Q-factor enhancement in all-dielectric anisotropic nanoresonators

Q-factor enhancement in all-dielectric anisotropic nanoresonators

Wei Liu wei.liu.pku@gmail.com College of Optoelectronic Science and Engineering, National University of Defense Technology, Changsha, Hunan 410073, China    Andrey E. Miroshnichenko Nonlinear Physics Centre, Research School of Physics and Engineering, Australian National University, Canberra, ACT 0200, Australia    Yuri S. Kivshar Nonlinear Physics Centre, Research School of Physics and Engineering, Australian National University, Canberra, ACT 0200, Australia

It is proposed and demonstrated that Q-factor of optical resonators can be significantly enhanced by introducing an extra anisotropic cladding. We study the optical resonances of all-dielectric core-shell nanoresonators and reveal that radially anisotropic claddings can be employed to squeeze more energy into the core area, leading to stronger light confinement and thus significant Q-factor enhancement. We further show that the required homogenous claddings of unusual anisotropy parameters can be realized through all-dielectric multi-layered isotropic structures, which offers realistic extra flexibilities of resonance manipulations for optical resonators.


Nonlinear Physics Centre, Research School of Physics and Engineering, Australian National University, Canberra, ACT 0200, Australia \SectionNumbersOff

Keywords: Q-factor Enhancement; Mie Scattering; All-Dielectric Nanoresonators.

Optical resonators serve almost ubiquitously as an indispensable platform for efficient light-matter interactions and constitute the cornerstone of many related fields 1. Different kinds of optical resonators correspond to different light confining mechanisms, which can be roughly categorized as: total internal reflection for whispering gallery resonators 2, 3, 1, photonic bandgap for photonic crystal cavities 4, 5, Anderson localization for random resonators 6, 7, electromagnetic surface waves for plasmonic and graphene resonators 8, 9, 10, 11, 12, 13, etc. For optical resonator based fundamental research and applications, such as cavity-enhanced spectroscopy and sensing 14, 15, cavity optomechanics 16, a nonlinear and quantum optics 17, 18, 19, high-Q resonators are required to achieve a significant field confinement and low scattering loss rate, thus providing an efficient platform for strong light-matter interactions.

To support high-Q resonances, the aforementioned mechanisms have different specific problems: photonic bandgap and random resonators are limited by fabrication and can not function beyond the diffraction limit; plasmonic and graphene resonators can be scaled down to the subwavelength spectral regime but, unfortunately, their performance is restricted by intrinsic losses of materials employed. Though extremely high-Q whispering gallery resonator is almost free from intrinsic loss and can be easily fabricated, it relies on the excitation of the high-order modes (higher-order mode corresponds to larger transverse light momentum, which leads to lower radiation losses and higher Q-factor 2, 20, 12) and, thus, is inevitably compromised by large footprint of the resonator and also large mode volume. It was found that the principle of total internal reflection (TIR) can be extended to the interface of isotropic and anisotropic materials 21, 22 (or the so-called relaxed total internal refection 23, 24, RTIR) and has been demonstrated that material anisotropy can be employed to accelerate the decay rate of evanescent waves, resulting in stronger light confinement capability in waveguiding systems 22, 23, 24.

Figure 1: (a) Schematic of the core-shell cylindrical resonator consisting of an isotropic core (refractive index and radius ) and a radially anisotropic cladding layer (radial index , transverse index and radius ). The anisotropy parameter is defined as and the incident plane wave to excite the TM resonances is polarized along direction. (b) Conventional TIR: the evanescent wave (dashed curve) resides within the lower-index () isotropic medium and decays exponentially away from the boundary. (c) RTIR: the evanescent wave decays much faster away from the boundary, which is due to the anisotropy of the medium involved.

