Excited Neutrino Search Potential of the FCC-Based Electron-Hadron Colliders

<div>The total cross sections as a function of the excited neutrino mass at the <svg height="10.2124pt" id="M114" style="vertical-align:-3.42943pt" version="1.1" viewbox="-0.0498162 -6.78297 12.3263 10.2124" width="12.3263pt" 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="M391 364C391 409 353 448 295 448C249 448 198 426 152 393C65 331 23 225 23 139C23 14 96 -12 146 -12C198 -12 280 9 367 101L351 124C300 78 242 48 194 48C129 48 109 107 109 162V191C208 213 391 266 391 364ZM313 350C313 305 268 261 113 223C132 334 187 381 217 398C227 404 244 405 261 405C290 405 313 385 313 350Z" id="g113-102"></path></g><g transform="matrix(.013,0,0,-0.013,4.469,0)"><path d="M570 304C570 398 525 448 414 448C385 448 343 445 312 434L329 511L321 518C297 504 262 482 244 460L233 411C195 397 159 381 128 358L135 332C160 347 189 360 224 373L111 -147C97 -210 84 -218 17 -231L13 -257L254 -247L259 -218L233 -216C183 -212 177 -202 189 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Advances in High Energy Physics

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Figure 3

Figure 3: Excited Neutrino Search Potential of the FCC-Based Electron-Hadron Colliders 