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Reflectionless Potentials in One Dimension
- Reflectionless Potentials in One Dimension. Introduction. Problem in wave mechanics. One dimensional potential problems ... Discussion and results ...
Reflectionless Potentials in One Dimension. Introduction. Problem in wave mechanics. One dimensional potential problems ... Discussion and results ...
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???????????????? ??????????? ????? ????? ???? ? ?????????????? ??????????????? ?????????????? ?. ?????(1), ?.?. ??????(1,2) ?THE NONREFLECTION TRANSMISSION OF WAVE THROUGH THE DIELECTRIC LAYER WITH THE MODULATED PERMETTIVITY? W. Frias and N.S. Erokhin (
- Title: ...
Title: ...
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Computational%20Photonics:%20Frequency%20and%20Time%20Domain%20Methods
- Computational Photonics: Frequency and Time Domain Methods Steven G. Johnson MIT Applied Mathematics
Computational Photonics: Frequency and Time Domain Methods Steven G. Johnson MIT Applied Mathematics
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Exact S-matrix for N=6 CS
- ... 4-loop SYM perturbation theory and with 2-loop string world-sheet perturbation ... Recent Developments in String/M Theory. 11 ...
... 4-loop SYM perturbation theory and with 2-loop string world-sheet perturbation ... Recent Developments in String/M Theory. 11 ...
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Computational Photonics: Frequency and Time Domain Methods
- run 'numerical experiment' to simulate E(x, t), H(x, t) Frequency-domain linear response ... Limit range of k: irreducible Brillouin zone. 2 ...
run 'numerical experiment' to simulate E(x, t), H(x, t) Frequency-domain linear response ... Limit range of k: irreducible Brillouin zone. 2 ...
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Communications 2 EE555
- Communications 2 EE555 Course Content Introduction & Review Transmission Line Characteristics Waveguides & Microwave Devices Radiowave Propagation Antennas Microwave ...
Communications 2 EE555 Course Content Introduction & Review Transmission Line Characteristics Waveguides & Microwave Devices Radiowave Propagation Antennas Microwave ...
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Dielectric Materials
- Reflection and transmission at each interface. The reflection coefficient at interface a is ... If each layer is l/2 thick, successive reflections are out of phase ...
Reflection and transmission at each interface. The reflection coefficient at interface a is ... If each layer is l/2 thick, successive reflections are out of phase ...
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