Photoreactivation of damage induced by ionizing radiation in yeast cells

Summary Experimental data on photoreactivation of damage induced by ionizing radiation in yeast cells are presented. The value of photoreactivation was found to be the highest for the following conditions predicted by us as optimum ones: large volume of irradiated suspension, hypoxia and high energy sparsely ionizing radiation. A comparison of data for yeast and bacterial cells shows that Cerenkov emission from ionizing radiation may produce photoreactivated pyrimidine dimers in both prokaryotic and eukaryotic cell systems.     

Induction of lethal damage in E. coli by Cerenkov emission associated with high-energy X-rays: the effect of bromouracil substitution

5.1. The damages induced in E. coli AB2487 recA by Cerenkov emission and ionizing radiation contribute in an additive fashion to the overall lethality, and do not interact in a synergistic fashion. 5.2. BU substitution enhances the lethal action of high energy X-irradiation on E. coli AB2487 recA by a mechanism involving enhanced radiosensitivity and enhanced photosensitivity.     

Cerenkov radiation energy transfer (CRET) imaging: a novel method for optical imaging of PET isotopes in biological systems

Background

Positron emission tomography (PET) allows sensitive, non-invasive analysis of the distribution of radiopharmaceutical tracers labeled with positron (β⁺)-emitting radionuclides in small animals and humans. Upon β⁺ decay, the initial velocity of high-energy β⁺ particles can momentarily exceed the speed of light in tissue, producing Cerenkov radiation that is detectable by optical imaging, but is highly absorbed in living organisms.

Principal Findings

To improve optical imaging of Cerenkov radiation in biological systems, we demonstrate that Cerenkov radiation from decay of the PET isotopes ⁶⁴Cu and ¹⁸F can be spectrally coupled by energy transfer to high Stokes-shift quantum nanoparticles (Qtracker705) to produce highly red-shifted photonic emissions. Efficient energy transfer was not detected with ^99mTc, a predominantly γ-emitting isotope. Similar to bioluminescence resonance energy transfer (BRET) and fluorescence resonance energy transfer (FRET), herein we define the Cerenkov radiation energy transfer (CRET) ratio as the normalized quotient of light detected within a spectral window centered on the fluorophore emission divided by light detected within a spectral window of the Cerenkov radiation emission to quantify imaging signals. Optical images of solutions containing Qtracker705 nanoparticles and [¹⁸F]FDG showed CRET ratios in vitro as high as 8.8±1.1, while images of mice with subcutaneous pseudotumors impregnated with Qtracker705 following intravenous injection of [¹⁸F]FDG showed CRET ratios in vivo as high as 3.5±0.3.

Conclusions

Quantitative CRET imaging may afford a variety of novel optical imaging applications and activation strategies for PET radiopharmaceuticals and other isotopes in biomaterials, tissues and live animals.     

Mutation induction in Escherichia coli WP2 uvrA by Cerenkov emission associated with 137Cs gamma irradiation

Evidence is presented for the mutation of the tryptophan-requiring bacterial strain Escherichia coli WP2 uvrA from auxotrophy to prototrophy, and from streptomycin sensitivity to resistance, by Cerenkov emission associated with 137Cs gamma irradiation. Furthermore, the data strongly suggest a more than additive interaction between the gamma-induced damage and that induced by Cerenkov emission for both mutations scored. An additional observation is that mutant yields (expressed as mutants/10(7) survivors) show a dependence on the number of viable cells plated for both uv (254 nm) and Cerenkov-induced mutations, but not for those induced by gamma irradiation. This demonstrates another similarity between uv- and Cerenkov-induced damage.     

Pyrimidine dimer induction in E. coli DNA by Cerenkov emission associated with high energy X-irradiation

The induction of pyrimidine dimers in E. coli DNA by secondary ultraviolet light associated with 6 MVp X-rays in the dose range 20-90 Gy has been demonstrated using T4 endonuclease V. Under the experimental conditions used in these experiments the major component of this secondary U.V. light is Cerenkov emission.     

Mechanism of the light flashes induced in human beings by ionizing particles

Exposure of a dark adapted human eye to weak proton beams of different energy for which the yield of Cerenkov radiation varies by approximately 50 times, the other characteristics being virtually the same, showed that this radiation was mainly responsible for visual sensation.     

