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Mev Amp published presentations and documents on DocSlides.

1 01/10/2018 Physics at the

1 01/10/2018 Physics at the

  • piper
  • 41 Slides

FCCs. a story of . synergy. and . complementarity...

Module 1 Why linear accelerators

Module 1 Why linear accelerators

  • emily
  • 30 Slides

Basic linac structure. Acceleration in periodic st...

Beta Decay – General Principles

Beta Decay – General Principles

  • elena
  • 92 Slides

Paul Mantica. Lecture 1. Euroschool. for Exotic B...

Atanu Maulik Center for

Atanu Maulik Center for

  • mackenzie
  • 27 Slides

Astroparticle. Physics and Space Science. Bose In...

Noble Element Detectors Michelle Stancari

Noble Element Detectors Michelle Stancari

  • obrien
  • 49 Slides

EDIT 2018. Michelle Stancari | Noble Element Det...

BINGO: B i- I sotope 0 ν

BINGO: B i- I sotope 0 ν

  • delcy
  • 15 Slides

2. β. . N. ext . G. eneration . O. bservatory. H...

David Morrissey Facility for Rare Isotope Beams

David Morrissey Facility for Rare Isotope Beams

  • bella
  • 49 Slides

18 September 2014. Production of Unstable Nuclei f...

NSDD LBNL Isotopes Project Collaboration Report

NSDD LBNL Isotopes Project Collaboration Report

  • jones
  • 16 Slides

Richard B. Firestone. Isotopes Project, Lawrence B...

Shell-model studies of the

Shell-model studies of the

  • isla
  • 37 Slides

. astrophysical mirror . rp. -reactions . 34. S(p,...

Accelerator Driven Subcritical Reactors

Accelerator Driven Subcritical Reactors

  • murphy
  • 14 Slides

Introduction:. Fission.. Conventional reactor.. Fa...

Hadron Resonance Gas Model : Freeze-out, Criticality and Fluctuations

Hadron Resonance Gas Model : Freeze-out, Criticality and Fluctuations

  • catherine
  • 28 Slides

Bedanga. Mohanty. NISER. (With STAR Collaborators...

2 Physics Beyond Colliders

2 Physics Beyond Colliders

  • ashley
  • 18 Slides

2016. Klaus . Blaum. , MPI . for. . Nuclear. . P...

Outline: Future UNILAC experiments

Outline: Future UNILAC experiments

  • jocelyn
  • 37 Slides

Lecturer:. . Hans-Jürgen . Wollersheim. e-mail: ...

High Power Linacs 3.5 MW

High Power Linacs 3.5 MW

  • okelly
  • 21 Slides

beam. . power. 1979. What. do . we. . call. as...

Interactions of particles with Matter

Interactions of particles with Matter

  • susan2
  • 63 Slides

Alfredo Ferrari,. CERN, Geneva. Vösendorf. , May ...

THE 16 th VIENNA CONFERENCE ON INSTRUMENTATION

THE 16 th VIENNA CONFERENCE ON INSTRUMENTATION

  • ava
  • 17 Slides

21 – 25 FEBRUARY 2022. ONLINE. Studies of LGAD p...

A CMOS Active Pixel Sensor for

A CMOS Active Pixel Sensor for

  • anastasia
  • 27 Slides

high resolution imaging of. the Jovian system. Mat...

Supported by the U.S. Department of Energy, Office

Supported by the U.S. Department of Energy, Office

  • phoebe
  • 12 Slides

of Fusion Energy Sciences. Roger E. Stoller (retir...

Looking for states analogous to the

Looking for states analogous to the

  • phoebe
  • 20 Slides

12. C Hoyle state in heavier nuclei . Marina . Bar...

A Reverse 230 U/ 226 Th Radionuclide Generator for Targeted Alpha Therapy Applications

A Reverse 230 U/ 226 Th Radionuclide Generator for Targeted Alpha Therapy Applications

  • claire
  • 15 Slides

August 23. rd. , 2022. LA-UR-18-28992. T.E. Mastre...

NDIAWG - Nonproliferation Scoping Studies

NDIAWG - Nonproliferation Scoping Studies

  • brooke
  • 14 Slides

(. a. ,n) Nuclear Data Scoping Study. Catherine Ro...

