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

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1 1 IAP NAN of Ukraine activity in field of High Energy Physics. Possible areas of cooperation in frame of PICS and beyond.

2 Institute of Applied Physics National Academy of Sciences of Ukraine 2 The Institute of Applied Physics (IAP), National Academy of Sciences of Ukraine (NAS of Ukraine), was established in 1991 to enlarge the fundamental and applied researches in nuclear physics. IAP NAS of Ukraine is a part of the Department of Nuclear Physics and Power Engineering, g, NAS of Ukraine. IAP NAN of Ukraine activity in field of High Energy Physics.

3 Institute of Applied Physics National Academy of Sciences of Ukraine 3 The main areas of research: Quantum electrodynamics in strong fields; Modeling of radiation effects and microstructural transformations in constructional materials; Studies of low-energy ion and electron interactions with matter; Development of electrostatic accelerator-based instrumentation for analysis of material structure and composition with submicron lateral resolution; Molecular radiation biophysics; Development of equipment for research and education.

4 Institute of Applied Physics National Academy of Sciences of Ukraine 4 The main experimental facilities at the IAP includes: Microanalytical facility: Ion luminescence channel, resonant nuclear reactions channel; scanning microprobe channel with 2 µm spatial resolution; RBS, PIXE, PIGE channels; ERDA channel with electrostatic spectrometer; X-ray quasimonochromatic source. User facility Based on Tandetron 1.0 MV, 4110Bo-AMS, HVEE. There are seven departments at the Institute: Department of Charged Particle Beam Physics. Department of Radiation Biophysics. Department of Nuclear Research. Department of Quantum Electrodynamics of Strong Fields. Department of Physical Methods of Ore Analysis. Department of Modeling of Radiation Effects and Microstructural Transformations in Constructional Materials. Research Center of Equipment for Education and Research.

5 QED test in strong fields 5 - Resonant and non-resonant QED processes in the strong pulsed laser field (PHELIX, XFEL) - Resonant and non-resonant QED processes in strong magnetic field between colliding nuclei, in particular, electron-positron pair production

6 Schrödinger equation QED test in strong fields H = Gs 6 i Ψ=αe β Equations for α, β : i 2 Ψ = ( + V) Ψ t 2m ρ + divρυ = 0 t υ 1 + ( υ ) υ = ( V B + V ) t m m 2mα Bohm potential ρ = α = Ψ, υ = β, V B = α Z e 1 e + Z 2 L = cm e - e + pair between colliding nuclei E.Madelung, Quantentheorie in hydrodynamischer form // Zeitschr. für Phys. 40, 322 (1926) E. Madelung

7 Electron cooling of charged particles theory 7 - Electron cooling of antiproton theory In the second Born approximation ( 1) ( 2) W = W + W k k k Analytical formulas de 2 ~ q dt Feynman diagram of the second Born approximation

8 Multiscale simulation 8 Radiation damage is inherently multiscale with interacting phenomena ranging from ps to decades and from nm to m.

9 Collaboration between CERN & IAP NAS of Ukraine 9 Compact LInear Collider (CLIC) is future electron-positron linear collider with center of mass energy 3 TeV. 3 TeV of center mass energy & accelerating ggradient 100 MV/m

10 Impurity determination at copper samples using thermal desorption, ERDA & RBS 10 S a m p l e Layer No.1 Layer No.2 Layer No.3 Layer No.4 Layer No.5 Depth No. of layer The width of Cu, H, layer, at. % at. at/cm 2 % <1 - C, at. % The energy spectra analysis shown the availability of film with thickness from at/cm 2 to at/cm 2 with high hydrogen content (27 at.%).

11 Optical spectroscopy of breakdown 11 Experimental setup The scheme of setup for optical spectroscopy of breakdowns, based on DC-spark system at CERN Results A comparison of the optical spectra for 20 consecutive breakdowns at the same spot.

12 DC spark system construction for further study of breakdowns parameters 12 at CERN at IAP NASU The main aim: testing the breakdown field strength of different kinds of materials in order to speed up the validation of different materials for rf structures. Vacuum level: mbar Max voltage: 12 kv Usual gap distance: 20 µm Vacuum chambers with electrodes The main aim: testing the breakdown field strength of samples after plasma and ion treatment, measuring work function of material after such treatment. Vacuum level: 10-5 mbar (will be improve) Max voltage: 70 kv Gap distance which h can be set as usual : 150 µm

13 2 MeV microanalytical facility 13 Ion luminescence channel, resonant nuclear reactions channel; scanning microprobe channel with 2 µm spatial resolution; RBS, PIXE, PIGE channels; ERDA channel with electrostatic spectrometer; X-ray quasimonochromatic source, defectoscopy channel (channeling, e - e + annihilation)

14 Scanning Nuclear Microprobe 14 Beams: H+, He+ with energy MeV Resolution: 2 µm with current 100 pa Analytical techniques: µpixe, µrbs, IBIC A new type of active ion optical Mapping of chemical elements distribution in zone of joint of element, an integrated doublet solid phase bounding of heterogeneous materials (stainless or quadrupole lenses steel -copper). Zone dimensions μm 2

15 Novel ERDA and RBS facility: beamline, scattering chamber and electrostatic spectrometer 15 High resolution elastic scattering channel is intended for non-destructive quantitative determination of hydrogen and its depth distribution in the sample material by recoil nuclei method. The main advantages The vacuum in the scattering chamber is 10-7 Pa, that makes contamination of samples impossible during the experiment. The limit of detection of hydrogen is about 10 ppm. It allows the exploration of the hydrogen content in metals, where it is present in trace amounts. The relative energy spread is , which is an order of magnitude higher than when using standard silicon surface-barrier detector.

16 Monochromatic x-ray source on the basis of electrostatic proton accelerator 16 The main advantages The combination of high-currenth low-energy proton beam with the radiation generation chamber allowed obtaining very intense source of monochromatic X-rays with low background and high monochromaticity. Areas of Application Determination of elements in the surface layers of structural materials and biomaterials by XRF and µxrf methods, study of the radiation influence on individual cells.

17 High-sensitivity isotope mass-spectrometer 17 AMS facility (model 4110Bo-AMS) is a 1 MV Tandetron, multielement machine designed to be able to detect not only low-mass isotopes such as 10Be, 14C and 26Al, but also heavy elements such as 129I. This type spectrometer was used to analyze the Shroud of Turin.

18 Development of equipment for research 18 Magnetic field diagnostics system High Intense non-cesium H - Ion Source Possible cooperation - IAP NASU is a participant of TESHEP since Ukrainian-French technology park is planned to create at the IAP NASU and SELMY Company - Manufacturing equipment components for accelerators - Ion beam irradiation of prototypes of electronics for LHC upgrade - Visit of our young researchers to LAL workshop and to Yanus experiment (Saclay), October International mobility of researchers, Marie Skłodowska Curie Actions (Horizon2020)

19 Thank you for attention! Adress: Institute of Applied Physics NAS of Ukraine 58 Petropavlivska St., 40000, Sumy, Ukraine Phone: +38 (0542) Fax: +38 (0542) web-page: iap.sumy.org

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