Novel biomedical applications of Cerenkov radiation and radioluminescence imaging

The main goals of this review is to provide an up-to-date account of the different uses of Cerenkov radiation (CR) and radioluminescence imaging for pre-clinical small animal imaging. We will focus on new emerging applications such as the use of Cerenkov imaging for monitoring radionuclide and external radiotherapy in humans. Another novel application that will be described is the monitoring of radiochemical synthesis using microfluidic chips.Several pre-clinical aspects of CR will be discussed such as the development of 3D reconstruction methods for Cerenkov images and the use of CR as excitation source for nanoparticles or for endoscopic imaging.We will also include a discussion on radioluminescence imaging that is a more general method than Cerenkov imaging for the detection using optical methods of alpha and gamma emitters.     

Laser surgery: using the carbon dioxide laser.

In 1917 Einstein theorized tha through an atomic process a unique kind of electromagnetic radiation could be produced by stimulated emission. When such radiation is in the optical or infrared spectrum it is termed laser (light amplification by stimulated emission of radiation) light. A laser, a high-intensity light source, emits a nearly parallel electromagnetic beam of energy at a given wavelength that can be captured by a lens and concentrated in the focal spot. The wavelength determines how the laser will be used. The carbon dioxide laser is now successfully employed for some surgical procedures in gynecology, otorhinolaryngology, neurosurgery, and plastic and general surgery. The CO2 laser beam is directed through the viewing system of an operating microscope or through a hand-held laser component. Its basic action in tissue is thermal vaporization; it causes minimal damage to adjacent tissues. Surgeons require special training in the basic methods and techniques of laser surgery, as well as in the safety standards that must be observed.     

The use of Cerenkov radiation for monitoring reactions performed in minute volumes: examples from recombinant DNA technology

A method in which minute volumes of initially unknown size are used to monitor reactions has been developed. It is applicable whenever 32P-labeled substrates can be distinguished from 32P-labeled products by a filter assay. Three determinations are required: the Cerenkov radiation emitted (1) by the unknown aliquots affixed to filters and dried; (2) by the identical filters after processing to remove either substrates or products; and (3) by a precisely measured, necessarily much larger, aliquot in solution. Given the value obtained in (3) and the efficiency with which Cerenkov radiation can be detected in the dry state (25%) compared with the liquid state (56%), the unknown volumes, together with their acid-insoluble radioactivity, can be calculated from (1) and (2), respectively. Since the known volume counted in solution is not lost to further manipulations, the entire procedure uses less than 0.5 microliter.     

Theoretical analysis of the effect of the photoreactivation of E. coli cells irradiated with gamma quanta

The assumption that the formation of pyrimidine dimers in E. coli cells, placed in a transient aqueous medium exposed to gamma-quanta, is conditioned by Cerenkov radiation laid the basis for the development of a biophysical model to explain the photoreactivation effect observed. The dependence of the effect upon gamma-radiation energy and the volume of the exposed suspension is predicted and compared with experimental data.     

Simultaneous demonstration of UV-type and ionizing radiation-type DNA repair by the nucleoid sedimentation technique

The nucleoid sedimentation technique is one of the most sensitive methods for measuring DNA excision repair. With this technique, we have shown that both UV- and ionizing radiation-type repair (the latter induced by bleomycin) can be discriminated in HeLa and normal diploid cells using 1-beta-D-arabinofuranosylcytosine. The latter compound inhibits UV-type repair synthesis, and thus causes DNA breaks due to enzymic incision to persist, but has no effect on rejoining DNA after ionizing radiation-type damage. It was then possible to prove that 4-nitroquinoline-1-oxide induces both types of lesions which are repaired simultaneously. This effect could be demonstrated in HeLa and normal human diploid cells in a single experimental set-up.     

Nanoscale spatial induction of ultraviolet photoproducts in cellular DNA by three-photon near-infrared absorption

The high-resolution spatial induction of ultraviolet (UV) photoproducts in mammalian cellular DNA is a goal of many scientists who study UV damage and repair. Here we describe how UV photoproducts can be induced in cellular DNA within nanometre dimensions by near-diffraction-limited 750 nm infrared laser radiation. The use of multiphoton excitation to induce highly localized DNA damage in an individual cell nucleus or mitochondrion will provide much greater resolution for studies of DNA repair dynamics and intracellular localization as well as intracellular signalling processes and cell–cell communication. The technique offers an advantage over the masking method for localized irradiation of cells, as the laser radiation can specifically target a single cell and subnuclear structures such as nucleoli, nuclear membranes or any structure that can be labelled and visualized by a fluorescent tag. It also increases the time resolution with which migration of DNA repair proteins to damage sites can be monitored. We define the characteristics of localized DNA damage induction by near-infrared radiation and suggest how it may be used for new biological investigations.     

