標(biāo)題: Titlebook: Luminescence; Data Analysis and Mo Vasilis Pagonis Book 2021 The Editor(s) (if applicable) and The Author(s), under exclusive license to Sp [打印本頁(yè)] 作者: 分類 時(shí)間: 2025-3-21 19:39
書目名稱Luminescence影響因子(影響力)
書目名稱Luminescence影響因子(影響力)學(xué)科排名
書目名稱Luminescence網(wǎng)絡(luò)公開度
書目名稱Luminescence網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱Luminescence被引頻次
書目名稱Luminescence被引頻次學(xué)科排名
書目名稱Luminescence年度引用
書目名稱Luminescence年度引用學(xué)科排名
書目名稱Luminescence讀者反饋
書目名稱Luminescence讀者反饋學(xué)科排名
作者: 誘使 時(shí)間: 2025-3-21 21:21
Analysis and Modeling of TL Dataitial rise method and the method of various heating rates, which allow evaluation of both the activation energy . and the frequency factor .. We present R codes for numerically integrating the simple one trap one recombination model (OTOR), as well as for numerically integrating the equations for fi作者: contradict 時(shí)間: 2025-3-22 04:05
Analysis of Experimental OSL Datad linearly modulated OSL (LM-OSL) signals. We present detailed examples for computerized analysis of OSL experimental data, using the R packages . and ., and how to extract the relevant optical cross sections. On the modeling side, we present the GOT equation derived from the OTOR model, show how th作者: BALK 時(shí)間: 2025-3-22 06:29
Dose Response of Dosimetric Materialsrimental data. We define the superlinearity index .(.), and the supralinearity index .(.), and discuss various functions commonly used to describe shape of dose response curves in TL, OSL, OA, and ESR signals: the saturating exponential, double saturating exponential, single exponential plus linear,作者: acrophobia 時(shí)間: 2025-3-22 09:12 作者: inflame 時(shí)間: 2025-3-22 15:06
Localized Transitions and Quantum Tunneling: ground state tunneling (GST) model, irradiation ground state tunneling (IGST) model, excited state tunneling (EST) model, and thermally assisted excited state tunneling (TA-EST) model. We provide R codes for exploring the properties of each model, discuss their physical principles, and code approx作者: affinity 時(shí)間: 2025-3-22 17:32
Localized Transitions: The LT and SLT Modelons model (SLT). We provide R codes for numerically solving the differential equations for the LT model, and compare the solution with the analytical equations involving the Lambert . function. Several examples are presented using the R package . to simulate these types of localized transition pheno作者: mighty 時(shí)間: 2025-3-23 01:01
Monte Carlo Simulations of Delocalized Transitionsc solutions of the corresponding differential equations. We present the R codes for fixed time interval MC methods to simulate CW-OSL, LM-OSL, TL, and ITL processes and discuss how luminescence processes can be described within the general framework of birth and death processes. Vectorized R codes a作者: FEAT 時(shí)間: 2025-3-23 04:53
Monte Carlo Simulations of Localized Transitionsples of R codes are provided for TL, CW-IRSL, and LM-IRSL signals in the excited state tunneling (EST) model, and the MC results are compared with the analytical Kitis–Pagonis equations (KP-CW, KP-TL). The R codes also provide estimates for the stochastic coefficients of variation CV% for a variety 作者: spinal-stenosis 時(shí)間: 2025-3-23 06:14
Kinetic Monte Carlo Simulationso (KMC) methods. KMC methods are based on the concept that the variable time intervals between random events follow an exponential distribution. R codes are provided here for KMC methods applied to luminescence signals as stochastic birth and death processes. The chapter concludes with a different e作者: 并排上下 時(shí)間: 2025-3-23 11:03
Comprehensive Luminescence Models for Quartzquartz. We show detailed R codes for the . and the . quartz models, by using the R programs . developed by Peng and Pagonis, and also using the R package . by Friedrich et al. We show how to simulate the history of natural quartz samples, and how to modify the models by changing one or more of the o作者: 性行為放縱者 時(shí)間: 2025-3-23 15:24
Comprehensive Models for Feldsparseling phenomena. These are the ground state tunneling (GST) model, irradiation GST (IGST) model, excited state tunneling (EST) model, and thermally assisted tunneling (TA-EST) model. We demonstrate appropriate R functions that can simulate a wide variety of processes in feldspars, for both natural a作者: faculty 時(shí)間: 2025-3-23 19:11
usion (ICF) drivers. Because of their intrinsic short wavelength (0.25 μm), broad bandwidth (～0.5%), smooth spatial beam profile, and precise and flexible temporal pulse-shaping capabilities, KrF lasers appear to be an attractive ICF driver candidate from the laser-target interaction physics standpo作者: choleretic 時(shí)間: 2025-3-24 01:33 作者: 燒瓶 時(shí)間: 2025-3-24 05:04 作者: 擁擠前 時(shí)間: 2025-3-24 08:50
Vasilis Pagonisy compressed with efficient energy transfer from the external energy source into the pellet. The simple model of a uniformly compressed DT sphere can be used to determine the fusion energy production. Figure (1) gives the ratio of fusion energy output to initial thermal energy for a uniform initial 作者: Feigned 時(shí)間: 2025-3-24 10:46 作者: 彎腰 時(shí)間: 2025-3-24 15:28 作者: 忘恩負(fù)義的人 時(shí)間: 2025-3-24 21:01
