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- 6-The electron
**oscillating**period as functions of the temperature and the cyclotron**frequency**in triangular quantum dot**qubit**under an electric field.docx... Fig.4. A-Function relationship between the first excited state energy and the temperature and the electron-phonon coupling constant for different cyclotron**frequencies**and ,,,; B-Function relationship between the first excited energy and the temperature and the electric field strength for different cyclotron**frequencies**and ,,,; C-Function relationship between the first excited energy and the temperature and the confinement length for different cyclotron**frequencies**and ,,,; D-Function relationship between the first excited energy and of the temperature and the Coulomb impurity potential for different cyclotron**frequencies**and ,,,... Fig.1. A-Function relationship between the ground state energy and the temperature and the cyclotron**frequency**for different electron-phonon coupling constants and ,,, ; B-Function relationship between the ground state energy and the temperature and the cyclotron**frequency**for different electric field strengths and ,,,; C-Function relationship between the ground state energy and the temperature and the cyclotron**frequency**for different confinement lengths and ,,,; D-Function relationship between the ground state energy and the temperature and the cyclotron**frequency**for different Coulomb impurity potentials and ,,,... Fig.6. A-The electron**oscillation**period as functions of the temperature and the cyclotron**frequency**for different electron-phonon coupling constants and ,,,; B-The electron**oscillation**period as functions of the temperature and the cyclotron**frequency**for different electric field strengths and,,,; C-The electron**oscillation**period as functions of the temperature and the cyclotron**frequency**for different confinement lengths and ,,,; D-The electron**oscillation**period as functions of the temperature and the cyclotron**frequency**for different Coulomb impurity potentials and ,,,... 7-The electron**oscillating**period as functions of the temperature and the electron-phonon coupling constant and etc. in triangular quantum dot**qubit**under an electric field.docx... 2-The first excited state energy as functions of the temperature and the cyclotron**frequency**in triangular quantum dot**qubit**under an electric field.docx... 3-The ground state energy as functions of the temperature and the electron-phonon coupling constant and etc. in triangular quantum dot**qubit**under an electric field.docx... Fig.7. A-The electron**oscillation**period as functions of the temperature and the electron-phonon coupling constant for different cyclotron**frequencies**and ,,,; B-The electron**oscillation**period as functions of the temperature and the electric field strength for different cyclotron**frequencies**and ,,,; C-The electron**oscillation**period as functions of the temperature and the confinement length for different cyclotron**frequencies**and ,,,; D-The electron**oscillation**period as functions of the temperature and the Coulomb impurity potential for different cyclotron**frequencies**and ,,,... 1-The ground state energy as functions of the temperature and the cyclotron**frequency**in triangular quantum dot**qubit**under an electric field.docx... Fig.3. A-Function relationship between the ground state energy and the temperature and the electron-phonon coupling constant for different cyclotron**frequencies**and ,,,; B-Function relationship between the ground state energy and the temperature and the electric field strength for different cyclotron**frequencies**and ,,,; C-Function relationship between the ground state energy and of the temperature and the confinement length for different cyclotron**frequencies**and ,,,; D-Function relationship between the ground state energy and the temperature and the Coulomb impurity potential for different cyclotron**frequencies**and ,,,Data Types:- Dataset
- Document

- Forced
**Oscillations**, All Data.xlsx...**Oscillation**...**Frequency**Data Types:- Image
- Tabular Data
- Dataset
- Text

- Nanofibrillated cellulose (NFC) was prepared from TEMPO-oxidized bleached pulp by mechanical delamination. Sonication and ultracentrifugation was subsequently used in order to remove large aggregates. The measurements were performed using Bohlin CVO rheometer (Malvern Instruments Limited, UK). A cone-plate geometry (4 °/40 mm) was used with a gap width of 150 μm. The experiments were performed at 20 °C. The sample and geometry were covered with a plastic lid in order to prevent sample evaporation. In the amplitude sweep experiments the shear stress amplitude was increased from 5-40 Pa at a fixed
**frequency**. The**frequency**sweep experiments, were performed at constant shear stress aplitude with the**frequency**sweeping from 0.1-40 Hz....**Frequency**Data Types:- Tabular Data
- Dataset

