the minimum threshold concentration of the contrast agent had to be 2.46 mg mL−1.86
Another study used dopamine (DA)-and hyaluronic acid (HA)-functionalized bismuth fluoride (BiF3) NPs (BiF3@PDA@HA) to accurately diagnose liver fibrosis using spectral CT.87 By modifying nanostructures with HA, cell-specific targeting of hepatic satellite cells is possible, which is a hallmark of liver fibrosis. In vitro studies confirmed faster cellular uptake of the HA-coated nanoparticles compared to PEG-modified systems (BiF3@PDA@PEG) used as a non-specific control. The in vivo assessment further validated the in vitro observations using the two formulations (HA versus PEG-modified systems) in a mouse model. The spectral CT results demonstrated significant enrichment of Bi for the targeted BiF3@PDA@HA group in the diseased liver tissue up to 80 min post-injection. On the other hand, the non-target group (BiF3@PDA@PEG) showed no signal enhancement in the hepatic parenchyma. Additionally, the targeted nanoformulation showed no contrast enhancement in the healthy liver, suggesting the potential utilization of this system for resolving diseased tissue from healthy liver tissue. Fig. 5(A–H) represents the SEM images of BiF3@PDA@HA nanoparticles along with the chemical analysis using FTIR, followed by a comparative image from traditional CT and spectral CT of the liver (and surrounding organs), pre-and post NPs injection, and an increase in intensity with time in the targeted group. The image also shows the energy-dependent attenuation of the targeted region after BiF3@PDA@HA NPs injection in the in vivo model, and changes in the spectral house units (HU) of the liver and tissue at different energy attenuations. Furthermore, because of the energy-dependent attenuation of Bi, the diseased area could be suitable for selecting different monochromatic energies via spectral CT.87
Fig. 5 (A) Scanning electron microscopy (SEM) images of BiF3@PDA@HA. (B) Fourier transformation infrared spectra (FT-IR) of BiF3@PDA@HA, BiF3@PDA, BiF3, HA, and PDA. (C) Representative CT images were acquired at two-time points (pre-injection and 30 min after the injection of BiF3@PDA@HA) for two groups via spectral CT (70 keV) and conventional CT (140 kVp). (D) Representative spectral CT images of the targeted group before and after the injection of BiF3@PDA@HA. (E) Dynamic time courses of CT value and CT value change (ΔCT value) of hepatic parenchyma of the targeted group (red line, n = 3) and control group (grey line, n = 3). (F) 40–70 keV monochromatic images of the targeted group. (G) Comparison between the targeted group (n = 3) and the control group (n = 3) in CT value of monochromatic images of 40–70 keV. Data were presented as mean ± standard deviation. (H) Spectral HU curves of the liver (yellow line) and muscle (red line) of the targeted group. (A–H: Reproduced from ref. 87 with permission from Wiley-VCH GmbH, copyright 2021.) (I) TEM images of Bi2S3 NPs. (J) HAADF-STEM images of Bi2S3 NPs and the EDX elemental mapping of Bi and S elements and the merged image. (K) XRD pattern of Bi2S3 NPs and the standard Bi2S3. (L) Traditional CT imaging of the mouse model with intestinal obstruction after oral administration of 400 μL Bi2S3 NPs (26 mg mL−1 Bi2S3 NPs) at 120 kV. (M) Spectral CT imaging of the mouse model with intestinal obstruction at 30 min after oral administration of 400 μL Bi2S3 NPs (26 mg mL−1 Bi2S3 NPs) at various X-ray energies (40, 60, 80, 120, and 140 keV). (N) Traditional CT imaging of the mouse model with intestinal obstruction after surgery to relieve intestinal obstruction at 120 kV. (O) Spectral CT imaging of the mouse with surgery to relieve intestinal obstruction at 6 h under various X-ray energies (40, 60, 80, 120, and 140 keV) (I–O: Reproduced from ref. 6 with permission from Royal Society of Chemistry, copyright 2022). Image assembled with https://BioRender.com. |