Vasilis Pagonisfor predicting the optical properties of inhomogeneous biolo.This book introduces readers to the principles of laser interaction with biological cells and tissues with varying degrees of organization. In addition to considering the problems of biomedical cell diagnostics, and modeling the scattering作者: leniency 時(shí)間: 2025-3-25 00:02
Vasilis Pagonisfor predicting the optical properties of inhomogeneous biolo.This book introduces readers to the principles of laser interaction with biological cells and tissues with varying degrees of organization. In addition to considering the problems of biomedical cell diagnostics, and modeling the scattering作者: 亞當(dāng)心理陰影 時(shí)間: 2025-3-25 06:10
r of years, the natural theoretical framework to understand this process was the time-dependent perturbation theory in the lowest non-vanishing order (LOPT) in which the radiation field induces transitions between unperturbed atomic states. The atom absorbs photons and jumps into virtual intermediat作者: SPECT 時(shí)間: 2025-3-25 10:07
Vasilis Pagonisl-time monitored thermal lesioning of tissue. It has found a particular niche in the treatment of medically refractory focal epilepsy for which it provides a less invasive alternative to craniotomy and resection for multiple pathologies such as mesial temporal lobe sclerosis, focal cortical dysplasi作者: 過(guò)分 時(shí)間: 2025-3-25 11:52
Vasilis Pagonisnecrosis following radiosurgery (known together as metastatic in-field recurrence). Current indications for LITT include patients who have KPS >70, have good expected survival or systemic therapy options, and are deemed suitable surgical candidates. While LITT treatment was previously offered when p作者: 色情 時(shí)間: 2025-3-25 19:46
higher dimensional accuracy and surface quality than those produced with conventional processes, and with higher material removal rates. Materials that can be machined by lasers include metals, ceramics, plastics, composites, wood, glass and rubber. . can produce holes as small as 0.05mm in diamete作者: affinity 時(shí)間: 2025-3-25 20:30 作者: Dungeon 時(shí)間: 2025-3-26 01:34 作者: Entrancing 時(shí)間: 2025-3-26 04:20 作者: contrast-medium 時(shí)間: 2025-3-26 10:23
978-3-030-67310-9The Editor(s) (if applicable) and The Author(s), under exclusive license to Springer Nature Switzerl作者: 思想靈活 時(shí)間: 2025-3-26 12:47
Luminescence978-3-030-67311-6Series ISSN 2197-5736 Series E-ISSN 2197-5744 作者: Odyssey 時(shí)間: 2025-3-26 16:47
Vasilis PagonisFeatures over 70 integrated R code examples, extensively annotated for reader comprehension.Includes several chapters devoted to Monte Carlo methods.Discusses how readers can employ and modify the inc作者: 騙子 時(shí)間: 2025-3-26 23:22
Use R!http://image.papertrans.cn/l/image/589027.jpg作者: 初學(xué)者 時(shí)間: 2025-3-27 01:34 作者: output 時(shí)間: 2025-3-27 06:27
Monte Carlo Simulations of Localized Transitions analytical Kitis–Pagonis equations (KP-CW, KP-TL). The R codes also provide estimates for the stochastic coefficients of variation CV% for a variety of processes. This chapter concludes with a MC simulation for the LT model.作者: 敵手 時(shí)間: 2025-3-27 10:47 作者: preeclampsia 時(shí)間: 2025-3-27 14:14 作者: Interstellar 時(shí)間: 2025-3-27 18:27 作者: 翻布尋找 時(shí)間: 2025-3-28 00:32
Time-Resolved OSL Experimentsd on the Mott–Seitz competition mechanism. We show how to analyze TR-OSL signals from . transitions and also TR-IRSL signals involving . transitions in feldspars involving quantum tunneling. This chapter concludes with the presentation of a TR-photoluminescence (TR-PL) model for the important dosimetric material Al.O.:C.作者: 精密 時(shí)間: 2025-3-28 04:20 作者: 用樹皮 時(shí)間: 2025-3-28 09:30 作者: 單調(diào)女 時(shí)間: 2025-3-28 13:59 作者: 打折 時(shí)間: 2025-3-28 18:28 作者: Physiatrist 時(shí)間: 2025-3-28 22:34 作者: 表否定 時(shí)間: 2025-3-29 00:48
Localized Transitions: The LT and SLT Modelmena. We present R codes for the important hybrid SLT model developed by Mandowski, which can be used to explain the anomalous heating rate effect observed in several dosimetric materials. Finally, the chapter concludes with the presentation of a simplified form of the SLT model, developed by Pagonis et al.作者: homeostasis 時(shí)間: 2025-3-29 03:47
Kinetic Monte Carlo Simulationsxample of the KMC method, which describes quantum tunneling processes and the anomalous fading effect from a microscopic point of view. We compare the stochastic KMC results and the corresponding CV% uncertainties with the solution of the corresponding deterministic differential equation.作者: 有助于 時(shí)間: 2025-3-29 08:34 作者: 臥虎藏龍 時(shí)間: 2025-3-29 11:58 作者: photophobia 時(shí)間: 2025-3-29 16:16
Book 2021 materials. This book will be useful to those who use the tools of luminescence dosimetry, including physicists, geologists, archaeologists, and for all researchers who use radiation in their research.作者: Inferior 時(shí)間: 2025-3-29 21:54
5 kJ to the target with a 5-ns pulse length and a spot size ～200 μm. Shaped pulses from 2–20 ns can also be tested. The system employs angular multiplexing, where 96 beam pulses are overlapped into a single, 500-ns beam train. The 96 beam paths are offset and staggered thorough the amplifier chain
