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Dive into the research topics where A.J. Kreiner is active.

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Featured researches published by A.J. Kreiner.


International Journal of Radiation Oncology Biology Physics | 2009

Induction and rejoining of DNA double strand breaks assessed by H2AX phosphorylation in melanoma cells irradiated with proton and lithium beams.

Irene L. Ibañez; Candelaria Bracalente; Beatriz L. Molinari; Mónica A. Palmieri; Lucia Policastro; A.J. Kreiner; Alejandro Burlón; A.A. Valda; Daniela Navalesi; Jorge Davidson; Miguel Davidson; Mónica Vázquez; Mabel Ozafrán; Hebe Durán

PURPOSE The aim of this study was to evaluate the induction and rejoining of DNA double strand breaks (DSBs) in melanoma cells exposed to low and high linear energy transfer (LET) radiation. METHODS AND MATERIALS DSBs and survival were determined as a function of dose in melanoma cells (B16-F0) irradiated with monoenergetic proton and lithium beams and with a gamma source. Survival curves were obtained by clonogenic assay and fitted to the linear-quadratic model. DSBs were evaluated by the detection of phosphorylated histone H2AX (gammaH2AX) foci at 30 min and 6 h post-irradiation. RESULTS Survival curves showed the increasing effectiveness of radiation as a function of LET. gammaH2AX labeling showed an increase in the number of foci vs. dose for all the radiations evaluated. A decrease in the number of foci was found at 6 h post-irradiation for low LET radiation, revealing the repair capacity of DSBs. An increase in the size of gammaH2AX foci in cells irradiated with lithium beams was found, as compared with gamma and proton irradiations, which could be attributed to the clusters of DSBs induced by high LET radiation. Foci size increased at 6 h post-irradiation for lithium and proton irradiations in relation with persistent DSBs, showing a correlation with surviving fraction. CONCLUSIONS Our results showed the response of B16-F0 cells to charged particle beams evaluated by the detection of gammaH2AX foci. We conclude that gammaH2AX foci size is an accurate parameter to correlate the rejoining of DSBs induced by different LET radiations and radiosensitivity.


Applied Radiation and Isotopes | 2014

Accelerator-Based BNCT

A.J. Kreiner

The activity in accelerator development for accelerator-based BNCT (AB-BNCT) both worldwide and in Argentina is described. Projects in Russia, UK, Italy, Japan, Israel, and Argentina to develop AB-BNCT around different types of accelerators are briefly presented. In particular, the present status and recent progress of the Argentine project will be reviewed. The topics will cover: intense ion sources, accelerator tubes, transport of intense beams, beam diagnostics, the (9)Be(d,n) reaction as a possible neutron source, Beam Shaping Assemblies (BSA), a treatment room, and treatment planning in realistic cases.


Applied Radiation and Isotopes | 2011

Development of a Tandem-Electrostatic-Quadrupole facility for Accelerator-Based Boron Neutron Capture Therapy.

A.J. Kreiner; W. Castell; H. Di Paolo; M. Baldo; J. Bergueiro; A.A. Burlon; D. Cartelli; V. Thatar Vento; J.M. Kesque; J. Erhardt; J.C. Ilardo; A.A. Valda; Mario E. Debray; H.R. Somacal; J.C. Suarez Sandin; M. Igarzabal; H. Huck; L. Estrada; M. Repetto; M. Obligado; J. Padulo; D.M. Minsky; María S. Herrera; S.J. González; M.E. Capoulat

We describe the present status of an ongoing project to develop a Tandem-ElectroStatic-Quadrupole (TESQ) accelerator facility for Accelerator-Based (AB)-BNCT. The project final goal is a machine capable of delivering 30 mA of 2.4 MeV protons to be used in conjunction with a neutron production target based on the (7)Li(p,n)(7)Be reaction. The machine currently being constructed is a folded TESQ with a high-voltage terminal at 0.6 MV. We report here on the progress achieved in a number of different areas.


Applied Radiation and Isotopes | 2011

AB-BNCT beam shaping assembly based on 7Li(p,n)7Be reaction optimization

D.M. Minsky; A.J. Kreiner; A.A. Valda

A numerical optimization of a Beam Shaping Assembly (BSA) for Accelerator Based-Boron Neutron Capture Therapy (AB-BNCT) has been performed. The reaction (7)Li(p,n)(7)Be has been considered using a proton beam on a lithium fluoride target. Proton energy and the dimensions of a simple BSA geometry have been varied to obtain a set of different configurations. The optimal configuration of this set is shown.


