Many Body Effects on Optical Properties of Graphene

By Subhasis Ghosh

Physical Sciences, Jawaharlal Nehru University, New Deli, India

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Abstract

Graphene, a two-­dimensional (2D) material shows remarkable optical and electronic properties, such as a linear energy dispersion, chirality and half-­integer quantum Hall effect. Multilayer graphene flakes, held together by weak van der Waals forces have also attracted attention due to their stacking dependent electronic and optical properties. Interestingly, a vast majority of these properties can be understood in terms of a non-interacting picture. In particular, the optical conductivity of monolayer graphene in the near infrared and visible range has been found to be independent of frequency, and equal to e2/4Ñ’. From experimental investigations of the optical properties of chemically exfoliated mono and multilayered graphene flakes, we probe the effect of electron-electron interactions on the universal optical transmittance and excitons in graphene. The electron-­electron or Coulomb interaction strength is varied both by modulating the dielectric constant of the exfoliating solvent, as well as changes in the carrier density. To vary the carrier density controllably, a method has been developed to dope (n-type and p-type) graphene monolayers through charge tranfer interaction by trapping selected oganic molecules between graphene and underneat substrates. Controllability has been demonstrated in terms of shift in Raman spectra and Dirac point in graphene monolayers. We find that the universality is robust throughout the visible range of the spectrum, and this is consistent with chiral symmetry as its origin. It has been shown that universality is broken if chiral symmetry can be broken. This is further supported by changes in the excitonic features which could disrupt the chiral symmetry. The shift and broadening of excitonic features are found to impact the onset of universality at low wavelengths. Our experiments also help to verify the theoretically predicted transmittance spectra in the presence of Coulomb interactions and resolve the discrepancy in the numerical factor governing the magnitude and frequency dependence of the transmittance in monolayer.

Bio

Subhasis Ghosh Subhasis Ghosh is professor of physics in School of Physical Sciences, Jawaharlal Nehru University, New Delhi. He graduated from University of Calcutta and received Ph.D. from Indian Institute of Sciences, Bangalore. Then he spent a couple of years at Max Planck Institute, Stuttgart, as a research associate. He has published more than 100 papers in reputed research journals. His research interests are transport and optical properties of condensed- and nano-phase of organic and inorganic semiconductors, in particular, (i) magnetism in oxide semiconductors, (ii) physics and technology of organic field effect transistors, and (iii) physics and technology of Dirac-Weyl materials (graphene, MoS2) and graphene based field effect transistor.

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Researchers should cite this work as follows:

  • Subhasis Ghosh (2016), "Many Body Effects on Optical Properties of Graphene," https://nanohub.org/resources/24654.

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Room 1001, Birck Nanotechnology Center, Purdue University, West Lafayette, IN

