Charged-Particle Multiplicity Moments as Described by Shifted Gompertz Distribution in <span class="nowrap"><svg xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg" style="vertical-align:-0.2723999pt" id="M1" height="14.5241pt" version="1.1" viewBox="-0.0657574 -14.2517 30.442 14.5241" width="30.442pt"><g transform="matrix(.017,0,0,-0.017,0,0)"><path id="g113-102" 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"/></g><g transform="matrix(.012,0,0,-0.012,7.104,-7.578)"><path id="g54-36" d="M556 236V289H337V504H275V289H56V236H275V-4H337V236H556Z"/></g><g transform="matrix(.017,0,0,-0.017,15.129,0)"><use xlink:href="#g113-102"/></g><g transform="matrix(.012,0,0,-0.012,22.234,-7.578)"><path id="g54-33" d="M556 236V289H56V236H556Z"/></g></svg>,</span> <span class="nowrap"><svg xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg" style="vertical-align:-4.5268pt" id="M2" height="17.7864pt" version="1.1" viewBox="-0.0657574 -13.2596 20.5595 17.7864" width="20.5595pt"><g transform="matrix(.017,0,0,-0.017,0,0)"><path id="g113-113" 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 -142L218 -1C238 -10 266 -12 283 -12C351 3 429 48 483 105C543 168 570 242 570 304ZM482 289C482 161 380 33 304 33C278 33 248 51 233 69L303 396C326 400 352 403 369 403C428 403 482 380 482 289Z"/></g><rect height="0.8612076" width="10.214014800000001" x="10.1774772" y="-12.3326016"/><g transform="matrix(.017,0,0,-0.017,10.177,0)"><use xlink:href="#g113-113"/></g></svg>,</span> and <svg xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg" style="vertical-align:-4.52687pt" id="M3" height="13.4804pt" version="1.1" viewBox="-0.0657574 -8.95353 19.3538 13.4804" width="19.3538pt"><g transform="matrix(.017,0,0,-0.017,0,0)"><use xlink:href="#g113-113"/></g><g transform="matrix(.017,0,0,-0.017,8.972,0)"><use xlink:href="#g113-113"/></g></svg> Collisions at High Energies

<div>Comparison of normalised factorial moments for <svg height="10.2124pt" id="M224" style="vertical-align:-3.42943pt" version="1.1" viewbox="-0.0498162 -6.78297 14.662 10.2124" width="14.662pt" 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="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 -142L218 -1C238 -10 266 -12 283 -12C351 3 429 48 483 105C543 168 570 242 570 304ZM482 289C482 161 380 33 304 33C278 33 248 51 233 69L303 396C326 400 352 403 369 403C428 403 482 380 482 289Z"></path></g><g transform="matrix(.013,0,0,-0.013,6.797,0)"><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 -142L218 -1C238 -10 266 -12 283 -12C351 3 429 48 483 105C543 168 570 242 570 304ZM482 289C482 161 380 33 304 33C278 33 248 51 233 69L303 396C326 400 352 403 369 403C428 403 482 380 482 289Z"></path></g></svg> and <svg height="13.4746pt" id="M225" style="vertical-align:-3.4295pt" version="1.1" viewbox="-0.0498162 -10.0451 15.5754 13.4746" width="15.5754pt" 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="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 -142L218 -1C238 -10 266 -12 283 -12C351 3 429 48 483 105C543 168 570 242 570 304ZM482 289C482 161 380 33 304 33C278 33 248 51 233 69L303 396C326 400 352 403 369 403C428 403 482 380 482 289Z"></path></g><rect height="0.65243" width="7.73789" x="7.71021" y="-9.34288"></rect><g transform="matrix(.013,0,0,-0.013,7.71,0)"><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 -142L218 -1C238 -10 266 -12 283 -12C351 3 429 48 483 105C543 168 570 242 570 304ZM482 289C482 161 380 33 304 33C278 33 248 51 233 69L303 396C326 400 352 403 369 403C428 403 482 380 482 289Z"></path></g></svg> interactions at the same c.m. energy in the same rapidity window.</div>

Advances in High Energy Physics

fig15

Figure 15

Figure 15: Charged-Particle Multiplicity Moments as Described by Shifted Gompertz Distribution in <span class="nowrap"><svg xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg" style="vertical-align:-0.2723999pt" id="M1" height="14.5241pt" version="1.1" viewBox="-0.0657574 -14.2517 30.442 14.5241" width="30.442pt"><g transform="matrix(.017,0,0,-0.017,0,0)"><path id="g113-102" 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"/></g><g transform="matrix(.012,0,0,-0.012,7.104,-7.578)"><path id="g54-36" d="M556 236V289H337V504H275V289H56V236H275V-4H337V236H556Z"/></g><g transform="matrix(.017,0,0,-0.017,15.129,0)"><use xlink:href="#g113-102"/></g><g transform="matrix(.012,0,0,-0.012,22.234,-7.578)"><path id="g54-33" d="M556 236V289H56V236H556Z"/></g></svg>,</span> <span class="nowrap"><svg xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg" style="vertical-align:-4.5268pt" id="M2" height="17.7864pt" version="1.1" viewBox="-0.0657574 -13.2596 20.5595 17.7864" width="20.5595pt"><g transform="matrix(.017,0,0,-0.017,0,0)"><path id="g113-113" 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 -142L218 -1C238 -10 266 -12 283 -12C351 3 429 48 483 105C543 168 570 242 570 304ZM482 289C482 161 380 33 304 33C278 33 248 51 233 69L303 396C326 400 352 403 369 403C428 403 482 380 482 289Z"/></g><rect height="0.8612076" width="10.214014800000001" x="10.1774772" y="-12.3326016"/><g transform="matrix(.017,0,0,-0.017,10.177,0)"><use xlink:href="#g113-113"/></g></svg>,</span> and <svg xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg" style="vertical-align:-4.52687pt" id="M3" height="13.4804pt" version="1.1" viewBox="-0.0657574 -8.95353 19.3538 13.4804" width="19.3538pt"><g transform="matrix(.017,0,0,-0.017,0,0)"><use xlink:href="#g113-113"/></g><g transform="matrix(.017,0,0,-0.017,8.972,0)"><use xlink:href="#g113-113"/></g></svg> Collisions at High Energies 

Advances in High Energy Physics

Charged-Particle Multiplicity Moments as Described by Shifted Gompertz Distribution in , , and Collisions at High Energies

Figure 15