Applied Radiation and Isotopes | 2009

Experimental feasibility studies on a SPECT tomograph for BNCT dosimetry.

D.M. Minsky; A.A. Valda; A.J. Kreiner; Stuart Green; C. Wojnecki; Z. Ghani

This article reports on the development of a prototype of a SPECT tomograph system for online dosimetry in BNCT based on LaBr(3)(Ce) scintillation detectors. The setup shielding was optimized to be used in the accelerator based BNCT facility of the University of Birmingham. The system was designed and built. An image of a (241)Am point source was reconstructed. A projection of a phantom with two tumors with 400 microg/g of (10)B was measured at the BNCT facility.


Ecotoxicology and Environmental Safety | 2004

Effects of long-term exposure to Cu2+ and Cd2+ on the pentose phosphate pathway dehydrogenase activities in the ovary of adult Bufo arenarum: possible role as biomarker for Cu2+ toxicity

Marcelo D Carattino; Susana Peralta; Cristina S. Pérez-Coll; Fabián Naab; Alejandro Burlón; A.J. Kreiner; Ana Preller; Teresa M. Fonovich de Schroeder

The effects of copper and cadmium on metabolism through the pentose phosphate pathway were evaluated in Bufo arenarum toad ovary. The effects of the two metals on dehydrogenases from this pathway were evaluated by three experiments: (1) in samples obtained from control females with addition of the metals to the reaction mixture (in vitro), (2) in samples obtained from control females and after long-term exposure of females to 4 and 100 microg/L of Cu or Cd in the incubation media (in vitro after exposure to the metals in vivo), and (3) 14CO2 production through the pentose phosphate pathway was evaluated after [U-14C]glucose microinjection on ovulated oocytes (in vivo after microinjection of the metals). Results from (1) evidenced inhibition of both enzyme activities but only above 1.5 mM Cu and Cd added to the reaction mixture. In (2) both glucose 6-phosphate dehydrogenase and 6-phosphogluconate dehydrogenase activities decreased in samples from the ovaries of females exposed in vivo to Cu, in a concentration-dependent manner (up to 90% in females exposed to 100 microg/L Cu: 2.12 +/- 1.57 NADPH micromol/min microg protein x 10(-5) vs 19.97 +/- 8.54 in control females). Cd treatment of the toads only rendered an inhibitory effect on 6-phosphogluconate dehydrogenase activity after exposure to 4 microg/L of the bivalent cation. (3) In vivo 14CO2 evolution significantly decreased in oocytes coinjected with 6.3 x 10(-3) mM Cu (calculated intracellular final concentration of the metal injected) and radioactive glucose. Cu and Cd concentration in samples from exposed females were always under detection limit by particle-induced X-ray emission. The results presented here are in agreement with a role for both glucose 6-phosphate dehydrogenase and 6-phosphogluconate dehydrogenase activities determination as biomarkers of effect and exposure for Cu but not for Cd toxicity.


Applied Radiation and Isotopes | 2011

Applicability of the 9Be(d,n)10B reaction to AB-BNCT skin and deep tumor treatment

M.E. Capoulat; D.M. Minsky; A.J. Kreiner

In the range of low bombarding energies (less than about 1.5 MeV) the (9)Be(d,n)(10)B reaction produces neutron spectra that can be moderated depending on the choice of the target thickness and the deuteron bombarding energy. In this work, a Monte Carlo simulation study to determine the capability of this reaction to deliver enough dose to efficiently control both skin and deep seated tumors has been performed by means of MCNP calculations using eight optimized (9)Be targets.


