ライフサイエンスコーパス: nucleon

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1 nergies greater than approximately 6 MeV per nucleon.

2 the isotopic species with the same number of nucleons.

3 t to a mean field generated by all the other nucleons.

4 yproducts of their occasional recoil against nucleons.

5 10 x 10(6) to 40 x 10(6) electron volts per nucleon and an increasing galactic cosmic-ray electron i

6 energy spread and energies up to 18 MeV per nucleon and approximately 5% conversion efficiency (that

7 volts (keV) to >/=50 megaelectron volts per nucleon and of electrons from >26 keV to >/=350 keV.

8 th at half-maximum approximately 0.5 MeV per nucleon) and a longitudinal emittance of less than 2 x 1

9 heavy ion (56)Fe radiation (energy: 1000 MeV/nucleon) and results were compared to gamma radiation do

10 anced dose deposition provided by antiproton-nucleon annihilation.

11 esponding to closed shells of strongly bound nucleons) are particularly stable.

12 The QED calculation treats the nucleons as point-like, whereas the latter approach incl

13 ergy can be released by the rearrangement of nucleons between the initial- and final-state nuclei.

14 The ions have a mean energy of 3 MeV per nucleon (full-width at half-maximum approximately 0.5 Me

15 driven ions with energies of several MeV per nucleon have also been produced.

16 emblance to the dynamical mass generation of nucleons in high-energy physics.

17 Values of m, the number of nucleons in the revolving cluster, and of R, the radius

18 ectrons and the spin-polarized electrons and nucleons in three laboratory experiments.

19 c (> approximately 10 kiloelectron volts per nucleon) ion at closest approach.

20 gment group by 137Cs gamma or Fe26+ (1.1 GeV/nucleon) irradiation vs the corresponding unirradiated D

21 lei using a technique involving one- and two-nucleon knockout from beams of exotic nuclei.

22 The number of nucleons m in each cluster is taken to be 2 for neutron

23 Values of the nucleon number of the revolving cluster are assigned on

24 Values of the nucleon numbers of clusters and spheres, of the radius o

25 nergies ~195 to ~500 mega-electron volts per nucleon, of which we identify 15 (60)Fe nuclei.

26 ns in a nucleus can form strongly correlated nucleon pairs.

27 The internal structure of nucleons (protons and neutrons) remains one of the great

28 c rays down to ~3 x 10(6) electron volts per nucleon, revealing H and He energy spectra with broad pe

29 s the latter approach includes the effect of nucleon structure in a systematic way.

30 ions (approximately62 megaelectron volts per nucleon) that peaked at approximately1.5RJ inside the br

31 nique that involves the transfer of a single nucleon to the nucleus.

32 rely restricted the consistent range for the nucleon-to-photon ratio: 3.7 </= eta10 </= 4.0.

33 ate the dynamics of quarks and gluons inside nucleons using deeply virtual Compton scattering (DVCS)-

34 ed to high energies (up to about 300 TeV per nucleon, where 1 TeV is 10(12) eV) in the expanding shoc

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