OSA's Digital Library

Optics Express

Optics Express

  • Editor: C. Martijn de Sterke
  • Vol. 20, Iss. 15 — Jul. 16, 2012
  • pp: 17192–17200
« Show journal navigation

Optical frequency comb generation through quasi-phase matched quadratic frequency conversion in a micro-ring resonator

Zi-jian Wu, Yang Ming, Fei Xu, and Yan-qing Lu  »View Author Affiliations


Optics Express, Vol. 20, Issue 15, pp. 17192-17200 (2012)
http://dx.doi.org/10.1364/OE.20.017192


View Full Text Article

Acrobat PDF (1175 KB)





Browse Journals / Lookup Meetings

Browse by Journal and Year


   


Lookup Conference Papers

Close Browse Journals / Lookup Meetings

Article Tools

Share
Citations

Abstract

We propose optical frequency comb generation in a monolithic micro-ring resonator. Being different from the previously reported nonlinear optical frequency combs, our scheme is based on more efficient quadratic frequency conversion rather than the third-order nonlinearity. To overcome the phase mismatch, a partly poled nonlinear ring is employed. Cascading second harmonic generation and parametric down conversion processes thus are realized through quasi-phase matching (QPM). Coupling equations are used to describe the related nonlinear interactions among different whispering-gallery modes, showing some interesting characteristics that are different from conventional QPM technology.

© 2012 OSA

1. Introduction

To obtain high quadratic nonlinear conversion efficiency in a dispersive material, quasi-phase matching (QPM) is a proven effective technique that has been widely used [6

6. J. A. Armstrong, N. Bloembergen, J. Ducuing, and P. S. Pershan, “Interactions between light waves in a nonlinear dielectric,” Phys. Rev. 127(6), 1918–1939 (1962). [CrossRef]

, 7

7. P. A. Franken and J. F. Ward, “Optical harmonics and nonlinear phenomena,” Rev. Mod. Phys. 35(1), 23–39 (1963). [CrossRef]

]. Up to date, QPM optical switching [8

8. Y. L. Lee, B. A. Yu, T. J. Eom, W. Shin, C. Jung, Y. C. Noh, J. Lee, D. K. Ko, and K. Oh, “All-optical AND and NAND gates based on cascaded second-order nonlinear processes in a Ti-diffused periodically poled LiNbO3 waveguide,” Opt. Express 14(7), 2776–2782 (2006). [CrossRef] [PubMed]

], single photon detection [9

9. X. S. Song, Z. Y. Yu, Q. Wang, F. Xu, and Y. Q. Lu, “Polarization independent quasi-phase-matched sum frequency generation for single photon detection,” Opt. Express 19(1), 380–386 (2011). [CrossRef] [PubMed]

] and nonlinear plasmonic or metamaterial frequency conversion [10

10. Z. J. Wu, X. K. Hu, Z. Y. Yu, W. Hu, F. Xu, and Y. Q. Lu, “Nonlinear plasmonic frequency conversion through quasiphase matching,” Phys. Rev. B 82(15), 155107 (2010). [CrossRef]

, 11

11. A. Rose and D. R. Smith, “Overcoming phase mismatch in nonlinear metamaterials,” Opt. Mater. Express 1(7), 1232–1243 (2011). [CrossRef]

] have been proposed or demonstrated from continuous wave to femtosecond pulsed lights [12

12. Y. Q. Lu, Y. L. Lu, C. C. Xue, J. J. Zheng, X. F. Chen, G. P. Luo, N. B. Ming, B. H. Feng, and X. L. Zhang, “Femtosecond violet light generation by quasi-phase-matched frequency doubling in optical superlattice LiNbO3,” Appl. Phys. Lett. 69(21), 3155–3157 (1996). [CrossRef]

]. It should be very attractive to further explore the QPM in optical frequency comb generation. As we know, the periodic modulation of nonlinear coefficient plays the key role in a QPM process. Applying QPM into a ring resonator means the basic structure and geometry of QPM material changes. The interacted frequency components also should match the cavity’s WGMs [13

13. J. U. Fürst, D. V. Strekalov, D. Elser, M. Lassen, U. L. Andersen, C. Marquardt, and G. Leuchs, “Naturally phase-matched second-harmonic generation in a whispering-gallery-mode resonator,” Phys. Rev. Lett. 104(15), 153901 (2010). [CrossRef] [PubMed]

16

16. Kiyotaka Sasagawa, and Masahiro Tsuchiya, “High efficiency third harmonic generation in PPMgLN disk resonator,” in CLEO 2007 - Laser Applications to Photonic Applications, OSA Technical Digest (CD) (Optical Society of America, 2011), Paper CThC6.

