Slab thickness tuning approach for solidstate strong coupling between photonic crystal slab nanocavity and a quantum dot
 Gengyan Chen^{1},
 JingFeng Liu^{1},
 Haoxiang Jiang^{1},
 XiaoLu Zhuo^{1},
 YiCong Yu^{1},
 Chongjun Jin^{1} and
 XueHua Wang^{1}Email author
DOI: 10.1186/1556276X8187
© Chen et al.; licensee Springer. 2013
Received: 18 March 2013
Accepted: 6 April 2013
Published: 23 April 2013
Abstract
The quality factor and mode volume of a nanocavity play pivotal roles in realizing the strong coupling interaction between the nanocavity mode and a quantum dot. We present an extremely simple method to obtain the mode volume and investigate the effect of the slab thickness on the quality factor and mode volume of photonic crystal slab nanocavities. We reveal that the mode volume is approximatively proportional to the slab thickness. As compared with the previous structure finely optimized by introducing displacement of the air holes, via tuning the slab thickness, the quality factor can be enhanced by about 22%, and the ratio between the coupling coefficient and the nanocavity decay rate can be enhanced by about 13%. This can remarkably enhance the capability of the photonic crystal slab nanocavity for realizing the strong coupling interaction. The slab thickness tuning approach is feasible and significant for the experimental fabrication of the solidstate nanocavities.
Keywords
Photonic crystal slab nanocavity Slab thickness Quality factor Mode volume Strong coupling interaction Cavity quantum electrodynamicsBackground
Photonic crystals (PCs) [1–3] are artificial dielectric nanostructures with a periodic variation of dielectric function in the length scale of optical wavelength, and provide a unique way to control the decay kinetic of the quantum emitters inside the PCs due to photonic bandgaps and a strong inhomogeneity of electromagnetic fields [4–10]. Since many sophisticated and mature fabrication technologies developed in microelectronics and optoelectronics can be applied to its fabrication, the PC slab, which is a thin semiconductor slab with twodimensional (2D) periodicity along the slab plane, has been investigated energetically in depth both theoretically and experimentally [11–15]. Owing to the strong vertical optical confinement and the 2D photonic bandgap effect, the overall spontaneous emission rate of the quantum emitter inside the PC slab decreases substantially [14].
By introducing an artificial point defect into the PC slab, the PC slab nanocavity [3] can be formed. The point defect traps a localized nanocavity mode, which decays in inverse proportion to the quality factor of the PC slab nanocavity. The PC slab nanocavity and a single twolevel quantum dot can realize the strong coupling interaction and thus constitute the solidstate strong coupling system (SSSCS) [16]. In this SSSCS, there is reversible exchange of a single photon between the quantum dot and the nanocavity mode before the photon leaks out of the nanocavity. The SSSCS realizes many fascinating but genuine quantum behaviors in cavity quantum electrodynamics [17], e.g., vacuum Rabi splitting [16, 18, 19] and lasing under strong coupling [20]. The SSSCS not only provides test beds for fundamental quantum physics but also has important applications in quantum information processing [21–23].
The realization of the strong coupling interaction relies on the condition that the coupling coefficient between the nanocavity mode and the quantum dot exceeds the intrinsic decay rate of the nanocavity [17]. To fulfill this condition, a great deal of efforts [24–27] have been devoted to design the nanocavities with the ultrahigh quality factor and ultrasmall mode volume.
To enhance the quality factor, various types of the PC slab nanocavities have been presented. The prominent types of the PC slab nanocavities with ultrahigh quality factor include the PC L3 nanocavity [25] and PC heterostructure nanocavity [27]. The PC L3 nanocavity is formed by missing three air holes in a line and displacing several pairs of air holes at both edges of the nanocavity, which can increase the quality factor substantially by following the principle that light should be confined gently in order to be confined strongly [25, 26]. The PC heterostructure nanocavity is formed by adjusting the lattice constant of several rows of air holes and introducing mode gap difference in the PC slab waveguide, which can obtain unprecedentedly ultrahigh quality factor by following the same principle [27]. Obviously, this principle requires the elaborately designed and optimized PC slab nanocavity with highly fine tuning of the positions and radii of the air holes around the nanocavity center, commonly up to the nanometer scale accuracy, which is a great challenge due to the technical limits of the semiconductor process [28]. However, the effect of the PC slab thickness on the quality factor has not been reported.
