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Dive into the research topics where M. Mocko is active.

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Featured researches published by M. Mocko.


Physical Review Letters | 2009

Isotopic dependence of the nuclear caloric curve

C. Sfienti; P. Adrich; T. Aumann; C.O. Bacri; T. Barczyk; R. Bassini; S. Bianchin; C. Boiano; A. S. Botvina; A. Boudard; J. Brzychczyk; A. Chbihi; J. Cibor; B. Czech; M. De Napoli; J.-É. Ducret; H. Emling; J.D. Frankland; M. Hellström; D. Henzlova; G. Imme; I. Iori; H. Johansson; K. Kezzar; A. Lafriakh; A. Le Fèvre; E. Le Gentil; Y. Leifels; J. Lühning; J. Łukasik

The A/Z dependence of projectile fragmentation at relativistic energies has been studied with the ALADIN forward spectrometer at SIS. A stable beam of (124)Sn and radioactive beams of (124)La and (107)Sn at 600 MeV per nucleon have been used in order to explore a wide range of isotopic compositions. Chemical freeze-out temperatures are found to be nearly invariant with respect to the A/Z of the produced spectator sources, consistent with predictions for expanded systems. Small Coulomb effects (DeltaT approximately 0.6 MeV) appear for residue production near the onset of multifragmentation.


Physical Review Letters | 2009

Mechanisms in Knockout Reactions

D. Bazin; R. J. Charity; R. T. de Souza; M. Famiano; A. Gade; V. Henzl; D. Henzlova; S. Hudan; Jenny Lee; S. M. Lukyanov; W. G. Lynch; S. McDaniel; M. Mocko; A. Obertelli; A. M. Rogers; L. G. Sobotka; J. R. Terry; J. A. Tostevin; M. B. Tsang; M. Wallace

We report the first detailed study of the relative importance of the stripping and diffraction mechanisms involved in nucleon knockout reactions, by the use of a coincidence measurement of the residue and fast proton following one-proton knockout reactions. The measurements used the S800 spectrograph in combination with the HiRA detector array at the NSCL. Results for the reactions 9Be(9C,8B+X)Y and 9Be(8B,7Be+X)Y are presented and compared with theoretical predictions for the two reaction mechanisms calculated using the eikonal model. The data show a clear distinction between the stripping and diffraction mechanisms and the measured relative proportions are very well reproduced by the reaction theory. This agreement adds support to the results of knockout reaction analyses and their applications to the spectroscopy of rare isotopes.


Physics of Plasmas | 2017

Laser-plasmas in the relativistic-transparency regime: Science and applications

Juan C. Fernandez; D. Cort Gautier; Chengkung Huang; S. Palaniyappan; B. J. Albright; W. Bang; G. Dyer; Andrea Favalli; James F. Hunter; Jacob Mendez; Markus Roth; Martyn T. Swinhoe; P. A. Bradley; O. Deppert; Michelle A. Espy; Katerina Falk; N. Guler; Christopher E. Hamilton; B. M. Hegelich; Daniela Henzlova; Kiril Dimitrov Ianakiev; Metodi Iliev; R. P. Johnson; A. Kleinschmidt; Adrian S. Losko; E. McCary; M. Mocko; R. O. Nelson; R. Roycroft; Miguel A. Santiago Cordoba

Laser-plasma interactions in the novel regime of relativistically induced transparency (RIT) have been harnessed to generate intense ion beams efficiently with average energies exceeding 10 MeV/nucleon (>100 MeV for protons) at “table-top” scales in experiments at the LANL Trident Laser. By further optimization of the laser and target, the RIT regime has been extended into a self-organized plasma mode. This mode yields an ion beam with much narrower energy spread while maintaining high ion energy and conversion efficiency. This mode involves self-generation of persistent high magnetic fields (∼104 T, according to particle-in-cell simulations of the experiments) at the rear-side of the plasma. These magnetic fields trap the laser-heated multi-MeV electrons, which generate a high localized electrostatic field (∼0.1 T V/m). After the laser exits the plasma, this electric field acts on a highly structured ion-beam distribution in phase space to reduce the energy spread, thus separating acceleration and energy-spread reduction. Thus, ion beams with narrow energy peaks at up to 18 MeV/nucleon are generated reproducibly with high efficiency (≈5%). The experimental demonstration has been done with 0.12 PW, high-contrast, 0.6 ps Gaussian 1.053 μm laser pulses irradiating planar foils up to 250 nm thick at 2–8 × 1020 W/cm2. These ion beams with co-propagating electrons have been used on Trident for uniform volumetric isochoric heating to generate and study warm-dense matter at high densities. These beam plasmas have been directed also at a thick Ta disk to generate a directed, intense point-like Bremsstrahlung source of photons peaked at ∼2 MeV and used it for point projection radiography of thick high density objects. In addition, prior work on the intense neutron beam driven by an intense deuterium beam generated in the RIT regime has been extended. Neutron spectral control by means of a flexible converter-disk design has been demonstrated, and the neutron beam has been used for point-projection imaging of thick objects. The plans and prospects for further improvements and applications are also discussed.