]. Ref. 13

13. J. U. Fürst, D. V. Strekalov, D. Elser, M. Lassen, U. L. Andersen, C. Marquardt, and G. Leuchs, “Naturally phase-matched second-harmonic generation in a whispering-gallery-mode resonator,” Phys. Rev. Lett. 104(15), 153901 (2010). [CrossRef] [PubMed]

-16

16. Kiyotaka Sasagawa, and Masahiro Tsuchiya, “High efficiency third harmonic generation in PPMgLN disk resonator,” in CLEO 2007 - Laser Applications to Photonic Applications, OSA Technical Digest (CD) (Optical Society of America, 2011), Paper CThC6.

have proposed SHG/OPG and sum frequency generation (SFG) processes through QPM or naturally phase-matching, but the cascading nonlinearity processes which combines SHG and OPG would be more complicated. It would be very interesting to investigate such a coupled nonlinear optical system with both technical applications and fundamental research interests.

In this paper, we theoretically prove that, the QPM optical frequency comb can be generated in a quadratic nonlinear micro ring. We propose the general theoretical model for second-order nonlinear-optical processes in a ring, and then apply the theory to a partly domain-inverted lithium niobate (LN) micro ring resonator. This partly poled ring just works like a periodically poled waveguide. The QPM frequency conversion thus could be realized. The characteristics for optical frequency comb generation are investigated and discussed.

2. Model and theory

Let’s consider a 2D nonlinear ring resonator coupled with an input bus waveguide as shown in Fig. 1(a)
Fig. 1 (a) Schematic of a partially poled LN ring coupled with a waveguide; (b) Schematic of the similarity between a partially poled LN ring and a PPLN.
. The coupling coefficient between the bus waveguide and ring is defined as τ. As an approximation, the build-up factor is 4/τ2 for such an “add-drop” system [17

17. J. Heebner, R. Grover, and T. A. Ibrahim, Optical Microresonators (Springer, 2008), Chap. 3.

]. We treat the nonlinear effects and the coupling between the waveguide and the ring resonator as perturbations. Therefore the ring’s WGMs will not change with the light intensity. To solve the Maxwell equations, the electric field of TE modes (the electric field is parallel to the z axis), are written as,
Ez=nanfn(r),
(1)
where an represents the amplitude of WGM n circulating in the ring; fn corresponds to the field distribution of a WGM, which also can be written as
fn(r,ϕ)=gn(r)einϕ,
(2)
φ is the angle in cylindrical coordinate; corresponds to field distribution along radial direction so it is a function of the radius r. Because the photons of WGMs are mainly constrained in a ring, which is different from the straight waveguides, their momentums would be zero. However, the circular movement of each photon would cause a nonzero angular momentum which is indicated with the mode index n.

To study the nonlinear effect, the coupled mode equations of WGMs [18

18. A. A. Savchenkov, A. B. Matsko, M. Mohageg, D. V. Strekalov, and L. Maleki, “Parametric oscillations in a whispering gallery resonator,” Opt. Lett. 32(2), 157–159 (2007). [CrossRef] [PubMed]

] are used. As SHG is the special case of SFG, we would take the more general coupling equations of SFG to describe the sum frequency of modes ωm and ωn to mode ωp.
dap(t)dt=-γpap+n,mωpκpnmanam,
(3)
and, for the reversed process, i.e., difference frequency generation (DFG) or OPG, the equation would be:
dan(t)dt=-γnan+n,mωnFnmκpnm*apam*,
(4)
and, if the pump wavelength matches a WGM, the power of pump light in coupling waveguide would be coupled into the ring, so intensity of the corresponding WGM follows:
12d|an(t)|2dt=-γn|an|2+n,mωn2Fnmκpnm*apam*an+τ2Pε0,
(5)
where Fnm={1nm2n=m, γn is the WGM decay rate that is dominated by the loss. In our configuration, both the ring-to-bus coupling loss and the round-trip bending loss may be taken into account. Smaller ring gives rise to higher bending loss. When the radius is around 12 μm and τ is 0.01, the major loss would be the coupling loss that is 109 times higher than the bending one. In this case, the decay rate is given by ωτ2/2n, meaning only the coupling loss is considered. P corresponds to the pump power in the input bus waveguide; ε0 represents the vacuum permittivity. κpnm is the coupling coefficient between three WGMs with frequencies of ωm, ωn and ωp, which could be expressed as:

