SEMIRAMIS operates an ion beam platform dedicated to pluridisciplinary physics and chemistry

Size: px
Start display at page:

Download "SEMIRAMIS operates an ion beam platform dedicated to pluridisciplinary physics and chemistry"

Transcription

1 SEMIRAMIS Since the sixties, the SEMIRAMIS group has developed skills concerning ion sources and ion beam handling from few hundred ev up to around 10 MeV, with the purpose of materials implantation, irradiation and analysis, and isotope separation for target creation. The equipment available is: a 2MV Van de Graaff/Tandem accelerator, ARAMIS; a 190kV implantor, IRMA; a 50kV isotope separator, SIDONIE; and 200kV Transmission Electron Microscope, TEM. Since 2009, the JANNuS-Orsay platform has started and provides each year 12 weeks of beam-time for experimental projects selected by the EMIR, a national network concerning material studies under irradiation. The following describes the JANNuS-Orsay facility and its integration inside the EMIR network, the instruments managed by the department and finish with a summary of the beam time s use. Members: C. Bachelet, C.O. Bacri, C. Baumier, J. Bourçois, L. Delbecq, O. Kaitasov, J. Moeyaert, E. Oliviero, N. Pauwels, S. Picard, S. Renouf. JANNuS/EMIR (introducing SCALP) SEMIRAMIS operates an ion beam platform dedicated to pluridisciplinary physics and chemistry such as astroparticles, materials for nuclear energy, nuclear physics, solid physics, physico-chemistry of materials, microelectronics, nanosciences, earth sciences... It is composed of a 2 MV Tandem/Van de Graaf Accelerator (ARAMIS) and a 190 kv ion implantor (IRMA), both being possibly coupled to a 200 kv Transmission Electron Microscope (TEM FEI TecnaiG2 20) allowing in-situ observation of irradiation effects (Figure 1). This coupling, JANNuS-Orsay, is part of a multi-ion beam irradia- Figure 1 Schematic view of the SCALP platform. Coupling of ARAMIS, IRMA and the MET constitutes JANNuS-Orsay. tion platform called JANNuS ( fr/), and managed by CEA/DEN, CEA/INSTN, CNRS/ IN2P3 and Paris-Sud University, in the framework of a Scientific Interest Group (GIS). JANNuS is part of the EMIR network ( which consist of five accelerator platforms dedicated to material irradiation with a shared scientific committee. JANNuS-Orsay is mainly used for controlled modification or synthesis of materials at the nanoscale by ion implantation and irradiation, simulation of radiation damage in nuclear materials, and education and training in the field of particle-matter interactions and its applications. CSNSM platform also operates a 50 kv electromagnetic isotope separator, SIDONIE, which is primarily used for the separation of high purity thin deposit and targets, mainly for nuclear physics experiments. Since 2015, all these CSNSM machines constitute the SCALP (Synthesis and Characterization using ion AcceLeration for Pluridisciplinary research) platform (Figure 1). It allows performing irradiation/ implantation, ion beam analysis, and target production for the study of elementary mechanisms governing the behavior of materials under irradiation. SCALP is managed through a technical and scientific committee, which examine the beam time requests, while maintaining flexibility in the management of the beam time. The platform is also used for education and training in the field of particle-matter interactions and its applications, through organization of Travaux Pratiques and trainees. Part of the beam time is also dedicated to some industrials needs of irradiations/implantations.

2 ARAMIS ARAMIS is a home-made 2MV s accelerator, for materials implantation/irradiation and ion beam analysis, in activity since ARAMIS can be used as a Van de Graaff accelerator; with a Penning ion source located at the high voltage stage and provides gaseous elements like hydrogen, helium, nitrogen or oxygen. ARAMIS can be used also as a Tandem, with the Middleton negative ion source at the ground potential and provides more than forty different elements. See Figure 3 for the elements available with ARAMIS. Three beam lines are available for different type of experiments. The characterization line is used for ion beam analysis of materials. A goniometer, with 2 translations and 2 rotations, allows characterization of several samples in the same run, and channelling inside the material s crystal. The ion beam analysis methods available are C/RBS, ERDA and PIXE. After a previous update of the goniometer with a PMC Multiflex card, instead of an old RS232 controller, and a LabView based user interface, the purchase of a new goniometer is on going, with the participation of the Physics and Chemistry of Irradiation group. The commissioning of the goniometer should be done within the first trimester of The C/RBS acquisition analogic system has also been replaced with a CAEN N1728B. This module allows signal digitizing from the preamplifier on 4 channels. A new user acquisition interface has been developed using LabView. The possibility to use 4 detectors at a time is currently in development. This option will reduce the acquisition time or increase the counting rate of the spectra. Finally, PIXE analysis has been added two years ago. Two silicon drift detectors (SDD) open the possibility to detect elements from beryllium to uranium. The implantation/irradiation beam line is used for materials modifications with several conditions. Different sample holders are available and permit to do materials implantation/irradiation with temperature running from 77K to 1200K. Another sample holder allows the implantation/irradiation on different samples with different parameters in the same run, with holders like the Translation, the Revolver or the Airlock. The third beam line is called the JANNuS line. This line is a connection from ARAMIS to the Transmission Electron Microscope (TEM). It allows in situ studies of materials implantation/irradiation under double ion beam of ARAMIS and IRMA (see JANNuS section). In 2015, the commissioning of a beamline linking ARA- MIS to IRMA has been done. Using +/-50 kv deflectors, we can drive a high energy beam, from ARAMIS, into the IRMA s irradiation chamber (Figure 2). With samples placed on a goniometer, the beamline allows in situ RBS/C of materials during irradiation. Figure 2 Electrostatic deflectors, driving the ARAMIS beam inside IRMA s irradiation chamber IRMA IRMA is an ion implanter of 190kV, home-made in IRMA can provide ion beam energy from 5 to 570 kev. Its Bernas-Nier ion source can produce almost all stable elements (Figure 3), with a current up to 100 µa. The purpose of IRMA is principally materials modification by ion implantation, in several conditions. The sample holders, available for IRMA, are the same as the one described in the ARAMIS section. During the last years, and taking advantage of the JANNuS platform development, IRMA had several updates and improvements. For example, the beam line after the acceleration section has been rejuvenated and now all the components at ground potential are computer-driven, and some at the high voltage stage. A complete migration to a digital control has been done in The moving electrode for ion extraction of the source has been replaced. A complete new design with motorised and independent moves has been developed in collaboration with the mechanical Figure 3 Elements available with ARAMIS-IRMA 6 CSNSM - SEMIRAMIS 89

