標(biāo)題: Titlebook: Atomic Masses and Fundamental Constants 6; Jerry A. Nolen,Walter Benenson Book 1980 Springer Science+Business Media New York 1980 Atomic m [打印本頁(yè)] 作者: hearken 時(shí)間: 2025-3-21 18:36
書目名稱Atomic Masses and Fundamental Constants 6影響因子(影響力)
書目名稱Atomic Masses and Fundamental Constants 6影響因子(影響力)學(xué)科排名
書目名稱Atomic Masses and Fundamental Constants 6網(wǎng)絡(luò)公開度
書目名稱Atomic Masses and Fundamental Constants 6網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱Atomic Masses and Fundamental Constants 6被引頻次
書目名稱Atomic Masses and Fundamental Constants 6被引頻次學(xué)科排名
書目名稱Atomic Masses and Fundamental Constants 6年度引用
書目名稱Atomic Masses and Fundamental Constants 6年度引用學(xué)科排名
書目名稱Atomic Masses and Fundamental Constants 6讀者反饋
書目名稱Atomic Masses and Fundamental Constants 6讀者反饋學(xué)科排名
作者: harmony 時(shí)間: 2025-3-21 23:52 作者: FILLY 時(shí)間: 2025-3-22 01:03 作者: hair-bulb 時(shí)間: 2025-3-22 05:04
Mass Measurements with Pion Double Charge Exchangeudy nuclei far from the line of stability. Early attempts by Gilly et al., at CERN failed because of the low pion intensities available at that time. The situation changed with the advent of high intensity pion beams at the ‘meson factories.’ DCX experiments by Burman et al.. at the Low Energy Pion 作者: lambaste 時(shí)間: 2025-3-22 10:44 作者: Lobotomy 時(shí)間: 2025-3-22 13:40 作者: 慢慢啃 時(shí)間: 2025-3-22 21:00
The Shell Correction Method and Its Application to Nuclear Massesplet model is used for the macroscopic energy and the microscopic energy is calculated from the single-particle orbitals of the modified oscillator potential. Results for nuclei with A?90 are presented. Except for some closed shell nuclei, the discrepancies between experimental and theoretical shell作者: 哭得清醒了 時(shí)間: 2025-3-22 22:51
Masses from Inhomogeneous Partial Difference Equations; A Shell-Model Approach for Light and Medium-ate difference operator D and calculate κ(N,Z) = D M(N,Z). The inhomogeneous partial difference equation . contains the original mass equation as a special solution. The most general solution of eq. (1) will include solutions of the homogeneous equation which can, for example, be used to generate sh作者: Omnipotent 時(shí)間: 2025-3-23 02:37 作者: 賭博 時(shí)間: 2025-3-23 09:33 作者: insurgent 時(shí)間: 2025-3-23 12:46
Atomic Mass Formulas with Empirical Shell Termsformula consists of a gross part and proton and neutron shell parts. The shell parameter values were determined by a new statistical method, whose essential point was to take into account the intrinsic error of the mass formula. Main characteristics of the formula thus obtained are presented.作者: 免除責(zé)任 時(shí)間: 2025-3-23 16:18
Nuclear Mass Relations and Equationsch relations is presented. Each member of this set gives a prediction of roughly equal statistical accuracy for the unknown mass of a given nuclide. The average and dispersion of the set give a “most probable” mass value and a measure of its uncertainty. The structure of these relations (considered 作者: 少量 時(shí)間: 2025-3-23 18:40 作者: 公共汽車 時(shí)間: 2025-3-24 00:25
High Resolution Penning Trap as a Precision Mass-Ratio Spectrometeras such is an ideal apparatus for isolating long lived charged particles, nearly at rest (thermalized by a cryogenic environment) and essentially free of other-particle interactions (due to the ultra-high vacuum used, ?10. Torr). The ability to determine mass arises from the inverse mass dependence 作者: nonchalance 時(shí)間: 2025-3-24 02:26