In this paper, we study the resonances of all-dielectric core-shell cylindrical nanoresonators of nanowires from new perspectives of the total internal reflection at the interface of anisotropic media. To take advantage of the faster evanescent wave decay induced by the RTIR condition, we study a resonator that consists of an isotropic core and radially anisotropic cladding layer (the refractive index of the core is larger and smaller than the radial and transverse refractive index of the cladding layer, respectively). We show that such an anisotropic cladding can squeeze more energy of the mode into the core area, which results in stronger field confinement and thus larger Q-factors for resonances of various orders of the resonator. We further demonstrate that the cladding layer of naturally inaccessible anisotropy can be substituted by realistic multi-layered isotropic metamaterial structures without compromising the property of significant Q-factor enhancement. The principle we have revealed is general and renders new possibilities for manipulations of resonances in terms of Q-factor enhancement, which can play a critical role in many related research directions and applications, such as cavity-enhanced spectroscopy and sensing, cavity optomechanics, resonant quantum and nonlinear optics, lasing and imaging, etc.

1 Results and Discussions

We begin with one of the most fundamental structures of two-dimensional (2D) nonmagnetic cylindrical resonator as is shown in Figure 1(a): the core layer (of radius ) is isotropic and the refractive index is ; the cladding layer (of radius ) is radially anisotropic on the plane with radial index of and transverse (along the azimuthal direction) index of ; the anisotropy parameter is defined as . The resonant modes of 2D cylindrical resonators can be classified into two sets: (i) the transverse-magnetic (TM) modes with no magnetic field in the direction of propagation, and (ii) the transverse-electric (TE) modes with no electric fields along the direction 25, 26, 27. Since the TE resonances are not affected by the radial anisotropy of the shell layer, here we study only the TM resonances with electric fields in the plane. As a result, the incident plane wave is fixed to be polarized along the direction (in terms of the electric field). According to the proposed principle of RTIR 23, 24, the radial anisotropy of the cladding layer can reduce the skin depth of the evanescent waves, as is shown schematically in Figure 1(b) and (c): Figure 1(b) shows the conventional TIR, where an evanescent wave (dashed curve) resides within the lower index media, and it decays exponentially away from the boundary; Figure 1(c) shows the RTIR geometry, where the evanescent waves decays faster, which is induced by the anisotropic layer employed.

Figure 2: (a) Scattering efficiency spectra for a homogeneous () and isotropic cylindrical resonator ( and  nm). Both the total scattering efficiency spectrum (black curve) and those contributions from ED (red curve), MD (green curve) and EQ (blue curve) are shown. Two points D ( nm) and Q ( nm), which corresponds to the resonant positions of ED and EQ respectively, are marked in (a) and the corresponding near fields (partial electric field intensity: ) are shown in (b) and (c). (d) The refractive index dependence of the Q-factors for the ED and EQ supported. The curves corresponds to the Q-factors obtained through Eq.(2) while circles correspond to Q-factors calculated based on FWHM of the scattering spectra.

As a first step, we study the scattering properties of the structure shown in Figure 1(a). This problem can be solved analytically 25, 28, 29, and the scattering efficiency (scattering cross-section divided by the geometrical cross-section of the structure) can be expressed as:


where is the angular wave number in the background material (vacuum in our work); is the radius of the outmost layer; and () are the scattering coefficients, which depend on the anisotropy parameter (see the Methods section for more details). To be more specific, corresponds to the magnetic dipole (MD), which has all the electric fields along the transverse direction on the plane 26. As the result, the MD resonance is only dependent on the transverse (azimuthal) refractive index of the cylindrical resonator, and consequently it is not affected by the radial anisotropy. While () corresponds to the electric resonance of the m order [e.g., and correspond to the electric dipole (ED) and electric quadrupole (EQ), respectively]. In Figure 2(a) we show the scattering efficiency spectra for a homogenous and isotropic cylinder (radius  nm and refractive index ) in terms of the total scattering together with the contributions from the first three dominant resonances: MD (green curve), ED and EQ. As MD is not affected by the radial anisotropy, throughout this work we focus only on the ED and EQ resonances which are both anisotropy sensitive. The indicated points D and Q in Figure 2(a) correspond to the resonant positions of ED and EQ respectively:  nm and  nm. The corresponding near-field distributions at those two points are shown in Figure 2(b) and (c). We show here only the partial fields of the ED and EQ resonances (fields associated with other multipoles are neglected), which as a result exhibit typical pure ED and EQ characteristics respectively.