In a simulation-based study comparing the spectral properties of Au, Ag, and Bi NPs with an average diameter of 50 nm, the AuNPs generated the highest CT and CNR values. AgNPs demonstrated better performance at 80 keV, whereas a higher energy of 120 keV was required for BiNPs to generate a high CNR. These results suggest that NP-based contrast agents are superior to iodine with a higher CT number and CNR.77 While another study suggested that iron oxide NPs coated with Bi (Fe3O4@Bi) or Au (Fe3O4@Au) produced the same image quality but better quality images were obtained between 100–120 keV for Bi-coated NPs.88 Furthermore, bismuth sulfide (Bi2S3, 276 nm size) flower-like nanostructures or nanoparticles synthesized by a green strategy (highly monodispersed) showed high biocompatibility and absorption in the NIR range and excellent spectral CT imaging capability. The administered formulation generated accurate spectral CT images for the gastrointestinal tract as well as assisted with the diagnosis of intestinal obstruction as a result of growing tumor in vivo, as shown in Fig. 5(I–O).6Fig. 5I–K show the TEM image of Bi2S3 NPs, HAADF-STEM images with EDX elemental mapping of Bi and S elements, and XRD analysis of Bi2S3 NPs, respectively. Fig. 5L shows a traditional CT image of a mouse model with intestinal obstruction after oral ingestion of 400 μL Bi2S3 NPs (26 mg mL−1 Bi2S3 NPs) at 120 kV. Fig. 5M shows an SPCCT image of an in vivo model with intestinal obstruction after 30 min of oral administration of Bi2S3 NPs (400 μL, 26 mg mL−1 Bi2S3 NPs) at different X-ray energies (40, 60, 80, 120, and 140 keV). Fig. 5N is a traditional CT image of a mouse with intestinal obstruction after surgery, confirming relief from intestinal obstruction at 120 kV; Fig. 5O represents an SPCCT image of the same after 6 h under various X-ray energies (40, 60, 80, 120, and 140 keV).
Fig. 6 (A) Schematic representation for the synthesis of Yb nano-colloids along with elemental information. (B) TEM image of Yb nanocolloid encapsulated in lipid NS. (C–E) AFM image of Yb nanocolloid dried on a glass slide, the number size distribution of colloid and different physicochemical properties of the same. (F) blood pool imaging using pseudo-conventional CT from the spectral measurement of the heart for non-targeted control in vivo model administered with Yb nanocolloid. (G and H) image reconstruction after 1 and 20 iterations of the same, respectively. (I) volume rendered CT image super-imposed with Yb signal (green dot/arrow) showing accumulation of targeted Yb nanocolloid in the heart. (A–I: Reproduced from ref. 93 with permission from American Chemical Society, copyright 2012.) (J) A 2D CT image of the mouse in coronal view, pre and post-YbNPs-hydrogel – blue color and AuNPs-hydrogel – yellow color injection after 5 min and 1 week. (K) total CT attenuation-based quantification of Yb and Au after 5 min and 1 week. (L) representing the 3D reconstruction of YbNPs-hydrogel based on data in (J). (M) Representative 3D volume rendered CT image of in vivo model introduced with Yb-blue and Au-yellow based hydrogels at different times. (N) information on biodistribution of Yb and Au in major organs and tissues and carcass administered with NPs hydrogels after 2 weeks. (J–N: Reproduced from ref. 94 with permission from American Chemical Society, copyright 2022.) Image assembled with https://BioRender.com. |