3 Figure 4 New moving electrode for ion extraction on IRMA. department (Figure 4). The installation of this electrode has been coupled with the control update, since the moves is now computer-driven. The electrode is now sold to Ion Beam Service to be used as a part of their new implanter. Transmission Electron Microscope (TEM) Figure 5 Schematic view of the separator SIDONIE The TEM of the CSNSM is part of the JANNuS-Orsay platform and has been designed for dual-irradiation/ implantation in-situ and dynamic experiments. The TEM is a FEI Tecnai G 2 20 Twin. The electron beam is extracted from a LaB 6 filament and the accelerating voltage can be set from 80 to 200 kv. The spatial resolution is 0.27 nm. This microscope is equipped today with 2 CCD cameras for imaging (a wide angle & high resolution camera). For the spectroscopy measurement the TEM proposed several techniques : EDX, EELS, EFTEM and a STEM (scanning transmission electron microscopy) mode with HAADF and BF-DF which allow the Spectrum Imaging (SI) with the coupled EELS and EDX measurement. In the best conditions, the energy resolution for the EELS is 1,1 ev. Since the end of 2015, all these techniques of measurements and analysis are available in dynamics with the video recording (when the ions beam is suitable with the Magnetic field of the TEM polar piece). The TEM of the platform is also equipped with several sample holders which allow double tilt and rotation; and a wide range of temperature from -170 C to 1300 C. Many sample holders are ultra-thin, a design dedicated to in situ irradiation. In order to keep the platform as a highly ranked in situ analysis facility, further development is foreseen (see Research, Development & Perspectives chapter). This TEM of JANNuS-Orsay is also accessible by the annual EMIR call, which allows scientists from all around the world to have their experiments granted. The experiments done on the microscope concern the fields of nuclear simulation, materials sciences, nanotechnology, semiconductors, nano-particles, amorphization/recrystallization, inorganic chemistry SIDONIE SIDONIE is an electromagnetic isotope separator, which is primarily used for the preparation of high purity thin deposit and targets, mainly in nuclear physics experiments. The separator is composed of a Bernas-Nier ion source, a high resolution analyzing magnet and a collecting device, which is used to prepare targets with the selected ion beam. A picture of the SIDONIE experimental apparatus is represented in Figure 5. The source can deliver almost all ions. They are mainly single-charged and the extracted beam intensity ranges from a few ma up to 20 ma. Their energy are typically around 40 kev. The separation power of the analyzing magnet is 1000, which means that masses 100 and 101 are separated with 1 cm in the focal plane. In order to complete the possibilities of the separator, a new setup has been installed. It consists in a near visible infrared spectrometer coupled with the beam line of SIDONIE. Called INGMAR (IrradiatioN de Glaces et Météorites Analysées par Réflectance VIS-IR), it was funded in close collaboration with the IAS (Institut d Astrophysique Spatiale). It allows analysing the molecular structure of samples under irradiation and is mainly used to understand the ageing of micrometeorites under irradiation by solar wind. 90 CSNSM - SEMIRAMIS

4 Beam Time Summary There are three ways of assignment of the beam time: via the yearly EMIR call for proposals; via the SEMIRAMIS council call every three months; or via the along the way time allocation versus payment. The use of ARAMIS and IRMA is between 140 and 160 days per year (Figure 6). ARAMIS is mainly used, around 60%; IRMA represents 23% and the dual beam represents 17%. The need of a more often maintenance of IRMA explains the difference of time use compared to ARAMIS. One day represents generally one experiment and lasting roughly 8 hours. Between 30% and 40% of the time is used for CSNSM s research (Figure 7). Around the same amount is dedicated to experiments granted by the EMIR s scientific council. Outside the EMIR s network context, external users can have access to the platform as a paid service; with academic fee for University and CNRS members and full fee for the others. These external users represent 28% of the total beam time, industrials around 10%. Teaching activities on the platform are slightly rising along the years. Our human-scale devices allow original and high technicality practical works for master s students. Teaching, using SCALP facility, is delivered by the SEMIRAMIS team or members of the Physics and Chemistry of Irradiation and Solid State Astrophysics research groups, and concerned several Masters of Université Paris-Saclay: Nuclear Energy, Physics and Engineering of Energy, Astronomical and Spaced-based Systems Engineering and recently Grands Instruments. Figure 6 Days of use of ARAMIS, IRMA and Dual-Beam Figure 7 Split of beam time allocation 6 Research, Development & Perspectives The SEMIRAMIS team has usually, in the past years, focussed on several research subjects, using its analytic capabilities. Recently, He diffusion in apatite studies, within the ANR HeDiff project, or oxygen density measurements in rareearth based cuprates superconductors were investigated. In addition to the Ion Beam Analysis techniques already used (RBS, ERDA, PIXE), the group aims to provide another technique called micropixe. MicroPIXE is an extension of PIXE (Particleinduced X-ray emission) using a beam focused down to 1 µm. The solution retained for the focusing system was not the classical one, using magnetic quadripole lenses, but a simple and low-cost method, using a tapered glass capillary. Figure 8 Split of the TEM use CSNSM - SEMIRAMIS 91

5 It is expected to complete the setup by summer 2016 and to carry out first micropixe experiments by the end of It will then be possible to produce elemental maps of samples e.g. for the astrophysics and geological communities. Once the micropixe technique available, a next step could be to investigate in-air analysis. This development has been funded by Paris-Sud university through the 2014 project call Equipement de Recherche Mutualisée, with the collaboration of the GEOPS laboratory, under the coordination of Céline Tanguy. The development of PIGE applications has been also initiate, in order to extend the scope of the platform and meet the needs of many scientific communities. Two channels are currently being explored: - the production of high-energy γ beam (up to 16 MeV) allowing the calibration of detectors, - the analysis method for determination of hydrogen and isotopic light elements in various samples. These new developments are under the coordination of Nicolas Pauwels. In order to extend in situ capabilities of the TEM, the project POMETILAT aim to build a new sample holder. POMETILAT consists a laser waveguide coupled to a heating element in the very thin manifold of the (3 mm diameter). This new tool will allow the in-situ study of the dynamics of structural changes resulting from photo-induced d-d electron charge transfert. This development is motivated by the study of Prussian Blue Analogues (ABP) photoswitchable molecular systems whose magnetic properties offer attractive prospects for the storage of high-density information. POMETI- LAT is funded by the interdisciplinary mission of the CNRS through the 2015 project call DEFI Instrumentation aux limites with the collaboration LCI/ICMMO, under the coordination of Cedric Baumier. Figure 9 Technical drawing of the POMETILAT sample holder 92 CSNSM - SEMIRAMIS