Figure 3: (a) Scattering efficiency spectra for both ED (red curve) and EQ (blue curve) supported by the isotropic core-anisotpric shell cylindrical resonator of inner radius  nm () and outer radius  nm (, ). For comparison, the ED and EQ scattering efficiency spectra for the homogenous and isotropic () resonator of radius  nm are also shown as dashed curves. The total scattering efficiency spectrum are shown as black curves (dashed for the isotropic case and solid for the anisotropic case). Four resonant points for both cases and ( nm,  nm,  nm,  nm) are indicated and the corresponding total near-field distributions () are shown in (c)-(f). (b) The dependence of the Q-factor for both ED and EQ on anisotropy parameter. The indexes of the cladding layer is constrained by and thus the anisotropy parameter is . (g) The dependence of and for ED on the anisotropy parameter.

Then, we study the Q-factors of the ED and EQ resonances of the homogeneous cylindrical nanowire. If we use to denote the complex resonant angular-frequency of the m order resonance, which corresponds to the singular point of the scattering matrix of the resonator, then the corresponding Q-factor can be expressed as 25, 3:


It is worth noticing that for a homogenous cylindrical resonator, the scattering matrix is dependent only on the normalized radius and refractive index . That is to say, for fixed mode order , is proportional to the resonator radius. As a result, according to Eq.(2), is -independent and depends only on the refractive index . The dependence of the Q-factors of ED and EQ on refractive index is shown in Figure 2(d). As is expected, with increasing the Q-factors of both ED and EQ increases monotonically, since larger momentum mismatch between the resonator and the background leads to stronger energy confinement capability 25, 3, 30, 12. We note that besides the definition shown in Eq.(2) [the results have been shown by curves in Figure 2(d)], Q-factors can be also obtained via calculating the full width at half maximum (FWHM) of the scattering spectrum 3: , where denotes the central resonant scattering frequency [such as the points indicated in Figure 2(a)]; and is width of the scattering spectrum curve measured between the points where the magnitudes are half of the maximum amplitude at the central resonant position. The calculated results through scattering spectrum are shown also in Figure 2(d) by circles and it is obvious they agree well with those obtained through Eq.(2). Throughout this paper, we focus on the ED and EQ resonances of the lowest frequency [besides the resonant peaks shown in Figure 2(a), there are other scattering peaks for ED and EQ at higher frequencies 25, 31] and calculate the Q-factor through Eq.(2). Nevertheless, it should be reminded that for ED and EQ of higher frequencies and for other ways to define and/or calculate the Q factors (or non-Lorentzian asymmetric line-widths of the scattering spectrum 32, 33), the conclusions drawn in our work are still valid.

As a next step, we switch to the cylindrical resonator with an anisotropic cladding and demonstrate how the RTIR mechanism can be employed to enhance the Q-factor and energy confinement ability of the resonances. Firstly we study the core-shell resonator with an isotropic core ( nm) and an anisotropic cladding. For better comparison with the homogenous resonator investigated above, we set the core index as , cladding layer radius as  nm and the indexes of the cladding satisfy: . As a result, the anisotropy parameter can be expressed as: . The scattering spectra of is shown in Figure 3(a), where only the contributions from ED and EQ are shown [for clearer comparison, results of homogenous case with the same outmost layer radius  nm shown already in Figure 2(a) are re-plotted here by dashed curves]. As is expected from the RTIR principle, the anisotropic cladding improves the energy confinement and thus can enhance the Q-factor for both ED and EQ, which can be justified by the presence of sharper and narrower scattering curves with anisotropy materials incorporated 25, 3. To quantitatively characterize the Q-factor enhancement, in Figure 3(b) we show the dependence of Q-factors of both resonances on the anisotropy parameter, which further verifies the anisotropy-origin of such enhancement. In principle, higher Q-factor indicates better energy confinement capability of the resonator. To confirm this directly, in Figure 3(a), the positions of the ED and EQ resonances for both isotropic and anisotropic cases are indicated by and ( nm,  nm,  nm,  nm) and the corresponding total electric field (combining the contributions of all multipoles) intensity () are shown in Figure 3(c)-(f). Compared to the isotropic case [Figure 3(c) and (e)], when anisotropy is introduced [Figure 3(d) and (f)] more energy of the mode is squeezed into the core-layer, indicating better energy confinement and as a result leading to more significant field enhancement [we note that to make the field distributions clearer, different scales of the color-bars for the fields at different points are employed in Figure 3(c)-(f)]. It worth mentioning that compared to the symmetric field distributions shown in Figure 2, those shown in 3 are asymmetric as here we show the total fields contributed by all the multipoles. This is also the case for 4-5.