Besides the quality factor, another important parameter for the realization of the strong coupling interaction is the mode volume of the nanocavity. Traditionally, the mode volume is calculated by simulating and then integrating the electric field distribution of the nanocavity mode around the whole nanocavity region [24–26, 29] (see Equation 6). This is a rather timeconsuming and difficult task. Obviously, a simple and efficient numerical method for the calculation of mode volume is desirable and remains a challenge so far.
In this paper, we present an extremely simple method to determine the volume of a nanocavity mode and investigate the effect of the slab thickness on the quality factor and mode volume of the PC slab nanocavities based upon projected local density of states for photons [30]. It is found that the mode volume monotonously expands with the increasing slab thickness. As compared with the previous structure finely optimized by introducing displacement of the air holes, via tuning the slab thickness, the quality factor can be enhanced by about 22%, and the ratio between the coupling coefficient and the nanocavity decay rate can be enhanced by about 13%. Our work provides a feasible approach to manipulate the quality factor and mode volume in the experiment. This is significant for the realization of the strong coupling interaction between the PC slab nanocavity and a quantum dot, which has important applications in quantum information processing [21–23].
Methods
where r_{0} is the location; ω, the frequency; $\widehat{d}$, the orientation; and E_{ λ }(r) and ω_{ λ }, the normalized eigen electric field and eigen frequency of the λ th eigenmode of the nanostructure, respectively.
where E_{ c }(r) and ω_{ c } are the normalized eigen electric field and eigen frequency of the nanocavity mode, respectively.
where κ = ω_{ c } / Q is the decay rate of the realistic nanocavity with loss and Q represents the quality factor. Apparently, when κ is infinitely small, Equation 3 of the loss nanocavity approaches to Equation 2 of the lossless nanocavity.
where ${\rho}_{\mathit{cpm}}={\rho}_{c}\left({\mathbf{r}}_{0m},{\omega}_{c},{\widehat{d}}_{m}\right)$ is the peak value of the PLDOS at the location r_{0m} along the direction ${\widehat{d}}_{m}$. Therefore, as soon as the PLDOS at the location r_{0m} along the direction ${\widehat{d}}_{m}$ is calculated by various numerical methods, ω_{ c }, κ, and ρ_{ cpm } can be determined by fitting the PLDOS by the Lorentz function of Equation 5. Based on them, we can finally obtain the mode volume of the nanocavity by Equation 8 and the quality factor of the nanocavity by Q = ω_{ c } / κ.
Traditionally [24–26, 29], the mode volume of the PC slab nanocavity is calculated directly by Equation 6. By this method, the electric field distribution of the nanocavity mode around the whole nanocavity region needs to be simulated and then integrated. This is rather timeconsuming. In contrast, using our method of Equation 8, we can calculate the mode volume simply and efficiently. We just need to calculate the PLDOS at only one known location and along one known direction, which make the calculation of the mode volume very efficient.
As mentioned previously, the realization of the strong coupling interaction requires that the coupling coefficient g exceeds the intrinsic decay rate of the nanocavity mode κ. Thus, the most important issue for the realization of the strong coupling is to increase the ratio of $g/\kappa \propto Q/\sqrt{V{\omega}_{c}}$[16], which can be obtained using our method.
Results and discussion
To compare our slab thickness tuning approach with previous air hole displacement approach, we investigate the PC L3 nanocavity that was finely optimized by the air hole displacement approach in [26], as shown in Figure 1a.
The 2D PC slab is composed of silicon (refractive index n = 3.4) with a triangular lattice of air holes. The lattice constant is a = 420 nm. The slab thickness is d = 0.6a, and the air hole radius is r = 0.29a. The PC L3 nanocavity is formed by missing three air holes in a line in the center of the PC slab and can be further optimized by firstly tuning the displacement A of the first nearest pair of air holes and then tuning the displacement B of the second nearest pair of air holes and, finally, the displacement C of the third nearest pair of air holes, as shown in Figure 1a.