Medical Physics | 2001

In-phantom dosimetry for the 13C(d,n)14N reaction as a source for accelerator-based BNCT

Alejandro Burlón; A.J. Kreiner; Susan M. White; Brandon W. Blackburn; David P. Gierga; Jacquelyn C. Yanch

The use of the 13C(d,n) 14N reaction at Ed=1.5 MeV for accelerator-based boron neutron capture therapy (AB-BNCT) is investigated. Among the deuteron-induced reactions at low incident energy, the 3C(d,n)14N reaction turns out to be one of the best for AB-BNCT because of beneficial materials properties inherent to carbon and its relatively large neutron production cross section. The deuteron beam was produced by a tandem accelerator at MITs Laboratory for Accelerator Beam Applications (LABA) and the neutron beam shaping assembly included a heavy water moderator and a lead reflector. The resulting neutron spectrum was dosimetrically evaluated at different depths inside a water-filled brain phantom using the dual ionization chamber technique for fast neutrons and photons and bare and cadmium-covered gold foils for the thermal neutron flux. The RBE doses in tumor and healthy tissue were calculated from experimental data assuming a tumor 10B concentration of 40 ppm and a healthy tissue 10B concentration of 11.4 ppm (corresponding to a reported ratio of 3.5:1). All results were simulated using the code MCNP, a general Monte Carlo radiation transport code capable of simulating electron, photon, and neutron transport. Experimental and simulated results are presented at 1, 2, 3, 4, 6, 8, and 10 cm depths along the brain phantom centerline. An advantage depth of 5.6 cm was obtained for a treatment time of 56 min assuming a 4 mA deuteron current and a maximum healthy tissue dose of 12.5 RBE Gy.


Physica Medica | 2014

Computational assessment of deep-seated tumor treatment capability of the 9Be(d,n)10B reaction for accelerator-based Boron Neutron Capture Therapy (AB-BNCT)

M.E. Capoulat; D.M. Minsky; A.J. Kreiner

The 9Be(d,n)10B reaction was studied as an epithermal neutron source for brain tumor treatment through Boron Neutron Capture Therapy (BNCT). In BNCT, neutrons are classified according to their energies as thermal (<0.5 eV), epithermal (from 0.5 eV to 10 keV) or fast (>10 keV). For deep-seated tumors epithermal neutrons are needed. Since a fraction of the neutrons produced by this reaction are quite fast (up to 5-6 MeV, even for low-bombarding energies), an efficient beam shaping design is required. This task was carried out (1) by selecting the combinations of bombarding energy and target thickness that minimize the highest-energy neutron production; and (2) by the appropriate choice of the Beam Shaping Assembly (BSA) geometry, for each of the combinations found in (1). The BSA geometry was determined as the configuration that maximized the dose deliverable to the tumor in a 1 h treatment, within the constraints imposed by the healthy tissue dose adopted tolerance. Doses were calculated through the MCNP code. The highest dose deliverable to the tumor was found for an 8 μm target and a deuteron beam of 1.45 MeV. Tumor weighted doses ≥40 Gy can be delivered up to about 5 cm in depth, with a maximum value of 51 Gy at a depth of about 2 cm. This dose performance can be improved by relaxing the treatment time constraint and splitting the treatment into two 1-h sessions. These good treatment capabilities strengthen the prospects for a potential use of this reaction in BNCT.


Applied Radiation and Isotopes | 2011

Design of a beam shaping assembly and preliminary modelling of a treatment room for accelerator-based BNCT at CNEA.

A.A Burlon; S. Girola; A.A. Valda; D.M. Minsky; A.J. Kreiner; G. Sánchez

This work reports on the characterisation of a neutron beam shaping assembly (BSA) prototype and on the preliminary modelling of a treatment room for BNCT within the framework of a research programme for the development and construction of an accelerator-based BNCT irradiation facility in Buenos Aires, Argentina. The BSA prototype constructed has been characterised by means of MCNP simulations as well as a set of experimental measurements performed at the Tandar accelerator at the National Atomic Energy Commission of Argentina.

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D.M. Minsky

National Scientific and Technical Research Council

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A.A. Valda

United States Atomic Energy Commission

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M.E. Capoulat

National Scientific and Technical Research Council

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H.R. Somacal

United States Atomic Energy Commission

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Mario E. Debray

United States Atomic Energy Commission

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Leonardo Gagetti

National Scientific and Technical Research Council

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María S. Herrera

National Scientific and Technical Research Council

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D. Cartelli

National Scientific and Technical Research Council

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M. Davidson

National Scientific and Technical Research Council

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A.A. Burlon

Lawrence Berkeley National Laboratory

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