To further quantify the capability of better energy confinement and more significant field enhancement, we denote the energy stored inside the core and shell cladding as and , which can be defined respectively as:


where and correspond to electric fields along the radial and transverse direction respectively, which can be calculated analytically 25, 28, 34; the total stored energy inside the resonator is ; and the core energy ratio is . In Figure 3(g) we show the dependence of and on the anisotropy parameter for the ED resonance. As is clearly shown, with larger both the total stored energy and the core energy ratio would increase, which proves convincingly tighter energy confinement and larger field enhancement inside the resonator that accompany the efficient Q-factor enhancement shown in Figure 3(a).

In the discussions above, we fixed the overall resonator radius to investigate the Q-factor dependence on anisotropy parameter. Now we fix the anisotropy parameter (with  nm, and ) and study the relationship between Q-factor and the shell cladding radius . The results are summarized in Figure 4(a) as solid curves for both ED and EQ resonances. It is clear that the Q-factor does not increase monotonically with increasing cladding radius, and there is actually an optimal radius of the shell to achieve the highest Q-factor for each resonance. To reveal the mechanism behind, we select three points for both ED [ nm,  nm (optimal radius for EQ),  nm] and EQ [ nm,  nm (optimal radius for ED),  nm], and show the corresponding total near-field distributions () in Figure 4(b)-(g). It is shown that before the optimal radius, for both resonances more energy is squeezed into the core region with increasing cladding radius, which leads to both Q-factor and near-field enhancement. In a sharp contrast, after the optimal radius, with increasing more and more energy will leak out from the core, reducing both the Q-factor and the field intensity within the resonator. This is due to the fact that when the cladding layer is becoming sufficiently large, resonances can be formed within the cladding layer, with comparably negligible energy distributed within the core layer [see Figure 4(d) and (g)]. To confirm directly this process of mode distribution transformation between the core and the shell cladding, we plot the Q-factor-radius relationship of a homogeneous anisotropic cylindrical resonator with and for both ED (dashed red curve) and EQ (dashed blue curve) in Figure 4(a): it is obvious that for sufficiently large the Q-factor would converge to that of a homogeneous anisotropic cylinder [it is worth mentioning that similar to the isotropic case studied in Figure 2, the Q-factor of an anisotropic homogeneous resonator is also independent on the radius]. The results presented here could be confusing at a first glance, as it is taken for granted that increasing the anisotropic layer width would not break the condition of RTIR and thus would not result in reduced Q-factor or near-field intensity. But one has to keep in mind that RTIR (and TIR itself) is a concept of geometric optics, and thus cannot be applied in a universal way. When the cladding layer is sufficiently large, potential distributions for photons would be changed drastically 20, resulting in more energy confinement within the cladding layer and undermining the features of Q-factor and near-field enhancement.

Figure 4: (a) Dependence of Q-factor (solid red curve for ED and solid blue curve for EQ) on the shell cladding radius with the following fixed parameters:  nm, , and . The dashed curves corresponds to the Q-factors (which is radius independent) for both ED (red) and EQ (blue) of the homogeneously anisotropic cylindrical resonator of and . Three points have been indicated for the core-shell configuration [ED resonance:  nm,  nm,  nm; EQ resonance: nm,  nm,  nm] and the total near-field distributions in terms of electric field intensity at those points are shown in (b)-(g) where  nm.


Figure 5: (a) Schematic of the cylindical resonator consisting of an isotropic core (refractive index and radius  nm) and a multi-layered cladding made of alternate and isotropic layers and the width of both layer is  nm. There are five layers of each medium, which leads to and  nm. (b) Scattering efficiency spectra of the cylindrical resonator shown in (a) for both ED (red solid curves) and EQ (red solid curves). The circles corresponds to the scattering efficiency spectra of a two-layered cylindrical resonator with the same core as that shown in (a) and a homogenous anisotropic cladding layer of , and  nm: both the spectra of ED (red circles) and EQ (blue circles) are shown. The total scattering efficiency spectrum is also shown by black curve (multilayer) and black circles (anisotropic cladding). Two points ( nm) and ( nm), which correspond to the resonant positions of ED and EQ respectively, are marked in (b) and the corresponding total near-field distributions () are shown in (c) and (e) for the multi-layered isotropic cylindrical resonator, and in Figure 5(d) and (f) for thetwo-layered core-shell resonator with a homogenous anisotropic cladding.