κpnm=-idr3χ(2)fp(r)fn(r)fm(r)=-igp(r)gn(r)gm(r)χ(2)(ϕ)ei(m+n-p)ϕdϕ.
(6)

In these nonlinear processes, the coupling coefficients κpnm are the dominating factors. Typically, if the coupling coefficients are equal to zero, the couplings among corresponding waves would also be zero and the nonlinear effect disappears. To realize a remarkable nonlinear effect, the coupling coefficient should be maximized. The larger coupling coefficients, the lower pump light power is required.

To analyze the coupling coefficient, the overlap integration of different WGMs should be considered first, especially the angle part of the integration. In the phase-matching cases, which means the three interaction photons obey the angular momentum conservation law [13

13. J. U. Fürst, D. V. Strekalov, D. Elser, M. Lassen, U. L. Andersen, C. Marquardt, and G. Leuchs, “Naturally phase-matched second-harmonic generation in a whispering-gallery-mode resonator,” Phys. Rev. Lett. 104(15), 153901 (2010). [CrossRef] [PubMed]

]:

Δ=m+np=0.
(7)

Without QPM, the nonlinear coefficient χ(2) would be a constant in the whole ring. The angle part of integration in Eq. (6) is ei(m+np)ϕdϕ=2π, the coupling coefficient is non-zero and nonlinear interaction happens. However, in most of the cases, the phase-matching condition would be difficult to satisfy due to dispersion. Δ ≠ 0, ei(m+np)ϕdϕ=0, the coupling coefficient is zero, neither SFG nor DFG could happen with noticeable efficiency. To solve this problem, the idea of QPM could be transplanted here to this system as shown in Fig. 1(a). The nonlinear ring is separated into two parts with opposite nonlinear coefficient. This may be realized by taking ferroelectric materials with partly reverse poling [4

4. S. N. Zhu, Y. Y. Zhu, and N.-B. Ming, “Quasi-phase-matched third-harmonic generation in a quasi-periodic optical superlattice,” Science 278(5339), 843–846 (1997). [CrossRef]

]. In this case, the angle part of overlap integration in Eq. (6) change to h(ϕ)ei(m+np)θdϕ, where h(φ) is defined as:
h(ϕ)={10<ϕθ1θ<ϕ2π.
(8)
θ is the open angle of the reversely poled domain. In the cases that Δ = odd, to maximize the overlap integration and the nonlinear coupling coefficient κpnm, the ring should be half poled, which means θ = π. The angular part of overlap integration is obtained as h(ϕ)ei(m+np)ϕdϕ=4/iΔ. If Δ is even, which means Δ = 2n × odd, to maximize the overlap integration, θ = π/2n should be satisfied. In this formulation, odd means an arbitrary odd number, then the integration givesh(ϕ)ei(m+np)ϕdϕ=4/iΔ.

From the above analysis, the differences between the normal QPM technique and the QPM in ring could be found. The diagram of these two types of QPM is shown in Fig. 1(b). The QPM technique in a waveguide needs periodically alternating ferroelectric domain structures [10

10. Z. J. Wu, X. K. Hu, Z. Y. Yu, W. Hu, F. Xu, and Y. Q. Lu, “Nonlinear plasmonic frequency conversion through quasiphase matching,” Phys. Rev. B 82(15), 155107 (2010). [CrossRef]

, 11

11. A. Rose and D. R. Smith, “Overcoming phase mismatch in nonlinear metamaterials,” Opt. Mater. Express 1(7), 1232–1243 (2011). [CrossRef]

]. The light experiences positive and negative nonlinear coefficients one by one. In a QPM ring, light propagates along the circular waveguide and goes through two reversely poled areas in each loop, which means the light still can see different domains periodically. It is just similar to the case in a straight QPM material. In another word, the necessary periodicity needed to achieve QPM process comes from a virtual unfolded straight waveguide rather than a practical periodic domain structure. From this point of view, a partly domain inverted LN ring with radius R is equivalent to a periodically poled waveguide with period 2πR. However, in ring system, due to the geometry difference, the momentum conversion law would change to angular momentum conversion law.