6 Publications PUBLISHED PAPERS Debelle A., Boulle A., Rakotovao, F. et al. Infl uence of elastic properties on the strain induced by ion irradiation in crystalline materials, J. Phys. D Appl. Phys. 46 (2013) Pauwels N., Horodynski J.M., Robert P., Tadjeddine A. Decommissioning of the LURE Nuclear Facility, Radioprotection 48 (2013) 545 Thome L., Debelle A., Garrido F. et al. Radiation effects in nuclear materials: Role of nuclear and electronic energy losses and their synergy, Nucl. Instr. Meth. in Phys. Res. B 307 (2013) 43 Chiuzbaian S.G., Hague C.F., Avila A. et al. Design and performance of AERHA, a high acceptance high resolution soft x-ray spectrometer, Rev. Sci. Instrum. 85 (2014) Roedel T.C., Bareille C., Fortuna F. et al. Orientational Tuning of the Fermi Sea of Confi ned Electrons at the SrTiO3 (110) and (111) Surfaces, Phys. Rev. Appl. 1 (2014) Sabathier C., Martin G., Michel A. et al. In-situ TEM observation of nano-void formation in UO2 under irradiation, Nucl. Instr. Meth. in Phys. Res. B 326 (2014) 247 Tien Hien N., Garrido F., Debelle A. et al. Radiation damage in urania crystals implanted with low-energy ions, Nucl. Instr. Meth. in Phys. Res. B 326 (2014) 264 Bergeard N., Schaffert S., Lopez-Flores V. et al. Irreversible transformation of ferromagnetic ordered stripe domains in singleshot infrared-pump/resonant-x-ray-scattering-probe experiments, Phys. Rev. B 91 (2015) Defresne A., Plantevin O., Sobkowicz I.P. et al. Interface defects in a-si:h/c-si heterojunction solar cells, Nucl. Instr. Meth. in Phys. Res. B 365 (2015) 133 Sengupta, S.; Li, C.; Baumier, C.; Kasumov, A.; Gueron, S.; Bouchiat, H.; Fortuna, F. Superconducting nanowires by electron-beam-induced deposition, App. Phys. Lett. 106 (2015) PROCEEDINGS Fang L., Bachelet C., Sagnes, I. et al. Ion implanted In0.53Ga0.47As for ultrafast saturable absorber device at 1.55 mu m, 26 th International Conference on Indium Phosphide and Related Materials (IPRM) (2014) CSNSM - SEMIRAMIS 93

), nano-objects (nano-particles, nano-wires, nano-bubbles) and the simulation of neutron irradiation effects in nuclear materials (UO 2.

), nano-objects (nano-particles, nano-wires, nano-bubbles) and the simulation of neutron irradiation effects in nuclear materials (UO 2. SEMIRAMIS Since the sixties, SEMIRAMIS has developed skills in ion source and ion beam handling ranging from a few hundred ev to around 10 MeV, with the goal of materials implantation, irradiation and

More information

Serge Bouffard EMIR User days

Serge Bouffard EMIR User days facilities Serge Bouffard EMIR User days October 20 th, 2011 EMIR network a national network of accelerators dedicated to material irradiation EMIR network gathers the French facilities for material irradiation

More information

High voltage electron microscopy facility. Jannus-Saclay facility (GIS with Jannus-Orsay) SRMA

High voltage electron microscopy facility. Jannus-Saclay facility (GIS with Jannus-Orsay) SRMA SRMA Jannus-Saclay facility (GIS with Jannus-Orsay) High voltage electron microscopy facility Lucile Beck - JANNUS laboratory - SRMP Jean Henry SRMA CEA Saclay CEA 10 AVRIL 2012 PAGE 1 Programs and objectives

More information

IAP NAN of Ukraine activity in. Possible areas of cooperation in. Roman Kholodov, PICS Meeting, Basivka, Ukraine,

IAP NAN of Ukraine activity in. Possible areas of cooperation in. Roman Kholodov, PICS Meeting, Basivka, Ukraine, 1 IAP NAN of Ukraine activity in field of High Energy Physics. Possible areas of cooperation in frame of PICS and beyond. Institute of Applied Physics National Academy of Sciences of Ukraine 2 The Institute

More information

Accelerator facilities - Ruđer Bošković Institute, Zagreb, Croatia

Accelerator facilities - Ruđer Bošković Institute, Zagreb, Croatia Accelerator facilities - Ruđer Bošković Institute, Zagreb, Croatia Milko Jaksic, Neven Soic Our capabilities (accelerator, sources, beamlines,...) Research activities (projects, users, int. collaborations,...)

More information

accelerating opportunities

accelerating opportunities accelerating opportunities 9 MV Pelletron FN Tandem Accelerator for basic and applied research The 9MV Tandem Accelerator has been built by the High Voltage Engineering Corporation (HVEC) in 1973 and it

More information

Opportunities for Advanced Plasma and Materials Research in National Security

Opportunities for Advanced Plasma and Materials Research in National Security Opportunities for Advanced Plasma and Materials Research in National Security Prof. J.P. Allain allain@purdue.edu School of Nuclear Engineering Purdue University Outline: Plasma and Materials Research

More information

The Groningen Cyclotron at Demokritos Athens

The Groningen Cyclotron at Demokritos Athens The Groningen Cyclotron at Demokritos Athens Anastasios Lagoyannis Tandem Accelerator Laboratory N.C.S.R. Demokritos Outline N.C.S.R. Demokritos The Tandem @ I.N.P. P. Basic Infrastructure - Research Interests

More information

MeV Particles, Huge Impact, Soft Desorption.

MeV Particles, Huge Impact, Soft Desorption. MeV Particles, Huge Impact, Soft Desorption. S. Della-Negra Institut de Physique Nucléaire d Orsay, UMR 8608 CNRS- Univ. Paris-Sud, F-91406Orsay Cedex (dellaneg@ipno.in2p3.fr) Since the first PDMS experiment

More information

object objective lens eyepiece lens

object objective lens eyepiece lens Advancing Physics G495 June 2015 SET #1 ANSWERS Field and Particle Pictures Seeing with electrons The compound optical microscope Q1. Before attempting this question it may be helpful to review ray diagram

More information

In situ TEM studies of helium bubble/platelet evolution in Si based materials

In situ TEM studies of helium bubble/platelet evolution in Si based materials In situ TEM studies of helium bubble/platelet evolution in Si based materials M. Vallet 1, M.F. Beaufort 1, J.F. Barbot 1, E. Oliviero 2 and S.E. Donnelly 3 1 Institut Pprime, CNRS-Université de Poitiers,

More information

Techniques EDX, EELS et HAADF en TEM: possibilités d analyse et applications

Techniques EDX, EELS et HAADF en TEM: possibilités d analyse et applications Techniques EDX, EELS et HAADF en TEM: possibilités d analyse et applications Thomas Neisius Université Paul Cézanne Plan Imaging modes HAADF Example: supported Pt nanoparticles Electron sample interaction

More information

Inside this Issue. Articles. Atmospheric pressure plasma system for Textiles

Inside this Issue. Articles. Atmospheric pressure plasma system for Textiles Facilitation Centre for Industrial Plasma Technologies Institute for Plasma Research Plasma Processing Update I s s u e Editor 8 3 A p r 2 0 1 8 Inside this Issue Articles Atmospheric pressure plasma system

More information

Chapter 9. Electron mean free path Microscopy principles of SEM, TEM, LEEM

Chapter 9. Electron mean free path Microscopy principles of SEM, TEM, LEEM Chapter 9 Electron mean free path Microscopy principles of SEM, TEM, LEEM 9.1 Electron Mean Free Path 9. Scanning Electron Microscopy (SEM) -SEM design; Secondary electron imaging; Backscattered electron

More information

Praktikum zur. Materialanalytik

Praktikum zur. Materialanalytik Praktikum zur Materialanalytik Energy Dispersive X-ray Spectroscopy B513 Stand: 19.10.2016 Contents 1 Introduction... 2 2. Fundamental Physics and Notation... 3 2.1. Alignments of the microscope... 3 2.2.