Joint Fuzzy Probability Distributions,xperiments, heavy ion beams have steadily increased in importance with the use first of transfer reactions and more recently deep-inelastic reactions for isotope production. In this talk, we shall discuss the application of yet another class of reaction, namely heavy ion fragmentation, to the production of very neutron-rich light nuclei.作者: 金絲雀 時(shí)間: 2025-3-24 08:06 作者: 格言 時(shí)間: 2025-3-24 14:22
Continuous Fuzzy Random Variables,formula consists of a gross part and proton and neutron shell parts. The shell parameter values were determined by a new statistical method, whose essential point was to take into account the intrinsic error of the mass formula. Main characteristics of the formula thus obtained are presented.作者: jabber 時(shí)間: 2025-3-24 15:13
https://doi.org/10.1007/978-1-4684-3716-4Atomic mass; applied physics; chemical physics; energy; gold; particles; physics作者: languid 時(shí)間: 2025-3-24 22:59 作者: 四海為家的人 時(shí)間: 2025-3-25 02:36
Production of New Isotopes by Heavy Ion Fragmentationxperiments, heavy ion beams have steadily increased in importance with the use first of transfer reactions and more recently deep-inelastic reactions for isotope production. In this talk, we shall discuss the application of yet another class of reaction, namely heavy ion fragmentation, to the production of very neutron-rich light nuclei.作者: 充滿裝飾 時(shí)間: 2025-3-25 06:05 作者: Flagging 時(shí)間: 2025-3-25 09:08
Atomic Mass Formulas with Empirical Shell Termsformula consists of a gross part and proton and neutron shell parts. The shell parameter values were determined by a new statistical method, whose essential point was to take into account the intrinsic error of the mass formula. Main characteristics of the formula thus obtained are presented.作者: flimsy 時(shí)間: 2025-3-25 15:34
Similarity relations and valued orders,A Q-value of -31.5762(30) MeV has been measured for the .C (.He, .He).C reaction. The mass of .C, when compared to its Coulomb analog levels in .B, .Be, and .Li, confirms a significant deviation from the quadratic form of the isobaric multiplet mass equation, with a cubic coefficient of d = 5.7 ± 1.5 keV.作者: 巡回 時(shí)間: 2025-3-25 16:33
Functions of Fuzzy Random Variables,The research on atomic masses started from early accidental measurements and simple empiric rules. The next step was to aim at a systematic collection of the masses of all nuclei, stable against particle emission, and at semi-empiric models to guide the experiments with predictions.作者: 光亮 時(shí)間: 2025-3-25 22:19 作者: 爆米花 時(shí)間: 2025-3-26 04:02
Functions of Fuzzy Random Variables,In 1833, Michael Faraday of the Royal Institution in London formulated the laws of electrolysis revealing the relationship between electric current, time, and chemical equivalent weight (mole). Translated into mathematical terms, this relationship can be expressed: ..作者: Immortal 時(shí)間: 2025-3-26 07:25
Mass of 9CA Q-value of -31.5762(30) MeV has been measured for the .C (.He, .He).C reaction. The mass of .C, when compared to its Coulomb analog levels in .B, .Be, and .Li, confirms a significant deviation from the quadratic form of the isobaric multiplet mass equation, with a cubic coefficient of d = 5.7 ± 1.5 keV.作者: Intruder 時(shí)間: 2025-3-26 08:59
Atomic Masses — Comments on Macro-Micro Mass-FormulaeThe research on atomic masses started from early accidental measurements and simple empiric rules. The next step was to aim at a systematic collection of the masses of all nuclei, stable against particle emission, and at semi-empiric models to guide the experiments with predictions.作者: 雪崩 時(shí)間: 2025-3-26 15:03
