1998
DOI: 10.1088/0953-8984/10/26/017
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A source of terahertz coherent phonons

Abstract: Resonant tunnelling in a double-barrier heterostructure (DBHS) designed in order to produce an intense coherent emission of phonons is studied theoretically. This emission is achieved when the energy difference between the first excited level and the ground state in the well is close to the LO-phonon energy. The LO phonons emitted during the electron transition decay into a pair of (LO and TA) phonons that leave the well in the [111] direction. These secondary TA phonons are coherent and form a beam that we ca… Show more

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Cited by 23 publications
(27 citation statements)
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References 51 publications
(68 reference statements)
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“…Different methods of coherent THz phonon generation (and amplification) have been suggested [15,16], but no turn-key THz acoustic analogue of the laser has been developed to date. However, previous studies of acoustic gain in semiconductor SLs have been made both theoretically [17,18] and experimentally [12], which have shown great promise for THz phonon amplification and oscillation in these systems.…”
Section: Introductionmentioning
confidence: 99%
“…Different methods of coherent THz phonon generation (and amplification) have been suggested [15,16], but no turn-key THz acoustic analogue of the laser has been developed to date. However, previous studies of acoustic gain in semiconductor SLs have been made both theoretically [17,18] and experimentally [12], which have shown great promise for THz phonon amplification and oscillation in these systems.…”
Section: Introductionmentioning
confidence: 99%
“…In these RTDs even when the LO phonons are confined to the well, they have a short lifetime [11] because they decay into a pair of LO and transverse acoustic (TA) phonons. The expectation that the secondary TA phonons can form a coherent beam inspired a proposal for the generation of a coherent sound beam (in the region of 2 THz) which justifies the name of SASER in analogy with LASER [12,13] for such device. The critical intensities required for stimulated decay of the primary phonons were recently discussed [14].…”
Section: Introductionmentioning
confidence: 99%
“…The devices considered previously in this context Refs. [13,15] required an energy difference between the first two electronic states in the well satisfying the resonant condition E 1 2 E 0 ¼ Év 0 (see Fig. 1(b)).…”
Section: Introductionmentioning
confidence: 99%
“…1); optomechanical devices at megahertz frequencies2; optically pumped trapped ions at very low frequencies3; and acoustic amplification at about half a THz, due to electron–phonon interactions in semiconductor superlattices (SLs)45. The latter is particularly important as it addresses the generation of coherent acoustic waves in the THz frequency range with corresponding acoustic wavelengths in the nanometre range, useful in a number of applications6.…”
mentioning
confidence: 99%