3. Simulation results and discussions

Because nonlinear optical conversion happens inside the ring, both the FW and SHW should be right at the cavity’s WGMs. Since each WGM satisfy a specific wavelength, both the FW wavelength and the SHW wavelength should be right at the WGM wavelength. This condition could be satisfied though proper ring parameter design with some matching wavelengths. It is even tunable through adjusting the operation temperature or applying an electric field. In our simulation, we set the fundamental mode at 1539.5 nm and the second harmonic mode at 769.7 nm, corresponding to two WGMs of a 2D LN ring with internal radius of 12.74 μm and width of 1 μm. When calculating the WGMs, both the material and waveguide dispersions are considered. The operation temperature is set at 25°C and index of air cladding is 1. The index of LN is obtained from the Sellmeier equation [19

19. D. H. Jundt, “Temperature-dependent Sellmeier equation for the index of refraction, n(e), in congruent lithium niobate,” Opt. Lett. 22(20), 1553–1555 (1997). [CrossRef] [PubMed]

] that is temperature sensitive. If errors occur in accuracy of the radius or width, the WGMs of the ring may have an offset from the design. The pumping wavelength thus should be finely adjusted to fit the WGMs. However, we may also change the temperature to tune the WGMs back in principle.

Before studying the SHG process, one factor should be noticed. Due to the character of this so-called “add-drop” system [17

17. J. Heebner, R. Grover, and T. A. Ibrahim, Optical Microresonators (Springer, 2008), Chap. 3.

], whether a quadratic or a third-order nonlinear ring, only part of the input power is able to couple into the ring and participate in frequency conversion. Based on this, the internal and external SHG efficiency of this system could be defined. The external SHG efficiency is the ratio between the output SHW power and the input pump power into the bus waveguide. And the internal SHG efficiency is defined as the output SHW power over the portion of the FW power coupled into the ring. Obviously, the internal efficiency should be always higher than the external one.

To derive the SHG internal and external efficiencies, Eqs. (3) and (4) should be used. We assume a stable state of the system, so the light field amplitude does not change with the time. This makes the formulations change to quadratic equations. The internal and external SHG efficiencies versus the pump power in the input bus waveguide thus could be easily obtained as shown in Figs. 2(a)
Fig. 2 The (a) internal and (b) external SHG efficiencies with different pump power, where the solid, dashed and dash-dot curves correspond to τ = 0.1, 0.2, 0.3, respectively; (c) The external SHG efficiencies with different τ, where the solid, dashed and dash-dot curves correspond to pump power = 0.1, 1, 3 MW/m.
and 2(b). Coupling coefficients τ = 0.1, 0.2, 0.3 have been simulated, corresponding Q-factors around 103~104, which are quite achievable. On the other hand, the ratio of internal efficiency to external efficiency is τ2/2. This is because the proportion of power coupled into the ring to the input pump power is τ2/2. Due to the nature of nonlinear effect, the SHG efficiencies all rise with the increase of pump power. They gradually saturate when the internal efficiency approaches 1. And, in this case, the external efficiency is close to τ2/2 as shown with the black solid curve in Fig. 2(b). For τ = 0.1, τ2/2 gives the highest limit of 5% for external efficiency.

In addition to the efficiency limit, other interesting phenomena could be found from the figures. Because of the reduction of light intensity with the increase of τ, the internal SHG efficiency simply reduces when τ increases. But for the external SHG efficiency, things are different. Although the internal efficiency still decreases, the internal to external efficiency ratio τ2/2 increases at the same time. That makes the external efficiency reach a maximum at a given τ value, as shown in Fig. 2(c). However, the efficiency peaks emerge at different τ values for different pump powers. This feature should be considered when design such a nonlinear ring system.

If we compare the QPM SHG in the ring with normal QPM in a bulk or waveguide PPLN, the characteristics shows both similarities and differences. Light in the ring also experiences different nonlinear coefficients, but the domain inverted area should match the involved cavity modes. The external SHG efficiency also rises with the increase of pump power, but it cannot go beyond a limit at τ2/2. In addition, the efficiency shows complicate relationship with the coupling coefficient τ. If the pump power is high enough, bigger coupling coefficient gives rise to larger external SHG efficiency, while in lower pump power cases, the internal SHG efficiency would not reaches a maximum, the external SHG efficiency will not simply rise with the increase of τ. The QPM in a nonlinear ring really has many interesting properties that worth studying.