More information

Surface analysis techniques

Surface analysis techniques Experimental methods in physics Surface analysis techniques 3. Ion probes Elemental and molecular analysis Jean-Marc Bonard Academic year 10-11 3. Elemental and molecular analysis 3.1.!Secondary ion mass

More information

The scanning microbeam PIXE analysis facility at NIRS

The scanning microbeam PIXE analysis facility at NIRS Nuclear Instruments and Methods in Physics Research B 210 (2003) 42 47 www.elsevier.com/locate/nimb The scanning microbeam PIXE analysis facility at NIRS Hitoshi Imaseki a, *, Masae Yukawa a, Frank Watt

More information

Neutron Source Capabilities at Ohio University

Neutron Source Capabilities at Ohio University Neutron Source Capabilities at Ohio University Carl R. Brune, Steven M. Grimes, David. C. Ingram, and Thomas N. Massey Department of Physics and Astronomy, Ohio University, Athens OH 45701, USA (Dated:

More information

Ion Implanter Cyclotron Apparatus System

Ion Implanter Cyclotron Apparatus System Ion Implanter Cyclotron Apparatus System A. Latuszyñski, K. Pyszniak, A. DroŸdziel, D. M¹czka Institute of Physics, Maria Curie-Sk³odowska University, Lublin, Poland Abstract In this paper the authors

More information

JANNUS: A multi-irradiation platform for experimental validation at the scale of the atomistic. modelling

JANNUS: A multi-irradiation platform for experimental validation at the scale of the atomistic. modelling JANNUS: A multi-irradiation platform for experimental validation at the scale of the atomistic modelling Y. Serruys 1, P. Trocellier 1, S. Miro 1, E. Bordas 1, M.O. Ruault 2, O. Kaïtasov 2, S. Henry 2,

More information

User Fees for the 4D LABS Characterization Facility

User Fees for the 4D LABS Characterization Facility User Fees for the 4D LABS Characterization Facility 1. Imaging Fees Service SEM 1 - Helios: SEM/EDS mode SEM/EDS mode with FIB functions Cryo mode setup SEM 2 Nova NanoSEM SEM/EDS mode SEM/EDS mode with

More information

NGN PhD Studentship Proposal

NGN PhD Studentship Proposal NGN PhD Studentship Proposal Note that proposals will be assessed against both the quality of the scientific content and of the proposed training experience. Proposed supervisors (lead first) Dr Laura

More information

Fission Fragment characterization with FALSTAFF at NFS

Fission Fragment characterization with FALSTAFF at NFS EPJ Web of Conferences 42, 01001 (2013) DOI: 10.1051/ epjconf/ 20134201001 C Owned by the authors, published by EDP Sciences, 2013 Fission characterization with FALSTAFF at NFS D. Doré 1, F. Farget 2,

More information

Silver Thin Film Characterization

Silver Thin Film Characterization Silver Thin Film Characterization.1 Introduction Thin films of Ag layered structures, typically less than a micron in thickness, are tailored to achieve desired functional properties. Typical characterization

More information

Photofission of 238-U Nuclei

Photofission of 238-U Nuclei Photofission of 238-U Nuclei International Thorium Energy Conference - ThEC18, 29-31st of October 2018, Belgium İsmail Boztosun This research has been supported by TÜBİTAK with grant number 114F220 Motivations

More information

Characterisation of Nanoparticle Structure by High Resolution Electron Microscopy

Characterisation of Nanoparticle Structure by High Resolution Electron Microscopy Journal of Physics: Conference Series OPEN ACCESS Characterisation of Nanoparticle Structure by High Resolution Electron Microscopy To cite this article: Robert D Boyd et al 2014 J. Phys.: Conf. Ser. 522

More information

The intense, pulsed positron source EPOS at the Research Centre Dresden-Rossendorf

The intense, pulsed positron source EPOS at the Research Centre Dresden-Rossendorf The intense, pulsed positron source EPOS at the Research Centre Dresden-Rossendorf The EPOS Team and R. Krause-Rehberg Martin-Luther University, Halle-Wittenberg, Dept. of Physics, 06099 Halle / Germany

More information

PHI 5000 Versaprobe-II Focus X-ray Photo-electron Spectroscopy

PHI 5000 Versaprobe-II Focus X-ray Photo-electron Spectroscopy PHI 5000 Versaprobe-II Focus X-ray Photo-electron Spectroscopy The very basic theory of XPS XPS theroy Surface Analysis Ultra High Vacuum (UHV) XPS Theory XPS = X-ray Photo-electron Spectroscopy X-ray

More information

Light ion recoil detector

Light ion recoil detector Light ion recoil detector Overall design The detector for light (target-like) particles is a substantial part of the R3B setup. It allows registration of recoils in coincidence with the heavy fragments,

More information

Characterization of Gold LMIS and Integration into Andromede Project

Characterization of Gold LMIS and Integration into Andromede Project Characterization of Gold LMIS and Integration into Andromede Project Michael J. Eller a,*, Bernard Rasser b, Nimer Wehbe c, Manale Noun a, Patrick Philipp c, Evelyne Cottereau a, Serge Della-Negra a a.

More information

Chapter 10. Nanometrology. Oxford University Press All rights reserved.

