派博傳思國際中心

標(biāo)題: Titlebook: Laser Physics; Proceedings of the T J. D. Harvey,D. F. Walls Conference proceedings 1983 Springer-Verlag Berlin Heidelberg 1983 Chaos (Math [打印本頁]

作者: mountebank    時(shí)間: 2025-3-21 16:55
書目名稱Laser Physics影響因子(影響力)




書目名稱Laser Physics影響因子(影響力)學(xué)科排名




書目名稱Laser Physics網(wǎng)絡(luò)公開度




書目名稱Laser Physics網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Laser Physics被引頻次




書目名稱Laser Physics被引頻次學(xué)科排名




書目名稱Laser Physics年度引用




書目名稱Laser Physics年度引用學(xué)科排名




書目名稱Laser Physics讀者反饋




書目名稱Laser Physics讀者反饋學(xué)科排名





作者: Budget    時(shí)間: 2025-3-21 23:16
978-3-540-12305-7Springer-Verlag Berlin Heidelberg 1983
作者: 極大的痛苦    時(shí)間: 2025-3-22 02:40

作者: Patrimony    時(shí)間: 2025-3-22 06:13
0075-8450 Overview: 978-3-540-12305-7978-3-540-39891-2Series ISSN 0075-8450 Series E-ISSN 1616-6361
作者: 縱欲    時(shí)間: 2025-3-22 10:21
Lecture Notes in Physicshttp://image.papertrans.cn/l/image/581543.jpg
作者: Monolithic    時(shí)間: 2025-3-22 14:22

作者: 古董    時(shí)間: 2025-3-22 18:51

作者: 原諒    時(shí)間: 2025-3-23 00:51
S. D. Smith,B. S. Wherrett both SGS models predict the aforementioned flow features in a similar manner. However, looked at closely, some noteworthy differences become evident. The most striking one concerns the shape and influence of the separation bubble. In the simulation with the Smagorinsky model the separation bubble i
作者: Creatinine-Test    時(shí)間: 2025-3-23 02:34
H. J. Kimble,D. E. Grant,A. T. Rosenberger,P. D. Drummond both SGS models predict the aforementioned flow features in a similar manner. However, looked at closely, some noteworthy differences become evident. The most striking one concerns the shape and influence of the separation bubble. In the simulation with the Smagorinsky model the separation bubble i
作者: 摘要    時(shí)間: 2025-3-23 08:38
W. R. MacGillivray both SGS models predict the aforementioned flow features in a similar manner. However, looked at closely, some noteworthy differences become evident. The most striking one concerns the shape and influence of the separation bubble. In the simulation with the Smagorinsky model the separation bubble i
作者: Tincture    時(shí)間: 2025-3-23 10:17

作者: 飛行員    時(shí)間: 2025-3-23 14:23

作者: Coordinate    時(shí)間: 2025-3-23 18:04
Lee W. Caspersonfocuses on the numerical simulation of the physical phenomena leading to disintegration of liquid jets. Although many researchers focused in the past on primary breakup phenomena and many experimental, analytical and also numerical results are available, these processes are not well understood. Ther
作者: Defiance    時(shí)間: 2025-3-23 22:15

作者: 使高興    時(shí)間: 2025-3-24 05:41

作者: Valves    時(shí)間: 2025-3-24 08:21
A. Seilmeier,W. Kaisernt times computational resources necessary to perform a (U)RANS simulation of the considered case does not cause a problem. Computations of flows through complex geometries at higher Reynolds numbers with LES are still the challenge for CFD and super computers.
作者: 細(xì)菌等    時(shí)間: 2025-3-24 12:47

作者: enormous    時(shí)間: 2025-3-24 16:32

作者: 用手捏    時(shí)間: 2025-3-24 21:40

作者: GET    時(shí)間: 2025-3-24 23:48
Charles M. Bowdenthat a sustained level of performance in the range of several Tera?ops is possible. ? To show that di?erent platforms (vector based systems, cluster systems) can be coupled to create a hybrid supercomputer system from which applications can harness an even higher level of sustained performance.
作者: concentrate    時(shí)間: 2025-3-25 04:34
B. J. Dalton,P. L. Knightented computation schemes lead to considerably less indirect addressing and at the same time packaging more instructions. Thus, the overall performance of the iterative solver can be improved..The last part discusses the input and output facility of parallel scientific software. Next to efficiency t
作者: 角斗士    時(shí)間: 2025-3-25 11:25

作者: NORM    時(shí)間: 2025-3-25 13:59
Optical bistability and non absorption resonance in atomic sodium,
作者: Ejaculate    時(shí)間: 2025-3-25 16:52
Polarization switching and optical bistability with resonantly driven J=1/2 to J=1/2 atoms in a rin
作者: 錯(cuò)事    時(shí)間: 2025-3-26 00:04
Experimental evidence for self-pulsing and chaos in CW-excited lasers,
作者: abstemious    時(shí)間: 2025-3-26 01:41

作者: 甜食    時(shí)間: 2025-3-26 05:39
Raman spectroscopy with ultrashort coherent excitation. Narrowing of spectral lines beyond the deph
作者: 不成比例    時(shí)間: 2025-3-26 11:24

作者: Fulminate    時(shí)間: 2025-3-26 14:04
Coherent population trapping and the effect of laser phase fluctuations,
作者: 人工制品    時(shí)間: 2025-3-26 19:18
Chaos in nonlinear optical systems, via a nonlinear medium. Nonlinear couplings are provided by a J=1/2 to J=1/2 transition, a two-photon transition, and a second-order nonlinear susceptibility, respectively. A new type of period-doubling to chaos which occurs in the first of these models, and also in the Lorenz equations, will be described.
作者: 破譯    時(shí)間: 2025-3-26 23:41