Some advantages of Yb-based NSs are the high abundance of Yb, lower toxicity when encapsulated within an appropriate carrier, and K-edge energy (61 keV) within the X-ray spectrum range recommended for clinical CT.95–97 In one study, oleic acid, and DSPE-PEG 200 stabilized YbNPs were intravenously administered (1.0 mL, 70 mg mL−1 Yb) in rats as contrast agents. The YbNP formulation remained in the systemic circulation for longer with minimal toxicity and showed high efficacy compared to the iodine-based suspension for enhanced vascular imaging and disease diagnosis.91 Another comparative study demonstrated higher contrast generation by YbNPs relative to traditional AuNPs for hydrogel labelling thus permitting its localization and tracking in vivo for different biomedical applications (Fig. 6J–N).94Fig. 6J shows a 2D CT image of the coronal view of a mouse model before and after YbNP-hydrogel (blue) and AuNP-hydrogel (yellow) administration for five minutes and 1 week, respectively. Fig. 6K shows the total CT attenuation-based quantification of Yb and Au at the same time points. Fig. 6L shows a 3D reconstruction of the YbNP hydrogel based on the information collected in Fig. 6J. Fig. 6M shows a 3D volume-rendered CT image of an in vivo model injected with the YbNP hydrogel (blue) and AuNP hydrogel (yellow) at different times. Fig. 6N shows the biodistribution of Yb and Au in the major organs, tissues, and carcasses at the end of the study after 2 weeks. By successfully modifying YbNPs with SiO2 and N-nitrilotriacetic acid (NTA), preferential calcium chelation was possible, which allowed specific targeting of the damaged bone. The crack-targeted Yb NPs successfully generated a high-contrast spectral CT image of the damaged tissue in real time and differentiated healthy and cracked bone tissue in vivo.98
Ytterbium is also known for its up-conversion luminescence, which makes Yb NSs suitable for multimodal imaging platforms. To harness the multi/bimodal capability of Yb, PEGylated NaYbF4:Tm3+ NPs (UCM, average size 20 nm) were used for SPCCT and NIR-fluorescence imaging. This allowed the generation of high contrast for SPCCT and strong NIR-fluorescent emission both in vitro and in vivo. The UCM NPs formulation showed 75% more CT contrast efficacy than clinically available iobitridol.99 Additionally, the nanoparticles were non-toxic to HL-7702 and RAW264.7 cells up to 1.6 mg Yb mL−1, while at 150 mg Yb kg−1 concentration in the in vivo model. The administered formulation showed low or no tissue damage and was removed from the systemic circulation via feces and urine within 7 days, with some accumulation in the spleen 1 month post-injection. In another study, silica- and PEG-stabilized hybrid Yb and barium NPs (BaYbF5@SiO2@PEG) significantly enhanced the image contrast with improved circulation time compared to clinical iodine-based contrast agents. The improved circulation time was attributed to the antifouling capability of PEG, suggesting the potential use of this nanoformulation as a blood pool CT contrast agent for diagnosing diseases such as myocardial infarction and thrombosis. This study validated the efficacy of the formulation for high-resolution blood pool imaging in both small (rat model) and large (rabbit) animal models with clear contrast enhancement within 2 h of administration.100 The long-term toxicity of the administered formulation was determined by histology, which showed no noticeable signs of tissue damage and/or inflammation.
