Agenda for today: Laser cavity design

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Presentation transcript:

Agenda for today: Laser cavity design Today we will use Lumerical FDTD to study a nanowire laser cavity Review conditions for lasing in general laser cavity Design and analysis of ZnO nanowire laser cavity

Review: basic laser concepts

Review: basic laser concepts

ZnO nanowire laser cavity As an interesting case study, let’s examine a somewhat exotic laser cavity consisting of a ZnO nanowire laser cavity “Bottom-up” fabricated ZnO nanowires grown on sapphire substrate Cavity is formed by mirror between top facet and air and bottom facet and sapphire substrate How much gain do we need to observe lasing in such a cavity? Huang, Michael H., et al. "Room-temperature ultraviolet nanowire nanolasers." Science 292.5523 (2001): 1897-1899.

Back-of-the envelope calculation of threshold gain for ZnO nanowire Mirror #1 Assume plane wave normal incidence: 𝑅= 𝑛 𝑍𝑛𝑂 − 𝑛 𝑎𝑖𝑟 𝑛 𝑍𝑛𝑂 + 𝑛 𝑎𝑖𝑟 2 =18% ZnO nanowire (n = 2.45) Mirror #2 Assume plane wave normal incidence: 𝑅= 𝑛 𝑍𝑛𝑂 − 𝑛 𝑠𝑎𝑝𝑝ℎ 𝑛 𝑍𝑛𝑂 + 𝑛 𝑠𝑎𝑝𝑝ℎ 2 =2% Sapphire (n = 1.8)

Back-of-the envelope calculation of threshold gain for ZnO nanowire 𝑔 𝑡ℎ = 𝛼 𝑖 Γ + 1 2Γ𝐿 ln 1 𝑅 1 𝑅 2 Mirror #1 Assume nanowire length is 10 µm, confinement factor is unity, and negligible internal loss ZnO nanowire (n = 2.45) 𝑔 𝑡ℎ ~ 1 (2)(1)(10× 10 −4 ) ln 1 (0.18)(0.02) Mirror #2 =2800 cm −1 Sapphire (n = 1.8) (this is pretty high!)

Lumerical simulation Let’s use Lumerical FDTD to get a more accurate value for the mirror reflectivity and confinement factor to determine the threshold gain We could simulate the entire structure and determine the Q-factor to get the threshold gain however it’s faster to simply simulate the mirror reflectivity for each mirror and use the expression on the previous page

FDTD procedure (3) Monitor reflected power with a field monitor (1) Launch waveguide mode (2) Guided mode will reflect off the mirror. Some light will radiate away but some will reflect in the backward direction reflected light radiated light

Mode source in FDTD When running FDTD simulation we often want to excite a particular waveguide mode This can be done using a mode source in Lumerical FDTD.

Guided mode source Open the file disc5_ZnO_nanowire_laser_mirror.fsp This file contains the geometry necessary to simulate reflectivity from both mirrors of the ZnO nanowire cavity ZnO has hexagonal cross-section with 130nm diameter We will assume lasing occurs at the ZnO bandgap wavelength of 370nm and therefore center our simulation range at that wavelength First, let’s simulation the ZnO-air interface Right click sapphire → Disable

Computational domain PML air nanowire Mode source Power monitor Movie monitor

Mode source

Mode source

Plotting mirror reflectivity Run simulation Right-click reflectionMonitor and select Visualize  T This will plot the percentage of power transmitted through the field-monitor. That is it will tell us much power was reflected from the nanowire laser cavity mirror (i.e. reflectivity)

ZnO-Air mirror reflectivity

ZnO-Air mirror reflectivity We measure a reflectivity of 11%. This is slightly lower than our back-of-the-envelope calculation of 18%, probably due to increased scattering at edges.

ZnO-Sapphire reflectivity Next, we need to simulate the reflectivity of the other mirror. Click on Layout (where the Run button was) to go back to Layout mode Right-click on sapphire → Enable. Re-run simulation and plot the reflectivity.

ZnO-Sapphire reflectivity

Confinement factor Finally, we need to determine the confinement factor (Γ) where: Γ= Power inside waveguide Total guided power = 𝑖𝑛𝑠𝑖𝑑𝑒 𝑅𝑒 𝐄× 𝐇 ∗ ⋅ 𝑧 𝑑𝑥𝑑𝑦 𝑡𝑜𝑡𝑎𝑙 𝑅𝑒 𝐄× 𝐇 ∗ ⋅ 𝑧 𝑑𝑥𝑑𝑦 We can do determine the confinement factor by using Lumerical MODE. Open the file ZnO_nanowire_laser_CF.lms Click Run, and Calculate modes

Confinement factor calculation

Confinement factor calculation

Confinement factor calculation We are limited to a circular or rectangular geometry when calculating confinement factor. When waveguide has more complicated geometry (such as ZnO nanowire with hexagonal cross-section) we may wish to more rigorously determine confinement factor by writing a Lumerical script.

Threshold gain calculation Now, let’s recalculate the threshold gain calculation with our more accurate values for mirror reflectivity and confinement factor. 𝑔 𝑡ℎ = 𝛼 𝑖 Γ + 1 2Γ𝐿 ln 1 𝑅 1 𝑅 2 Assume nanowire length is 10 µm, and negligible internal loss 𝑔 𝑡ℎ ~ 1 (2)(0.82)(10× 10 −4 ) ln 1 (0.11)(0.008) =4300 𝑐 𝑚 −1 Original estimate was 2800 𝑐 𝑚 −1