Only two WGMs are considered in the SHG calculations above. However, there could be many modes in this ring system. In optical frequency comb generation processes [1

1. T. J. Kippenberg, R. Holzwarth, and S. A. Diddams, “Microresonator-based optical frequency combs,” Science 332(6029), 555–559 (2011). [CrossRef] [PubMed]

], cascading SHG and OPG process should be considered with more WGMs involved. In comparison with a straight waveguide [4

4. S. N. Zhu, Y. Y. Zhu, and N.-B. Ming, “Quasi-phase-matched third-harmonic generation in a quasi-periodic optical superlattice,” Science 278(5339), 843–846 (1997). [CrossRef]

], the ring system makes the cascading nonlinear processes much more complicated. The involved lights should be right at the ring cavity’s WGMs. We assume the pump light at a mode frequency of ωp and generate a pair of modes at ωm and ωn with 2ωp = ωsh = ωm + ωn. The SHG process could be described as the system absorbs two photons with the frequency ωp and generate the photon at second harmonic mode with frequency ωsh = 2ωp. Then the OPG process could be described as the system absorbs the photon at the SH mode and generates a photon pair with different frequencies ωm and ωn. Due to the dispersion of the ring, this condition could not be severely satisfied. However, if the line shapes of the ring resonances are considered, then the generated SHW and frequency down-converted signal and idler waves can be made to fit within a specific mode-spacing. Furthermore, if there is a frequency spacing mismatch between the WGMs and the signals generated via SHG and spontaneous down-conversion, there should be a finite bandwidth over which the generated comb can fit in the ring’s resonances. So as an approximation, the modes that satisfy the condition Δωsh > ωsh – ωm – ωn are selected. Δωsh represents the full width of the maximum of the SH mode. It depends on the Q-factor and the coupling condition of our system. We set τ at 0.01 and Δωsh = 0.1 THz for the simulation. In order to include more comb modes, the wavelength of pump changes to 1556.7 nm, thus a SHW at 778.35 nm is obtained. In this case, there would be 22 WGMs included in the calculation, including the pump mode, the SH mode and 20 modes with the resonating wavelength around the pump mode. The mode number of these modes are p ± 1, 2, 3, ..., 10. Here ‘p’ indicates the mode number of pump light that is equal to 111. The mode number of SHW WGM is 234. As a consequence, Δ = 12 and the open angle of the reversely poled domain is set at π/4. If error occurs for the open angle, the nonlinear conversion efficiency may be affected. The tolerance could be obtained through calculating the angular part integration of Eq. (6). With a 5° offset, the coupling coefficient κpnm would only be reduced by 1.5%. The pump power is set at 10 MW/cm.

Figure 3(a) shows the output spectra of SH mode through QPM. The output power of this mode is 0.31 W/cm. Compare with the pure SHG, it is a much smaller value. This is due to the couplings between second harmonic mode and the other 20 modes around the pump mode. The power of the second harmonic mode is further transferred to these 20 modes with the help of OPG processes.

Figure 3(b) shows the output spectra of pump mode and the comb modes that are generated from QPM OPG. The typical line-width of the comb modes is still around 0.1 THz. The output power of the pump mode is 9.999 MW/cm. It is approximately equal to the input pump power. This is because the coupling coefficient is set to a relatively low value 0.01. And it leads to the 500 W/cm input power from waveguide to ring. The other part of the power will just propagate through the waveguide without the participation of nonlinear process. According to the simulation results, each of the 20 degenerated modes has an output power around 14 W/cm. So the total power of these modes would be 280 W/cm; the internal efficiency of the 20 modes generation is 56%, which is a quite high value, means efficient optical frequency comb generation really may be achieved in such a nonlinear ring. Adjusting the pump power, different internal efficiencies also could be obtained.

Considering from the system level, our optical frequency comb shares a similar regime with the traditional third-order nonlinearity ones, as both systems are typical ‘add-drop’ systems. The overall comb generation rate thus should be limited by the waveguide-to-ring coupling coefficient. However, as long as the pump light is coupled in the ring, the internal efficiency could reach a very high level due to the intrinsically more efficient quadratic nonlinear optical process. In addition, although the dispersion between FWs and SH has been compensated through QPM, the dispersion among the FWs still limits the number of participant modes. In our proposal, a simple 2D system is investigated to better display the mechanism of QPM comb generation. However, although it is quite simplified with respect to a 3D counterpart, they have basically very similar characteristics in ring QPM and comb generation. Both of them are based on the nonlinear interaction among WGMs rather than straightforwardly propagating lights. For a 3D system, as longs as the FW and SHW are at the WGMs, QPM SHG is able to achieve just like in a 2D ring. In this case, the 2D and 3D systems are equivalent in physics and nonlinear optical behaviors.