Fig. 7 Bone microdamage detection (A–J). (A–D) TEM image of targeted hafnia NPs, hydrodynamic diameter by frequency distribution along with surface zeta potential before and after immobilization of targeting molecule and 1H NMR spectra of NTA ‘i’, ‘as prepared’ ‘ii’ and surface modified ‘iii’ Hf NPs. (E) Showing the micro-CT image of bones clean, soaked in targeted Hf solution, and soaked in ‘as prepared’ Hf NPs solution. (F) (i–v) show spectral CT 3D images of ex vivo human bone microdamage and distribution of targeted Hf NPs (red color) and bone (white/gray) with the color scale. The arrow shows the location of the microdamage. (G) The bone microdamage was investigated using traditional CT in an in vivo model (control sham-operated model-ii, ‘as prepared’ NPs 30 min-iii, ‘as prepared’ NPs 5 h-iv, and targeted Hf NPs after 30 min and 5 h-v and vi respectively). (H) The 3D reconstructed spectral CT image of G, the arrow represents Hf NPs accumulation (i – control, ii – nontargeted NPs 30 min, iii – nontargeted NPs 5 h, iv – targeted NPs 30 min, v – targeted NPs 5 h). (I) TEM image of injection site showing no NPs aggregation and accumulation. (J) in vivo bone microdamage evaluation and Hf NPs differentiation from bone and surrounding tissue using spectral CT, gray is bone, cyan-green is a high concentration of Hf NPs, blue is low concentration and white is calcium. (A–J: Reproduced from ref. 61 with permission from Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim, copyright 2019). Gastrointestinal tract imaging using hafnium oxide NPs (K–T). (K) A conventional CT of a rat model fed with HfO2 NPs, showing the accumulation of NPs in the abdominal region. (L) Coronal view of one energy bin showing NPs and bone. (M) is the coronal view for hafnia channel overlay with energy bin while N is a 3D volumetric reconstruction of material decomposition differentiating bone and HfO2 NPs. (O & P) are the magnified images of the bright green region in image (N). (Q–T) are the material weight spectral photon-counting images of the GI tract where the rat was fed with an HfO2 capsule. (Q) Yellow color represents lipid, cyan is for HfO2 NPs, (R) cyan – HfO2 NPs and gray – hydroxyapatite, (S & T) cyan – HfO2 NPs. (K–T: Reproduced from ref. 102 with permission from Royal Society of Chemistry, copyright 2022.) Image assembled with https://BioRender.com. |
In a recent study, ultra-small 1–2 nm HfO2 NPs were designed for oral ingestion and hitchhiking probiotic bacterial cells for spectral CT imaging of the gastrointestinal (GI) tract. The nano–bio interaction for engineered NPs delivery combines natural delivery with harnessing probiotic cell functions. The nano–bio-hybrid formulation was prepared by the passive uptake of HfO2 by probiotic bacteria, including E. coli and L. lactis, following which the bacteria were freeze-dried and could be effectively revived post-processing. The idea behind this was that the modified probiotic can be effectively packed in an oral formulation, such as a capsule, to be administered to the patient. As a proof of concept, the authors prepared bio-HfO2 by incubating E. coli with 54 mg of NPs for 4 h after which the bacteria were washed, freeze-dried, and resuspended in PBS for imaging using spectral CT. The imaging results confirmed that bio-HfO2 could generate a high-contrast colored image of the GI tract, intestine, cecum, and small bowel diverticula within 30 min of oral ingestion. The results confirmed that the nanoparticle system was protected from degradation under harsh GI conditions and systemic absorption, thus offering a platform that can be used for GI imaging (Fig. 7K–T).102Fig. 7K is a traditional clinically available CT image of a rat model fed with HfO2 and a high-resolution image showing the accumulation of NPs in the abdominal region. Fig. 7L shows the coronal view of one energy bin showing NPs and bone, and Fig. 7M shows the coronal view of the hafnia channel overlay with an energy bin. In addition, Fig. 7N shows a 3D volumetric reconstruction of the MD analysis with clearly distinguishing bone and HfO2 NPs. Fig. 7O and P are magnified images of the bright green region in Fig. 7N. Fig. 7Q–T are the SPCCT images of the GI tract where rats were fed with HfO2 capsule where lipid is represented by a yellow color, HfO2 NPs are shown by cyan, and HA by gray color.