Proceedings of SPIE | 2009

The Raytheon-SORDS trimodal imager

Michael V. Hynes; Maurice Toolin; Bernard Harris; John McElroy; M. Wallace; Larry J. Schultz; Mark Corrado Galassi; Andrew S. Hoover; M. Mocko; David M. Palmer; Shawn Tornga; Daniel Wakeford; H. R. Andrews; Edward T. H. Clifford; Liqian Li; Nick Bray; Darren Locklin; Richard C. Lanza; Berthold K. P. Horn; David K. Wehe

The Raytheon Trimodal Imager (TMI) uses coded aperture and Compton imaging technologies as well as the nonimaging shadow technology to locate an SNM or radiological threat in the presence of background. The coded aperture imaging is useful for locating and identifying radiological threats as these threats generally emit lower energy gammas whereas the Compton imaging is useful for SNM threats as in addition to low energy gammas which can be shielded, SNM threats emit higher energy gammas as well. The shadow imaging technology utilizes the structure of the instrument and its vehicle as shadow masks for the individual detectors which shadow changes as the vehicle moves through the environment. Before a radioactive source comes into the fields of view of the imagers it will appear as a shadow cast on the individual detectors themselves. This gives the operator advanced notice that the instrument is approaching something that is radiological and on which side of the vehicle it is located. The two nuclear images will be fused into a combined nuclear image along with isotope ID. This combined image will be further fused with a real-time image of the locale where the vehicle is passing. A satellite image of the locale will also be made available. This instrument is being developed for the Standoff Radiation Detection System (SORDS) program being conducted by Domestic Nuclear Detection Office (DNDO) of the Department of Homeland Security (DHS).


ieee nuclear science symposium | 2009

Simulation and modeling for the Stand-Off Radiation Detection System (SORDS) using GEANT4

Andrew S. Hoover; M. Wallace; Mark Corrado Galassi; M. Mocko; David M. Palmer; Larry J. Schultz; Shawn Tornga

A Stand-Off Radiation Detection System (SORDS) is being developed through a joint effort by Raytheon, Los Alamos National Laboratory, Bubble Technology Industries, Radiation Monitoring Devices, and the Massachusetts Institute of Technology, for the Domestic Nuclear Detection Office (DNDO). The system is a mobile truck-based platform performing detection, imaging, and spectroscopic identification of gamma-ray sources. A Tri-Modal Imaging (TMI) approach combines active-mask coded aperture imaging, Compton imaging, and shadow imaging techniques. Monte Carlo simulation and modeling using the GEANT4 toolkit was used to generate realistic data for the development of imaging algorithms and associated software code.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2012

Neutron recognition in the LAND detector for large neutron multiplicity

P. Pawlowski; J. Brzychczyk; Y. Leifels; W. Trautmann; P. Adrich; T. Aumann; C.O. Bacri; T. Barczyk; R. Bassini; S. Bianchin; C. Boiano; K. Boretzky; A. Boudard; A. Chbihi; J. Cibor; B. Czech; M. De Napoli; J.-É. Ducret; H. Emling; J.D. Frankland; T. Gorbinet; M. Hellström; Daniela Henzlova; S. Hlavac; J. Immè; I. Iori; H. Johansson; K. Kezzar; S. Kupny; A. Lafriakh

The performance of the LAND neutron detector is studied. Using an event-mixing technique based on one-neutron data obtained in the S107 experiment at the GSI laboratory, we test the efficiency of various analytic tools used to determine the multiplicity and kinematic properties of detected neutrons. A new algorithm developed recently for recognizing neutron showers from spectator decays in the ALADIN experiment S254 is described in detail. Its performance is assessed in comparison with other methods. The properties of the observed neutron events are used to estimate the detection efficiency of LAND in this experiment


