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Extraction of the Landau-Migdal Parameter from the Gamow-Teller Giant Resonance in ^{132}SnA search for deeply bound kaonic nuclear statesDiscovery of a strange tribaryon S0(3115) in 4He(stopped K − , p ) reactionWell Developed Deformation inSi42How Robust is the N=34 Subshell Closure? First Spectroscopy of Ar52S17(0) determined from the Coulomb breakup of 83 MeV /nucleon 8BDirect evidence for the breakdown of the N = 8 shell closure in 12BeAnomalously hindered E2 strength B(E2;2+(1)-->0+) in 16CDecay property of 20Na for the onset mechanism of the rapid-proton processSpectroscopic study of neutron shell closures via nucleon transfer in the near-dripline nucleus 23OObservation of strong low-lying E1 strength in the two-neutron halo nucleus 11LiDecay pattern of pygmy states observed in neutron-rich 26NeDevelopment of large deformation in 62CrHalo structure of the island of inversion nucleus 31NeSpectroscopy of 32Ne and the "Island of Inversion"Hindered proton collectivity in 16(28)S12: possible magic number at Z=16N=16 spherical shell closure in ^{24}oDeformation-driven p-wave halos at the drip line: 31NeObservation of a p-wave one-neutron halo configuration in (37)MgNucleus ^{26}O: A Barely Unbound System beyond the Drip LineFirst Observation of ^{20}B and ^{21}BQuasifree Neutron Knockout from ^{54}Ca Corroborates Arising N=34 Neutron Magic NumberLocation of the Neutron Dripline at Fluorine and Neon
P50
Q57490450-AD167881-D554-440C-84DD-39E38775EE50Q57840830-EA3A75D4-AA32-42C5-BE0B-BAFF7B7EF971Q57840871-13324FF1-42DD-449A-ABE5-18B49C4790C5Q60529128-A7870682-F9F3-4201-96A7-996521EC464BQ63388184-862394ED-9968-494C-83C0-D8F3DBC6DF3FQ73718365-E4F56BB1-A745-4E96-880C-644CE24BB88FQ74324153-EB2DD077-17F3-4BF8-954D-5F11C906F04FQ76397602-595BC355-E92D-4BE5-AA93-BAD8283D70A1Q78091337-9B478815-0A7D-4648-8CBF-FF7FA1E24244Q79941159-C62C7F10-9B80-4EC4-8247-5737FB12F1ABQ80106844-AC97DA8F-4F02-4858-BD41-978BB54DE645Q83113810-C11F9134-CFB2-4F8E-B56D-2D609D893E3FQ83417339-633A22CF-1DE8-4E31-9163-4687133190FDQ83995864-596FEDA8-1B48-47E6-B0D6-D952235F9D22Q84359086-4E8AF0AD-7830-4BE1-BBCD-26E23AD5AA43Q87359396-AD6C7F78-4617-4859-894F-7A8D6C814FC2Q87403200-FC42A0E8-AB9C-487B-BF98-D0EE56A7D392Q87752748-5BCC238E-4843-455D-B584-D7613CE769A4Q88219613-AC990380-5C54-4BF9-A88E-D93BDC0060B9Q89064369-AA7C44E4-1A35-493C-95BC-965ED51B3BB6Q91014844-5CD27179-17B6-4F84-B1CE-6C9FEA085F2EQ91184712-1DF02543-BEDE-4492-B0F7-E04D98A7ADE7Q91754636-D2FFDB41-D574-4DD6-962F-E6A9849C5C64
P50
description
forsker
@nb
researcher ORCID ID = 0000-0002-1838-9363
@en
wetenschapper
@nl
name
T. Nakamura
@ast
T. Nakamura
@nl
Takashi Nakamura
@en
Takashi Nakamura
@nb
type
label
T. Nakamura
@ast
T. Nakamura
@nl
Takashi Nakamura
@en
Takashi Nakamura
@nb
altLabel
T. Nakamura
@en
prefLabel
T. Nakamura
@ast
T. Nakamura
@nl
Takashi Nakamura
@en
Takashi Nakamura
@nb
P31
P496
0000-0002-1838-9363