Up to now, we have demonstrated the efficient Q-factor enhancement based on anisotropic materials. Unfortunately, for natural materials the anisotropy parameters employed here may not be realistic. Such a problem is not insurmountable considering the recent development in the field of artificial metamaterials, where other extreme refractive indices and anisotropy parameters can be achieved 35, 36, 37, 30, 38, 39, 34. Here, we employ a cladding layer consisting of multilayers of two kinds of realistic isotropic materials ( and respectively and ) to substitute the homogeneous anisotropic layer, as shown in Figure 5(a). According to the effective medium theory 40, 39, 34, the effective indexes for the multi-layered cladding in the plane are:


where is the filling factor of the layer of index . When the largest anisotropy parameter can be achieved: for positive and , and . As a proof of concept, we set and (e.g. for Germanium), which leads to the following parameters for : , and . The structure we employ is shown schematically in Figure 5(a), where the cladding is made of alternate and layers and the width of both layer is  nm [which is far smaller then the effective wavelength and then the effective medium theory Eq.(4) can be applied]. There are five layers of each medium, which makes and the overall cladding layer of radius  nm (for direct comparisons with the previous discussions, the core is set to be isotropic with radius  nm and of ). The scattering efficiency spectra of such isotropic -layered cylindrical resonator can be calculated analytically 25 and the results are shown in Figure 5(b) by solid curves for both ED and EQ resonances. It is worth mentioning that here the periodicity of the cladding is not important as far as the layer width is far smaller than the wavelength when the effective medium theory can be applied. This distinguishes our design from those based on photonic bandgap structures 4, 5. To verify the effective medium theory applied for the multi-layered cladding, we also show in Figure 5(b) by circles the scattering efficiency spectra when the multi-layered cladding is replaced by a homogenous anisotropic layer [according to Eq.(4)] of , , and . It is obvious that both sets of results agree excellently well, indicating the same Q-factor for both cases [this has already been included in Figure 3(b)]. The two indicated points and in Figure 5(a) correspond to the resonant position of ED and EQ respectively:  nm and  nm. The corresponding total near-field distributions () are shown in Figure 5(c) and (e) for the multi-layered isotropic cylindrical resonator, and in Figure 5(d) and (f) for the core-shell anisotropic resonator. The strong field confinement is clearly demonstrated by comparing Figure 5(c-f) with Figure 3(c) and (e). Although the field distributions within the cladding layer are contrastingly different (the fields are significantly enhanced within the layers due to the continuity condition along the radial direction, which is similar to that shown in Ref. 41), the fields inside the core and outside the resonator are almost the same, proving further the feasibility of applying the RTIR principle to obtain high-Q cavity resonators.

2 Conclusion and Outlook

In summary, based one the recently proposed principle of light localization in anisotropic media, we have studied all-dielectric cylindrical resonators with an isotropic core and anisotropic cladding, focusing on the Q-factor enhancement of the resonances supported. Due to the RTIR effect, we have demonstrated that more energy can be confined within the core-layer structure, which leads to simultaneous Q-factor and near-field enhancement for the resonances. We have also shown that with a fixed radial anisotropy parameter of the cladding, there exist optimal cladding layer widths to achieve the highest Q-factors for resonances of different orders, thus succeeding in revealing the limitation of the RTIR principle. To verify the feasibility of our approach to achieve high-Q resonators, we have shown that naturally inaccessible anisotropy parameters of the cladding can be realized by employing multi-layered isotropic metamaterial structures with the property of significant Q-factor enhancement preserved.