Chapter 10. Nanometrology. Oxford University Press All rights reserved. Chapter 10 Nanometrology Oxford University Press 2013. All rights reserved. 1 Introduction Nanometrology is the science of measurement at the nanoscale level. Figure illustrates where nanoscale stands

More information

Modified Physics Course Descriptions Old

Modified Physics Course Descriptions Old Modified Physics Course Descriptions Old New PHYS 122, General Physics II, 4 cr, 3 cl hrs, 2 recitation hrs Prerequisite: PHYS 121 Corequisites: MATH 132; PHYS 122L Continuation of PHYS 121 including electricity

More information

Dual Beam Helios Nanolab 600 and 650

Dual Beam Helios Nanolab 600 and 650 Dual Beam Helios Nanolab 600 and 650 In the Clean Room facilities of the INA LMA, several lithography facilities permit to pattern structures at the micro and nano meter scale and to create devices. In

More information

Developments of the RCNP cyclotron cascade

Developments of the RCNP cyclotron cascade CYCLOTRONS 2007 The 18th International Conference on Cyclotrons and Their Applications Developments of the RCNP cyclotron cascade K. Hatanaka,, M. Fukuda, T. Saito, T. Yorita,, H. Tamura, M. Kibayashi,

More information

Method of active correlations in the experiment 249 Cf+ 48 Ca n

Method of active correlations in the experiment 249 Cf+ 48 Ca n Method of active correlations in the experiment 249 Cf+ 48 Ca 297 118 +3n Yu.S.Tsyganov, A.M.Sukhov, A.N.Polyakov Abstract Two decay chains originated from the even-even isotope 294 118 produced in the

More information

Nova 600 NanoLab Dual beam Focused Ion Beam IITKanpur

Nova 600 NanoLab Dual beam Focused Ion Beam IITKanpur Nova 600 NanoLab Dual beam Focused Ion Beam system @ IITKanpur Dual Beam Nova 600 Nano Lab From FEI company (Dual Beam = SEM + FIB) SEM: The Electron Beam for SEM Field Emission Electron Gun Energy : 500

More information

EPOS an intense positron beam project at the Research Center Rossendorf

EPOS an intense positron beam project at the Research Center Rossendorf EPOS an intense positron beam project at the Research Center Rossendorf R. Krause-Rehberg 1, G. Brauer 2, S. Sachert 1, V. Bondarenko 1, A. Rogov 2, K. Noack 2 1 Martin-Luther-University Halle 2 Research

More information

2012/01/20. Thierry EPICIER. MATEIS-CLYM, umr CNRS5510, Director METSA (FR 3507 CNRS) M. AOUINE, JP MILLET et al.

2012/01/20. Thierry EPICIER. MATEIS-CLYM, umr CNRS5510, Director METSA (FR 3507 CNRS) M. AOUINE, JP MILLET et al. 2012/01/20 Thierry EPICIER MATEIS-CLYM, umr CNRS5510, Director METSA (FR 3507 CNRS) thierry.epicier@insa-lyon.fr M. AOUINE, JP MILLET et al. MATERIALS SCIENCES & NANOTECHNOLOGIES HIGH RESOLUTION MICROSCOPY

More information

Determination of the boron content in polyethylene samples using the reactor Orphée

Determination of the boron content in polyethylene samples using the reactor Orphée Determination of the boron content in polyethylene samples using the reactor Orphée F. Gunsing, A. Menelle CEA Saclay, F-91191 Gif-sur-Yvette, France O. Aberle European Organization for Nuclear Research

More information

SYSTEM FOR PIXE TRACE ELEMENT ANALYSIS AT MTF. M. Beňo, J. Dobrovodský, D. Vaňa, S. Minárik

SYSTEM FOR PIXE TRACE ELEMENT ANALYSIS AT MTF. M. Beňo, J. Dobrovodský, D. Vaňa, S. Minárik SYSTEM FOR PIXE TRACE ELEMENT ANALYSIS AT MTF M. Beňo, J. Dobrovodský, D. Vaňa, S. Minárik Slovak University of Technology in Bratislava, Faculty of Materials Science and Technology in Trnava (MTF), Advanced

More information

Remote Access to Hi-tech Equipment

Remote Access to Hi-tech Equipment Remote Access to Hi-tech Equipment From Your Classroom to Ours Sebastien Maeder Outline What is Remote Access? The Method vs. the Goal The role within NACK Why should we try? Confines of Classroom Characterization

More information

Hands on LUNA: Detector Simulations with Geant4

Hands on LUNA: Detector Simulations with Geant4 : Detector Simulations with Geant4 Gran Sasso Science Institute E-mail: axel.boeltzig@gssi.infn.it Andreas Best Laboratori Nazionali del Gran Sasso E-mail: andreas.best@lngs.infn.it For the evaluation

More information

A DIVISION OF ULVAC-PHI. Quantera II. Scanning XPS Microprobe

A DIVISION OF ULVAC-PHI. Quantera II. Scanning XPS Microprobe A DIVISION OF ULVAC-PHI Quantera II Scanning XPS Microprobe X-ray Photoelectron Spectroscopy (XPS/ESCA) is the most widely used surface analysis technique and has many well established industrial and

More information

HOW TO APPROACH SCANNING ELECTRON MICROSCOPY AND ENERGY DISPERSIVE SPECTROSCOPY ANALYSIS. SCSAM Short Course Amir Avishai

HOW TO APPROACH SCANNING ELECTRON MICROSCOPY AND ENERGY DISPERSIVE SPECTROSCOPY ANALYSIS. SCSAM Short Course Amir Avishai HOW TO APPROACH SCANNING ELECTRON MICROSCOPY AND ENERGY DISPERSIVE SPECTROSCOPY ANALYSIS SCSAM Short Course Amir Avishai RESEARCH QUESTIONS Sea Shell Cast Iron EDS+SE Fe Cr C Objective Ability to ask the

More information

The intense Positron Source EPOS at ELBE Radiation Source of Research Center Rossendorf

The intense Positron Source EPOS at ELBE Radiation Source of Research Center Rossendorf The intense Positron Source EPOS at ELBE Radiation Source of Research Center Rossendorf R. Krause-Rehberg 1, G. Brauer 2, 1 Martin-Luther-University Halle 2 Research Center Rossendorf Martin-Luther-Universität

More information

Spin-resolved photoelectron spectroscopy

Spin-resolved photoelectron spectroscopy Spin-resolved photoelectron spectroscopy Application Notes Spin-resolved photoelectron spectroscopy experiments were performed in an experimental station consisting of an analysis and a preparation chamber.

More information

Comparison of the Photo-peak Efficiencies between the Experimental Data of 137 Cs Radioactive Source with Monte Carlo (MC) Simulation Data

Comparison of the Photo-peak Efficiencies between the Experimental Data of 137 Cs Radioactive Source with Monte Carlo (MC) Simulation Data International Journal of Advanced Research in Physical Science (IJARPS) Volume 5, Issue 10, 2018, PP 24-28 ISSN No. (Online) 2349-7882 www.arcjournals.org Comparison of the Photo-peak Efficiencies between

More information

IMAGING DIFFRACTION SPECTROSCOPY

IMAGING DIFFRACTION SPECTROSCOPY TEM Techniques TEM/STEM IMAGING DIFFRACTION SPECTROSCOPY Amplitude contrast (diffracion contrast) Phase contrast (highresolution imaging) Selected area diffraction Energy dispersive X-ray spectroscopy

More information

Imaging Methods: Scanning Force Microscopy (SFM / AFM)

Imaging Methods: Scanning Force Microscopy (SFM / AFM) Imaging Methods: Scanning Force Microscopy (SFM / AFM) The atomic force microscope (AFM) probes the surface of a sample with a sharp tip, a couple of microns long and often less than 100 Å in diameter.