The E_{ y } component of the electric field E_{ c }(r) of the nanocavity mode is shown in Figure 1b,c, obtained by finitedifference timedomain method [32]. This spatial distribution is typical among all the PC L3 nanocavities. Obviously, most electromagnetic energy of the nanocavity mode is localized in the three missed air holes due to the 2D photonic bandgap effect and is also confined inside the slab by the total internal reflection. The E_{ y } component reaches its maximum at the nanocavity center r_{0m} = (0, 0, 0).
However, as the three pairs of air holes near the PC L3 nanocavity center are further moved outward, the nanocavity mode is confined inside the nanocavity more and more gently [25], as shown in Figure 1b. Consequently, the mode volume of nanocavity mode becomes large, as shown in Figure 2c. The calculated mode volume of the optimized PC L3 nanocavity with air hole displacements A = 0.2a, B = 0.025a, and C = 0.2a is 0.0754 μm^{3}, which agrees well with the reported mode volume as 0.074 μm^{3} in [26]. This excellent agreement validates our method of Equation 8 for calculating the mode volume.
Based on the calculated quality factor, resonant frequency, and mode volume, we can obtain the ratio of g/κ, which assesses the PC L3 nanocavity for the realization of the strong coupling interaction between a quantum dot and the nanocavity mode. As the air hole displacements A, B, and C are tuned and optimized in turn, g/κ is also enhanced remarkably, as shown in Figure 2d, which is mainly due to the sharply decreased decay rate κ of the nanocavity.
As shown in Figure 3b, as we tune the slab thickness, the quality factor varies remarkably and reaches its maximum at the slab thickness d = 0.8a. By the slab thickness tuning approach, we can further optimize the quality factor from Q = 265,985 for d = 0.6a in [26] to Q = 325,121 for d = 0.8a, with increase of about 22%. This optimized PC L3 nanocavity with higher quality factor is desirable and beneficial to the realization of the SSSCS.
Along the vertical (z) direction perpendicular to the slab plane, the electric field of the nanocavity mode is mostly confined inside the slab by the total internal reflection, as shown in Figure 1c. Thus, when the slab thickness increases from d = 0.5a to d = 1.0a, the nanocavity mode is confined inside the slab more and more loosely, and hence, the mode volume expands almost linearly along with the increasing slab thickness, as shown in Figure 3c.
As we tune the slab thickness, the ratio of g/κ varies substantially and also reaches its maximum at the slab thickness d = 0.7a. The optimized g/κ at the slab thickness d = 0.7a is about 13% higher than that of d = 0.6a in [26]. From Figure 3d, we can notice that there is an optimization region for the slab thickness from d = 0.7a to 0.8a, in which the ratio g/κ varies little. This is very beneficial for the experimental fabrication of the PC L3 nanocavity.
In a word, the nanocavity mode is confined inside the PC L3 nanocavity by the 2D photonic bandgap effect along the slab plane and also by the total internal reflection in the outofplane direction. Thus, as we displace the air holes near the nanocavity center outwards or as we increase the slab thickness, the nanocavity mode is confined inside the nanocavity more gently and loosely. In this case, the mode volume of the nanocavity mode expands, and the electric field maximum at the nanocavity center decreases, which results in the decrease of the coupling coefficient g between a quantum dot and the nanocavity mode. Since the ratio g/κ between the coupling coefficient and the nanocavity decay rate characterizes the capability of the PC L3 nanocavity for realizing the strong coupling interaction between a quantum dot and the nanocavity mode, we should pay more attention to enhance the ratio g/κ, instead of only pursuing higher quality factor.
Conclusions
In summary, we have presented a simple and efficient method based upon the projected local density of states for photons to obtain the mode volume of a nanocavity. The effect of the slab thickness on the quality factor and mode volume of photonic crystal slab nanocavities has been investigated, which both play pivotal roles in cavity quantum electrodynamics.
We find that the mode volume is approximatively proportional to the slab thickness. Furthermore, by tuning the slab thickness, the quality factor can be increased by about 22%, and the ratio g/κ between the coupling coefficient and the nanocavity decay rate can be enhanced by about 13%, as compared with the previous PC L3 nanocavity that is finely optimized by introducing displacement of the air holes at both edges of the nanocavity. Based on these results, we can conclude that the optimization of the slab thickness can remarkably enhance the capability of the PC slab nanocavity for the realization of the strong coupling interaction between a quantum dot and the nanocavity mode. The slab thickness tuning approach is feasible and significant for the experimental fabrication of the solidstate nanocavities.