- These files are the schematic files of the quadrature
**oscillator**, proposed in the paper. The files are related to the Cadence integrated circuit design environment.Data Types:- Dataset
- File Set

- Abstract GLoBES (General Long Baseline Experiment Simulator) is a flexible software package to simulate neutrino
**oscillation**long baseline and reactor experiments. On the one hand, it contains a comprehensive abstract experiment definition language (AEDL), which allows to describe most classes of long baseline experiments at an abstract level. On the other hand, it provides a C-library to process the experiment information in order to obtain**oscillation**probabilities, rate vectors, and Δ χ^2 -values. ... Title of program: GLoBES version 3.0.8 Catalogue Id: ADZI_v1_0 Nature of problem Neutrino**oscillations**are now established as the leading flavor transition mechanism for neutrinos. In a long history of many experiments, see, e.g., [1], two**oscillation****frequencies**have been identified: The fast atmospheric and the slow solar**oscillations**, which are driven by the respective mass squared differences. In addition, there could be interference effects between these two**oscillations**, provided that the coupling given by the small mixing angle θ 13 is large enough. Such interference ... Versions of this program held in the CPC repository in Mendeley Data ADZI_v1_0; GLoBES version 3.0.8; 10.1016/j.cpc.2007.05.007 This program has been imported from the CPC Program Library held at Queen's University Belfast (1969-2019)Data Types:- Dataset
- File Set

- Abstract A detailed study is undertaken, using various techniques, in deriving analytical formula of Franck-Condon overlap integrals and matrix elements of various functions of power (x^l ), exponential (exp (- 2 c x)) and Gaussian (exp (- c x^2 )) over displaced harmonic
**oscillator**wave functions with arbitrary**frequencies**. The results suggested by previous experience with various algorithms are presented in mathematically compact form and consist of generalization. The relationships obtained are val... Title of program: FRANCK (Franck-Condon factors and matrix elements programs) Catalogue Id: ADXX_v1_0 Nature of problem The programs calculate the Franck-Condon factors and matrix elements over displaced harmonic**oscillator**wave functions with arbitrary quantum numbers (n, n1),**frequencies**(a, a1) and displacement (d) for the various functions of power (x l ), exponential (exp(-2cx)) and Gaussian (exp(-cx 2 )). Versions of this program held in the CPC repository in Mendeley Data ADXX_v1_0; FRANCK (Franck-Condon factors and matrix elements programs); 10.1016/j.cpc.2006.04.002 This program has been imported from the CPC Program Library held at Queen's University Belfast (1969-2019)Data Types:- Dataset
- File Set

- High
**Frequency****Oscillations**... Natural**frequencies**of laminated composite plates using thirData Types:- Other
- Dataset
- File Set

- Examples of simulations in the associated articles can be reproduced by adjusting the model parameters in Main.m. An example parameter set resulting in
**frequency**lock-in is included....**frequency**...**oscillator**Data Types:- Software/Code
- Dataset
- Document

- Abstract A method is described for constructing numerical high and low
**frequency**filters for the filtration of the trajectories of strongly non-stationary stochastic processes (e.g. with a trend of the type of resonance functions). Measures of function**oscillations**and function variability are introduced, and by making use of them the problem of constructing the above-mentioned filters is formulated in terms of the calculus of variations. A compact algorithm for the numerical implementation of the met... Title of program: SMOOS,SMOSI Catalogue Id: ABVQ_v1_0 Nature of problem The program either smoothes a statistical series with a strongly non- stationary (e.g. resonance-like) trend or extracts from it a low**frequency**envelope from below. Versions of this program held in the CPC repository in Mendeley Data ABVQ_v1_0; SMOOS,SMOSI; 10.1016/0010-4655(81)90014-X This program has been imported from the CPC Program Library held at Queen's University Belfast (1969-2018)Data Types:- Dataset
- File Set

**oscillate**...**frequency**...**frequency**....**Frequency**...**oscillation**Data Types:- Dataset
- Document