More information

Photoemission Spectroscopy

Photoemission Spectroscopy FY13 Experimental Physics - Auger Electron Spectroscopy Photoemission Spectroscopy Supervisor: Per Morgen SDU, Institute of Physics Campusvej 55 DK - 5250 Odense S Ulrik Robenhagen,

More information

MICRO-TOMOGRAPHY AND X-RAY ANALYSIS OF GEOLOGICAL SAMPLES

MICRO-TOMOGRAPHY AND X-RAY ANALYSIS OF GEOLOGICAL SAMPLES THE PUBLISHING HOUSE PROCEEDINGS OF THE ROMANIAN ACADEMY, Series A, OF THE ROMANIAN ACADEMY Volume 18, Number 1/2017, pp. 42 49 MICRO-TOMOGRAPHY AND X-RAY ANALYSIS OF GEOLOGICAL SAMPLES Ion GRUIA University

More information

A DIVISION OF ULVAC-PHI

A DIVISION OF ULVAC-PHI A DIVISION OF ULVAC-PHI X-ray photoelectron spectroscopy (XPS/ESCA) is the most widely used surface analysis technique and has many well established industrial and research applications. XPS provides

More information

EEE4106Z Radiation Interactions & Detection

EEE4106Z Radiation Interactions & Detection EEE4106Z Radiation Interactions & Detection 2. Radiation Detection Dr. Steve Peterson 5.14 RW James Department of Physics University of Cape Town steve.peterson@uct.ac.za May 06, 2015 EEE4106Z :: Radiation

More information

Gaetano L Episcopo. Scanning Electron Microscopy Focus Ion Beam and. Pulsed Plasma Deposition

Gaetano L Episcopo. Scanning Electron Microscopy Focus Ion Beam and. Pulsed Plasma Deposition Gaetano L Episcopo Scanning Electron Microscopy Focus Ion Beam and Pulsed Plasma Deposition Hystorical background Scientific discoveries 1897: J. Thomson discovers the electron. 1924: L. de Broglie propose

More information

Detectors in Nuclear and High Energy Physics. RHIG summer student meeting June 2014

Detectors in Nuclear and High Energy Physics. RHIG summer student meeting June 2014 Detectors in Nuclear and High Energy Physics RHIG summer student meeting June 2014 Physics or Knowledge of Nature Experimental Data Analysis Theory ( application) Experimental Data Initial Conditions /

More information

International Journal of Scientific & Engineering Research, Volume 5, Issue 3, March-2014 ISSN

International Journal of Scientific & Engineering Research, Volume 5, Issue 3, March-2014 ISSN 316 Effective atomic number of composite materials by Compton scattering - nondestructive evaluation method Kiran K U a, Ravindraswami K b, Eshwarappa K M a and Somashekarappa H M c* a Government Science

More information

MSE 321 Structural Characterization

MSE 321 Structural Characterization Auger Spectroscopy Auger Electron Spectroscopy (AES) Scanning Auger Microscopy (SAM) Incident Electron Ejected Electron Auger Electron Initial State Intermediate State Final State Physical Electronics

More information

Quantum Technologies CCEM Workshop March 23 rd, 2017

Quantum Technologies CCEM Workshop March 23 rd, 2017 Quantum Technologies CCEM Workshop March 23 rd, 2017 JT Janssen Welcome to the National Physical Laboratory The first quantum revolution h V n f 2 e 1 The second quantum revolution Superposition Entanglement

More information

OPERATION STATUS OF HIGH INTENSITY ION BEAMS AT GANIL

OPERATION STATUS OF HIGH INTENSITY ION BEAMS AT GANIL OPERATION STATUS OF HIGH INTENSITY ION BEAMS AT GANIL F. Chautard, G. Sénécal, GANIL, Caen, France Abstract The Grand Accélérateur National d s Lourds (GANIL, Fig. ) facility (Caen, France) is dedicated

More information

Práctica de laboratorio número 6: Non-Rutherford scattering near the MeV 12 C(p,p) 12 C resonance

Práctica de laboratorio número 6: Non-Rutherford scattering near the MeV 12 C(p,p) 12 C resonance Práctica de laboratorio número 6: Non-Rutherford scattering near the 1.734 MeV 12 C(p,p) 12 C resonance 1) Scope In this experiment, the yield of protons backscattered from a thin gold foil deposited over

More information

Ion-beam techniques. Ion beam. Electrostatic Accelerators. Van de Graaff accelerator Pelletron Tandem Van de Graaff

Ion-beam techniques. Ion beam. Electrostatic Accelerators. Van de Graaff accelerator Pelletron Tandem Van de Graaff Ion-beam techniques RBS Target nucleus Ion beam STIM RBS: Rutherford backscattering ERD: Elastic recoil detection PIXE: Particle induced x-ray emission PIGE: Particle induced gamma emission NRA: Nuclear

More information

Aberration-corrected TEM studies on interface of multilayered-perovskite systems

Aberration-corrected TEM studies on interface of multilayered-perovskite systems Aberration-corrected TEM studies on interface of multilayered-perovskite systems By Lina Gunawan (0326114) Supervisor: Dr. Gianluigi Botton November 1, 2006 MSE 702(1) Presentation Outline Literature Review

More information

Introduction to Accelerator Physics Part 1

Introduction to Accelerator Physics Part 1 Introduction to Accelerator Physics Part 1 Pedro Castro / Accelerator Physics Group (MPY) Introduction to Accelerator Physics DESY, 28th July 2014 Pedro Castro / MPY Accelerator Physics 28 th July 2014

More information

Chapter 12. Nanometrology. Oxford University Press All rights reserved.

Chapter 12. Nanometrology. Oxford University Press All rights reserved. Chapter 12 Nanometrology Introduction Nanometrology is the science of measurement at the nanoscale level. Figure illustrates where nanoscale stands in relation to a meter and sub divisions of meter. Nanometrology

More information

Local Anodic Oxidation with AFM: A Nanometer-Scale Spectroscopic Study with Photoemission Microscopy

Local Anodic Oxidation with AFM: A Nanometer-Scale Spectroscopic Study with Photoemission Microscopy Local Anodic Oxidation with AFM: A Nanometer-Scale Spectroscopic Study with Photoemission Microscopy S. Heun, G. Mori, M. Lazzarino, D. Ercolani,* G. Biasiol, and L. Sorba* Laboratorio Nazionale TASC-INFM,

More information

CHARACTERIZATION of NANOMATERIALS KHP

CHARACTERIZATION of NANOMATERIALS KHP CHARACTERIZATION of NANOMATERIALS Overview of the most common nanocharacterization techniques MAIN CHARACTERIZATION TECHNIQUES: 1.Transmission Electron Microscope (TEM) 2. Scanning Electron Microscope

More information

Dalton Cumbrian Facility. A state-of-the-art national user facility for nuclear research and development.