Tags

Many Body Effects on Optical Properties of Graphene
  • Many Body Effects on Optical Properties of Graphene 1. Many Body Effects on Optical P… 0
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  • Research Activities 2. Research Activities 22.489155822489156
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  • Plan of this talk 3. Plan of this talk 174.44110777444112
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  • What is graphene? 4. What is graphene? 232.8661995328662
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  • Novel Phenomena in Graphene 5. Novel Phenomena in Graphene 276.00934267600934
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  • 2 different ways of orienting bonds 6. 2 different ways of orienting … 347.84784784784785
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  • Bandstructure of Monolayer Graphene 7. Bandstructure of Monolayer Gra… 473.70704037370706
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  • Unit Cell 8. Unit Cell 511.87854521187859
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  • Tight binding model of monolayer graphene 9. Tight binding model of monolay… 553.65365365365369
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  • Low Energy Properties 10. Low Energy Properties 645.77911244577911
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  • Schrodinger equation to Dirac equation at low energy 11. Schrodinger equation to Dirac … 778.31164497831162
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  • Electrons in usual solids (Schrodinger equation) 12. Electrons in usual solids (Sch… 845.7123790457124
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  • Plan of this talk 13. Plan of this talk 1002.1688355021689
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  • Growth and Characterization Graphene 14. Growth and Characterization Gr… 1011.7117117117117
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  • How we grow graphene monolayer 15. How we grow graphene monolayer 1017.1171171171171
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  • Controllability & Reproducibility 16. Controllability & Reproducibil… 1032.1988655321989
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  • Organic Molecules Also with water 17. Organic Molecules Also with wa… 1040.7407407407409
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  • Atomic Force Microscopy 18. Atomic Force Microscopy 1153.2866199532866
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  • Transnission electron microscopy 19. Transnission electron microsco… 1176.2429095762429
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  • Excellent Control of No of Layers 20. Excellent Control of No of Lay… 1234.4678011344679
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  • Plan of this talk 21. Plan of this talk 1299.8665331998666
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  • 97.7% 22. 97.7% 1348.2816149482817
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  • What about bilayer, trilayer…….multilayer ? 23. What about bilayer, trilayer  1483.8505171838506
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  • Untitled: Slide 24 24. Untitled: Slide 24 1509.9099099099099
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  • Universal in monolayer to multilayer graphene. 25. Universal in monolayer to mult… 1696.52986319653
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  • Monolayer 26. Monolayer 1973.8738738738739
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  • Bilayer Graphene : 4 atoms per unit cell 27. Bilayer Graphene : 4 atoms per… 2045.2118785452119
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  • H. Min and A. H. MacDonald, Phys. Rev. Lett. 103, 067402 (2009). 28. H. Min and A. H. MacDonald, Ph… 2170.0033366700036
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  • Inspite of inter layer coupling 29. Inspite of inter layer couplin… 2245.6456456456458
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  • Plan of this talk 30. Plan of this talk 2284.9516182849516
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  • What is the effect of e-e interaction on this universality ? 31. What is the effect of e-e inte… 2315.7824491157826
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  • Europhys. Lett. 83, 17005 (2008) (c=0.01) Phys. Rev. B 80, 193411 (2009) (c=0.51) Phys. Rev. B 86, 115408 (2012). (c=0.12) 32. Europhys. Lett. 83, 17005 (200… 2321.287954621288
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  • Schrodinger Materials-Dirac Materials 33. Schrodinger Materials-Dirac Ma… 2398.7320653987322
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  • How to dope graphene ? 34. How to dope graphene ? 2482.3490156823491
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  • Various routes to dope Graphene 35. Various routes to dope Graphen… 2490.9242575909243
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  • -low mobility -disorder 36. -low mobility -disorder 2553.3533533533537
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  • Impermeability of Graphene 37. Impermeability of Graphene 2673.8071404738071
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  • Untitled: Slide 38 38. Untitled: Slide 38 2689.3893893893896
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  • Doping tunability: Donor and acceptor nature of trapped molecules 39. Doping tunability: Donor and a… 2729.2959626292959
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  • DFT calculations 40. DFT calculations 2782.8495161828496
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  • Toluene 41. Toluene 2842.8428428428429
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  • DMF 42. DMF 2958.9589589589591
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  • PC 43. PC 3245.4120787454121
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  • ↑ ᵋ 44. ↑ ᵋ 3270.0033366700036
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  • Untitled: Slide 45 45. Untitled: Slide 45 3288.7554220887555
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  • DFT Results 46. DFT Results 3320.3536870203538
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  • Untitled: Slide 47 47. Untitled: Slide 47 3323.4567901234568
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  • Untitled: Slide 48 48. Untitled: Slide 48 3336.036036036036
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  • Untitled: Slide 49 49. Untitled: Slide 49 3369.7030363697031
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  • Plan of this talk 50. Plan of this talk 3374.5412078745412
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  • How to break universality ? 51. How to break universality ? 3444.377711044378
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  • How to break CHIRAL SYMMETRY in GRAPHENE ? 52. How to break CHIRAL SYMMETRY i… 3459.4928261594928
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  • Exciton in Graphene 53. Exciton in Graphene 3496.4631297964634
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  • Universality is broken. 54. Universality is broken. 3552.5859192525859
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  • Strong Effect of e-e Interaction 55. Strong Effect of e-e Interacti… 3589.055722389056
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  • Conclusions 56. Conclusions 3648.0146813480146
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  • Thank You 57. Thank You 3705.5388722055391
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