Absorbed dose distribution of the auger emitters 67GA and 125I and the beta-emitters 67CU, 90Y, 131I, and 186RE as a function of tumor size, uptake, and intracellular distribution

Perspectives on metals-based radioimmunotherapy (RIT): moving forward

Radioimmunotherapy (RIT) is FDA-approved for the clinical management of liquid malignancies, however, its use for solid malignancies remains a challenge. The putative benefit of RIT lies in selective targeting of antigens expressed on the tumor surface using monoclonal antibodies, to systemically deliver cytotoxic radionuclides. The past several decades yielded dramatic improvements in the quality, quantity, recent commercial availability of alpha-, beta- and Auger Electron-emitting therapeutic radiometals. Investigators have created new or improved existing bifunctional chelators. These bifunctional chelators bind radiometals and can be coupled to antigen-specific antibodies. In this review, we discuss approaches to develop radiometal-based RITs, including the selection of radiometals, chelators and antibody platforms (i.e. full-length, F(ab')2, Fab, minibodies, diabodies, scFv-Fc and nanobodies). We cite examples of the performance of RIT in the clinic, describe challenges to its implementation, and offer insights to address gaps toward translation.

Dosimetry study of [I-131] and [I-125]- meta-iodobenz guanidine in a simulating model for neuroblastoma metastasis

The physical properties of I-131 may be suboptimal for the delivery of therapeutic radiation to bone marrow metastases, which are common in the natural history of neuroblastoma. In vitro and preliminary clinical studies have implied improved efficacy of I-125 relative to I-131 in certain clinical situations, although areas of uncertainty remain regarding intratumoral dosimetry. This prompted our study using human neuroblastoma multicellular spheroids as a model of metastasis. 3D dose calculations were made using voxel-based Medical Internal Radiation Dosimetry (MIRD) and dose-point-kernel (DPK) techniques. Dose distributions for I-131 and I-125 labeled mIBG were calculated for spheroids (metastases) of various sizes from 0.01 cm to 3 cm diameter, and the relative dose delivered to the tumors was compared for the same limiting dose to the bone marrow. Based on the same data, arguments were advanced based upon the principles of tumor control probability (TCP) to emphasize the potential theoretical utility of I-125 over I-131 in specific clinical situations. I-125-mIBG can deliver a higher and more uniform dose to tumors compared to I-131 mIBG without increasing the dose to the bone marrow. Depending on the tumor size and biological half-life, the relative dose to tumors of less than 1 mm diameter can increase several-fold. TCP calculations indicate that tumor control increases with increasing administered activity, and that I-125 is more effective than I-131 for tumor diameters of 0.01 cm or less. This study suggests that I-125-mIBG is dosimetrically superior to I-131-mIBG therapy for small bone marrow metastases from neuroblastoma. It is logical to consider adding I-125-mIBG to I-131-mIBG in multi-modality therapy as these two isotopes could be complementary in terms of their cumulative dosimetry.

Pulsed high intensity focused ultrasound increases penetration and therapeutic efficacy of monoclonal antibodies in murine xenograft tumors

The success of radioimmunotherapy for solid tumors remains elusive due to poor biodistribution and insufficient tumor accumulation, in part, due to the unique tumor microenvironment resulting in heterogeneous tumor antibody distribution. Pulsed high intensity focused ultrasound (pulsed-HIFU) has previously been shown to increase the accumulation of (111)In labeled B3 antibody (recognizes Lewis(y) antigen). The objective of this study was to investigate the tumor penetration and therapeutic efficacy of pulsed-HIFU exposures combined with (90)Y labeled B3 mAb in an A431 solid tumor model. The ability of pulsed-HIFU (1 M Hz, spatial averaged temporal peak intensity=2685 W cm(-2); pulse repetition frequency=1 Hz; duty cycle=5%) to improve the tumor penetration and therapeutic efficacy of (90)Y labeled B3 mAb ((90)Y-B3) was evaluated in Le(y)-positive A431 tumors. Antibody penetration from the tumor surface and blood vessel surface was evaluated with fluorescently labeled B3, epi-fluorescent microscopy, and custom image analysis. Tumor size was monitored to determine treatment efficacy, indicated by survival, following various treatments with pulsed-HIFU and/or (90)Y-B3. The pulsed-HIFU exposures did not affect the vascular parameters including microvascular density, vascular size, and vascular architecture; although 1.6-fold more antibody was delivered to the solid tumors when combined with pulsed-HIFU. The distribution and penetration of the antibodies were significantly improved (p-value<0.05) when combined with pulsed-HIFU, only in the tumor periphery. Pretreatment with pulsed-HIFU significantly improved (p-value<0.05) survival over control treatments.

