On the Optical Stark Effect of Excitons in InGaAs Prolate Ellipsoidal Quantum Dots

<div>The dependence of transition rate on the photon energy of probe laser in a prolate ellipsoidal quantum dot in the absence of the pump laser (dotted line) and in the presence of the pump laser with different amplitude of pump laser <svg height="17.0656pt" id="M196" style="vertical-align:-5.474199pt" version="1.1" viewbox="-0.0498162 -11.5914 68.4638 17.0656" width="68.4638pt" 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="M686 28C612 35 607 44 591 112C563 234 541 360 519 489L489 666L457 658L147 121C100 40 89 36 24 28L17 0H240L250 28C168 34 159 41 190 101L262 237H482C495 180 503 137 510 91C517 47 514 35 441 28L433 0H677L686 28ZM475 280H285L429 541H431L475 280Z"></path></g><g transform="matrix(.0091,0,0,-0.0091,10.244,3.132)"><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 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Journal of Nanomaterials

fig9

Figure 9

Figure 9: On the Optical Stark Effect of Excitons in InGaAs Prolate Ellipsoidal Quantum Dots 