Three-Level Optical Stark Effect of Excitons in GaAs Cylindrical Quantum Wires

<div>The wavelength of probe laser <svg height="12.5794pt" id="M132" style="vertical-align:-3.29107pt" version="1.1" viewbox="-0.0498162 -9.28833 11.5574 12.5794" width="11.5574pt" 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="M529 97L508 118C475 75 449 58 438 58C428 58 421 66 415 104C393 234 374 403 364 496C345 670 307 712 254 712C220 712 174 691 153 669L161 645C176 653 194 658 206 658C237 658 261 640 278 562C287 522 290 483 293 434C223 269 110 105 23 9L32 -12C59 -6 85 0 108 7C152 64 251 252 300 366C307 297 315 221 337 82C346 24 363 -12 393 -12C425 -12 475 13 529 97Z"></path></g><g transform="matrix(.0091,0,0,-0.0091,7.761,3.132)"><path d="M329 433H203L239 587L230 596L147 534L123 433H57L30 395L34 388H115L61 129C37 16 59 -12 85 -12C147 -12 222 58 260 98L241 125C212 95 160 62 144 62C132 62 127 71 138 126L192 386L305 394L329 433Z"></path></g></svg> as a function of wire radius.</div>

Journal of Nanomaterials

fig7

Figure 7

Figure 7: Three-Level Optical Stark Effect of Excitons in GaAs Cylindrical Quantum Wires 