It is worth mentioning that though in this work we confine our study to the two lowest order of modes (dipole and quadruple modes) of cylindrical structures, the principle we have demonstrated is quite general. The Q-factor enhancement can certainly be achieved in spherical resonators and resonators of other shapes, for other kinds of anisotropy such as magnetic anisotropy and for modes of higher orders. Actually the higher the mode order is, the stronger the Q-factor enhancement effect would be [see Figure 3(b)]. Since more energy is confined within the core of the resonator by the RTIR effect, it is expected that for a cluster of such resonators the near-field coupling between them can significantly be reduced 42, 43. For the proof of concept demonstration, we have employed the multi-layered positive-index isotropic cladding with modest anisotropy parameter of . Other more unusual anisotropy parameters, even including those complex ones, can be made available for realistic applications relying on the artificial metamaterials 35, 36, 37, 30, 38, 39, 34. We believe that our work of employing effective anisotropic media to enhance the Q-factor opens a new dimension of freedom for manipulations of various resonators, which can incubate many new resonator based fundamental research and applications in the fields of cavity-enhanced spectroscopy and sensing, cavity optomechanics, resonant quantum and nonlinear optics, lasing and imaging, etc.

3 Methods

The seminal problem of two-dimensional (2D) plane wave scattering by cylindrical resonators (single or multilayered) consisting of isotropic materials has been studied analytically 25 [e.g., for the scattering configuration shown in 5(a) with the corresponding scattering efficiency shown in 5(b) by solid curves]. Such analytical investigations have also been extended to 2D cylindrical resonators made of radially anisotropic materials 28, 29 [e.g., for geometries shown in 1(a)]. It has been revealed that for both isotropic and radially-anisotropic cases, the expressions for the field expansion coefficients (both inside and outside the resonator) and far-field scattering properties are identical [see Eq.(1)], except that in the anisotropic case the orders of some Bessel and Hankel functions need to be modified by the anisotropy parameter.

To be more specific, we take for example the simplest case of a homogeneous radially anisotropic cylinder (radius and anisotropy parameter ) in vacuum. The scattering efficiency can be expressed by Eq.(1) where the scattering coefficients for the incident plane waves of TM polarizations can be expressed as  25, 28:


where is the modified function order , and are the Bessel and Hankel functions of the first kind 25 and the accompanying primes indicate their differentiation with respect to the entire argument. Obviously the results will be reduced to the those of isotropic case when . It is clear that the MD mode of is independent of the anisotropy, which is consistent with our former argument based on field distribution. Similar to Eq.(5), all the field expansion coefficients within the resonator can be obtained in all the layers through simply modifying the function order when the radially anisotropic materials are present. As a result the energy stored within the resonator [see 3] can also be calculated analytically.

4 Acknowledgements

We acknowledge a financial support from the National Natural Science Foundation of China (Grant number: ), the Australian Research Council and the Basic Research Scheme of College of Optoelectronic Science and Engineering, National University of Defence Technology. W. L. thanks the Nonlinear Physics Centre for a warm hospitality during his visit to Canberra.


