EM resonators and applicationsCap the ends with metal plates [2] 𝐡 =𝐡0 + βˆ’ +𝐡 0 βˆ’ cos...

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Electromagnetic Resonators EE2025: Uday Khankhoje EE, IIT Madras 1

Transcript of EM resonators and applicationsCap the ends with metal plates [2] 𝐡 =𝐡0 + βˆ’ +𝐡 0 βˆ’ cos...

Electromagnetic Resonators

EE2025: Uday KhankhojeEE, IIT Madras

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Waveguides (recap)

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Waveguides (recap) [1]

1. Maxwell:

2. Expand fields into components:

𝐸 π‘₯, 𝑦, 𝑧, 𝑑 = 𝐸0 π‘₯, 𝑦 𝑒𝑗 πœ”π‘‘βˆ’π‘˜π‘§

𝐸0 = 𝐸π‘₯ π‘₯ + 𝐸𝑦 𝑦 + 𝐸𝑧 𝑧

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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:

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Waveguides (recap) [1]

β€’ TE Solutions of the form

𝐡𝑧(π‘₯, 𝑦, 𝑧, 𝑑) = 𝐡0 cosπ‘šπœ‹π‘₯

π‘Žcos

π‘›πœ‹π‘¦

𝑏𝑒𝑗(πœ”π‘‘βˆ’π‘˜π‘§)

i.e. a fwd travelling wave

Cut off freqs:

πœ”π‘šπ‘› = π‘πœ‹π‘š

π‘Ž

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+𝑛

π‘Ž

2

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Cap the ends with metal plates [2]

𝐡𝑧 = 𝐡0+π‘’βˆ’π‘—π‘˜π‘§ + 𝐡0

βˆ’π‘’π‘—π‘˜π‘§ cosπ‘šπœ‹π‘₯

π‘Žcos

π‘›πœ‹π‘¦

π‘π‘’π‘—πœ”π‘‘

Fwd and bkwd waves

Boundary conditions at 𝑧 = 0, 𝑧 = 𝑑:

𝛻 Γ— 𝐸𝑧= βˆ’π‘—πœ”π΅π‘§

=πœ•πΈπ‘₯

πœ•π‘¦βˆ’

πœ•πΈπ‘¦

πœ•π‘₯= 0

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Cap the ends with metal plates [2]

This implies that 𝐡0+ = βˆ’π΅0

βˆ’ , π‘˜π‘‘ = π‘πœ‹ and :

𝐡𝑧 = βˆ’2𝑗𝐡0+sin

pπœ‹π‘§

𝑑cos

π‘šπœ‹π‘₯

π‘Žcos

π‘›πœ‹π‘¦

π‘π‘’π‘—πœ”π‘‘

The frequency of a waveguide mode earlier was

π‘π‘˜ = πœ”2 βˆ’ πœ”π‘šπ‘›2

Now, k is restricted, so

πœ”0 = π‘πœ‹π‘

𝑑

2

+π‘š

π‘Ž

2

+𝑛

𝑏

2

Waveguide frequency 8

Losses in a resonator

β€’ Perfect metal ⟢ No losses

β€’ Finite 𝜎 β‡’ Boundary conditions get slightly modified β‡’ System supports small range of frequencies around πœ”0

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Waveguide resonator [2]

𝑄 = πœ”0

πΈπ‘›π‘’π‘Ÿπ‘”π‘¦ π‘†π‘‘π‘œπ‘Ÿπ‘’π‘‘

π‘ƒπ‘œπ‘€π‘’π‘Ÿ π‘™π‘œπ‘ π‘‘

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Waveguide resonator [2]

𝑄 β‰ˆπœ”0

Ξ”πœ”

Calculating resonator loss allows Q calc.11

Resonators in the real world

β€’ Fiber-Bragg mirrors [3]

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Resonators in the real world

β€’ Fiber-based resonator [4]

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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(βˆ’

Δ𝐸

π‘˜π‘‡)

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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!

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Laser Physics in brief [5]

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Laser Physics in brief [5]

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

Called β€œdoping” – Erbium Doped Fiber

Energy band diagram of πΈπ‘Ÿ3+

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Applications [7]

β€’ As a gain medium in a fiber-laser

β€’ As an amplifier in fiber optics: backbone of ALL telecom!

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VCSEL

β€’ Vertical Cavity Surface Emitting Laser [8]

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Electro-optic modulator

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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

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

6th Ed. β€’ [3] http://www.hoestarinsp.com.sg/FBG1-large.jpgβ€’ [4] http://spie.org/x8609.xmlβ€’ [5] http://www.orc.soton.ac.uk/61.htmlβ€’ [6] http://www.rp-

photonics.com/erbium_doped_gain_media.htmlβ€’ [7] http://www.rp-

photonics.com/erbium_doped_fiber_amplifiers.htmlβ€’ [8] http://japaneseclass.jp/trends/about/VCSEL

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

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