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Positron and electron collisions with anti-protons in strong magnetic fields
Positron and electron collisions with anti-protons in strong magnetic fields

... velocities, impact parameters, etc and the averaging process tends to reduce the size of quantum effects. As an example, a positron in a 1 T field has h̄ωcyc = 1.3 K compared to the minimum expected temperature of 4 K for these experiments; thus, even the cyclotron motion will have several quanta. O ...
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... • One amu is one-twelfth of the mass of a 12C atom • One amu is close to the mass of one proton or one neutron. • One amu is a very small mass – 1.66 x 10-24 g • One mole is 6.022 x 1023 units of anything • One mole (of atoms) of an element will have a mass in grams equal to the mass in amu of one a ...
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... surface cross–sections perpendicular to B (see Figure 9.2). Equations 9.10 and 9.11 can therefore give information about the cross-sectional areas of a section of Fermi surface. Note that the sign of (∂A/∂E) allows the carriers on a section of Fermi surface to be identified as hole-like ((∂A/∂E) < 0 ...
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... (Received 19 August 1991; accepted for publication 21 October 1991) The carrier capture times in multiple quantum well semiconductor amplifiers of different structures are studied under high plasma density conditions. Fast ( < 1 ps), slow ( > 150 ps), and intermediate time constants (2-7 ps) are ide ...
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Rutherford backscattering spectrometry



Rutherford backscattering spectrometry (RBS) is an analytical technique used in materials science. Sometimes referred to as high-energy ion scattering (HEIS) spectrometry, RBS is used to determine the structure and composition of materials by measuring the backscattering of a beam of high energy ions (typically protons or alpha particles) impinging on a sample.
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