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In this change, the RamanSolver is completely restructured in order to obtain a simplified and faster solution of the Raman equation. Additionally, the inter-channel Raman effect can be evaluated also in the standard fiber, when no Raman pumping is present. The same is true for the GGN model. The Raman pump parameter pumps_loss_coef has been removed as it was not used. The loss coefficient value evaluated at the pump frequency can be included within the fiber loss_coef parameter. This change induces variations in some expected test results as the Raman profile solution is calculated by a completely distinct algorithm. Nevertheless, these variations are negligible being lower than 0.1dB. Change-Id: Iaa40fbb23c555571497e1ff3bf19dbcbfcadf96b
38 lines
775 B
JSON
38 lines
775 B
JSON
{
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"uid": "Span1",
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"params": {
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"length": 80,
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"loss_coef": 0.2,
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"length_units": "km",
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"att_in": 0,
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"con_in": 0.5,
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"con_out": 0.5,
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"type_variety": "SSMF",
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"dispersion": 0.0000167,
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"effective_area": 83e-12,
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"pmd_coef": 1.265e-15
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},
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"operational": {
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"temperature": 283,
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"raman_pumps": [
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{
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"power": 224.403e-3,
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"frequency": 205e12,
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"propagation_direction": "counterprop"
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},
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{
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"power": 231.135e-3,
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"frequency": 201e12,
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"propagation_direction": "counterprop"
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}
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]
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},
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"metadata": {
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"location": {
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"latitude": 1,
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"longitude": 0,
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"city": null,
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"region": ""
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}
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}
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} |