To implement this idea, we may take a patterned poled LN according to our design with a suitable open angle. Then we may make a waveguide layer through proton-exchange that is mature in industry. To obtain a nice ring and input/output bus, femtosecond laser may be used to machine it precisely. The final 3D LN ring waveguide still has air cladding at top and two sides, while LN with slightly lower index acts as the bottom cladding. Obviously, the coupling and WGMs simulations would be much more complicated than a 2D system. FEM/FDTD methods might be used. However, it also gives the feasibility to further design the waveguide for dispersion compensation between different comb modes [2

2. J. S. Levy, A. Gondarenko, M. A. Foster, A. C. Turner-Foster, A. L. Gaeta, and M. Lipson, “CMOS-compatible multiple-wavelength oscillator for on-chip optical interconnects,” Nat. Photonics 4(1), 37–40 (2010). [CrossRef]

]. Through geometry optimization and careful fabrication, a broad band comb generation is expected.

4. Conclusion

In summary, the QPM technique is applied to a ring system. The general three wave coupling processes are studied theoretically. We found that a partly poled nonlinear ring could be just equivalent to a periodically poled QPM material. However, depending on the involved WGMs, the required poling areas are different. As an example, the SHG of a LN ring is investigated. The overall and internal SHG efficiencies are studied with various parameters, including the pump power, coupling coefficient and WGMs. Based on these results, an optical frequency comb solution is proposed that is from the cascading SHG and OPG processes in the ring. Higher comb generation efficiency is expected.

Acknowledgments

This work is financially supported by 973 programs under contract No. 2011CBA00205, 2012CB921803 and 2010CB327803, and by NSFC programs No. 11074117 and 60977039. We also thank the support from PAPD, Fundamental Research Funds for the Central Universities. Correspondences about this paper should be addressed to Yan-qing Lu or Fei Xu.

References and links

1.

T. J. Kippenberg, R. Holzwarth, and S. A. Diddams, “Microresonator-based optical frequency combs,” Science 332(6029), 555–559 (2011). [CrossRef] [PubMed]

2.

J. S. Levy, A. Gondarenko, M. A. Foster, A. C. Turner-Foster, A. L. Gaeta, and M. Lipson, “CMOS-compatible multiple-wavelength oscillator for on-chip optical interconnects,” Nat. Photonics 4(1), 37–40 (2010). [CrossRef]

3.

I. H. Agha, Y. Okawachi, and A. L. Gaeta, “Theoretical and experimental investigation of broadband cascaded four-wave mixing in high-Q microspheres,” Opt. Express 17(18), 16209–16215 (2009). [CrossRef] [PubMed]

4.

S. N. Zhu, Y. Y. Zhu, and N.-B. Ming, “Quasi-phase-matched third-harmonic generation in a quasi-periodic optical superlattice,” Science 278(5339), 843–846 (1997). [CrossRef]

5.

P. Del’Haye, A. Schliesser, O. Arcizet, T. Wilken, R. Holzwarth, and T. J. Kippenberg, “Optical frequency comb generation from a monolithic microresonator,” Nature 450(7173), 1214–1217 (2007). [CrossRef] [PubMed]

6.

J. A. Armstrong, N. Bloembergen, J. Ducuing, and P. S. Pershan, “Interactions between light waves in a nonlinear dielectric,” Phys. Rev. 127(6), 1918–1939 (1962). [CrossRef]

7.

P. A. Franken and J. F. Ward, “Optical harmonics and nonlinear phenomena,” Rev. Mod. Phys. 35(1), 23–39 (1963). [CrossRef]

8.

Y. L. Lee, B. A. Yu, T. J. Eom, W. Shin, C. Jung, Y. C. Noh, J. Lee, D. K. Ko, and K. Oh, “All-optical AND and NAND gates based on cascaded second-order nonlinear processes in a Ti-diffused periodically poled LiNbO3 waveguide,” Opt. Express 14(7), 2776–2782 (2006). [CrossRef] [PubMed]

9.

X. S. Song, Z. Y. Yu, Q. Wang, F. Xu, and Y. Q. Lu, “Polarization independent quasi-phase-matched sum frequency generation for single photon detection,” Opt. Express 19(1), 380–386 (2011). [CrossRef] [PubMed]

10.

