Plasmonic nanoparticles

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Plasmonic nanoparticles are particles whose electron density can couple with electromagnetic radiation of wavelengths that are far larger than the particle due to the nature of the dielectric-metal interface between the medium and the particles: unlike in a pure metal where there is a maximum limit on what size wavelength can be effectively coupled based on the material size.[1]

What differentiates these particles from normal surface plasmons is that plasmonic nanoparticles also exhibit interesting scattering, absorbance, and coupling properties based on their geometries and relative positions.[2][3] These unique properties have made them a focus of research in many applications including solar cells, spectroscopy, signal enhancement for imaging, and cancer treatment.[4][5]

Plasmons are the oscillations of free electrons that are the consequence of the formation of a dipole in the material due to electromagnetic waves. The electrons migrate in the material to restore its initial state; however, the light waves oscillate, leading to a constant shift in the dipole that forces the electrons to oscillate at the same frequency as the light. This coupling only occurs when the frequency of the light is equal to or less than the plasma frequency and is greatest at the plasma frequency that is therefore called the resonant frequency. The scattering and absorbance cross-sections describe the intensity of a given frequency to be scattered or absorbed. Many fabrication processes or chemical synthesis methods exist for preparation of such nanoparticles, depending on the desired size and geometry.

The nanoparticles can form clusters (the so-called "plasmonic molecules") and interact with each other to form cluster states. The symmetry of the nanoparticles and the distribution of the electrons within them can affect a type of bonding or antibonding character between the nanoparticles similarly to molecular orbitals. Since light couples with the electrons, polarized light can be used to control the distribution of the electrons and alter the mulliken term symbol for the irreducible representation. Changing the geometry of the nanoparticles can be used to manipulate the optical activity and properties of the system, but so can the polarized light by lowering the symmetry of the conductive electrons inside the particles and changing the dipole moment of the cluster. These clusters can be used to manipulate light on the nano scale.[6]


The quasistatic equations that describe the scattering and absorbance cross-sections for very small spherical nanoparticles are:

where is the wavenumber of the electric field, is the radius of the particle, is the relative permittivity of the dielectric medium and is the relative permittivity of the nanoparticle defined by

also known as the Drude Model for free electrons where is the plasma frequency, is the relaxation frequency of the charge carries, and is the frequency of the electromagnetic radiation. This equation is the result of solving the differential equation for a harmonic oscillator with a driving force proportional to the electric field that the particle is subjected to. For a more thorough derivation, see surface plasmon.

It logically follows that the resonance conditions for these equations is reached when the denominator is around zero such that

When this condition is fulfilled the cross-sections are at their maximum.

These cross-sections are for single, spherical particles. The equations change when particles are non-spherical, or are coupled to 1 or more other nanoparticles, such as when their geometry changes. This principle is important for several applications.

Rigorous electrodynamic analysis of plasma oscillations in a spherical metal nanoparticle of a finite size was performed in [7].


Plasmonic solar cells[edit]

Due to their ability to scatter light back into the photovoltaic structure and low absorption, plasmonic nanoparticles are under investigation as a method for increasing solar cell efficiency.[8][4] Forcing more light to be absorbed by the dielectric increases efficiency.[9]

Plasmons can be excited by optical radiation and induce an electric current from hot electrons in materials fabricated from gold particles and light-sensitive molecules of porphin, of precise sizes and specific patterns. The wavelength to which the plasmon responds is a function of the size and spacing of the particles. The material is fabricated using ferroelectric nanolithography. Compared to conventional photoexcitation, the material produced three to 10 times the current.[10][11]


In the past 5 years plasmonic nanoparticles have been explored as a method for high resolution spectroscopy. One group utilized 40 nm gold nanoparticles that had been functionalized such that they would bind specifically to epidermal growth factor receptors to determine the density of those receptors on a cell. This technique relies on the fact that the effective geometry of the particles change when they appear within one particle diameter (40 nm) of each other. Within that range, quantitative information on the EGFR density in the cell membrane can be retrieved based on the shift in resonant frequency of the plasmonic particles.[12]

Cancer treatment[edit]

Preliminary research indicates that the absorption of gold nanorods functionalized with epidermal growth factor is enough to amplify the effects of low power laser light such that it can be used for targeted radiation treatments.[13]

See also[edit]


