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Surface segregation is studied via the evolution of reflection high-energy electron diffraction (RHEED) patterns under different values of As 4 BEP for InGaAs films. When the As 4 BEP is set to be zero, the RHEED pattern keeps a 4×3/(n×3) structure with increasing temperature, and surface segregation takes place until 470 C. The RHEED pattern develops into a metal-rich (4×2) structure as temperature increases to 495 C. The reason for this is that surface segregation makes the In inside the InGaAs film climb to its surface. With the temperature increasing up to 515 C, the RHEED pattern turns into a GaAs(2×4) structure due to In desorption. While the As 4 BEP comes up to a specific value (1.33×10 4 Pa–1.33×10 3 Pa), the surface temperature can delay the segregation and desorption. We find that As 4 BEP has a big influence on surface desorption, while surface segregation is more strongly dependent on temperature than surface desorption.
Surface segregation is studied via the evolution of reflection high-energy electron diffraction (RHEED) patterns under different values of As 4 BEP for InGaAs films. When the As 4 BEP is set to zero, the RHEED pattern keeps a 4 × 3 / ( n × 3) structure with increasing temperature, and surface segregation takes place until 470 C. The RHEED pattern develops into a metal-rich (4 × 2) structure as temperature increases to 495 C. The reason for this is that surface segregation makes the With the temperature increasing up to 515 C, the RHEED pattern turns into a GaAs (2 × 4) structure due to In desorption. While the As 4 BEP comes up to a specific value (1.33 × 10 4 Pa-1.33 × 10 3 Pa), the surface temperature can delay the segregation and desorption. We find that As 4 BEP has a big influence on surface desorption, while surface segregation is more dependent on temperature than surface desorption.