Experimental investigation demonstrates non-Maxwellian electron beams from surface plasma waves, suggesting influence of contaminants.
The acceleration of electrons by surface plasma waves (SPWs) generated during the interaction of ultrashort, linearly polarized, and contrast-enhanced laser pulses at a peak intensity of <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:mo>∼</a:mo><a:mn>6</a:mn><a:mo>×</a:mo><a:msup><a:mrow><a:mn>10</a:mn></a:mrow><a:mrow><a:mn>20</a:mn></a:mrow></a:msup><a:mtext> </a:mtext><a:mtext> </a:mtext><a:msup><a:mrow><a:mi mathvariant="normal">W</a:mi><a:mtext> </a:mtext><a:mi>cm</a:mi></a:mrow><a:mrow><a:mo>−</a:mo><a:mn>2</a:mn></a:mrow></a:msup></a:mrow></a:math> with flat, noncorrugated foils at parallel incidence (with respect to the target surface) is investigated. We experimentally demonstrate the generation of a collimated electron beam (<d:math xmlns:d="http://www.w3.org/1998/Math/MathML" display="inline"><d:mrow><d:mo><</d:mo><d:mn>0.6</d:mn><d:mtext> </d:mtext><d:mtext> </d:mtext><d:mi>mrad</d:mi></d:mrow></d:math>) with a non-Maxwellian spectrum, characterized by peaks at superponderomotive energies (30–36 MeV) and total charge <f:math xmlns:f="http://www.w3.org/1998/Math/MathML" display="inline"><f:mrow><f:mo>∼</f:mo><f:mn>120</f:mn><f:mtext> </f:mtext><f:mtext> </f:mtext><f:mi>pC</f:mi></f:mrow></f:math>. Through particle-in-cell (PIC) simulations, we identify the <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"><h:mrow><h:mi mathvariant="bold">J</h:mi><h:mo>×</h:mo><h:mi mathvariant="bold">B</h:mi></h:mrow></h:math> force at the front edge as the primary mechanism for injecting electrons into the SPW, where they are further accelerated. Furthermore, our simulation findings reveal that lateral surface contaminants influence SPW dynamics and give rise to a long-ranging plasmonic mode.
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McCay et al. (2025) studied this question.
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