Z. J. Wu, X. K. Hu, Z. Y. Yu, W. Hu, F. Xu, and Y. Q. Lu, “Nonlinear plasmonic frequency conversion through quasiphase matching,” Phys. Rev. B 82(15), 155107 (2010). [CrossRef]

11.

A. Rose and D. R. Smith, “Overcoming phase mismatch in nonlinear metamaterials,” Opt. Mater. Express 1(7), 1232–1243 (2011). [CrossRef]

12.

Y. Q. Lu, Y. L. Lu, C. C. Xue, J. J. Zheng, X. F. Chen, G. P. Luo, N. B. Ming, B. H. Feng, and X. L. Zhang, “Femtosecond violet light generation by quasi-phase-matched frequency doubling in optical superlattice LiNbO3,” Appl. Phys. Lett. 69(21), 3155–3157 (1996). [CrossRef]

13.

J. U. Fürst, D. V. Strekalov, D. Elser, M. Lassen, U. L. Andersen, C. Marquardt, and G. Leuchs, “Naturally phase-matched second-harmonic generation in a whispering-gallery-mode resonator,” Phys. Rev. Lett. 104(15), 153901 (2010). [CrossRef] [PubMed]

14.

V. S. Ilchenko, A. B. Matsko, A. A. Savchenkov, and L. Maleki, “Low-threshold parametric nonlinear optics with quasi-phase-matched whispering-gallery modes,” J. Opt. Soc. Am. B 20(6), 1304–1308 (2003). [CrossRef]

15.

V. S. Ilchenko, A. A. Savchenkov, A. B. Matsko, and L. Maleki, “Nonlinear optics and crystalline whispering gallery mode cavities,” Phys. Rev. Lett. 92(4), 043903 (2004). [CrossRef] [PubMed]

16.

Kiyotaka Sasagawa, and Masahiro Tsuchiya, “High efficiency third harmonic generation in PPMgLN disk resonator,” in CLEO 2007 - Laser Applications to Photonic Applications, OSA Technical Digest (CD) (Optical Society of America, 2011), Paper CThC6.

17.

J. Heebner, R. Grover, and T. A. Ibrahim, Optical Microresonators (Springer, 2008), Chap. 3.

18.

A. A. Savchenkov, A. B. Matsko, M. Mohageg, D. V. Strekalov, and L. Maleki, “Parametric oscillations in a whispering gallery resonator,” Opt. Lett. 32(2), 157–159 (2007). [CrossRef] [PubMed]

19.

D. H. Jundt, “Temperature-dependent Sellmeier equation for the index of refraction, n(e), in congruent lithium niobate,” Opt. Lett. 22(20), 1553–1555 (1997). [CrossRef] [PubMed]

OCIS Codes
(160.3730) Materials : Lithium niobate
(190.4410) Nonlinear optics : Nonlinear optics, parametric processes
(190.4975) Nonlinear optics : Parametric processes

ToC Category:
Nonlinear Optics

History
Original Manuscript: May 29, 2012
Revised Manuscript: July 5, 2012
Manuscript Accepted: July 5, 2012
Published: July 12, 2012

Citation
Zi-jian Wu, Yang Ming, Fei Xu, and Yan-qing Lu, "Optical frequency comb generation through quasi-phase matched quadratic frequency conversion in a micro-ring resonator," Opt. Express 20, 17192-17200 (2012)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-20-15-17192


