A General Method for Transforming Nonphysical Configurations in BPS States

<div>Time evolution of the analytical EoS parameter derived from our two-field model. 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20Z"></path></g></svg>.</span> There we observe two expansion eras where <svg height="8.69875pt" id="M171" style="vertical-align:-0.3499298pt" version="1.1" viewbox="-0.0498162 -8.34882 37.2711 8.69875" width="37.2711pt" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink"><g transform="matrix(.013,0,0,-0.013,0,0)"><path d="M615 290C615 392 563 448 529 448C511 448 491 441 484 434L483 425C518 400 546 349 546 273C546 158 504 46 417 46C381 46 356 77 356 142C356 184 380 293 392 334L387 340L307 323C305 288 296 228 287 188C265 94 221 52 180 52C144 52 112 89 112 171C112 278 164 372 241 430L226 454C106 394 23 288 23 155C23 40 79 -12 139 -12C184 -12 245 32 285 85C292 31 322 -12 376 -12C423 -12 470 18 501 45C570 104 615 184 615 290Z"></path></g><g transform="matrix(.013,0,0,-0.013,11.927,0)"><path d="M537 353L508 390C487 357 455 333 417 333C389 333 344 353 309 370C265 391 212 414 172 414C122 414 79 382 50 340L81 307C101 339 134 364 172 364C198 364 245 343 280 326C324 305 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Advances in High Energy Physics

fig6

Figure 6

Figure 6: A General Method for Transforming Nonphysical Configurations in BPS States 