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Electromagnetic Resonators EE2025: Uday Khankhoje EE, IIT Madras 1

EM resonators and applicationsCap the ends with metal plates [2] 𝐵 =𝐵0 + − +𝐵 0 − cos 𝜋 cos 𝜋 𝜔𝑡 Fwd and bkwd waves Boundary conditions atCap the ends with

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Electromagnetic Resonators

EE2025: Uday KhankhojeEE, IIT Madras

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Waveguides (recap)

2

Waveguides (recap) [1]

1. Maxwell:

2. Expand fields into components:

𝐸 𝑥, 𝑦, 𝑧, 𝑡 = 𝐸0 𝑥, 𝑦 𝑒𝑗 𝜔𝑡−𝑘𝑧

𝐸0 = 𝐸𝑥 𝑥 + 𝐸𝑦 𝑦 + 𝐸𝑧 𝑧

3

Waveguides (recap) [1]

3. Transverse components in terms of Ez, Bz:

(Note: replace i by –j above)4

Waveguides (recap) [1]

4. Solve for Ez, Bz from here:

5

Waveguides (recap) [1]

• TE Solutions of the form

𝐵𝑧(𝑥, 𝑦, 𝑧, 𝑡) = 𝐵0 cos𝑚𝜋𝑥

𝑎cos

𝑛𝜋𝑦

𝑏𝑒𝑗(𝜔𝑡−𝑘𝑧)

i.e. a fwd travelling wave

Cut off freqs:

𝜔𝑚𝑛 = 𝑐𝜋𝑚

𝑎

2

+𝑛

𝑎

2

6

Cap the ends with metal plates [2]

𝐵𝑧 = 𝐵0+𝑒−𝑗𝑘𝑧 + 𝐵0

−𝑒𝑗𝑘𝑧 cos𝑚𝜋𝑥

𝑎cos

𝑛𝜋𝑦

𝑏𝑒𝑗𝜔𝑡

Fwd and bkwd waves

Boundary conditions at 𝑧 = 0, 𝑧 = 𝑑:

𝛻 × 𝐸𝑧= −𝑗𝜔𝐵𝑧

=𝜕𝐸𝑥

𝜕𝑦−

𝜕𝐸𝑦

𝜕𝑥= 0

7

Cap the ends with metal plates [2]

This implies that 𝐵0+ = −𝐵0

− , 𝑘𝑑 = 𝑝𝜋 and :

𝐵𝑧 = −2𝑗𝐵0+sin

p𝜋𝑧

𝑑cos

𝑚𝜋𝑥

𝑎cos

𝑛𝜋𝑦

𝑏𝑒𝑗𝜔𝑡

The frequency of a waveguide mode earlier was

𝑐𝑘 = 𝜔2 − 𝜔𝑚𝑛2

Now, k is restricted, so

𝜔0 = 𝑐𝜋𝑝

𝑑

2

+𝑚

𝑎

2

+𝑛

𝑏

2

Waveguide frequency 8

Losses in a resonator

• Perfect metal ⟶ No losses

• Finite 𝜎 ⇒ Boundary conditions get slightly modified ⇒ System supports small range of frequencies around 𝜔0

9

Waveguide resonator [2]

𝑄 = 𝜔0

𝐸𝑛𝑒𝑟𝑔𝑦 𝑆𝑡𝑜𝑟𝑒𝑑

𝑃𝑜𝑤𝑒𝑟 𝑙𝑜𝑠𝑡

10

Waveguide resonator [2]

𝑄 ≈𝜔0

Δ𝜔

Calculating resonator loss allows Q calc.11

Resonators in the real world

• Fiber-Bragg mirrors [3]

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Resonators in the real world

• Fiber-based resonator [4]

13

Laser Physics in brief [5]

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Laser Physics in brief [5]

The presence of a photon encourages another photon to be emitted: Stimulated emission

Only 2 level system, 𝑁2

𝑁1= exp(−

Δ𝐸

𝑘𝑇)

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FastSlow

Laser Physics in brief [5]

So, the resonant frequency of the resonator must match the energy transition of the gain/laser medium!

16

Laser Physics in brief [5]

17

Laser Physics in brief [5]

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Gain medium in the fiber? [6]• Introduce a rare Earth ion into the fiber:

Called “doping” – Erbium Doped Fiber

Energy band diagram of 𝐸𝑟3+

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Applications [7]

• As a gain medium in a fiber-laser

• As an amplifier in fiber optics: backbone of ALL telecom!

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VCSEL

• Vertical Cavity Surface Emitting Laser [8]

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Electro-optic modulator

22

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GRACE mission (NASA) [9]

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GRACE mission (NASA) [9]

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Revealed ground water depletion over North India to be 1 ft (2002-08)

References

• [1] Griffiths, Introduction to Electrodynamics, 4th Ed. • [2] Ulaby et al., Fundamentals of applied electromagnetics,

6th Ed. • [3] http://www.hoestarinsp.com.sg/FBG1-large.jpg• [4] http://spie.org/x8609.xml• [5] http://www.orc.soton.ac.uk/61.html• [6] http://www.rp-

photonics.com/erbium_doped_gain_media.html• [7] http://www.rp-

photonics.com/erbium_doped_fiber_amplifiers.html• [8] http://japaneseclass.jp/trends/about/VCSEL

[9] http://www.csr.utexas.edu/grace/

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