This disclosure relates to nanosensors for measuring therapeutic levels of ionizing radiation.
Radiation therapy is a common primary treatment modality for multiple malignancies, including cancers of the head and neck, breast, lung, prostate, and rectum. Depending on the disease, radiation doses ranging from 20 to 70 Gy are often employed for therapeutic use. Diseased tissue and normal organ radiation sensitivities also vary. In order to maximize disease treatment relative to radiation-induced side-effects, various methods of delivery including hyperfractionation (0.5-1.8 Gy), conventional fractionation (1.8-2.2 Gy), and hypofractionation (3-10 Gy) have been explored. These delivery methods explore different regimes of radiation sensitivity in order to maximize tumor cell killing while optimizing treatment times.
Despite obvious advantages with radiotherapy, there can be significant radiation-induced toxicity in tissues. For example, radiation-induced proctitis can be a significant morbidity for patients undergoing prostate or endometrial cancer treatment. For centrally located lung cancer radiotherapy, the esophagus can be incidentally irradiated during treatments, resulting in esophagitis. In the head and neck, radiation of salivary gland or pharyngeal tumors can induce radiation-induced osteonecrosis. Another concern during radiotherapy is the motion of the patient as well as the natural peristalsis of internal organs. These issues highlight the importance of appropriately dosing the cancerous tumors while sparing the normal tissue in order to prevent significant morbidity that arises from radiation toxicity.
Despite several transformative advances since its inception in the late 19th century, radiation therapy is a complex process aimed at maximizing the dose delivered to the tumor environments while sparing normal tissue of unnecessary radiation. This has led to the development of image-guided and intensity modulated radiation therapy. The process of treatment planning requires initial simulation followed by verification of dose delivery with anthropomorphic phantoms which simulate human tissue with more or less homogeneous, polymeric materials. The accuracy of the planning is measured using either anthropomorphic phantom or 3D dosimeters. During the treatment, actual dose delivery can be verified with a combination of entry, exit or luminal dose measurements. Administered in vivo doses can be measured with diodes (surface or implantable), thermoluminescent detectors (TLDs), or other scintillating detectors. However, these detectors are either invasive, difficult to handle (due to fragility or sensitivity to heat and light), require separate read-out device, or measure surface doses only. TLDs are typically laborious to operate and require repeated calibration while diodes suffer from angular, energy and dose rate dependent responses. Although MOSFETs can overcome some of these limitations, they typically require highly stable power supplies. In addition, these dosimeters require sophisticated and therefore, expensive, fabrication processes in many cases. In light of these drawbacks, there is still a need for the development of robust and simple sensors in order to assist or replace existing dosimeters that can be employed during sessions of fractionated radiotherapy.
This invention describes lipid-templated formation of colored dispersions of gold nanoparticles from colorless metal salts as a facile, visual and colorimetric indicator of therapeutic levels of ionizing radiation (X-rays), leading to applications in radiation dosimetry. The current nanosensor can detect radiation doses as low as 0.5 Gy, and exhibit a linear response for doses relevant in therapeutic administration of radiation (0.5-2 Gy). Modulating the concentration and chemistry of the templating lipid results in linear response in different dose ranges, indicating the versatility of the current plasmonic nanosensor platform.
Facile radiation sensors have the potential to transform methods and planning in clinical radiotherapy. Below are described results of studies on a colorimetric, liquid-phase nanosensor that can detect therapeutic levels of ionizing radiation. X-rays, in concert with templating lipid micelles, were employed to induce the formation of colored dispersions of gold nanoparticles from corresponding metal salts, resulting in a easy to use visible indicator of ionizing radiation.
The novel plasmonic nanosensor employs a colorless metal salt solution comprising a mixture of auric chloride (HAuCl4), L-Ascorbic acid (AA) and cetyl (C16), dodecyl (C12), or octyl (C8) trimethylammonium bromide (Cx; x=16/12/8TAB) surfactant molecules (
First, attempts were made to convert trivalent gold to its univalent state, since the reduction of Au(I) to Au(0) is thermodynamically favored over the reduction of Au(III) to Au(0), due to a higher standard reduction potential of the former. Au(I) has an electronic configuration of 4f145d10, and requires a single electron for conversion (reduction) to Au(0). This formation of zerovalent gold or Au(0) is a prerequisite step for nanoparticle formation. In the current plasmonic nanosensor, the electron transfer required for converting Au(I) to Au(0) is facilitated by splitting water into free radicals following exposure to ionizing radiation (X-rays).