  • Vahala 2004 Vahala, K. Optical microcavities; World Scientific, 2004.
  • Lam et al. 1992 Lam, C. C.; Leung, P. T.; Young, K. Explicit asymptotic formulas for the positions, widths, and strengths of resonances in Mie scattering. J. Opt. Soc. Am. B 1992, 9, 1585.
  • Yariv and Yeh 2006 Yariv, A.; Yeh, P. Photonics: optical electronics in modern communications; Oxford University Press, Inc., 2006.
  • Akahane et al. 2003 Akahane, Y.; Asano, T.; Song, B. S.; Noda, S. High-Q photonic nanocavity in a two-dimensional photonic crystal. Nature 2003, 425, 944.
  • Joannopoulos 2008 Joannopoulos, J. D. Photonic crystals : molding the flow of light, 2nd ed.; Princeton University Press: Princeton, 2008.
  • Abrahams 2010 Abrahams, E. 50 years of Anderson Localization; World Scientific, 2010; Vol. 24.
  • Segev et al. 2013 Segev, M.; Silberberg, Y.; Christodoulides, D. N. Anderson localization of light. Nat. Photon. 2013, 7, 197.
  • Boardman 1982 Boardman, A. D. Electromagnetic surface modes; Wiley: Chichester; New York, 1982.
  • Maier 2007 Maier, S. A. Plasmonics : fundamentals and applications; Springer: New York, 2007.
  • Min et al. 2009 Min, B.; Ostby, E.; Sorger, V.; Ulin Avila, E.; Yang, L.; Zhang, X.; Vahala, K. High-Q surface-plasmon-polariton whispering-gallery microcavity. Nature 2009, 457, 455.
  • Koppens et al. 2011 Koppens, F. H.; Chang, D. E.; Garcia de Abajo, F. J. Graphene plasmonics: a platform for strong light-matter interactions. Nano letters 2011, 11, 3370.
  • Liu et al. 2015 Liu, W.; Oulton, R. F.; Kivshar, Y. S. Geometric interpretations for resonances of plasmonic nanoparticles. Sci. Rep. 2015, 5, 12148.
  • Li et al. 2015 Li, R.; Lin, X.; Lin, S.; Liu, X.; Chen, H. Tunable deep-subwavelength superscattering using graphene monolayers. Opt. Lett. 2015, 40, 1651.
  • Gagliardi and Loock 2014 Gagliardi, G.; Loock, H. P. Cavity-Enhanced Spectroscopy and Sensing; Springer, 2014.
  • Zhu et al. 2010 Zhu, J.; Ozdemir, S. K.; Xiao, Y. F.; Li, L.; He, L.; Chen, D. R.; Yang, L. On-chip single nanoparticle detection and sizing by mode splitting in an ultrahigh-Q microresonator. Nat. Photon. 2010, 4, 4649.
  • Aspelmeyer et al. 2014 Aspelmeyer, M.; Kippenberg, T. J.; Marquardt, F. Cavity optomechanics. Rev. Mod. Phys. 2014, 86, 1391.
  • Slusher et al. 1985 Slusher, R.; Hollberg, L.; Yurke, B.; Mertz, J.; Valley, J. Observation of squeezed states generated by four-wave mixing in an optical cavity. Phys. Rev. Lett. 1985, 55, 2409.
  • Haroche and Raimond 2006 Haroche, S.; Raimond, J. M. Exploring the Quantum: Atoms, Cavities, and Photons; Oxford Univ. Press, 2006.
  • Srinivasan and Painter 2007 Srinivasan, K.; Painter, O. Linear and nonlinear optical spectroscopy of a strongly coupled microdisk-quantum dot system. Nature 2007, 450, 862.
  • Johnson 1993 Johnson, B. R. Theory of morphology-dependent resonances: shape resonances and width formulas. J. Opt. Soc. Am. A 1993, 10, 343.
  • Chew 1995 Chew, W. C. Waves and fields in inhomogeneous media; IEEE Press New York, 1995.
  • Catrysse and Fan 2011 Catrysse, P. B.; Fan, S. Transverse electromagnetic modes in aperture waveguides containing a metamaterial with extreme anisotropy. Phys. Rev. Lett. 2011, 106, 223902.
  • Jahani and Jacob 2014 Jahani, S.; Jacob, Z. Transparent subdiffraction optics: nanoscale light confinement without metal. Optica 2014, 1, 96.
  • Jahani and Jacob 2015 Jahani, S.; Jacob, Z. Photonic skin-depth engineering. J. Opt. Soc. Am. B 2015, 32, 1346.
  • Kerker 1969 Kerker, M. The scattering of light, and other electromagnetic radiation; Academic Press: New York, 1969.
  • Liu et al. 2013 Liu, W.; Miroshnichenko, A. E.; Oulton, R. F.; Neshev, D. N.; Hess, O.; Kivshar, Y. S. Scattering of Core-Shell Nanowires with the Interference of Electric and Magnetic Resonances. Opt. Lett. 2013, 38, 2621.