Dalton Cumbrian Facility. A state-of-the-art national user facility for nuclear research and development. Dalton Cumbrian Facility A state-of-the-art national user facility for nuclear research and development Dalton Cumbrian Facility The University of Manchester has established the world-leading Dalton Cumbrian

More information

Plasma Spectroscopy in ISTTOK

Plasma Spectroscopy in ISTTOK Plasma Spectroscopy in ISTTOK J. Figueiredo 1, R. B. Gomes 1, T. Pereira 1, H. Fernandes 1, A. Sharakovski 2 1 Associação EURATOM/IST, Centro de Fusão Nuclear, IST, 1049-001 Lisboa, Portugal 2 Association

More information

Information on the test material EDS-TM002 and the BAM software package EDX Spectrometer Test for determination of the spectrometer performance

Information on the test material EDS-TM002 and the BAM software package EDX Spectrometer Test for determination of the spectrometer performance BAM 6.8 8.5.213 Information on the test material EDS-TM2 and the BAM software package EDX Spectrometer Test for determination of the spectrometer performance 1. Introduction Energy dispersive spectrometers

More information

Chemical Analysis in TEM: XEDS, EELS and EFTEM. HRTEM PhD course Lecture 5

Chemical Analysis in TEM: XEDS, EELS and EFTEM. HRTEM PhD course Lecture 5 Chemical Analysis in TEM: XEDS, EELS and EFTEM HRTEM PhD course Lecture 5 1 Part IV Subject Chapter Prio x-ray spectrometry 32 1 Spectra and mapping 33 2 Qualitative XEDS 34 1 Quantitative XEDS 35.1-35.4

More information

V.Storizhko Institute of Applied Physics, National Academy of Sciences of Ukraine

V.Storizhko Institute of Applied Physics, National Academy of Sciences of Ukraine IAP accelerator based facility for simulation and studies of radiation induced defects in materials V.Storizhko Institute of Applied Physics, National Academy of Sciences of Ukraine IAEA Technical Meeting

More information

AMS MEASUREMENTS OF DEUTERIUM CAPTURED IN TUNGSTEN LAYERS DEPOSITED BY MAGNETRON SPUTTERING

AMS MEASUREMENTS OF DEUTERIUM CAPTURED IN TUNGSTEN LAYERS DEPOSITED BY MAGNETRON SPUTTERING Romanian Reports in Physics, Vol. 65, No. 4, P. 1258 1264, 2013 AMS MEASUREMENTS OF DEUTERIUM CAPTURED IN TUNGSTEN LAYERS DEPOSITED BY MAGNETRON SPUTTERING A.R. PETRE 1,3, T. ACSENTE 2, M. ENACHESCU 1,

More information

Microscopy: Principles

Microscopy: Principles Low Voltage Electron Microscopy: Principles and Applications Edited by David C. Bell Harvard University, USA and Natasha Erdman JEOL USA Inc., USA Published in association with the Royal Microscopical

More information

The intense positron source EPOS at Research Center Rossendorf

The intense positron source EPOS at Research Center Rossendorf The intense positron source EPOS at Research Center Rossendorf R. Krause-Rehberg 1, G. Brauer 2, S. Sachert 1, A. Krille 1, V. Bondarenko 1 1 -Wittenberg 2 FZ Rossendorf Martin-Luther-Universität RK Halle

More information

A Project for High Fluence 14 MeV Neutron Source

A Project for High Fluence 14 MeV Neutron Source A Project for High Fluence 14 MeV Neutron Source Mario Pillon 1, Maurizio Angelone 1, Aldo Pizzuto 1, Antonino Pietropaolo 1 1 Associazione ENEA-EURATOM Sulla Fusione, ENEA C.R. Frascati, via E. Fermi,

More information

Free Electron Laser. Project report: Synchrotron radiation. Sadaf Jamil Rana

Free Electron Laser. Project report: Synchrotron radiation. Sadaf Jamil Rana Free Electron Laser Project report: Synchrotron radiation By Sadaf Jamil Rana History of Free-Electron Laser (FEL) The FEL is the result of many years of theoretical and experimental work on the generation

More information

2D Materials Research Activities at the NEST lab in Pisa, Italy. Stefan Heun NEST, Istituto Nanoscienze-CNR and Scuola Normale Superiore, Pisa, Italy

2D Materials Research Activities at the NEST lab in Pisa, Italy. Stefan Heun NEST, Istituto Nanoscienze-CNR and Scuola Normale Superiore, Pisa, Italy 2D Materials Research Activities at the NEST lab in Pisa, Italy Stefan Heun NEST, Istituto Nanoscienze-CNR and Scuola Normale Superiore, Pisa, Italy 2D Materials Research Activities at the NEST lab in

More information

New Concept of EPOS Progress of the Mono-energetic Positron Beam (MePS) Gamma-induced Positron Spectroscopy (GiPS)

New Concept of EPOS Progress of the Mono-energetic Positron Beam (MePS) Gamma-induced Positron Spectroscopy (GiPS) Progress of the EPOS Project: Gamma Induced Positron Spectroscopy (GiPS) R. Krause-Rehberg 1,*,W.Anwand 2,G.Brauer 2, M. Butterling 1,T.Cowan 2,M. Jungmann 1, A. Krille 1, R. Schwengner 2, A. Wagner 2

More information

Transmission Electron Microscopy

Transmission Electron Microscopy L. Reimer H. Kohl Transmission Electron Microscopy Physics of Image Formation Fifth Edition el Springer Contents 1 Introduction... 1 1.1 Transmission Electron Microscopy... 1 1.1.1 Conventional Transmission

More information

EBSS: Hands-on Activity #8. Operation of an electromagnetic isotope separator (EMIS) Dan Stracener Jon Batchelder

EBSS: Hands-on Activity #8. Operation of an electromagnetic isotope separator (EMIS) Dan Stracener Jon Batchelder EBSS: Hands-on Activity #8 Operation of an electromagnetic isotope separator (EMIS) Dan Stracener Jon Batchelder Schematic of RIB Production at the HRIBF ISOL: Isotope Separation On-Line 2 Managed by UT-Battelle

More information

Title: Ultrafast photocurrent measurement of the escape time of electrons and holes from

Title: Ultrafast photocurrent measurement of the escape time of electrons and holes from Title: Ultrafast photocurrent measurement of the escape time of electrons and holes from carbon nanotube PN junction photodiodes Authors: Nathaniel. M. Gabor 1,*, Zhaohui Zhong 2, Ken Bosnick 3, Paul L.