Water splitting by ionizing radiation generates three key free radicals, two of which, e− and H., are reducing, and the other (.OH.) oxidizing in nature. Excess ascorbic acid is an antioxidant capable of removing the detrimental (oxidizing) OH. radicals generated in the system. CxTAB surfactants were employed due for their ability to template gold nanoparticles. These three species, namely ascorbic acid, CxTAB, and gold salt, form the key constituents of the current plasmonic nanosensor for ionizing radiation.
First, the concentration of ascorbic acid (AA) was optimized in the presence of the surfactant (C16TAB) and gold salt employed in the plasmonic nanosensor; the maximal dose of 47 Gy was delivered in order to study the effect of ascorbic acid on nanoparticle formation (
Next, the efficacy of three cationic surfactants, C8TAB C12TAB, and C16TAB was investigated, for inducing nanoparticle formation in presence of different doses of ionizing radiation (
Nanoparticle formation was seen as early as 1 h following irradiation in many cases, although 2 h were required for samples irradiated with lower doses (1, 3 and 5 Gy) (
The critical micelle concentration (CMC) of C16TAB is reported to be approximately 1 mM. Using the pyrene fluorescence assay, we determined the CMC of C16TAB in the nanosensor precursor solution (i.e. gold salt and ascorbic acid in water) to be ˜0.7±0.1 mM, which is slightly lower than ˜1.2±0.02 mM in THIS solvent (
Use of C16TAB concentrations at and below the CMC (i.e. 0.7 and 0.2 mM) resulted in spontaneous formation of gold nanoparticles in absence of ionizing radiation; gold nanoparticle formation can be seen by the characteristic absorbance peak of the dispersion in
Visual colorimetric sensors possess advantages of convenience and likely, cost, over those that employ fluorescence changes or electron spin resonance measurements for detecting ionizing radiation. The current plasmonic nanosensor shows increasing color intensity with increasing radiation dose (
Free radicals generated upon radiolysis are thought to be localized in finite volumes called spurs. These spurs can expand, diffuse, and simultaneously, react, leading to the formation of molecular products. These highly reactive free radicals have very short lifetimes of ˜10−7-10−6 s at 25° C. Reaction volumes consisting of nanoscale features can facilitate enhanced reaction kinetics and ensure efficient utilization of these free radicals for the formation of nanoparticles. In case of the current plasmonic nanosensor, this was achieved by the use of amphiphilic molecules that self-assemble into micelles above their respective critical micellar concentrations (CMCs). A strong interaction is possible between the positively charged head group of the lipid surfactant micelles and the negatively charged AuCl4− ions (
Nanoparticles formed in presence and absence of ionizing radiation were characterized for their morphology and hydrodynamic diameter using transmission electron microscopy (TEM;
The growth of gold nuclei from zerovalent gold species proceeds through continuous diffusion of unreacted metal ions and smaller seeds onto the growing nanocrystal surface. This, in turn, is governed by electrostatic interactions between the cationic micelle loaded with gold seeds and unreacted metal ions. In this case, it is likely that the gold nanoparticles aggregate more rapidly in situ due to the strong hydrophobic nature of the long of C16TAB chains, leading to the formation of quasi-spherical nanoparticles and not anisotropic nanostructures.
