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<div>The energy dependence of the total cross sections for the process of <svg height="15.0613pt" id="M203" style="vertical-align:-3.4033pt" version="1.1" viewbox="-0.0498162 -11.658 73.4386 15.0613" width="73.4386pt" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink"><rect height="0.69159" width="7.79008" x="0" y="-9.55172"></rect><g transform="matrix(.013,0,0,-0.013,0,0)"><path d="M573 302C573 402 527 451 414 451C386 451 343 446 313 437L330 513L320 522C295 508 261 484 243 463L230 415C194 400 159 383 126 359L131 330C159 344 187 357 222 368L109 -147C96 -204 80 -214 18 -223L13 -255L256 -244L259 -212L236 -210C184 -205 180 -195 191 -141L219 -1C240 -10 268 -12 284 -12C352 4 431 48 484 104C543 166 573 240 573 302ZM481 290C481 165 381 37 305 37C280 37 249 56 235 71L302 395C328 399 353 402 372 402C427 402 481 378 481 290Z" id="g50-113"></path><glyph.data ascent="3443" descent="-2856" horiz-adv-x="597" vert-adv-y="597"></glyph.data></g><g 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Advances in High Energy Physics

fig6

Figure 6

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Advances in High Energy Physics

Discovery Potential for the Neutral Charmonium-Like by Annihilation

Figure 6