Molecular mechanisms of ultraviolet radiation-induced immunosuppression

Solar ultraviolet radiation (UVR) is well known for its immunosuppressive properties. UVR can suppress immune reactions both in a local and a systemic fashion. One of the major molecular mediators of photoimmunosuppression is UVR-induced DNA damage. In contrast to immunosuppressive drugs, UVR does not act in a general but antigen-specific fashion. This is due to the induction of regulatory T cells. Epidermal Langerhans cells harboring UVR-induced DNA damage appear to be essentially involved in the induction of these cells. Cytokines including interleukin (IL)-12, -18 and -23 exert the capacity to reduce UVR-induced DNA damage via induction of DNA repair. Accordingly, these cytokines prevent UVR-mediated immunosuppression. In contrast to IL-18, IL-12 and IL-23 can also inhibit the suppressive activity of regulatory T cells by a mechanism which still needs to be determined. Clarification of the molecular mechanisms underlying UVR-induced immunosuppression will help to develop new immunosuppressive therapeutic strategies by utilizing UVR-induced regulatory T cells for the treatment of immune-mediated diseases. In addition, these insights will contribute to a better understanding of photocarcinogenesis since suppression of the immune system by UVR essentially contributes to the induction of skin cancer.     

Mutation and inactivation of cultured mammalian cells exposed to beams of accelerated heavy ions. II. Chinese hamster V79 cells.

Inactivation and mutation to thioguanine-resistance of V79 hamster cells were studied after irradiation with accelerated helium, boron or nitrogen ions covering a range of linear energy transfer from 28 to 470 keV micrometers-1. For all radiation qualities a dose-dependent increase in mutant frequency was found for doses giving surviving fractions greater than about 0.20. The effectiveness per unit dose for both inactivation and mutation induction increased with the linear energy transfer of the radiation to a maximum in the range 90-200 keV micrometer-1. However, the maximum mutagenic effectiveness relative to gamma-rays was about two or more times that for inactivation. It is suggested that a proportion of the radiation-induced mutants suffer extensive genetic damage, and that some forms of this damage may be induced with high efficiency by radiations of high linear energy transfer.     

Temporal separation of Cerenkov radiation and scintillation using artificial neural networks in Clinical LINACs

The irradiation of scintillator-fiber optic dosimeters by clinical LINACs results in the measurement of scintillation and Cerenkov radiation. In scintillator-fiber optic dosimetry, the scintillation and Cerenkov radiation responses are separated to determine the dose deposited in the scintillator volume. Artificial neural networks (ANNs) were trained and applied in a novel single probe method for the temporal separation of scintillation and Cerenkov radiation. Six dose profiles were measured using the ANN, with the dose profiles compared to those measured using background subtraction and an ionisation chamber. The average dose discrepancy of the ANN measured dose was 2.2% with respect to the ionisation chamber dose and 1.2% with respect to the background subtraction measured dose, while the average dose discrepancy of the background subtraction dose was 1.6% with respect to the ionisation chamber dose. The ANNs performance was degraded when compared with background subtraction, arising from an inaccurate model used to synthesise ANN training data.     

Delayed activation of DNA damage checkpoint and radiation-induced genomic instability

Ionizing radiation induces genomic instability, transmitted over many generations through the progeny of surviving cells. It is manifested as the expression of delayed effects such as delayed cell death, delayed chromosomal instability and delayed mutagenesis. Induced genomic instability exerts its delayed effects for prolonged periods of time, suggesting the presence of a mechanism by which the initial DNA damage in the surviving cells is memorized. Our recent studies have shown that transmitted memory causes delayed DNA breakage, which in turn activates DNA damage checkpoint, and is involved in delayed manifestation of genomic instability. Although the mechanism(s) involved in DNA damage memory remain to be determined, we suggest that ionizing radiation-induced mega-base deletion destabilizes chromatin structure, which can be transmitted many generations through the progeny, and is involved in initiation and perpetuation of genomic instability. The possible involvement of delayed activation of a DNA damage checkpoint in the delayed induction of genomic instability in bystander cells is also discussed.     