TEM images indicated a reduction in the size of the metal nanoparticles with increasing radiation dose. Dynamic light scattering (DLS) studies on irradiated samples (
The translational potential of a plasmonic nanosensor for detecting X-ray radiation was investigated under conditions that simulate those employed in human prostate radiotherapy. Endorectal balloons are typically used for holding the prostate in place and for protecting the rectal wall during radiotherapy treatments in humans. The efficacy of the plasmonic nanosensor was evaluated in these balloons ex vivo; no studies on human patients were carried out. 1.5 ml of the precursor solution (C16TAB (20mM)+AA+HAuCl4) was incorporated into endorectal balloons as shown in
Based on the above findings in the endorectal balloon, the detection efficacy of the plasmonic nanosensor in a phantom that is employed to simulate prostate radiotherapy treatments was investigated. In these studies, 200 μL of the precursor solution (C16TAB (2 mM)+AA+HAuCl4) was filled in microcentrifuge tubes, which were then taped to the outside surface of an endorectal balloon such that they were aligned along the stem (
Optical images (
The application discloses an easy to use, versatile and powerful nanoscale platform for dosimetry of therapeutically relevant doses of radiation. This method involves readily available chemicals, is easy to visualize due to the colorimetric nature of detection, and does not need expensive equipment for detection. While a ‘yes/no’ determination may be made by the naked eye, only an absorbance spectrophotometer is required for quantifying the radiation dose. A visible color change also ensures the ease of detecting the radiation dose with the naked eye. It was found that both, C12TAB and C16TAB were able to function as templating molecules in the plasmonic nanosensor at concentrations above their critical micelle concentration (CMC). The sensitivity of the sensor to lower radiation doses is enhanced by modifying the concentration of C16TAB, thus making this a highly versatile platform for a variety of applications. Apart from the surfactants used a list of other potential surfactants which could be employed are listed in the Table 4. The chemicals included in the list along with their derivatives are potential chemicals which could be used along with our sensor in its current form or in any other formulation. The metal ions used is not limited to gold. Any species either metallic or non-metallic can be used along with the sensor in its current form or in any other formulation. To name a few, ions of cobalt, iron, silver could be potential replacement for the proof of concept gold employed .The utility of the plasmonic nanosensor was demonstrated in translational applications; the plasmonic nanosensor was able to detect the delivered radiation dose with satisfactory accuracy when placed in an endorectal balloon ex vivo. In addition, the nanosenor was able to detect doses as low as 0.5 Gy and was able to report on the spatial distribution of radiation dose delivered when investigated using an endorectal balloon placed in a prostate tissue phantom. The translational application of such a dosimeter can help therapists with treatment planning and potentially enhance selectivity and efficacy of treatment. Apart from the medical field, this sensor could be employed where there is a need to detect ionizing radiation directly or indirectly.
The container 805 holds the solution 803. Containers 805 suitable for use in connection with the apparatus 801 are not limited to particular types of containers. In some embodiments, the container 805 includes an endorectal balloon.
In operation, the solution 803 of the apparatus 801 receives a low dose of ionizing radiation 813 to form a radiated solution 815. In some embodiments, the irradiated solution 815 includes a plasmonic nanoparticle 816. A plasmonic nanoparticle is a particle whose electron density can couple with electromagnetic radiation having wavelengths that are larger than the particle due to the nature of the dielectric-metal interface between the medium and the particles.
In some embodiments, the low dose of ionizing radiation 813 is not limited to a particular radiation value. In some embodiments, the low dose of ionizing radiation 813 includes a therapeutic range of values such as between about 0.5 Gy and about 2.0 Gy. In some embodiments, the low dose of ionizing radiation 813 includes a range of values of between about 1.7 Gy and about 2.2 Gy. In some embodiments, the low dose of ionizing radiation 813 includes a value of between about 3.0 Gy and about 10.0 Gy
In some embodiments the solution 803 has a substantially linear response to the low dose of ionizing radiation 813. For a substantially linear response, the intensity of the color of the solution 817 increases substantially linearly as the low dose of ionizing radiation 813 increases.
The apparatus 801 may further include a detector 819 to analyze the radiated solution 815. In some embodiments, the detector 819 comprises a spectrophotometer. A spectrophotometer is an instrument for measuring electromagnetic radiation in different areas of the electromagnetic spectrum. In some embodiments, the detector 819 includes a human visual system. A human visual system is suitable for use in a variety of color measurement tasks and in particular for identifying changes in color. In some embodiments, the radiated solution 815 has a color and the color has a color intensity that increases with an increase in the low dose of ionizing radiation 813. In come embodiments, the surfactant 809 has a concentration and the solution 803 has a color response and modifying the concentration of the surfactant 809 changes the color response of the solution 803 to the low dose of ionizing radiation 813.