Targeted radionuclide therapy: theoretical study of the relationship between tumour control probability and tumour radius for a 32P/33P radionuclide cocktail

As revealed by previous theoretical studies, targeted radionuclide therapy (TRT) that relies on a single beta-emitting radioisotope is likely to be inappropriate for clinical scenarios such as disseminated malignancy. For a patient with a vast number of tumours and metastases of largely differing sizes a high level of therapeutical efficiency might be achieved only for a restricted range of tumour sizes. This is due to the limited range of beta-electrons in human tissue, essentially causing the therapeutical impact to vary tremendously with tumour size. The dependence of curability on the tumour dimension is expected to be significantly altered if a radionuclide cocktail, consisting of a long-range and a short-range beta-emitter, such as (32)P and (33)P, is involved in the treatment. In this study, a radiation transport simulation was performed, using the MCNP4c2 Monte Carlo code, in order to investigate the relationship between tumour control probability (TCP) and tumour size, associated with concurrent use of (32)P and (33)P. Two different models of intratumoural distribution of cumulated activity were taken into account. One simulated an ideal radionuclide uptake in tumour tissue and the other referred to a limited radiotracer penetration. The results were examined in comparison to tumours targeted with pure (32)P, (33)P and (131)I. For both uptake scenarios a considerable reduction of the overall variation of TCP and thus an increasing chance of achieving tumour cure was observed for tumour sizes ranging from microscopic dimensions up to macroscopic diameters, if the targeted radionuclide treatment relies on a (32)P/(33)P cocktail. It was revealed that particular attention has to be given to the ratio of the (32)P and (33)P specific cumulated activities (SCA) in the tumour, since this is a significant determinant of the resulting behaviour of tumour control probability as the tumour diameter varies. This study suggests that a 32P/33P approach is more applicable to diseases that involve a variety of tumours and metastases differing in size.

Theoretical study of the influence of a heterogeneous activity distribution on intratumoral absorbed dose distribution

Radioimmunotherapy of hematopoeitic cancers and micrometastases has been shown to have significant therapeutic benefit. The treatment of solid tumors with radionuclide therapy has been less successful. Previous investigations of intratumoral activity distribution and studies on intratumoral drug delivery suggest that a probable reason for the disappointing results in solid tumor treatment is nonuniform intratumoral distribution coupled with restricted intratumoral drug penetrance, thus inhibiting antineoplastic agents from reaching the tumor's center. This paper describes a nonuniform intratumoral activity distribution identified by limited radiolabeled tracer diffusion from tumor surface to tumor center. This activity was simulated using techniques that allowed the absorbed dose distributions to be estimated using different intratumoral diffusion capabilities and calculated for tumors of varying diameters. The influences of these absorbed dose distributions on solid tumor radionuclide therapy are also discussed. The absorbed dose distribution was calculated using the dose point kernel method that provided for the application of a three-dimensional (3D) convolution between a dose rate kernel function and an activity distribution function. These functions were incorporated into 3D matrices with voxels measuring 0.10 x 0.10 x 0.10 mm3. At this point fast Fourier transform (FFT) and multiplication in frequency domain followed by inverse FFT (iFFT) were used to effect this phase of the dose calculation process. The absorbed dose distribution for tumors of 1, 3, 5, 10, and 15 mm in diameter were studied. Using the therapeutic radionuclides of 131I, 186Re, 188Re, and 90Y, the total average dose, center dose, and surface dose for each of the different tumor diameters were reported. The absorbed dose in the nearby normal tissue was also evaluated. When the tumor diameters exceed 15 mm, a much lower tumor center dose is delivered compared with tumors between 3 and 5 mm in diameter. Based on these findings, the use of higher beta-energy radionuclides, such as 188Re and 90Y is more effective in delivering a higher absorbed dose to the tumor center at tumor diameters around 10 mm.

