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<ref>B.Ph. van Milligen et al, Statistically robust linear and non-linear wavelet analysis applied to plasma edge turbulence, Rev. Sci. Instrum. '''68''' (1997) 967</ref> | <ref>B.Ph. van Milligen et al, Statistically robust linear and non-linear wavelet analysis applied to plasma edge turbulence, Rev. Sci. Instrum. '''68''' (1997) 967</ref> | ||
<ref>[http://link.aps.org/doi/10.1103/PhysRevLett.84.4842 P.H. Diamond et al, In search of the elusive zonal flow using cross-bicoherence analysis, Phys. Rev. Lett. '''84''', 12 (2000) 4842]</ref> | <ref>[http://link.aps.org/doi/10.1103/PhysRevLett.84.4842 P.H. Diamond et al, In search of the elusive zonal flow using cross-bicoherence analysis, Phys. Rev. Lett. '''84''', 12 (2000) 4842]</ref> | ||
<ref>B.Ph. van Milligen et al, Bicoherence during confinement transitions in the TJ-II stellarator, Nucl. Fusion '''48''' (2008) 115003</ref> | <ref>[http://dx.doi.org/10.1088/0029-5515/48/11/115003 B.Ph. van Milligen et al, Bicoherence during confinement transitions in the TJ-II stellarator, Nucl. Fusion '''48''' (2008) 115003]</ref> | ||
=== Self-similarity === | === Self-similarity === | ||
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<ref>B.Ph. van Milligen et al, Quantifying profile stiffness, Plasma and Fusion Research, '''3''' (2008) S1070</ref> | <ref>B.Ph. van Milligen et al, Quantifying profile stiffness, Plasma and Fusion Research, '''3''' (2008) S1070</ref> | ||
power degradation, the rapid propagation of perturbations, | power degradation, the rapid propagation of perturbations, | ||
<ref>B.Ph. van Milligen et al, Pulse propagation in a simple probabilistic transport model, Nucl. Fusion '''47''' (2007) 189</ref> | <ref>[http://dx.doi.org/10.1088/0029-5515/47/3/004 B.Ph. van Milligen et al, Pulse propagation in a simple probabilistic transport model, Nucl. Fusion '''47''' (2007) 189]</ref> | ||
and the Bohm scaling of plasma confinement might be explained on the basis of profile self-regulation in the framework of the [[Self-Organised Criticality]] paradigm. This paradigm predicts that transport is regulated by avalanches, which would generate self-similar behaviour in space and time of the turbulent data. | and the Bohm scaling of plasma confinement might be explained on the basis of profile self-regulation in the framework of the [[Self-Organised Criticality]] paradigm. This paradigm predicts that transport is regulated by avalanches, which would generate self-similar behaviour in space and time of the turbulent data. | ||
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to determine its relation with local plasma parameters (rational surfaces, gradients, electric fields), | to determine its relation with local plasma parameters (rational surfaces, gradients, electric fields), | ||
<ref>M.A. Pedrosa et al, Role of rational surfaces on fluctuations and transport in the plasma edge of the TJ-II stellarator, Czechoslovak Journal of Physics, '''50''', 12 (2000) 1463</ref> | <ref>M.A. Pedrosa et al, Role of rational surfaces on fluctuations and transport in the plasma edge of the TJ-II stellarator, Czechoslovak Journal of Physics, '''50''', 12 (2000) 1463</ref> | ||
<ref>B. Gonçalves et al, Experimental investigation of dynamical coupling between density gradients, radial electric fields and turbulent transport in the JET plasma boundary region, Nucl. Fusion '''42''' (2002) 1205</ref> | <ref>[http://dx.doi.org/10.1088/0029-5515/42/10/305 B. Gonçalves et al, Experimental investigation of dynamical coupling between density gradients, radial electric fields and turbulent transport in the JET plasma boundary region, Nucl. Fusion '''42''' (2002) 1205]</ref> | ||
<ref>M.A. Pedrosa et al, Edge turbulence during limiter biasing experiments in the TJ-II stellarator, Czechoslovak Journal of Physics, '''53''' (2003) 877</ref> | <ref>M.A. Pedrosa et al, Edge turbulence during limiter biasing experiments in the TJ-II stellarator, Czechoslovak Journal of Physics, '''53''' (2003) 877</ref> | ||
and to visualise turbulent structures. | and to visualise turbulent structures. |