Authors’ information
GC, XLZ, and YCY are Ph.D. students in Sun Yatsen University. JFL and HJ are Ph.D. degree holders in Sun Yatsen University. CJ and XHW are professors of Sun Yatsen University.
Abbreviations
 PC:

photonic crystal
 PLDOS:

projected local density of states
 SSSCS:

solidstate strong coupling system
 2D:

twodimensional.
Declarations
Acknowledgments
This work was financially supported by the National Basic Research Program of China (2010CB923200), the National Natural Science Foundation of China (grant U0934002), and the Ministry of Education of China (grant V200801).
Authors’ Affiliations
References
 Yablonovitch E: Inhibited spontaneous emission in solidstate physics and electronics. Phys Rev Lett 1987, 58: 2059–2062. 10.1103/PhysRevLett.58.2059View ArticleGoogle Scholar
 John S: Strong localization of photons in certain disordered dielectric superlattices. Phys Rev Lett 1987, 58: 2486–2489. 10.1103/PhysRevLett.58.2486View ArticleGoogle Scholar
 Joannopoulos J, Johnson S, Winn J, Meade R: Photonic Crystals: Molding the Flow of Light. Princeton: Princeton University Press; 2008.Google Scholar
 Petrov EP, Bogomolov VN, Kalosha II, Gaponenko SV: Spontaneous emission of organic molecules embedded in a photonic crystal. Phys Rev Lett 1998, 81: 77–80. 10.1103/PhysRevLett.81.77View ArticleGoogle Scholar
 Lodahl P, Floris van Driel A, Nikolaev IS, Irman A, Overgaag K, Vanmaekelbergh D, Vos WL: Controlling the dynamics of spontaneous emission from quantum dots by photonic crystals. Nature 2004, 430: 654–657. 10.1038/nature02772View ArticleGoogle Scholar
 Jorgensen MR, Galusha JW, Bartl MH: Strongly modified spontaneous emission rates in diamondstructured photonic crystals. Phys Rev Lett 2011, 107: 143902.View ArticleGoogle Scholar
 Noda S, Fujita M, Asano T: Spontaneousemission control by photonic crystals and nanocavities. Nature Photonics 2007, 1: 449–458. 10.1038/nphoton.2007.141View ArticleGoogle Scholar
 Englund D, Shields B, Rivoire K, Hatami F, Vuckovic J, Park H, Lukin MD: Deterministic coupling of a single nitrogen vacancy center to a photonic crystal cavity. Nano Lett 2010, 10: 3922–3926. 10.1021/nl101662vView ArticleGoogle Scholar
 Wang XH, Wang R, Gu BY, Yang GZ: Decay distribution of spontaneous emission from an assembly of atoms in photonic crystals with pseudogaps. Phys Rev Lett 2002, 88: 093902.View ArticleGoogle Scholar
 Wang XH, Gu BY, Wang R, Xu HQ: Decay kinetic properties of atoms in photonic crystals with absolute gaps. Phys Rev Lett 2003, 91: 113904.View ArticleGoogle Scholar
 Krauss TF, Rue RMDL, Brand S: Twodimensional photonicbandgap structures operating at nearinfrared wavelengths. Nature 1996, 383: 699–702. 10.1038/383699a0View ArticleGoogle Scholar
 Johnson SG, Fan S, Villeneuve PR, Joannopoulos JD, Kolodziejski LA: Guided modes in photonic crystal slabs. Phys Rev B 1999, 60: 5751. 10.1103/PhysRevB.60.5751View ArticleGoogle Scholar
 Sakoda K: Optical Properties of Photonic Crystals. Berlin: Springer Verlag; 2005.Google Scholar
 Fujita M, Takahashi S, Tanaka Y, Asano T, Noda S: Simultaneous inhibition and redistribution of spontaneous light emission in photonic crystals. Science 2005, 308: 1296–1298. 10.1126/science.1110417View ArticleGoogle Scholar