Absorbed dose estimates at the cellular level for 131I

Microdosimetric calculations of 131I have been evaluated for a single cell and for cell clusters. A VsBasic program has been used to calculate stopping power, linear energy transfer, range values and deposited energies per decay for beta particles, Auger and conversion electrons of 131I. The chemical composition of the cell has been taken into account in this model; results were compared with water medium. Besides, total absorbed doses have been calculated for the radionuclides distributed randomly within the cell and clusters. Cross-fire irradiation has been considered for clusters of cells. In this case, absorbed doses per cell within a cluster were found to be significantly higher than absorbed doses per single cell, depending on the cluster size. Results showed that 131I is a promising radionuclide for therapy of tumors from millimeter to centimeter dimensions.

Synchrotron radiation-based experimental determination of the optimal energy for cell radiotoxicity enhancement following photoelectric effect on stable iodinated compounds

This study was designed to experimentally evaluate the optimal X-ray energy for increasing the radiation energy absorbed in tumours loaded with iodinated compounds, using the photoelectric effect. SQ20B human cells were irradiated with synchrotron monochromatic beam tuned at 32.8, 33.5, 50 and 70 keV. Two cell treatments were compared to the control: cells suspended in 10 mg ml⁻¹ of iodine radiological contrast agent or cells pre-exposed with 10 μM of iodo-desoxyuridine (IUdR) for 48 h. Our radiobiological end point was clonogenic cell survival. Cells irradiated with both iodine compounds exhibited a radiation sensitisation enhancement. Moreover, it was energy dependent, with a maximum at 50 keV. At this energy, the sensitisation calculated at 10% survival was equal to 2.03 for cells suspended in iodinated contrast agent and 2.60 for IUdR. Cells pretreated with IUdR had higher sensitisation factors over the energy range than for those suspended in iodine contrast agent. Also, their survival curves presented no shoulder, suggesting complex lethal damages from Auger electrons. Our results confirm the existence of the 50 keV energy optimum for a binary therapeutic irradiation based on the presence of stable iodine in tumours and an external irradiation. Monochromatic synchrotron radiotherapy concept is hence proposed for increasing the differential effect between healthy and cancerous tissue irradiation.

Radiotoxic effect and dosimetry of 67GA in multicellular spheroids as compared to single cells of the lymphoma cell line U715

PURPOSE

The purpose of the present study was to investigate if there were differences between U715 spheroids and single cells in the radiotoxic effect of 67Ga on cell growth and clonogenic capacity in vitro and to generate dosimetric approaches for the multicellular tumor model.

METHODS AND MATERIALS

Human lymphoma U715 cells were cultured in vitro as single cells and multicellular spheroids, grown with the use of a combination of fibrin clot technique, spinner flasks, and liquid-overlay culture. Cells were incubated with 2.96-8.88 MBq/ml 67Gallium for 4 days. Spheroids were dispersed to single cells by treatment with plasmin. Residual proliferative and clonogenic capacity after 67Ga incubation were assayed using the MTT-test and clonogenic test, respectively. Autoradiography was performed with 1 microm sections and Ilford L4 liquid photographic emulsion. Dosimetric approaches were made, based on the MIRD-approach.

RESULTS

During 67Ga incubation proliferation was inhibited. The residual proliferative or clonogenic capacity was inhibited by 8.88 MBq/ml for 39 and 88%, respectively. For single cells with 6.66 MBq/ml these inhibitions were 64 and 96%, respectively. Autoradiography showed an homogeneous distribution of 67Ga in spheroids and single cells. In single cells a 2.1-3.5 times higher 67Ga uptake/cell than in spheroids produced an equitoxic effect. The uptake parameters were implemented in new dosimetric approaches and showed that the efficacy of intracellular 67Ga was two times higher in spheroid clusters than in single cells due to energy deposition of internal conversion electrons within the cell clusters with a mean diameter size of nine cells. Both for proliferative and clonogenic capacity the exponential survival curves were superimposed.

CONCLUSIONS

With the new approaches made in our dosimetric model the discrepancy found between 67Ga accumulation and radiotoxic effect in spheroids as compared to single cells can be explained by additional effects of the crossfire of internal conversion electrons within clusters of about nine cells in diameter in spheroids. Only twice as much 67Ga was needed to reach equitoxic absorbed doses in spheroids than was needed in single cells. Such might be important for the use of 67Ga treatment of small metastasis of malignant lymphoma.