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標(biāo)題: Titlebook: An Advanced Course in Computational Nuclear Physics; Bridging the Scales Morten Hjorth-Jensen,Maria Paola Lombardo,Ubirajar Book 2017 Spri [打印本頁]

作者: FLUX    時間: 2025-3-21 16:06
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書目名稱An Advanced Course in Computational Nuclear Physics讀者反饋




書目名稱An Advanced Course in Computational Nuclear Physics讀者反饋學(xué)科排名





作者: craving    時間: 2025-3-21 23:26
978-3-319-53335-3Springer International Publishing AG 2017
作者: 口訣    時間: 2025-3-22 03:39
Morten Hjorth-Jensen,Maria Paola Lombardo,UbirajarModern, up-to-date and self-contained primer on this fast evolving subject matter.Edited and authored by leading specialists in the field.Each course makes a link with actual numerical software
作者: aerial    時間: 2025-3-22 06:25
Lecture Notes in Physicshttp://image.papertrans.cn/a/image/154798.jpg
作者: figment    時間: 2025-3-22 10:16

作者: 類型    時間: 2025-3-22 13:06
https://doi.org/10.1007/978-3-662-42516-9 aspects of effective field theories and their application to few-body physics. In particular, we consider an effective field theory for non-relativistic particles with resonant short-range interactions where certain parts of the interaction need to be treated nonperturbatively. As an application, w
作者: 項目    時間: 2025-3-22 20:29

作者: 失敗主義者    時間: 2025-3-22 21:57
,Die Innervation der Schilddrüse,alculations using chiral effective field theory and some recent applications. We then describe several methods for computing scattering on the lattice. After that we focus on the main goal, explaining the theory and algorithms relevant to lattice simulations of nuclear few- and many-body systems. We
作者: LVAD360    時間: 2025-3-23 03:03
,Die Innervation der Blutgef??e,n the first part particular attention is devoted to two methods useful to account for bound state properties. They are both based on the diagonalization of the full many-body Hamiltonian matrix, but share in addition the use of similarity transformations. Transforming the bare potential into an effe
作者: 織物    時間: 2025-3-23 07:00

作者: 詼諧    時間: 2025-3-23 09:58

作者: Instantaneous    時間: 2025-3-23 15:58

作者: 比目魚    時間: 2025-3-23 20:22
Verzeichnis der zitierten Literaturral strength. Green’s function methods closely relate to other polynomial scaling approaches discussed in Chaps. 8 and 10. However, here we aim directly at a global view of the many-fermion structure. We derive the working equations for calculating many-body propagators, using both the Algebraic Dia
作者: 無畏    時間: 2025-3-24 00:35

作者: GLIDE    時間: 2025-3-24 06:26

作者: 青少年    時間: 2025-3-24 08:23

作者: spinal-stenosis    時間: 2025-3-24 11:00

作者: 淘氣    時間: 2025-3-24 16:12

作者: receptors    時間: 2025-3-24 22:37
Lattice Quantum Chromodynamics,ypercubic lattice, the strong coupling expansion and the weak coupling expansions are reviewed to see the vital role played by the quantum fluctuations in QCD. Fundamental techniques for numerical LQCD simulations such as the Markov Chain Monte Carlo method and the Hybrid Monte Carlo method are disc
作者: 除草劑    時間: 2025-3-25 02:46
General Aspects of Effective Field Theories and Few-Body Applications, aspects of effective field theories and their application to few-body physics. In particular, we consider an effective field theory for non-relativistic particles with resonant short-range interactions where certain parts of the interaction need to be treated nonperturbatively. As an application, w
作者: 我的巨大    時間: 2025-3-25 04:16
Lattice Methods and Effective Field Theory,rical calculations and has quantifiable systematic errors. In these lectures we apply these techniques to nuclear Effective Field Theory (EFT), a non-relativistic theory for nuclei involving the nucleons as the basic degrees of freedom. The lattice formulation of Endres et al. (Phys Rev A 84:043644,
作者: Definitive    時間: 2025-3-25 11:33

作者: negligence    時間: 2025-3-25 14:52

作者: BIPED    時間: 2025-3-25 19:53
Computational Nuclear Physics and Post Hartree-Fock Methods,. These lectures are closely linked with those of Chaps. 9, 10 and 11 and serve as input for the correlation functions employed in Monte Carlo calculations in Chap. 9, the in-medium similarity renormalization group theory of dense fermionic systems of Chap. 10 and the Green’s function approach in Ch
作者: 美麗的寫    時間: 2025-3-25 22:25

