1975
DOI: 10.1103/physrevlett.35.1022
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Picosecond Optical Measurements of Band-to-Band Auger Recombination of High-Density Plasmas in Germanium

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Cited by 102 publications
(26 citation statements)
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“…The third term refers to free carrier diffusion with ambipolar diffusion coefficient D = 67 cm 2 /s, 25 the fourth term to radiative recombination with lifetime τ = 100 µs, 26 and the final term to Auger recombination with Auger coefficient A = 2 × 10 -31 cm 6 /s. 27,28 This pair of coupled differential equations was solved numerically using a time-and-spacediscreet pulse propagation simulation, with consideration given to the profile of the micropulses in time and space (assumed to be Gaussian in both cases), multiple reflections inside the sample using the usual Fresnel coefficients, and to the accumulation of carriers between micropulses. The simulation code was verified for accuracy by comparison with simpler analytical models.…”
Section: Methodsmentioning
confidence: 99%
“…The third term refers to free carrier diffusion with ambipolar diffusion coefficient D = 67 cm 2 /s, 25 the fourth term to radiative recombination with lifetime τ = 100 µs, 26 and the final term to Auger recombination with Auger coefficient A = 2 × 10 -31 cm 6 /s. 27,28 This pair of coupled differential equations was solved numerically using a time-and-spacediscreet pulse propagation simulation, with consideration given to the profile of the micropulses in time and space (assumed to be Gaussian in both cases), multiple reflections inside the sample using the usual Fresnel coefficients, and to the accumulation of carriers between micropulses. The simulation code was verified for accuracy by comparison with simpler analytical models.…”
Section: Methodsmentioning
confidence: 99%
“…Like in conventional semiconductors, strong optical excitation results in a population-inverted state [15][16][17][18][19][20]. On the other hand, photo-generated electron-hole pairs in a conventional semiconductor typically relax by Auger recombination [21][22][23][24], a process that is strongly suppressed in photo-excited graphene due to the abence of occupied states at the bottom of the conduction band. Hence, in contrast to conventional semiconductors, primary thermalization events in graphene are dominated by impact ionization [25][26][27][28], where the excess energy of the photo-excited electron is used to generate additional electron-hole pairs.…”
Section: Introductionmentioning
confidence: 99%
“…However, previous studies on the ultrafast spectroscopy of Ge showed inconsistent results. [8][9][10][11][12][13] For example, instead of observing optical gain, in Refs. 8 and 9, a significant decrease in transmittance at 1550 nm was observed upon ultrafast pulse pumping with photon energy well above the direct gap of Ge ($360 meV higher).…”
mentioning
confidence: 99%
“…U intervalley scattering absorption, which has been observed recently in the infrared absorption spectra of 0.25% tensile strained n þ Ge films 14 yet never reported in n þ bulk Ge. 8 On the other hand, pressure-dependent ab initio calculation shows that the contributions of various phonons to the intervalley scattering are quite dependent on the conduction band energy separation. 25 Further combination of tensile strain and phonon engineering with nanostructures 26 may help to achieve this goal.…”
mentioning
confidence: 99%