Holographic Fermions in Anisotropic Einstein-Maxwell-Dilaton-Axion Theory

<div>The dispersion relation (a) and the scaling behavior of <svg height="13.1057pt" id="M122" style="vertical-align:-3.427799pt" version="1.1" viewbox="-0.0498162 -9.6779 114.456 13.1057" width="114.456pt" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink"><g transform="matrix(.0135,0,0,-0.0135,0,0)"><path d="M303 0V28C221 34 213 39 213 125V525C213 610 221 616 303 622V650H38V622C120 616 128 610 128 525V125C128 40 120 34 38 28V0H303Z" id="g121-71"></path><glyph.data ascent="989" descent="-360" horiz-adv-x="341" vert-adv-y="341"></glyph.data></g><g transform="matrix(.0135,0,0,-0.0135,4.402,0)"><path d="M797 0V26C739 32 732 36 732 103V296C732 394 682 449 605 449C576 449 550 437 529 423C504 407 475 389 446 366C425 418 382 449 334 449C303 449 279 437 253 421C222 403 201 385 180 371V452C135 432 85 419 41 411V388C99 379 102 374 102 310V103C102 38 93 32 27 26V0H238V26C189 32 180 38 180 103V338C210 363 250 390 289 390C351 390 377 348 377 275V103C377 37 368 32 306 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Advances in High Energy Physics

fig7

Figure 7

Figure 7: Holographic Fermions in Anisotropic Einstein-Maxwell-Dilaton-Axion Theory 