Progress in Particle and Nuclear Physics | 2009

Isotopic dependence of the caloric curve

W. Trautmann; P. Adrich; T. Aumann; C.O. Bacri; T. Barczyk; R. Bassini; S. Bianchin; C. Boiano; A. S. Botvina; A. Boudard; J. Brzychczyk; A. Chbihi; J. Cibor; B. Czech; M. De Napoli; J.-É. Ducret; H. Emling; J.D. Frankland; M. Hellström; D. Henzlova; G. Imme; I. Iori; H. Johansson; K. Kezzar; A. Lafriakh; A. Le Fèvre; E. Le Gentil; Y. Leifels; J. Lühning; J. Łukasik

Isotopic effects in projectile fragmentation at relativistic energies have been studied with the ALADIN forward spectrometer at SIS. Stable and radioactive Sn and La beams with an incident energy of 600 MeV per nucleon have been used in order to explore a wide range of isotopic compositions. Chemical freeze-out temperatures are found to be nearly invariant with respect to the A/Z ratio of the produced spectator sources, consistent with predictions for expanded systems. Consequences for the proposed interpretation of chemical breakup temperatures as representing the limiting temperatures predicted by microscopic models are discussed.


Archive | 2016

Redesign of the Target-Moderator-Reflector-Shield Assembly for Optimization of the Neutron Flux in the 0.001 – 1 MeV at LANSCE

Suzanne F. Nowicki; M. Mocko; S.A. Wender; Laurent Ferres

These are the slides for a presentation at the 2016 Postdoc Summer Seminar Series at Los Alamos National Laboratory. The conclusions of the research presented are the following: we can provide a significant gain in intensity in the upper tier; lower and upper tier are coupled: translating the target in the FOV of the upper tier decreases the intensity in the lower tier; it is possible to balance the production between the upper and lower tier if we keep some of the material between the tiers.


Archive | 2015

Prospects for a measurement of the 237U(n,f) cross section at the LANSCE Lujan Center

M. Devlin; M. Mocko; Victor A. Gavron; M. Jandel; G. Rusev; T. A. Bredeweg

A new measurement of the 237U(n, f) cross section from thermal to ≈ 100 keV is discussed, using one of the flightpaths at the LANSCE Lujan Center. Previous energy-resolved resonance-region measurements have been conducted using weapon test time-of-flight[1] and the LANSCE Lead Slowing Down Spectrometer[2], the former of which is limited in its energy range, and the latter in its energy resolution and range. We present here a proposal, based on simulations of the Lujan Center neutron flux and a hypothetical experiment, that is expected to adequately address both of these issues.


Archive | 2014

2012-13 Blue Room Low Enriched Uranium Sample Irradiation, Associated Gas Handling System, and Subsequent Separation Chemistry

Iain May; Aaron S. Anderson; Leo J. Bitteker; Michael A. Connors; Roy Copping; Matthew Cover; William J. Crooks; Gregory E. Dale; Dale A. Dalmas; Michael J. Gallegos; Eduardo Garcia; Jack G. Gioia; Robert Gonzales; Debra Graves; W. Kirk Hollis; Michael T. Janicke; Charles T. Kelsey; M. Mocko; Martin Pieck; Mohini Rawool-Sullivan; Sean D. Reilly; Daniel Rios; Tobias J. Romero; Francis H. Stephens; Felicia L. Taw; David L. Thorn; Keith Albert Woloshun

Author(s): May, Iain; Anderson, Aaron S.; Bitteker, Leo J. Jr.; Connors, Michael A.; Copping, Roy; Cover, Matthew; Crooks, William J.; Dale, Gregory E.; Dalmas, Dale A.; Gallegos, Michael J.; Garcia, Eduardo; Gioia, Jack G.; Gonzales, Robert; Graves, Debra; Hollis, W. Kirk; Janicke, Michael T.; Kelsey, Charles T. IV; Mocko, Michal; Pieck, Martin; Rawool-Sullivan, Mohini; Reilly, Sean D.; Rios, Daniel; Romero, Tobias J.; Stephens, Francis H.; Taw, Felicia L.; Thorn, David L.; Woloshun, Keith A.

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W. G. Lynch

Michigan State University

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M. B. Tsang

Michigan State University

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D. Henzlova

Michigan State University

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A. M. Rogers

Argonne National Laboratory

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G. Muhrer

Los Alamos National Laboratory

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M. Wallace

Los Alamos National Laboratory

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M. Famiano

Western Michigan University

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A. Boudard

GSI Helmholtz Centre for Heavy Ion Research

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H. Emling

GSI Helmholtz Centre for Heavy Ion Research

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J.-É. Ducret

GSI Helmholtz Centre for Heavy Ion Research

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