 Wang Q, Stobbe S, Lodahl P: Mapping the local density of optical states of a photonic crystal with single quantum dots. Phys Rev Lett 2011, 107: 167404.View ArticleGoogle Scholar
 Yoshie T, Scherer A, Hendrickson J, Khitrova G, Gibbs HM, Rupper G, Ell C, Shchekin OB, Deppe DG: Vacuum Rabi splitting with a single quantum dot in a photonic crystal nanocavity. Nature 2004, 432: 200–203. 10.1038/nature03119View ArticleGoogle Scholar
 Khitrova G, Gibbs HM, Kira M, Koch SW, Scherer A: Vacuum Rabi splitting in semiconductors. Nat Phys 2006, 2: 81–90. 10.1038/nphys227View ArticleGoogle Scholar
 Hennessy K, Badolato A, Winger M, Gerace D, Atature M, Gulde S, Falt S, Hu EL, Imamoglu A: Quantum nature of a strongly coupled single quantum dotcavity system. Nature 2007, 445: 896–899. 10.1038/nature05586View ArticleGoogle Scholar
 Englund D, Faraon A, Fushman I, Stoltz N, Petroff P, Vuckovic J: Controlling cavity reflectivity with a single quantum dot. Nature 2007, 450: 857–861. 10.1038/nature06234View ArticleGoogle Scholar
 Nomura M, Kumagai N, Iwamoto S, Ota Y, Arakawa Y: Laser oscillation in a strongly coupled singlequantumdotnanocavity system. Nat Phys 2010, 6: 279–283. 10.1038/nphys1518View ArticleGoogle Scholar
 Walther H, Varcoe BTH, Englert BG, Becker T: Cavity quantum electrodynamics. Rep Progr Phys 2006, 69: 1325. 10.1088/00344885/69/5/R02View ArticleGoogle Scholar
 Faraon A, Fushman I, Englund D, Stoltz N, Petroff P, Vuckovic J: Coherent generation of nonclassical light on a chip via photoninduced tunnelling and blockade. Nat Phys 2008, 4: 859–863. 10.1038/nphys1078View ArticleGoogle Scholar
 Sato Y, Tanaka Y, Upham J, Takahashi Y, Asano T, Noda S: Strong coupling between distant photonic nanocavities and its dynamic control. Nat Photon 2012, 6: 56–61.View ArticleGoogle Scholar
 Vučković J, Lončar M, Mabuchi H, Scherer A: Design of photonic crystal microcavities for cavity QED. Phys Rev E 2001, 65: 016608.View ArticleGoogle Scholar
 Akahane Y, Asano T, Song BS, Noda S: HighQ photonic nanocavity in a twodimensional photonic crystal. Nature 2003, 425: 944–947. 10.1038/nature02063View ArticleGoogle Scholar
 Akahane Y, Asano T, Song BS, Noda S: Finetuned highQ photoniccrystal nanocavity. Opt Express 2005, 13: 1202–1214. 10.1364/OPEX.13.001202View ArticleGoogle Scholar
 Song BS, Noda S, Asano T, Akahane Y: UltrahighQ photonic doubleheterostructure nanocavity. Nat Mater 2005, 4: 207–210. 10.1038/nmat1320View ArticleGoogle Scholar
 Hagino H, Takahashi Y, Tanaka Y, Asano T, Noda S: Effects of fluctuation in air hole radii and positions on optical characteristics in photonic crystal heterostructure nanocavities. Phys Rev B 2009, 79: 085112.View ArticleGoogle Scholar
 Painter O, Lee RK, Scherer A, Yariv A, O'Brien JD, Dapkus PD, Kim I: Twodimensional photonic bandgap defect mode laser. Science 1999, 284: 1819–1821. 10.1126/science.284.5421.1819View ArticleGoogle Scholar
 Sprik R, Tiggelen BA, Lagendijk A: Optical emission in periodic dielectrics. Europhysics Letters 1996, 35: 265. 10.1209/epl/i199600564yView ArticleGoogle Scholar
 Scully MO, Zubairy MS: Quantum Optics. Cambridge: Cambridge University Press; 1997.View ArticleGoogle Scholar
 Taflove A, Hagness S: Computational Electrodynamics: The FiniteDifference TimeDomain Method. 3rd edition. Norwood: Artech House; 2005.Google Scholar
Copyright
This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.