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{ | |
"$schema": "https://json.schemastore.org/resume", | |
"meta": { "theme": "kendall" } , | |
"basics": { | |
"name": "Adwiteey Mauriya", | |
"label": "Data Scientist", | |
"image": "http://adwiteeymauriya.com/photo.jpg", | |
"summary": "Experienced Doctoral Researcher with a demonstrated history of working in the research industry. Skilled in Statistical Data Analysis, Linux System Administration, High performance computing, and Data Analytics. Strong research skills with a Doctor of Philosophy - PhD: focused on Plasma and High-Temperature Physics from Instituto Superior Tecnico, Lisbon, Portugal.", | |
"website": "http://adwiteeymauriya.com", | |
"email": "adwiteeymauriya@gmail.com", |
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Automatically generated by Mendeley Desktop 1.19.1 | |
Any changes to this file will be lost if it is regenerated by Mendeley. | |
BibTeX export options can be customized via Options -> BibTeX in Mendeley Desktop | |
@article{Helander2015a, | |
abstract = {Recent progress in the gyrokinetic theory of stellarator microinstabilities$\backslash$nand turbulence simulations is summarized. The simulations have been$\backslash$ncarried out using two different gyrokinetic codes, the global particle-in-cell$\backslash$ncode EUTERPE and the continuum code GENE, which operates in the geometry$\backslash$nof a flux tube or a flux surface but is local in the radial direction.$\backslash$nIon-temperature-gradient (ITG) and trapped-electron modes are studied$\backslash$nand compared with their counterparts in axisymmetric tokamak geometry.$\backslash$nSeveral interesting differences emerge. Because of the more complicated$\backslash$nstructure of the magnetic field, the fluctuations are much less evenly$\backslash$ndistributed over each |
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================================================ | |
GNU coreutils 8.28: ./tests/test-suite.log | |
================================================ | |
# TOTAL: 600 | |
# PASS: 488 | |
# SKIP: 108 | |
# XFAIL: 0 | |
# FAIL: 3 | |
# XPASS: 0 |
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import numpy as np | |
import matplotlib.pyplot as plt | |
def f1(x,y): | |
return x**y-y**x | |
def f2(x,y): | |
return x-y | |
x0=int(raw_input("x0 = ") or '0') | |
xlast=int(raw_input("xlast = ") or '100') | |
xwindow=int(raw_input("xwindow = ") or '1') | |
y0=int(raw_input("y0 = ") or '0') |