Another study utilized the ability of Hf to excite surface phonon polariton nodes in the mid-infrared region, which is like surface plasmons for metal NPs such as Au and Ag. This study highlights yet another application of HfO2 NPs (7–31 nm size range), which can potentially be used for photonic biosensing applications as well as contrast agents for MARS spectral CT applications.103 The literature has also proposed the potential use of PVP-stabilized Hf NPs (10–20 nm) to target human tumor xenograft murine models and differentiate the tumor and its vasculature system. Furthermore, the surfaces of these three NP types were conjugated with antibodies using CLICK chemistry, which successfully targeted the cdl33(+) SKOV3-IP cells both in vitro and in vivo, which are primarily responsible for the metastasis and poor prognosis of ovarian cancer.83,104
Fig. 8 (A–(C) Physico-chemical characterization of tantalum NPs, showing TEM images for ‘as prepared’, PEG-RITC modified NPs and absorbance-fluorescence spectra for free RITC and PEG-RITC-TaOx colloid. (D) H & E-stained tissue samples from organs (top-bottom: liver, spleen, heart, kidney, and lung) at different time points (control, day 1, 3, 7 and 15) showing minor toxicity of NPs (injected with 1 mL of NPs colloid in the tail vein at 840 mg kg−1 concentration) in the liver. (E) A 3D volumetric render of in vivo spectral CT model top-ventral and bottom-lateral side of the heart and great vessel immediately after injection. (F) Top-heart and liver coronal view along the dotted line in (E), and bottom showing spleen, kidney, and inferior vena cava for the same. (G) Showing the sentinel lymph node mapping and resection in the in vivo model using spectral CT volumetric rendering after 2 h of intradermal injection of 100 μL of PEG-RITC-TaOx colloidal suspension (210 mg mL−1), yellow circle highlights the location of the lymph node. Reproduced from ref. 108 with permission from American Chemical Society, copyright 2011. Image assembled with https://BioRender.com. |
The precise location of the sentinel lymph node is critical for determining tumor metastasis and can be useful in avoiding unnecessary tissue removal during surgery. By carefully mapping the lymph nodes, this can be avoided, and the study demonstrated that by intradermal administration of PEG-RITC-TaOx, the lymph node location could be monitored. This was feasible due to the enhanced X-ray contrast, following which the tissue could be removed using fluorescence imaging. The results presented in this study confirmed the presence of NPs in excised tissue, but no histological changes were observed.
A recent study used rhenium sulfide (ReS2) nanoparticles as preclinical drugs for spectral CT imaging of the GI tract, along with CT-assisted photothermal therapy of tumors. The spectral CT imaging results confirmed that the ReS2 NPs significantly enhanced the contrast relative to the background. Thus, ReS2 NPs are good candidates for high-sensitivity spectral CT imaging for in vivo studies. Additionally, the ReS2 NPs were able to image the tumor via spectral CT post-administration in a 4T1 tumor-bearing mouse model. There was a significant improvement in contrast enhancement for the tumor, up to threefold upon nanoparticle injection, thus offering the possibility of disease diagnosis and therapy. In addition, when exposed to a low-intensity 808 nm laser, ReS2 NPs were able to cause hyperthermia within the tumor environment, and complete eradication of the tumor was observed (Fig. 9).115 The synthesized ReS2 NPs demonstrated strong X-ray absorption at various energies for enhanced spectral CT imaging. This study also reported a significantly higher signal-to-noise ratio, thus offering a platform for theranostic applications without posing any safety concerns. Moreover, the biomedical imaging applications of Re-based nanostructures are not limited to spectral photon-counting CT imaging but have been explored for photoluminescence imaging, as reported elsewhere.116Fig. 9A–D shows the physicochemical characterization of ReS2 NPs (TEM image, XPS analysis, and UV-Vis-NIR absorbance spectra) Fig. 9E is CT image of GI tract (in vivo model) using traditional CT system. The in vivo model consumed 400 μL of a 10 mg mL−1 ReS2 NPs suspension. Fig. 9F shows the SPCCT image of the GI tract after oral administration of NPs and iohexol at different energy levels. Fig. 9G represents the SPCCT images of tumor-bearing mice before and after ReS2 NPs (100 μL, 5 mg mL−1, 17.5 mM Re) or iohexol (100 μL, 17.5 mM I) injection (tumor location highlighted with green circle).
