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Alfvén wave collisions, the fundamental building block of plasma turbulence. IV. Laboratory experiment
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10.1063/1.4813242
/content/aip/journal/pop/20/7/10.1063/1.4813242
http://aip.metastore.ingenta.com/content/aip/journal/pop/20/7/10.1063/1.4813242

Figures

Image of FIG. 1.
FIG. 1.

Schematic of the experimental setup for the Alfvén wave turbulence experiment in the LaPD. The ASW antenna generates a small amplitude Alfvén wave (blue line) with a magnetic field polarized in the direction traveling down the mean magnetic field, , and the loop antenna generates a larger amplitude Alfvén wave (red line) with a magnetic field polarized in the direction traveling up the mean magnetic field. Reprinted with permission from Howes , Phys. Rev. Lett. , 255001 (2012). Copyright (2012) American Physical Society.

Image of FIG. 2.
FIG. 2.

Iowa ASW antenna (a) diagram and (b) a colormap of the component with vectors indicating the perpendicular component of the magnetic field measured in mG at  = 14 m and  = 8.3 ms after the beginning of the discharge.

Image of FIG. 3.
FIG. 3.

UCLA loop antenna (a) diagram and (b) a colormap of the component with vectors indicating the perpendicular component of the magnetic field measured in mG at  = 6.4 m and  = 8.2 ms after the beginning of the discharge. The offset in the data for the UCLA loop antenna was due to a slight biasing issue with the Elsässer probes.

Image of FIG. 4.
FIG. 4.

Colormap of the component of the daughter wave with vectors indicating the perpendicular component of the magnetic field at  = 8.30 ms.

Image of FIG. 5.
FIG. 5.

Color map of the predicted coupling between the loop and ASW antennas. The dark spot at ( = 3 cm,  = 7 cm) indicates the position in the plane where the nonlinear effect is predicted to have the largest amplitude.

Image of FIG. 6.
FIG. 6.

Plot of the amplitude of the daughter wave in frequency where the maximum of the nonlinear signal occurs, ( = 3 cm,  = 5 cm, ). We show the results for when both antennas are at full power (blue), the ASW antenna is at half power and the loop antenna is at full power (green), and when the loop antenna is at half and the ASW antenna is at full (red).

Image of FIG. 7.
FIG. 7.

Contour plots of the two-dimensional Fourier power spectrum of the (a) component of the daughter signal, (b) the component of the loop signal, (c) the component of the ASW antenna signal, and (d) is the diagram of the perpendicular wavevectors for the loop antenna (red line) and the ASW antenna (blue line). The daughter wave should be a vector sum of the type, . The bullseyes indicate the predicted values for the daughter wave. Reprinted with permission from Howes , Phys. Rev. Lett. , 255001 (2012). Copyright (2012) American Physical Society.

Tables

Generic image for table
Table I.

Summary of the five experimental trials.

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/content/aip/journal/pop/20/7/10.1063/1.4813242
2013-07-15
2014-04-17
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Alfvén wave collisions, the fundamental building block of plasma turbulence. IV. Laboratory experiment
http://aip.metastore.ingenta.com/content/aip/journal/pop/20/7/10.1063/1.4813242
10.1063/1.4813242
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