  • Liu et al. 2015 Liu, W.; Zhang, J.; Lei, B.; Hu, H.; Miroshnichenko, A. E. Invisible nanowires with interfering electric and toroidal dipoles. Opt. Lett. 2015, 40, 2293.
  • Chen and Gao 2012 Chen, H.; Gao, L. Anomalous electromagnetic scattering from radially anisotropic nanowires. Phys. Rev. A 2012, 86, 033825.
  • Chen and Gao 2013 Chen, H.; Gao, L. Tunablity of the unconventional Fano resonances in coated nanowires with radial anisotropy. Opt. Express 2013, 21, 23619.
  • Yang et al. 2012 Yang, X.; Yao, J.; Rho, J.; Yin, X.; Zhang, X. Experimental realization of three-dimensional indefinite cavities at the nanoscale with anomalous scaling laws. Nat. Photon. 2012, 6, 450.
  • Liu 2015 Liu, W. Ultra-directional super-scattering of homogenous spherical particles with radial anisotropy. Opt. Express 2015, 23, 14734.
  • Ruan and Fan 2009 Ruan, Z.; Fan, S. Temporal Coupled-Mode Theory for Fano Resonance in Light Scattering by a Single Obstacle? J. Phys. Chem. C 2009, 114, 7324.
  • Tribelsky and Miroshnichenko 2015 Tribelsky, M. I.; Miroshnichenko, A. E. Giant In-Particle Field Concentration and Fano Resonances at Light Scattering by High-Refractive Index Particles. arXiv:1511.02931 2015,
  • Kim et al. 2015 Kim, K. H.; No, Y. S.; Chang, S.; Choi, J. H.; Park, H. G. Invisible Hyperbolic Metamaterial Nanotube at Visible Frequency. Sci. Rep. 2015, 5, 16027.
  • Soukoulis and Wegener 2011 Soukoulis, C. M.; Wegener, M. Past Achievements and Future Challenges in the Development of Three-Dimensional Photonic Metamaterials. Nat.Photon. 2011, 5, 523.
  • Zheludev and Kivshar 2012 Zheludev, N. I.; Kivshar, Y. S. From metamaterials to metadevices. Nat. Mater. 2012, 11, 917.
  • Choi et al. 2011 Choi, M.; Lee, S. H.; Kim, Y.; Kang, S. B.; Shin, J.; Kwak, M. H.; Kang, K. Y.; Lee, Y. H.; Park, N.; Min, B. A terahertz metamaterial with unnaturally high refractive index. Nature 2011, 470, 369.
  • Wu et al. 2014 Wu, C.; Salandrino, A.; Ni, X.; Zhang, X. Electrodynamical light trapping using Whispering-Gallery resonances in hyperbolic cavities. Phys. Rev. X 2014, 4, 021015.
  • Poddubny et al. 2013 Poddubny, A.; Iorsh, I.; Belov, P.; Kivshar, Y. Hyperbolic metamaterials. Nat. Photon. 2013, 7, 948.
  • Agranovich and Kravtsov 1985 Agranovich, V.; Kravtsov, V. Notes on crystal optics of superlattices. Solid State Commun. 1985, 55, 85.
  • Oulton et al. 2008 Oulton, R. F.; Sorger, V. J.; Genov, D. A.; Pile, D. F. P.; Zhang, X. A hybrid plasmonic waveguide for subwavelength confinement and long-range propagation. Nat. Photon. 2008, 2, 496.
  • Liu et al. 2012 Liu, W.; Miroshnichenko, A. E.; Neshev, D. N.; Kivshar, Y. S. Broadband Unidirectional Scattering by Magneto-Electric Core-Shell Nanoparticles. ACS Nano 2012, 6, 5489.
  • Miroshnichenko and Kivshar 2012 Miroshnichenko, A. E.; Kivshar, Y. S. Fano Resonances in All-Dielectric Oligomers. Nano Lett. 2012, 12, 6459.
Comments 0
Request Comment
You are adding the first comment!
How to quickly get a good reply:
  • Give credit where it’s due by listing out the positive aspects of a paper before getting into which changes should be made.
  • Be specific in your critique, and provide supporting evidence with appropriate references to substantiate general statements.
  • Your comment should inspire ideas to flow and help the author improves the paper.

The better we are at sharing our knowledge with each other, the faster we move forward.
The feedback must be of minimum 40 characters and the title a minimum of 5 characters
Add comment
Loading ...
This is a comment super asjknd jkasnjk adsnkj
The feedback must be of minumum 40 characters
The feedback must be of minumum 40 characters

You are asking your first question!
How to quickly get a good answer:
  • Keep your question short and to the point
  • Check for grammar or spelling errors.
  • Phrase it like a question
Test description