Trends in Nuclear Mass SystematicsWe describe empirical trends in nuclear masses and relate them, to successively higher approximations of the shell model, emphasizing regularities reaching beyond the lowest-seniority approximation.作者: Mortar 時(shí)間: 2025-3-26 17:41 作者: 模范 時(shí)間: 2025-3-26 22:28 作者: Folklore 時(shí)間: 2025-3-27 03:10 作者: 同義聯(lián)想法 時(shí)間: 2025-3-27 06:48 作者: 多節(jié) 時(shí)間: 2025-3-27 09:33 作者: triptans 時(shí)間: 2025-3-27 14:10 作者: STAT 時(shí)間: 2025-3-27 17:51 作者: Indelible 時(shí)間: 2025-3-28 01:05 作者: obsolete 時(shí)間: 2025-3-28 03:32 作者: 策略 時(shí)間: 2025-3-28 09:05
Discrete Fuzzy Random Variables,as well as those based on semi-microscopic and microscopic theories — of the nuclear binding energies. However the interrelationship of these quantities with low energy excitation spectra of the involved nuclei and/or with the effective interactions giving rise to these spectra has seldom been inves作者: 火海 時(shí)間: 2025-3-28 14:08 作者: adj憂郁的 時(shí)間: 2025-3-28 15:58 作者: 晚間 時(shí)間: 2025-3-28 21:35 作者: 影響深遠(yuǎn) 時(shí)間: 2025-3-29 01:15 作者: Common-Migraine 時(shí)間: 2025-3-29 05:10
Conclusions and Future Research,as such is an ideal apparatus for isolating long lived charged particles, nearly at rest (thermalized by a cryogenic environment) and essentially free of other-particle interactions (due to the ultra-high vacuum used, ?10. Torr). The ability to determine mass arises from the inverse mass dependence 作者: –scent 時(shí)間: 2025-3-29 07:29
http://image.papertrans.cn/b/image/164744.jpg作者: Thrombolysis 時(shí)間: 2025-3-29 14:36 作者: conference 時(shí)間: 2025-3-29 16:05 作者: GRIN 時(shí)間: 2025-3-29 20:21 作者: 北京人起源 時(shí)間: 2025-3-30 02:42 作者: 冰雹 時(shí)間: 2025-3-30 07:07 作者: arousal 時(shí)間: 2025-3-30 09:45 作者: locus-ceruleus 時(shí)間: 2025-3-30 12:42
Functions of a Fuzzy Random Variable, effects seldom exceed 1 MeV. For medium-heavy nuclei and outside the regions where the parameters have been fitted, the general trends appear to be much better described within the liquid drop than within the droplet model.作者: 跑過 時(shí)間: 2025-3-30 20:08 作者: 有毒 時(shí)間: 2025-3-30 23:28 作者: 價(jià)值在貶值 時(shí)間: 2025-3-31 02:02
The Shell Correction Method and Its Application to Nuclear Masses effects seldom exceed 1 MeV. For medium-heavy nuclei and outside the regions where the parameters have been fitted, the general trends appear to be much better described within the liquid drop than within the droplet model.作者: 偏離 時(shí)間: 2025-3-31 06:13 作者: Inelasticity 時(shí)間: 2025-3-31 11:33 作者: GIST 時(shí)間: 2025-3-31 14:06
https://doi.org/10.1007/978-3-540-77926-1 mass-separated radioactivity, complementing the much more extensive investigations by this technique of heavy nuclei off the stability line.. Such studies provide new insights into the limits of nuclear stability, the behavior of nuclear shapes and the onset of new radioactive decay modes.作者: 原始 時(shí)間: 2025-3-31 21:14 作者: 反饋 時(shí)間: 2025-3-31 22:53 作者: craven 時(shí)間: 2025-4-1 03:36 作者: magnate 時(shí)間: 2025-4-1 09:17
Masses of Medium Weight Nuclei by Transfer Reactionsuadratic form: ., where T. is the isospin projection. There are numerous derivations of this formula in the literature,. which employ perturbation methods to expand the nuclear Hamiltonian. In the above form, the lowest isospin multiplet which can be used to test the IMME is T = 3/2.