Intraoperative imaging of positron emission tomographic radiotracers using Cerenkov luminescence emissions

Imaging the location and extent of cancer provides invaluable information before, during, and after surgery. The majority of "image-guided" methods that use, for example, positron emission tomography (PET) involve preoperative imaging and do not provide real-time information during surgery. It is now well established that the inherent optical emissions (Cerenkov radiation) from various β-emitting radionuclides can be visualized by Cerenkov luminescence imaging (CLI). Here we report the full characterization of CLI using the positron-emitting radiotracer 89Zr-DFO-trastuzumab for target-specific, quantitative imaging of HER2/neu-positive tumors in vivo. We also provide the first demonstration of the feasibility of using CLI for true image-guided, intraoperative surgical resection of tumors. Analysis of optical CLIs provided accurate, quantitative information on radiotracer biodistribution and tissue uptake that correlated well with the concordant PET images. CLI, PET, and biodistribution studies revealed target-specific uptake of 89Zr-DFO-trastuzumab in BT-474 (HER2/neu positive) versus MDA-MB-468 (HER2/neu negative) xenografts in the same mice. Competitive inhibition (blocking) studies followed by CLI also confirmed the in vivo immunoreactivity and specificity of 89Zr-DFO-trastuzumab for HER2/neu. Overall, these results strongly support the continued development of CLI as a preclinical and possible clinical tool for use in molecular imaging and surgical procedures for accurately defining tumor margins.     

DNA lesions that signal the induction of radioresistance and DNA repair in yeast

DNA recombinational repair, and an increase in its capacity induced by DNA damage, is believed to be the major mechanism that confers resistance to killing by ionizing radiation in yeast. We have examined the nature of the DNA lesions generated by ionizing radiation that induce this mechanism, using two different end points: resistance to cell killing and ability of the error-free recombinational repair system to compete for other DNA lesions and thereby suppress chemical mutation. Under the various conditions examined in this study, the "maximum" inducible radiation resistance was increased approximately 1.5- to 3-fold and suppression of mutation about 10-fold. DNA lesions produced by low-LET gamma rays at doses greater than about 20 Gy given in oxygen were shown to be more efficient, per unit dose, at inducing radioresistance to killing than were lesions produced by neutrons (high-LET radiation). This suggests that DNA single-strand breaks are more important lesions in the induction of radioresistance than DNA double-strand breaks. Oxygen-modified lesions produced by gamma rays (low-LET radiation) were particularly efficient as induction signals. DNA damage due to hydroxyl radicals (OH.) derived from the radiolytic decomposition of H2O produced lesions that strongly induced this DNA repair mechanism. Similarly, OH. derived from aqueous electrons (e-aq) in the presence of N2O also efficiently induced the response. Cells induced to radioresistance to killing with high-LET radiation did not suppress N-methyl-N'-nitro-N-nitrosoguanidine (MNNG)-generated mutations as well as cells induced with low-LET radiation, supporting the conclusion that the type of DNA damage produced by low-LET radiation is a better inducer of recombinational repair. Surprisingly, however, cells induced with gamma radiation in the presence of N2O that became radioresistant to killing were unable to suppress MNNG mutations. This result indicates that OH. generated via e-aq (in N2O) may produce unusual DNA lesions which retard normal repair and render the system unavailable to compete for MNNG-generated lesions. We suggest that the repairability of these unique lesions is restricted by either their chemical nature or topological accessibility. Attempted repair of these lesions has lethal consequences and accounts for N2O radiosensitization of repair-competent but not incompetent cells. We conclude that induction of radioresistance in yeast by ionizing radiation responds variably to different DNA lesions, and these affect the availability of the induced recombinational repair system to deal with subsequent damage.     

Counting of p32 in plant tissues using the Cerenkov effect

Summary A procedure for counting p³² in plant tissues is presented. The method, based on the use of Cerenkov radiation, involves practically no sample preparation. Plant tissue are placed into vials containing water or hexane and counted with a liquid scintillation counter. Counts obtained, using this procedure were found to be linearily related to that obtained with a G.M. tube. The counting efficiency was, however, higher with the proposed method. The use of hexane is advantageous if leakage of p³² from the tissue is possible, or when higher counting efficiency is desireable. The use of different liquids may also enable a discriminative count of different beta emitters. As suggested recently⁸ use of wavelength shifter may further increase efficiency of counting Cerenkov radiation.