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Theory of phonon-assisted luminescence: application to h-BN

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In this talk, I present a theory of phonon-assisted luminescence in terms of non-equilibrium Green's functions and time-dependent perturbation theory. This theory is then applied to the phonon-assisted luminescence in hexagonal boron nitride

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Theory of phonon-assisted luminescence: application to h-BN

  1. 1. Theory of phonon­assisted  luminescence: application to h­BN Claudio Attaccalite
  2. 2. Opto­electronic devices
  3. 3. Light emission
  4. 4. The problem of indirect semiconductors Indirect band gap semiconductors are not good for  photonics/optoelectronics
  5. 5. Silicon Laser : solutions Nanostructures Defects  and more…. hybrid lasers etc...
  6. 6. Silicon Laser in the news
  7. 7. The other colors and the UV
  8. 8. Hexagonal Boron Nitride h­BN is a  layered  crystal homo­structural to graphite. As graphite, h­BN can be easily exfoliated, and for this  reason it finds applications as lubrificant .
  9. 9. Hexagonal Boron Nitride h­BN has a large band  gap and it’s transparent  h­BN emits light in the  ultraviolet
  10. 10. Breaking news on h-BN !!! Direct­bandgap properties and evidence for  ultraviolet lasing of h­BN single crystal K. Watanabe et al. Nature Materials 3, 404 (2004)*
  11. 11. Breaking news on h-BN !!! Direct­bandgap properties and evidence for  ultraviolet lasing of h­BN single crystal K. Watanabe et al. Nature Materials 3, 404 (2004)* Hexagonal boron nitride is an indirect band­gap  semiconductor G. Cassabois et al.,  Nature Photonics, 10, 262 (2016)* *) results from Luminescence measurements
  12. 12. Internal quantum yield 50% ZnO Bright Luminescence from Indirect and Strongly Bound Excitons in h-BN L. Schué, L. Sponza et al., Phys. Rev. Lett. 122, 067401(2019)
  13. 13. Internal quantum yield 50% 0.1% ZnO Diamond Bright Luminescence from Indirect and Strongly Bound Excitons in h-BN L. Schué, L. Sponza et al., Phys. Rev. Lett. 122, 067401(2019)
  14. 14. Internal quantum yield 45% 0.1% ZnO DiamondhBN 50% Bright Luminescence from Indirect and Strongly Bound Excitons in h-BN L. Schué, L. Sponza et al., Phys. Rev. Lett. 122, 067401(2019)
  15. 15. h­BN band structure and ARPES Direct observation of the band structure in bulk hexagonal boron nitride H. Henck, et al. PRB 95, 085410(2017)
  16. 16. h­BN optical properties Excitons in boron nitride nanotubes: dimensionality effects. Wirtz, Ludger, Andrea Marini, and Angel Rubio. " PRL 96, 126104 (2006) RPA
  17. 17. h­BN optical properties Excitons in boron nitride nanotubes: dimensionality effects. Wirtz, Ludger, Andrea Marini, and Angel Rubio. " PRL 96, 126104 (2006) RPA BSE
  18. 18. Electron loss spectroscopy on h­BN
  19. 19. Direct Observation of the Lowest Indirect Exciton State in the Bulk of Hexagonal Boron Nitride R. Schuster C. Habenicht, M. Ahmad, M. Knupfer, B. Büchner, PRB 97, 041201 (2018) May we probe indirect nature of h­BN  with EELS?
  20. 20. Origin of the EELS peaks Loss function  Peaks of L(q, ω) can be put in relation  to inter­band excitations (  Im[∝ ε(q, ω)]) and plasmon resonances (|ε|   0)≈ Exciton interference in hexagonal boron nitride L. Sponza, H. Amara, C. Attaccalite, F. Ducastelle, A. Loiseau PRB 97 (7), 075121(2017) Direct Observation of the Lowest Indirect Exciton State in the Bulk of Hexagonal Boron Nitride R. Schuster C. Habenicht, M. Ahmad, M. Knupfer, B. Büchner, PRB 97, 041201 (2018)
  21. 21. What about luminescence?
  22. 22. Luminescence Theory NON­EQUILIBRIUM GREEN’S FUNCTION Theory of photoluminescence in semiconductors  K. Hannewald, S. Glutsch, and F. Bechstedt  PRB 62, 4519 (2000). Non­equilibrium Bethe­Salpeter  equation  Emission  DENSITY MATRIX Semiconductor Quantum Optics M. Kira and S. W. Koch Cambridge Univ. Press. (2012). Absorption In the limit of low  excited carriers
  23. 23. Phonon­assisted  absorption and emission Average on phonon modes Derive BSE in presence of EPC (first order, cumulant) Polaron transformation Perturbation Theory in the excitonic space
  24. 24. Average on phonons +non-perturbative +an-harmonic effects -no dynamical effects -supercells Average  on phonon  modes Stochastic Approach to Phonon­Assisted Optical  Absorption M. Zacharias, C. E. Patrick, and F. Giustino Phys. Rev. Lett. 115, 177401(2015) Electron–phonon coupling from finite  differences B. Monserrat J. of Phys.: Cond. Matt. 30, 083001(2018)
