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Complex Atoms I L-S Coupling - Astrophysik Uni
Complex Atoms I L-S Coupling - Astrophysik Uni

... Φa = Φb , then Ψ(1, 2) = 0 . This solution is not allowed. Hence solutions which have the two particle occupying the same spin-orbital are ecluded. The Pauli exclusion principle: ...
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Inertial fusion advance towards ignition

... high-intense laser (PW-1015w) system can provide intensities 1018-21w/cm2 for each beam. Interaction of the petawatt (PW) laser with matter may accelerate charged particles (electrons, protons and heavy ions) to kinetic energy over GeV. The acceleration of high-energy charged particle beam generated ...
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Developing an Efficient Low-Temperature Nuclear Fusion Reactor

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Radio and X-ray signatures of merging neutron stars

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... current research activity, list of publications. Registration fee for participants is 200€ and includes access to the conference facility, lunches and coffees, training material. Partial financial support will be available for deserving students with limited access to institutional funding. Particip ...
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The Virial Theorem, MHD Equilibria, and Force

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Astronomy 112: The Physics of Stars Class 7 Notes: Basics of

... iron-56. This is the most bound nucleus. At smaller atomic masses the binding energy per nucleon generally increases with atomic number, while at larger atomic masses it decreases. This marks the divide between fusion and fission reactions. At atomic masses below 56, energy is released by increasing ...
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Notes 4, p. 1-3

... How does that energy get out? It is transported, and that transport has great bearing on the structure of the star • Early on, you learned there were three energy trnasport mechanisms: conduction, convection and radiation. We will state without proof that conduction is generally not important in sta ...
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A Direct Empirical Proof of the Existence of Dark Matter
A Direct Empirical Proof of the Existence of Dark Matter

Document
Document

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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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