A New Proton Low Altitude Radiation Belt (LARB) Model

A New Proton Low Altitude Radiation Belt (LARB) Model

  • paige
  • 18 Slides

D. . Heynderickx. DH Consultancy, Leuven, Belgium....

The Neutrino Anomalies NS2016

The Neutrino Anomalies NS2016

  • danya
  • 23 Slides

Outline. The 3. n. oscillation framework. The cur...

Benchmark calculation of the PHITS code for neutron attenuation in iron and concrete on shielding e

Benchmark calculation of the PHITS code for neutron attenuation in iron and concrete on shielding e

  • eliza
  • 38 Slides

Norihiro. Matsuda. 1. , Yosuke Iwamoto. 1. , . Ta...

THE BERYLLIUM ANOMALY AND NEW PHYSICS

THE BERYLLIUM ANOMALY AND NEW PHYSICS

  • melody
  • 34 Slides

Invisibles/. Elusives. Network. Jonathan . Feng. ...

Neutrinoless Double Beta Decay – Status and Plans

Neutrinoless Double Beta Decay – Status and Plans

  • esther
  • 25 Slides

FNAL PAC 20 June 2016. Caveats. I am n...

7/23/2015 1 NN 2015, Md. Moin Shaikh SRF, SINP

7/23/2015 1 NN 2015, Md. Moin Shaikh SRF, SINP

  • ivy
  • 17 Slides

Measurement of fusion excitation function for . 7....

RADNEXT Work Package 10 Proton and Heavy-Ion Facilities

RADNEXT Work Package 10 Proton and Heavy-Ion Facilities

  • erica
  • 15 Slides

1. Françoise BEZERRA, CNES, France (WP Leader), ....

Chapter 2. Radiation

Chapter 2. Radiation

  • joyce
  • 91 Slides

Radioactivity. 2.Radiation interaction with Matter...

Directional x-ray radiation

Directional x-ray radiation

  • jalin
  • 20 Slides

produced by plasma magneto-static . undulator. pro...

Exploring an updated evaluation methodology at the example of

Exploring an updated evaluation methodology at the example of

  • layla
  • 30 Slides

an iron evaluation. . Georg Schnabel. Nuclear D...

Status and hadron physics program

Status and hadron physics program

  • claire
  • 35 Slides

of. . J-PARC. K. Ozawa (KEK). Contents. Status of...

Isospin Effects in Dissipative

Isospin Effects in Dissipative

  • ivy
  • 27 Slides

Reactions. Maria Colonna. . IN. F. N. - Labora...

Accelerators and Sources

Accelerators and Sources

  • joanne
  • 16 Slides

Report from Discussion Session. Jose Alonso. 1. Ch...

Namur Research Institute for Life Science

Namur Research Institute for Life Science

  • kylie
  • 26 Slides

IN VITRO RADIOBIOLOGY AND RELATED TOPICS:. descrip...

Investigation of Strangeness Photo-Production

Investigation of Strangeness Photo-Production

  • zoe
  • 62 Slides

near the Threshold. Masashi Kaneta . for the NKS2 ...

Beams of the “lightest radionuclide useful for hadron therapy”:

Beams of the “lightest radionuclide useful for hadron therapy”:

  • delilah
  • 33 Slides

neutron beams for BNCT. Maria Pedrosa. 1,2. , . Ig...

The TALYS nuclear model code I

The TALYS nuclear model code I

  • hailey
  • 50 Slides

. Arjan Koning. . . Nuclear Data Section, NAPC....

(Some) Open Issues in Nuclear modeling for (General Purpose) (Monte Carlo) Numerical Simulations

(Some) Open Issues in Nuclear modeling for (General Purpose) (Monte Carlo) Numerical Simulations

  • amey
  • 54 Slides

A.Ferrari. Catania, November 2012. CERN, . Geneva....

Predicting cell death and mutation frequency for a wide spectrum of LET by assuming DNA break clust

Predicting cell death and mutation frequency for a wide spectrum of LET by assuming DNA break clust

  • eliza
  • 21 Slides

domains. Ianik Plante. 1. , Eloise . Pariset. 2,3....

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