  25. 25. BSE with EPC Theory of exciton­phonon coupling  G. Antonius and S. G. Louie, arXiv:1705.04245  Phonon satellite bands in the spectral function of  ZnO from first principles Y. Chan G. Antonius and S. Louie Meeting/MAR18/Session/R07.14 +dynamical effects +no-supercells -complicated eqs. -dynamics BSE First order  self­energy or  cumulant etc..
  26. 26. Polaron transformation Phonon­assisted luminescence .. A. Chernikov, et al. Phys. Rev. B 85, 035201(2012)  Phonon sidebands  in semiconductor luminescence  T. Feldtmann, M. Kira, and S. W. Koch Phys. Stat. Solidi B 246, 332(2009) +stardard BSE +non-perturbative -difficult improv.?
  27. 27. Perturbation theory  in the excitonic space Effect of Exciton­Phonon Coupling in the  Calculated Optical Absorption of Carbon  Nanotubes V. Perebeinois, J. Tersoff, P. Avoris PRL 94, 027402(2005) Phonon and Electronic Nonradiative Decay  Mechanisms of Excitons in Carbon Nanotubes V.i Perebeinos and P. Avouris Phys. Rev. Lett. 101, 057401 (2008) +simple eqs. -miss no-exc terms. -high orders more difficult
  28. 28. 30 Westart with theelectron-phonon Hamiltonian: Time­dependent perturbation  theory in the excitonic space 1/3 electron-phonon coupling in thetwo-particlebasis Westart with theelectron-phonon Hamiltonian: rotation in theexcitonic basis First order correction to theexcitonic wave-functions:
  29. 29. 31 Time­dependent perturbation  theory in the excitonic space 2/3 Phonon Emission Phonon Absorption Usethenew wave-function to calculateemission and absorption perturbativecorrection to thedipolescan bemapped in aderivative respect to thephonon mode One­shot calculation of temperature­dependent optical spectra .. M. Zacharias and F. Giustino  Physical Review B 94, 075125 (2016).
  30. 30. Infrared absorption spectrum of germanium LH. Hall, J. Bardeen, FJ. Blatt  Phys. Rev., 95, 559 (1954) Electron–phonon coupling from finite differences B. Monserrat J. of Phys.: Cond. Matt. 30, 083001(2018) perturbative correction of the  BSE due to the electron­ phonon coupling + electron­phonon matrix  elements calculated  by finite difference We constructed a non­diagonal  supercell that maps K and M  points at  Time­dependent perturbation  theory in the excitonic space 3/3
  31. 31. Which phonons are involved  in luminescence?
  32. 32. Luminescence in h­BN Theory* Experiment Hexagonal boron nitride is an  indirect band­gap  semiconductor G. Cassabois et al.,   Nature Photonics, 10, 262 (2016) Theory of phonon­assisted  luminescence in solids: application  to hexagonal boron nitride E Cannuccia,et al. Rev. B 99, 081109(R) (2019) *) similar results obtained also by F. Paleari et al:  arXiv:1810.08976.  
  33. 33. Luminescence intensity  from bulk to monolayer This ratio in MoS2  is about 104 Dimensionality effects on the luminescence properties of hBN L. Schué et al.,  Nanoscale 8, 6986 (2016). Excitons in few­layer hexagonal boron nitride: Davydov splitting  and surface localization F. Paleari,  et al.  2D Materials 5, 045017 (2018)
  34. 34. Conclusions Codes  Exciton interference in hexagonal boron nitride L. Sponza, H. Amara, C. Attaccalite, F. Ducastelle, A. Loiseau Phys. Rev. B 97, 075121 (2017) Theory of phonon-assisted luminescence in solids: application to hexagonal boron nitride E. Cannuccia, B. Monserrat and C. Attaccalite Rev. B 99, 081109(R) (2019) Direct and indirect excitons in boron nitride polymorphs: a story of atomic configuration and electronic correlation L Sponza, H Amara, C Attaccalite, S Latil, T Galvani, F Paleari, L Wirtz, F. Ducastelle Phys. Rev. B 98, 125206 (2018) ● The indirect nature of hBN can be probed by EELS ● We extended luminescence theory to include phonon scattering and reproduce the luminescence spectra ● Why so efficient? References 
  35. 35. Acknowledgments  Lorenzo Sponza François Ducastelle Hakim Amara Elena Cannuccia Bartomeu Monserrat Elena Cannuccia L. Wirtz,   M. Gruning,   F. Paleari,   S. Latil 
  36. 36. What next?  Higher­order  phonon sidebands  Temperature  dependence of  luminescence Overtones of interlayer shear modes in the phonon- assisted emission spectrum of hexagonal boron nitride. T. Q. P. Vuong et al, PRB, 95(4), 045207 (2017) Bright Luminescence from Indirect and Strongly Bound Excitons in h-BN L. Schué, L. Sponza et al., Phys. Rev. Lett. 122, 067401(2019)
  37. 37. Theory vs experiments Angular resolved electron energy loss spectroscopy in hexagonal boron nitride F. Fossard et al. Phys. Rev. B 96 115304 (2017)
  38. 38. Theory: how to calculate e(w)  Excitons in boron nitride single layer T. Galvani et al., Phys. Rev. B 94, 125303 (2016)G. Strinati, Nuovo Cimento 11, 1 (1988)
  39. 39. EELS ­ theory and experiments  Exciton interference in hexagonal boron nitride L. Sponza, et al. PRB 97(7), 075121(2017)

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