作者: sebaceous-gland    時(shí)間: 2025-3-27 02:20

作者: 煩擾    時(shí)間: 2025-3-27 05:38
ns were carried out using large-eddy simulations (LES) applying two different subgrid-scale (SGS) models, namely the Smagorinsky model and the dynamic model by Germano/Lilly. For this kind of flow simulations high-performance computers such as the presently used SMP cluster Hitachi SR8000-F1 are ine
作者: AMBI    時(shí)間: 2025-3-27 10:58
S. D. Smith,B. S. Wherrettns were carried out using large-eddy simulations (LES) applying two different subgrid-scale (SGS) models, namely the Smagorinsky model and the dynamic model by Germano/Lilly. For this kind of flow simulations high-performance computers such as the presently used SMP cluster Hitachi SR8000-F1 are ine
作者: Hirsutism    時(shí)間: 2025-3-27 13:42

作者: Hallowed    時(shí)間: 2025-3-27 17:54
W. R. MacGillivrayns were carried out using large-eddy simulations (LES) applying two different subgrid-scale (SGS) models, namely the Smagorinsky model and the dynamic model by Germano/Lilly. For this kind of flow simulations high-performance computers such as the presently used SMP cluster Hitachi SR8000-F1 are ine
作者: plasma-cells    時(shí)間: 2025-3-27 22:15
W. J. Sandle,M. W. Hamiltonld quantum gasses and high-.. superconductivity. Recent advances in cooling techniques of quantum gasses allow to reach the degenerate regime for fermionic samples. Loading these systems on optical lattices can bring the gas to a strongly correlated regime. We analyze the properties of trapped degen
作者: menopause    時(shí)間: 2025-3-28 05:41
H. J. CarmichaelThe numerical simulation has delivered detailed aerodynamical information as well as showed problems and the importance of a proper mesh generation for LES. The mesh down to the wall and along the wall must be fine enough in order to resolve the expected structures..The importance of upstream turbul
作者: 北極熊    時(shí)間: 2025-3-28 07:38
Lee W. Caspersonntal and analytical description of fluid flow phenomena. One of these tools is the . (DNS) technique relying on a very high spatial and temporal resolution of fluid systems. Thus, all length scales of a fluid flow, only limited by the grid size, are captured by DNS. Since investigations of many flui
作者: 字的誤用    時(shí)間: 2025-3-28 11:51

作者: 裝飾    時(shí)間: 2025-3-28 16:19
Paul Mandel,T. Erneuxntal and analytical description of fluid flow phenomena. One of these tools is the . (DNS) technique relying on a very high spatial and temporal resolution of fluid systems. Thus, all length scales of a fluid flow, only limited by the grid size, are captured by DNS. Since investigations of many flui
作者: COW    時(shí)間: 2025-3-28 19:11

作者: Vsd168    時(shí)間: 2025-3-29 02:10
W. Zinth,W. Kaiseraboratory (GFDL) SKYHI model, and an ocean model descended from the Bryan-Cox-Semtner ocean general circulation model. These parallel models are being developed as part of a long-term research collaboration between Los Alamos National Laboratory (LANL) and the GFDL. The goal of this collaboration is
作者: curriculum    時(shí)間: 2025-3-29 03:20

作者: Hyperplasia    時(shí)間: 2025-3-29 10:08

作者: Outmoded    時(shí)間: 2025-3-29 13:38
Charles M. Bowden the range of Tera?ops. The workshop held at the High Performance Computing Center Stuttgart (HLRS) was the second of this kind. The ?rst one had been held in May 2004. At both workshops hardware and software issues were presented and applications were discussed that have the potential to scale and
作者: Anonymous    時(shí)間: 2025-3-29 19:27
B. J. Dalton,P. L. Knight large scale Computational Fluid Dynamics (CFD) and Fluid-Structure Interaction (FSI) problems efficiency and robustness of the algorithms are two key requirements..In the first part of this paper a straightforward concept is described to increase the performance of the integration of finite element
作者: Desert    時(shí)間: 2025-3-29 21:34
B. Luther-DaviesSimulation (LES) of the flow field containing the acoustic source region is carried out from which then the acoustic sources are extracted. These are then used in the second computational Aeroacoustics (CAA) step in which the acoustic field is determined by solving linear acoustic perturbation equat
作者: decipher    時(shí)間: 2025-3-30 01:30

作者: Friction    時(shí)間: 2025-3-30 07:08
Chaos in nonlinear optical systems,ng stability analysis. Three other systems which also show self-oscillations and chaos are discussed. Each comprises two ring-cavity modes interacting via a nonlinear medium. Nonlinear couplings are provided by a J=1/2 to J=1/2 transition, a two-photon transition, and a second-order nonlinear suscep
作者: tinnitus    時(shí)間: 2025-3-30 11:00
Pump dynamical effects in superfluorescent quantum initiation and pulse evolution,rescence (SF) time, τ. , are such that τ./τ. < 1, the effect of coherent pumping on a three-level system can cause a significant contribution to the quantum mechanical SF initiation and corresponding amplified temporal fluctuations. Other recent work shows, furthermore, that for τ./τ. > > 1, but τ./
作者: 你正派    時(shí)間: 2025-3-30 14:30

作者: GRAIN    時(shí)間: 2025-3-30 19:43
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作者: 重疊    時(shí)間: 2025-3-30 22:57
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作者: 吞下    時(shí)間: 2025-3-31 02:09
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作者: 多節(jié)    時(shí)間: 2025-3-31 07:49
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作者: malapropism    時(shí)間: 2025-3-31 12:16
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作者: 愛管閑事    時(shí)間: 2025-3-31 17:10
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