More information

IN THE NAME OF ALLAH, THE MOST MERCIFUL AND COMPASSIONATE

IN THE NAME OF ALLAH, THE MOST MERCIFUL AND COMPASSIONATE IN THE NAME OF ALLAH, THE MOST MERCIFUL AND COMPASSIONATE Ion Beam Analysis of Diamond Thin Films Sobia Allah Rakha Experimental Physics Labs 04-03-2010 Outline Diamond Nanostructures Deposition of Diamond

More information

Structure of MLL Tandem operation Experiments

Structure of MLL Tandem operation Experiments Maier-Leibnitz-Laboratorium Tandem Operation and Experiments Structure of MLL Tandem operation Experiments Dr. L. Beck 1 Maier-Leibnitz-Laboratorium MP 8-1970 Am Coulombwall 6 85748 Garching Germany Tel.

More information

SRF GUN CHARACTERIZATION - PHASE SPACE AND DARK CURRENT MEASUREMENTS AT ELBE*

SRF GUN CHARACTERIZATION - PHASE SPACE AND DARK CURRENT MEASUREMENTS AT ELBE* SRF GUN CHARACTERIZATION - PHASE SPACE AND DARK CURRENT MEASUREMENTS AT ELBE* E. Panofski #, A. Jankowiak, T. Kamps, Helmholtz-Zentrum Berlin, Berlin, Germany P.N. Lu, J. Teichert, Helmholtz-Zentrum Dresden-Rossendorf,

More information

Black phosphorus: A new bandgap tuning knob

Black phosphorus: A new bandgap tuning knob Black phosphorus: A new bandgap tuning knob Rafael Roldán and Andres Castellanos-Gomez Modern electronics rely on devices whose functionality can be adjusted by the end-user with an external knob. A new

More information

Accelerator Physics, BAU, First Semester, (Saed Dababneh).

Accelerator Physics, BAU, First Semester, (Saed Dababneh). Accelerator Physics 501503746 Course web http://nuclear.bau.edu.jo/accelerators/ edu or http://nuclear.dababneh.com/accelerators/ com/accelerators/ 1 Grading Mid-term Exam 25% Projects 25% Final Exam 50%

More information

4H SiC Schottky diodes under ESD and thermal stresses: A failure analysis method.

4H SiC Schottky diodes under ESD and thermal stresses: A failure analysis method. 4H SiC Schottky diodes under ESD and thermal stresses: A failure analysis method. Pascal DHERBECOURT Groupe de Physique des Matériaux UMR CNRS 6634 The first part of the presentation reports electrical

More information

Fadei Komarov Alexander Kamyshan

Fadei Komarov Alexander Kamyshan Fadei Komarov Alexander Kamyshan Institute of Applied Physics Problems, Belarusian State University, Minsk, Belarus KomarovF@bsu.by Tasks and Objects 2 Introduction and motivation Experimental setup designed

More information

NUCL 3000/5030 Laboratory 2 Fall 2013

NUCL 3000/5030 Laboratory 2 Fall 2013 Lab #2: Passive Gamma Spec Measurements in Decoding Natural Radioactivity in SLC Area Objectives a. Learn basics of gamma spectroscopy b. Learn the equipment in Counting stations #4, #5 and #8 c. Apply

More information

First steps towards a target laboratory at GANIL

First steps towards a target laboratory at GANIL First steps towards a target laboratory at GANIL C. Stodel, G. Frémont, G. Auger, C. Spitaels To cite this version: C. Stodel, G. Frémont, G. Auger, C. Spitaels. First steps towards a target laboratory

More information

h p λ = mν Back to de Broglie and the electron as a wave you will learn more about this Equation in CHEM* 2060

h p λ = mν Back to de Broglie and the electron as a wave you will learn more about this Equation in CHEM* 2060 Back to de Broglie and the electron as a wave λ = mν h = h p you will learn more about this Equation in CHEM* 2060 We will soon see that the energies (speed for now if you like) of the electrons in the

More information

6. Analytical Electron Microscopy

6. Analytical Electron Microscopy Physical Principles of Electron Microscopy 6. Analytical Electron Microscopy Ray Egerton University of Alberta and National Institute of Nanotechnology Edmonton, Canada www.tem-eels.ca regerton@ualberta.ca

More information

A new detector for neutron beam monitoring

A new detector for neutron beam monitoring A new detector for neutron beam monitoring European Organization for Nuclear Research (CERN), Geneva, Switzerland in collaboration with Commissariat à l Energie Atomique (CEA), Saclay, France, Instituto

More information

Novel materials and nanostructures for advanced optoelectronics

Novel materials and nanostructures for advanced optoelectronics Novel materials and nanostructures for advanced optoelectronics Q. Zhuang, P. Carrington, M. Hayne, A Krier Physics Department, Lancaster University, UK u Brief introduction to Outline Lancaster University

More information

The accelerators at LNS - INFN and diagnostics aspects of the radioactive beams

The accelerators at LNS - INFN and diagnostics aspects of the radioactive beams The accelerators at LNS - INFN and diagnostics aspects of the radioactive beams L. Cosentino, P. Finocchiaro, A. Pappalardo LNS INFN Catania J. Harasimowicz Univ. of Liverpool Cockroft Institute LNS INFN

More information

Research Center Dresden Rossendorf

Research Center Dresden Rossendorf News of the EPOS Project at the ELBE Radiation Source in the Research Center Dresden Rossendorf EPOS-Team & R. Krause-Rehberg Extended Concept of EPOS Progress of the mono-energetic Positron Beam (MePS)

More information

Time-Resolved μ-xrf and Elemental Mapping of Biological Materials

Time-Resolved μ-xrf and Elemental Mapping of Biological Materials 296 Time-Resolved μ-xrf and Elemental Mapping of Biological Materials K. Tsuji 1,2), K. Tsutsumimoto 1), K. Nakano 1,2), K. Tanaka 1), A. Okhrimovskyy 1), Y. Konishi 1), and X. Ding 3) 1) Department of

More information

SLS Symposium on X-Ray Instrumentation

SLS Symposium on X-Ray Instrumentation SLS Symposium on X-Ray Instrumentation Tuesday, December 7, 2010 10:00 to 12:15, WBGB/019 10:00 The optics layout of the PEARL beamline P. Oberta, U. Flechsig and M. Muntwiler 10:30 Instrumentation for

More information

Applications of Nuclear Analytical Techniques in Geoscience

Applications of Nuclear Analytical Techniques in Geoscience Applications of Nuclear Analytical Techniques in Geoscience J. Aspiazu a,1, J. López a, J. Ramírez a, M. E. Montero b, P. Villaseñor a a Intituto Nacional de Investigaciones Nucleares (ININ), Carretera

More information

VERDI a double (v, E) fission-fragment fragment spectrometer

VERDI a double (v, E) fission-fragment fragment spectrometer EFNUDAT Slow and Resonance Neutrons, Budapest (HU), Sep. 23-25, 2009 1 VERDI a double (v, E) fission-fragment fragment spectrometer S. Oberstedt, R. Borcea,, Th. Gamboni,, W. Geerts, F.-J. Hambsch, A.

More information