作者: 投射    時間: 2025-3-26 03:39

作者: 愚笨    時間: 2025-3-26 05:30
,Self-Consistent Green’s Function Approaches,ral strength. Green’s function methods closely relate to other polynomial scaling approaches discussed in Chaps. 8 and 10. However, here we aim directly at a global view of the many-fermion structure. We derive the working equations for calculating many-body propagators, using both the Algebraic Dia
作者: Diskectomy    時間: 2025-3-26 08:55
Book 2017 span the entire range, from our smallest components – quarks and gluons as the mediatorsof the strong force – to the computation of the equation of state for neutron star matter..The lectures presented provide an in-depth exposition of the underlying theoretical and algorithmic approaches as well d
作者: 假    時間: 2025-3-26 14:30

作者: 模仿    時間: 2025-3-26 20:34

作者: 遭遇    時間: 2025-3-26 22:58

作者: Mumble    時間: 2025-3-27 04:47
Lattice Quantum Chromodynamics,ussed in some details. As examples of the high precision LQCD simulations, numerical results of the heavy quark potential and the hadron masses are shown. Recent LQCD results on the baryon-baryon interactions are briefly discussed.
作者: 反饋    時間: 2025-3-27 07:39

作者: 不容置疑    時間: 2025-3-27 12:46

作者: FAST    時間: 2025-3-27 15:19
https://doi.org/10.1007/978-3-662-42516-9ussed in some details. As examples of the high precision LQCD simulations, numerical results of the heavy quark potential and the hadron masses are shown. Recent LQCD results on the baryon-baryon interactions are briefly discussed.
作者: Facilities    時間: 2025-3-27 18:01

作者: 雪白    時間: 2025-3-28 01:36
,Die Nervenversorgung der Brustdrüse,ap. 11 We provide extensive code examples and benchmark calculations, allowing thereby an eventual reader to start writing her/his own codes. We start with an object-oriented serial code and end with discussions on strategies for porting the code to present and planned high-performance computing facilities.
作者: 痛恨    時間: 2025-3-28 06:08

作者: 粘土    時間: 2025-3-28 07:29
,Die Innervation der Blutgef??e,he continuum part of the nuclear spectrum is described, with emphasis on perturbation induced reactions. They are based on integral transforms which make it possible to reduce the many-body scattering problem to a bound state problem, allowing to take advantage of any of the methods described in the first part.
作者: 充滿人    時間: 2025-3-28 12:36
,Die Nervenversorgung der Brustdrüse,d by making use of auxiliary fields (Auxiliary Field Diffusion Monte Carlo, AFDMC). Finally, we present the Configuration Interaction Monte Carlo algorithm (CIMC) a method to compute the ground state of general, local or non-local, Hamiltonians based on the configuration space sampling.
作者: Systemic    時間: 2025-3-28 17:47
Verzeichnis der zitierten LiteraturCoupled cluster theory (Chap.?8), Configuration-Interaction Monte Carlo (Chap.?9), and the Self-Consistent Green’s Function approach discussed in Chap.?11 The chapter concludes with an expanded overview of current research directions, and a look ahead at upcoming developments.
作者: 殺人    時間: 2025-3-28 19:04

作者: 古文字學(xué)    時間: 2025-3-29 02:30
Lattice Methods and the Nuclear Few- and Many-Body Problem,th auxiliary fields, and transfer matrix operator with auxiliary fields. Along with our analysis we include several coding examples and a number of exercises for the calculations of few- and many-body systems at leading order in chiral effective field theory.
作者: 潰爛    時間: 2025-3-29 05:41

作者: abnegate    時間: 2025-3-29 10:33
Variational and Diffusion Monte Carlo Approaches to the Nuclear Few- and Many-Body Problem,d by making use of auxiliary fields (Auxiliary Field Diffusion Monte Carlo, AFDMC). Finally, we present the Configuration Interaction Monte Carlo algorithm (CIMC) a method to compute the ground state of general, local or non-local, Hamiltonians based on the configuration space sampling.
作者: 領(lǐng)袖氣質(zhì)    時間: 2025-3-29 14:40





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