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X-ray heating of the chromosphere
X-ray heating of the chromosphere

In situ-XAS and catalytic study of acrolein hydrogenation over silver
In situ-XAS and catalytic study of acrolein hydrogenation over silver

... has been found in a pressure range from 20 bar down to 7.5 mbar, which is displayed in Fig. 1 for the silica supported silver catalyst. The values of Fig. 1 have been obtained from the three different set-ups. A more detailed investigation of the pressure dependence has revealed that, at least for t ...
Low-energy charged particle measurement by MAP-PACE onboard SELENE
Low-energy charged particle measurement by MAP-PACE onboard SELENE

... inside the mass analyzer and their positions are detected by one-dimensional circular resistive anode that is placed behind the MCP. These start electrons also generate start signals when they pass through a grid anode that is placed between the position-sensitive anode and the MCP. Most of the ions ...
Non-thermal hard X-ray emission from stellar coronae
Non-thermal hard X-ray emission from stellar coronae

Observation of a Strongly Interacting Degenerate
Observation of a Strongly Interacting Degenerate

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Physics of Particle Detection

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Interpretation of the Helix Planetary Nebula using Hydro

Objective 2 - Austin Community College
Objective 2 - Austin Community College

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L and T Dwarfs - Indiana University
L and T Dwarfs - Indiana University

... Better spatial resolution (seeing improvements, AO) IR and multi-color surveys (2MASS, DENIS, and Sloan) Breakthrough in understanding appearance of spectra ...
The Sun The Sun is a very typical main sequence star. It contains 1000
The Sun The Sun is a very typical main sequence star. It contains 1000

... supplementary  notes  for  more  detail.   Results  from  solar  models  are  shown  below.  All  energy  genera9on  through  nuclear   reac9ons  occurs  within  the  inner  20  %  of  the  radius,  where  the  temperature  is  high   e ...
ASTR3007/4007/6007, Class 6: Nuclear Reactions 10 March In this
ASTR3007/4007/6007, Class 6: Nuclear Reactions 10 March In this

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Slide 1 - Experimental Elementary Particle Physics Group

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ph507lecnote07

Clathrates - An Exploration of the Chemistry of Caged Compounds
Clathrates - An Exploration of the Chemistry of Caged Compounds

... Na gSi46, Nax Si 136 (X= 1-24) etc. are formed. Rb+ and Cs+ are too large to be incorporated into the cages of Si and Ge. Sn, however, forms clathrates with Rb + and Cs +yielding solids like RbzCS6 Sn46, Cs gSn46, K1.6CS6.4Sn44 and others. Figure 5 shows the inorganic clathrate structure. Inorganic ...
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The  on­ quilibrium  ISIS

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Chapter 5 Nuclear reactions in stars

... Chapter 11 of K&W. The main purpose of this chapter is to briefly analyse the differential equations of stellar evolution and their boundary conditions, and to see how the full set of equations can be simplified in some cases to allow simple or approximate solutions - so-called simple stellar models ...
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Cluster mission and data analysis for the March 2001

The current status of ”Troitsk nu-mass”
The current status of ”Troitsk nu-mass”

... experiment are the Windowless Gaseous Tritium Source (WGTS) and the Electrostatic Spectrometer with Magnetic Adiabatic Collimation (ESMAC). Gaseous source, while being very complex to manufacture and maintain, is needed to avoid solid state effects such as source charging, neighbor excitation and ba ...
The Energy of Electron Affinity to a Zirconium Atom
The Energy of Electron Affinity to a Zirconium Atom

... S2. Then for the second set we carried out a calculation by the determinant PT method with the initial approximation corresponding to the set S1. This allowed us to determine the error of the PT for the set S2 (see Tables 1 and 2). The first basis set S1 for Zr included one-, two-, and three-particl ...
Components of the Milky Way
Components of the Milky Way

Free energy and surface tension of arbitrarily large
Free energy and surface tension of arbitrarily large

< 1 ... 26 27 28 29 30 31 32 33 34 ... 85 >

Microplasma



Microplasmas are plasmas of small dimensions, ranging from tens to thousands of micrometers. They can be generated at a variety of temperatures and pressures, existing as either thermal or non-thermal plasmas. Non-thermal microplasmas that can maintain their state at standard temperatures and pressures are readily available and accessible to scientists as they can be easily sustained and manipulated under standard conditions. Therefore, they can be employed for commercial, industrial, and medical applications, giving rise to the evolving field of microplasmas.
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