The solution 803 shown in
Several methods may be employed to make the solution 803 shown in
The apparatus 801 may be employed in a variety of methods useful in detecting radiation.
The apparatus 801 shown in
Materials: Gold(III) chloride trihydrate (HAuCl4.3H2O), trimethyloctylammonium bromide (C8TAB) (>98%), dodecyltrimethylammonium bromide (C12TAB) (≥98%) and L-Ascorbic acid (AA) were purchased from Sigma-Aldrich. Cetyl trimethylammonium bromide (C16TAB) was purchased from MP chemicals. All chemicals were used as received from the manufacturer without any additional purification.
Sample preparation for irradiation: First, 30 μL of 0.01 M HAuCl4 were mixed with 600 μL of 0.05 M Cx=8,12,16TAB. Upon addition of 30 μL (0.196 mM), 300 μL (1.96 mM), 600 μL (3.92 mM approximated as 4 mM) and 900 μL (5.88 mM) of 0.01 M L-Ascorbic acid, the solution turned colorless after shaking; the concentrations of ascorbic acid were thus varied in order to examine its effect on nanoparticle formation (
Radiation Conditions: A TrueBeam linear accelerator was used to irradiate the samples. Samples were radiated at a dose rate of (15.6 Gy/min). The samples containing surfactant at a concentration of 20 mM and 10 mM were radiated at doses of 0 (Control), 1.1, 3.2, 5.3, 10.5, 15.8, 26.3, 36.9 and 47.4 Gy. These are reported as 0, 1, 3, 5, 10, 16, 26, 37 and 47 Gy respectively in the article. The samples containing surfactant at a concentration 2 mM and 4 mM were irradiated with 0 (Control), 0.5, 1, 1.5, 2, 2.5, 3, 5, 7.5, 10, 12.5 and 15 Gy. After irradiation the samples were transported back to Arizona State University in Tempe, Ariz. (one-way travel time of approximately 30 minutes).
Absorbance Spectroscopy: Absorbance profiles of the radiated and the control samples were measured using a BioTek Synergy 2 plate reader. Absorbance values from 150 μL of sample were measured from 300 to 900 nm with a step size of 10 nm in a 96 well plate. Nanopure water (18.2 MΩcm) was used as a blank in all cases. The absorbance was corrected for offset by subtracting A900 nm and the presence of a peak between 500 and 700 nm was used as an indicator for gold nanoparticle formation.
Determination of Critical Micellar Concentration (CMC): Pyrene (60 μL of 2×10−5M) in acetone was added to 20 ml glass vials. Upon acetone evaporation, 2 ml of C16TAB of varying concentrations was added and stirred for 6 hours at room temperature. To achieve the similar conditions as the irradiation experiments, 30 μL of 10 mM gold salt+600 μL of the above prepared C16TAB+900 μL of 10 mM ascorbic acid were mixed. A fluorescence spectrophotometer with an excitation scan range of 300-360 nm and an emission wavelength of 390 nm was used. Ratio of I337/I334 determined as a function of the surfactant concentration was used to calculate the CMC using pyrene as the probe based on methods described in the literature.
Dynamic Light Scattering (DLS) Measurements: 50 μL of the sample was transferred into a cuvette and placed into a Zetasizer Nano instrument. The software was set up to carry out measurements with autocorrelation. Thereafter, the average diameter along with the polydispersity index (PDI) were recorded based on the software readout.
Transmission Electron Microscopy (TEM): Samples for TEM were prepared by casting a drop of the solution onto a carbon film on a copper mesh grid. The samples were then dried in air. The above process was repeated several times to ensure good coverage. Dried samples were visualized using a CM200-FEG instrument operating at 200 kV.
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This application claims priority to U.S. Provisional Application No. 62/275,168 that was filed on Jan. 5, 2016. The entire content of the applications referenced above are hereby incorporated by reference herein.
This invention was made with government support under 1403860 awarded by the National Science Foundation. The government has certain rights in the invention.
Number | Date | Country | |
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62275168 | Jan 2016 | US |
Number | Date | Country | |
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Parent | 15398590 | Jan 2017 | US |
Child | 17357138 | US |