Sort:  Author  |  Year  |  Journal  |  Reset  

References

  1. T. J. Kippenberg, R. Holzwarth, and S. A. Diddams, “Microresonator-based optical frequency combs,” Science332(6029), 555–559 (2011). [CrossRef] [PubMed]
  2. J. S. Levy, A. Gondarenko, M. A. Foster, A. C. Turner-Foster, A. L. Gaeta, and M. Lipson, “CMOS-compatible multiple-wavelength oscillator for on-chip optical interconnects,” Nat. Photonics4(1), 37–40 (2010). [CrossRef]
  3. I. H. Agha, Y. Okawachi, and A. L. Gaeta, “Theoretical and experimental investigation of broadband cascaded four-wave mixing in high-Q microspheres,” Opt. Express17(18), 16209–16215 (2009). [CrossRef] [PubMed]
  4. S. N. Zhu, Y. Y. Zhu, and N.-B. Ming, “Quasi-phase-matched third-harmonic generation in a quasi-periodic optical superlattice,” Science278(5339), 843–846 (1997). [CrossRef]
  5. P. Del’Haye, A. Schliesser, O. Arcizet, T. Wilken, R. Holzwarth, and T. J. Kippenberg, “Optical frequency comb generation from a monolithic microresonator,” Nature450(7173), 1214–1217 (2007). [CrossRef] [PubMed]
  6. J. A. Armstrong, N. Bloembergen, J. Ducuing, and P. S. Pershan, “Interactions between light waves in a nonlinear dielectric,” Phys. Rev.127(6), 1918–1939 (1962). [CrossRef]
  7. P. A. Franken and J. F. Ward, “Optical harmonics and nonlinear phenomena,” Rev. Mod. Phys.35(1), 23–39 (1963). [CrossRef]
  8. Y. L. Lee, B. A. Yu, T. J. Eom, W. Shin, C. Jung, Y. C. Noh, J. Lee, D. K. Ko, and K. Oh, “All-optical AND and NAND gates based on cascaded second-order nonlinear processes in a Ti-diffused periodically poled LiNbO3 waveguide,” Opt. Express14(7), 2776–2782 (2006). [CrossRef] [PubMed]
  9. X. S. Song, Z. Y. Yu, Q. Wang, F. Xu, and Y. Q. Lu, “Polarization independent quasi-phase-matched sum frequency generation for single photon detection,” Opt. Express19(1), 380–386 (2011). [CrossRef] [PubMed]
  10. Z. J. Wu, X. K. Hu, Z. Y. Yu, W. Hu, F. Xu, and Y. Q. Lu, “Nonlinear plasmonic frequency conversion through quasiphase matching,” Phys. Rev. B82(15), 155107 (2010). [CrossRef]
  11. A. Rose and D. R. Smith, “Overcoming phase mismatch in nonlinear metamaterials,” Opt. Mater. Express1(7), 1232–1243 (2011). [CrossRef]
  12. Y. Q. Lu, Y. L. Lu, C. C. Xue, J. J. Zheng, X. F. Chen, G. P. Luo, N. B. Ming, B. H. Feng, and X. L. Zhang, “Femtosecond violet light generation by quasi-phase-matched frequency doubling in optical superlattice LiNbO3,” Appl. Phys. Lett.69(21), 3155–3157 (1996). [CrossRef]
  13. J. U. Fürst, D. V. Strekalov, D. Elser, M. Lassen, U. L. Andersen, C. Marquardt, and G. Leuchs, “Naturally phase-matched second-harmonic generation in a whispering-gallery-mode resonator,” Phys. Rev. Lett.104(15), 153901 (2010). [CrossRef] [PubMed]
  14. V. S. Ilchenko, A. B. Matsko, A. A. Savchenkov, and L. Maleki, “Low-threshold parametric nonlinear optics with quasi-phase-matched whispering-gallery modes,” J. Opt. Soc. Am. B20(6), 1304–1308 (2003). [CrossRef]
  15. V. S. Ilchenko, A. A. Savchenkov, A. B. Matsko, and L. Maleki, “Nonlinear optics and crystalline whispering gallery mode cavities,” Phys. Rev. Lett.92(4), 043903 (2004). [CrossRef] [PubMed]
  16. Kiyotaka Sasagawa, and Masahiro Tsuchiya, “High efficiency third harmonic generation in PPMgLN disk resonator,” in CLEO 2007 - Laser Applications to Photonic Applications, OSA Technical Digest (CD) (Optical Society of America, 2011), Paper CThC6.
  17. J. Heebner, R. Grover, and T. A. Ibrahim, Optical Microresonators (Springer, 2008), Chap. 3.
  18. A. A. Savchenkov, A. B. Matsko, M. Mohageg, D. V. Strekalov, and L. Maleki, “Parametric oscillations in a whispering gallery resonator,” Opt. Lett.32(2), 157–159 (2007). [CrossRef] [PubMed]
  19. D. H. Jundt, “Temperature-dependent Sellmeier equation for the index of refraction, n(e), in congruent lithium niobate,” Opt. Lett.22(20), 1553–1555 (1997). [CrossRef] [PubMed]

Cited By

Alert me when this paper is cited

OSA is able to provide readers links to articles that cite this paper by participating in CrossRef's Cited-By Linking service. CrossRef includes content from more than 3000 publishers and societies. In addition to listing OSA journal articles that cite this paper, citing articles from other participating publishers will also be listed.

Figures

Fig. 1 Fig. 2 Fig. 3
 

« Previous Article  |  Next Article »

OSA is a member of CrossRef.

CrossCheck Deposited