Fig. 9 (A–(D) Physico-chemical characterization of ReS2 NPs. (A) TEM image of NPs, (B) Re 4f orbital XPS spectra, (C) S 2p orbital XPS spectra for ReS2 NPs, and (D) UV-Vis-NIR absorbance spectra of Ns at different concentrations. (E) is conventional CT image of the GI tract of in vivo model fed with 400 μL, 10 mg mL−1 ReS2 NPs colloid while (F) is the spectral CT image of the GI tract after 5 minutes of NPs and iohexol (400 μL, 35 mM) oral administration at different keV. (G) Spectral CT images of tumor-bearing mice pre and post-ReS2 NPs (100 μL, 5 mg mL−1, 17.5 mM Re) or iohexol (100 μL, 17.5 mM I) injection (tumor location highlighted with green circle). Reproduced from ref. 115 with permission from American Chemical Society, copyright 2019. Image assembled with https://BioRender.com. |
The development of multimodality agents, as attractive as it may seem, needs to be thoroughly assessed from clinical and regulatory standpoints. Therefore, the major challenge is to engineer CT contrast agents that have a much higher contrast efficacy at different operating voltages and longer circulation times in vivo relative to clinical iodinated agents. The current formulations work well in small animal models; however, their translation into humans is still impossible. This is in part related to the potential CNR production via the beam-hardening effect, causing fewer photons below the K-edge energies of these elements to reach the detector. In this case, elements with higher atomic numbers produce a higher CNR. For example, this might lead to the contrast generation of tantalum being higher than that of ytterbium. All these limitations of the study can be addressed in the future in larger phantoms or animal models as the technology approaches the clinical stage of development. More recently, successful attempts have been performed by MARS bioimaging Ltd, New Zealand, using SPCCT by scanning the first human wrist and ankle (as shown in Fig. 1B) and generating clinically relevant images using the permissible clinical radiation doses. This demonstrates the potential of SPCCT as an imaging modality for human clinical trials.
Nanomaterials offer great potential for tuning the composition, shape, and targeting ligands, and early clinical diagnosis using spectral CT can be achieved. However, there are several challenges associated with nanoparticles, such as reproducible batch-to-batch synthesis, uniformity in properties, upscaling of nanoparticle production, toxicity, and intrinsic properties that influence biodistribution, elimination, and target site accumulation. These limitations must be addressed to yield their intended translation into clinical diagnosis. The targeting ability of nanomaterials can be realized by surface modification of nanoparticles to make them target-specific and facilitate the binding and internalization in targeted cells with lower accumulation in non-specific and healthy tissues. With the advancement of medical diagnosis in the future, clinicians will be able to provide complete health checks rapidly and regularly in a non-invasive manner. Personalized medicine is a futuristic solution that would allow the design and administration of therapeutics based on the genetic makeup of a patient or person. Early detection or diagnosis based on genetic markers using a nanoparticulate approach for tailoring disease progression at the molecular level would incline the healthcare system towards preventive measures. Therefore, nanomaterials are expected to be used towards the development of platforms, supporting personalized medicine, and offering higher safety and better patient care at lower costs.
High-Z | High atomic number |
CT | Computed tomography |
FL | Fluorescence imaging |
USG | Ultrasonography |
US | Ultrasound |
PET | Positron emission tomography |
SPECT | Single photon emission tomography |
MRI | Magnetic resonance imaging |
PAT | Photoacoustic tomography |
CT | Computed tomography |
SPCCT | Spectral photon-counting CT |
NPs | Nanoparticles |
NRs | Nanorods |
NSs | Nanostructures |
NCs | Nanocrystals |
DECT | Dual-energy CT |
CNR | Contrast-to-noise ratio |
MD | Material decomposition |
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