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Exotic nuclei and drip lines
Exotic nuclei and drip lines
by WhereTheWildThingsAre
Part I. . Unstable. vs. . stable. nuclei: . neu...
γ - ray spectroscopy γ
γ - ray spectroscopy γ
by GymRat
-decay is an . electromagnetic process . where the...
Proposal for uranium micro-beam linac at the APS for reactor fuel and structural materials studies
Proposal for uranium micro-beam linac at the APS for reactor fuel and structural materials studies
by Sunshine
1 MeV/u heavy ions up to uranium includes “fissi...
5/1/2012 PHY 114 A Spring 2012 -- Lecture 26
5/1/2012 PHY 114 A Spring 2012 -- Lecture 26
by BabyDoll
1. PHY 114 A General Physics II. 11 AM-12:15 . P. ...
 Isotope Production at European Spallation Source
 Isotope Production at European Spallation Source
by HappyHippie
A potential new access to neutrons.  . Yong. . J...
ANALYSIS OF VELOCITY AND ISOTOPE DISTRIBUTIONS IN PROJECTILE FRAGMENTATION REACTIONS OF
ANALYSIS OF VELOCITY AND ISOTOPE DISTRIBUTIONS IN PROJECTILE FRAGMENTATION REACTIONS OF
by FriendlyFox
18. O AT 35 MEV/NUCLEON ON . 9. BE AND . 181. TA T...
Lepton flavour violation experiments with
Lepton flavour violation experiments with
by anastasia
muon. beams. Fabrizio. . Cei. INFN . &. . U...
Chemical abundances near the surface of AGB stars
Chemical abundances near the surface of AGB stars
by ella
Shuya Ota. Cyclotron Institute. 2/28/2020 . Joint ...
Potential Description of
Potential Description of
by oryan
a+. 208. Pb Elastic Scattering. M . Nure. . Alam....
1 01/10/2018 Physics at the
1 01/10/2018 Physics at the
by piper
FCCs. a story of . synergy. and . complementarity...
future production of
future production of
by eve
medical radioisotopes. Sytze Brandenburg. 99Mo. 18...
Module 1 Why linear accelerators
Module 1 Why linear accelerators
by emily
Basic linac structure. Acceleration in periodic st...
Beta Decay – General Principles
Beta Decay – General Principles
by elena
Paul Mantica. Lecture 1. Euroschool. for Exotic B...
Atanu Maulik Center for
Atanu Maulik Center for
by mackenzie
Astroparticle. Physics and Space Science. Bose In...
Noble Element Detectors Michelle Stancari
Noble Element Detectors Michelle Stancari
by obrien
EDIT 2018. Michelle Stancari | Noble Element Det...
BINGO: B i- I sotope 0 ν
BINGO: B i- I sotope 0 ν
by delcy
2. β. . N. ext . G. eneration . O. bservatory. H...
David Morrissey Facility for Rare Isotope Beams
David Morrissey Facility for Rare Isotope Beams
by bella
18 September 2014. Production of Unstable Nuclei f...
NSDD LBNL Isotopes Project Collaboration Report
NSDD LBNL Isotopes Project Collaboration Report
by jones
Richard B. Firestone. Isotopes Project, Lawrence B...
Shell-model studies of the
Shell-model studies of the
by isla
. astrophysical mirror . rp. -reactions . 34. S(p,...
Accelerator Driven Subcritical Reactors
Accelerator Driven Subcritical Reactors
by murphy
Introduction:. Fission.. Conventional reactor.. Fa...
Pakistan Dr. Shabana Saeed
Pakistan Dr. Shabana Saeed
by mila-milly
Prof, Head, . Dept. of Medical Sciences. Pakistan...
Hadron Resonance Gas Model : Freeze-out, Criticality and Fluctuations
Hadron Resonance Gas Model : Freeze-out, Criticality and Fluctuations
by catherine
Bedanga. Mohanty. NISER. (With STAR Collaborators...
2 Physics Beyond Colliders
2 Physics Beyond Colliders
by ashley
2016. Klaus . Blaum. , MPI . for. . Nuclear. . P...
Outline: Future UNILAC experiments
Outline: Future UNILAC experiments
by jocelyn
Lecturer:. . Hans-Jürgen . Wollersheim. e-mail: ...
High Power Linacs 3.5 MW
High Power Linacs 3.5 MW
by okelly
beam. . power. 1979. What. do . we. . call. as...
Interactions of particles with Matter
Interactions of particles with Matter
by susan2
Alfredo Ferrari,. CERN, Geneva. Vösendorf. , May ...
Beam Injection and Capture
Beam Injection and Capture
by natalie
Chandra Bhat. Fermilab. Acknowledgements. W. . Pel...
THE 16 th VIENNA CONFERENCE ON INSTRUMENTATION
THE 16 th VIENNA CONFERENCE ON INSTRUMENTATION
by ava
21 – 25 FEBRUARY 2022. ONLINE. Studies of LGAD p...
A CMOS Active Pixel Sensor for
A CMOS Active Pixel Sensor for
by anastasia
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
by phoebe
of Fusion Energy Sciences. Roger E. Stoller (retir...
Systematic analysis of inelastic alpha scattering off self-conjugate A = 4n nuclei
Systematic analysis of inelastic alpha scattering off self-conjugate A = 4n nuclei
by ximena
Satoshi Adachi. Research Center for Nuclear Physic...
Looking for states analogous to the
Looking for states analogous to the
by phoebe
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
by claire
August 23. rd. , 2022. LA-UR-18-28992. T.E. Mastre...
NDIAWG - Nonproliferation Scoping Studies
NDIAWG - Nonproliferation Scoping Studies
by brooke
(. 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
by paige
D. . Heynderickx. DH Consultancy, Leuven, Belgium....
The Neutrino Anomalies NS2016
The Neutrino Anomalies NS2016
by danya
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
by eliza
Norihiro. Matsuda. 1. , Yosuke Iwamoto. 1. , . Ta...
THE BERYLLIUM ANOMALY AND NEW PHYSICS
THE BERYLLIUM ANOMALY AND NEW PHYSICS
by melody
Invisibles/. Elusives. Network. Jonathan . Feng. ...
Neutrinoless Double Beta Decay – Status and Plans
Neutrinoless Double Beta Decay – Status and Plans
by esther
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
by ivy
Measurement of fusion excitation function for . 7....