  1. ^ Eustis, S., El-Sayed, M. A., "Why gold nanoparticles are more precious than pretty gold: Noble metal surface plasmon resonance and its enhancement of the radiative and nonradiative properties of nanocrystals of different shapes", The Royal Society of Chemistry, vol. 35, pp. 209-217, 2006.
  2. ^ Chen, Tianhong; Pourmand, Mahshid; Feizpour, Amin; Cushman, Bradford; Reinhard, Björn M. (2013-07-03). "Tailoring Plasmon Coupling in Self-Assembled One-Dimensional Au Nanoparticle Chains through Simultaneous Control of Size and Gap Separation". The Journal of Physical Chemistry Letters. 4 (13): 2147–2152. doi:10.1021/jz401066g. ISSN 1948-7185. PMC 3766581Freely accessible. PMID 24027605. 
  3. ^ Zeng, Shuwen; Yu, Xia; Law, Wing-Cheung; Zhang, Yating; Hu, Rui; Dinh, Xuan-Quyen; Ho, Ho-Pui; Yong, Ken-Tye (2013). "Size dependence of Au NP-enhanced surface plasmon resonance based on differential phase measurement". Sensors and Actuators B: Chemical. 176: 1128. doi:10.1016/j.snb.2012.09.073. 
  4. ^ a b Yu, Peng; Yao, Yisen; Wu, Jiang; Niu, Xiaobin; Rogach, Andrey L.; Wang, Zhiming (2017-08-09). "Effects of Plasmonic Metal Core -Dielectric Shell Nanoparticles on the Broadband Light Absorption Enhancement in Thin Film Solar Cells". Scientific Reports. 7 (1). doi:10.1038/s41598-017-08077-9. ISSN 2045-2322. 
  5. ^ Wu, Jiang; Yu, Peng; Susha, Andrei S.; Sablon, Kimberly A.; Chen, Haiyuan; Zhou, Zhihua; Li, Handong; Ji, Haining; Niu, Xiaobin (2015-04-01). "Broadband efficiency enhancement in quantum dot solar cells coupled with multispiked plasmonic nanostars". Nano Energy. 13: 827–835. doi:10.1016/j.nanoen.2015.02.012. 
  6. ^ Chuntonov, Lev; Haran, Gilad (10 May 2011). "Trimeric Plasmonic Molecules: The Role of Symmetry". Nano Letters. 11 (6): 2440–2445. Bibcode:2011NanoL..11.2440C. doi:10.1021/nl2008532. PMID 21553898. Retrieved 1 December 2014. 
  7. ^ Belyaev B.A. and Tyurnev, V.V. "Resonances of Electromagnetic Oscillations in a Spherical Metal Nanoparticle," Microwave and Optical Technology Letters, 2016, Vol. 58, No 8, p. 1883. doi:10.1002/mop.29930
  8. ^ Yue, Zengji; Cai, Boyuan; Wang, Lan; Wang, Xiaolin; Gu, Min (2016-03-01). "Intrinsically core-shell plasmonic dielectric nanostructures with ultrahigh refractive index". Science Advances. 2 (3): e1501536. Bibcode:2016SciA....2E1536Y. doi:10.1126/sciadv.1501536. ISSN 2375-2548. PMC 4820380Freely accessible. PMID 27051869. 
  9. ^ Ferry, V. E., Munday, J. N., Atwater, H. A. " Design Considerations for Plasmonic Photovoltaics," Advanced Materials, vol. 22, Sept 2010.
  10. ^ "A new method for harvesting energy from light". KurzweilAI. Retrieved 2013-09-12. 
  11. ^ Conklin, D.; Nanayakkara, S.; Park, T. H.; Lagadec, M. F.; Stecher, J. T.; Chen, X.; Therien, M. J.; Bonnell, D. A. (2013). "Exploiting Plasmon-Induced Hot Electrons in Molecular Electronic Devices". ACS Nano. 7 (5): 4479–4486. doi:10.1021/nn401071d. PMID 23550717. 
  12. ^ Wang, J., Boriskina, S. V., Wang, H., Reinhard, B. M. "Illuminating Epidermal Growth Factor Receptor Densities on Filopodia through Plasmon Coupling," ACS Nano, vol. 5, pp. 6619-6628, 2011.
  13. ^ Rejiya, C.S., Kumar, J., Raji, V., Vibin, M., Abraham, A. "Laser Immunotherapy with Gold Nanorods Causes Selective Killing of Tumour Cells," Pharmacological Research, 2011.