Difference between revisions of "Optical effects"

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(Wild "photonic steampunk" implementation idea (light generation): added todo)
(Related: added * Ligand field theory)
 
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== Wild "photonic steampunk" implementation idea (light generation) ==
 
== Wild "photonic steampunk" implementation idea (light generation) ==
  
One idea would be to have a dead end of an optical fiber and pass by with an attachment chain (over some stretch) electronically excited material
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The idea is to  
in such a way that the dradgging by catalyses a radiation emitting electronic de-excitation.
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* excite long lived (phosphorescent) electronic states on '''excitation carrier blocks'''
(could probably be combined with laser like stimulated emission).
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* carry them over to an optical fiber via attachment chain
At an other location along the attachment chain the material is electronically re-excited.
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* enforce a controlled deexcitation there (posibly in phase doing for lasing)
Electronically re-excited either by mechanical means, electronic means or in any other suitable way.
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Note that this approach with a chain only makes sense if in-place-re-excitation is a bottleneck. <br>
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See main page: [[Mechanooptical conversion]]
(Kinda hope so, transporting metastable electronic excitations on an nanoscale attachment chain sounds kinda cool.)
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'''Long enough phosphorescent decay time needed''': <br>
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The phosphorescent transition will need to have a long enough decay time to be mechanically transportable from excitation-site to (catalyzed) de-excitation-site. <br>
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Maybe with advanced atomically precise manufacturing capabilities (and fine tunable unusaually large intermolecular forces) a lot bigger range of <br>
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phosphorescent systems will be acessible/developable. {{todo|Investigate design of phosphorescent centers assuming advanced [[gem-gum technology]] is available.}}
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'''No photo-bleaching''': <br>
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Having the photoactive molecules in machine phase may make it possible to avoid "photobleaching" (photoactive molecules taking damage) entirely.
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== Direct electromagnetic wave to mechanical conversions (light reception) ==
 
== Direct electromagnetic wave to mechanical conversions (light reception) ==
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= Related =
 
= Related =
  
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* [[Photonics]]
 
* '''[[Fun with spins]]'''
 
* '''[[Fun with spins]]'''
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* '''[[Electronic transitions]]'''
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* [[Organometallic gemstone-like compound]] – tuning of energy gaps discussed there
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* [[Ligand field theory]]
 
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* [[Energy conversion]] – the conversions that have optical on one side
 
* [[Energy conversion]] – the conversions that have optical on one side
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* [https://en.wikipedia.org/wiki/Photoexcitation Photoexcitation]
 
* [https://en.wikipedia.org/wiki/Photoexcitation Photoexcitation]
 
* [https://en.wikipedia.org/wiki/Category:Photochemistry Category:Photochemistry]
 
* [https://en.wikipedia.org/wiki/Category:Photochemistry Category:Photochemistry]
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----
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* [https://en.wikipedia.org/wiki/Grotrian_diagram Grotrian_diagram] – visualizing the energy levels to see possible transitions and sizes
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* [https://en.wikipedia.org/wiki/Molecular_orbital_diagram Molecular orbital diagram] – visualizing how energy levels change (split up) when bonds (in molecules) are formed
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* Ligand field diagram (or scheme) – [https://en.wikipedia.org/wiki/Ligand_field_theory Ligand field theory]
 
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* [https://en.wikipedia.org/wiki/Ultraviolet Ultraviolet]
 
* [https://en.wikipedia.org/wiki/Ultraviolet Ultraviolet]

Latest revision as of 11:32, 26 August 2022

The mechanical to optical and back conversion challenge

Difference in size-scales

Even rather short optical wavelengths (300nm – near UV) are huge compared to carbon atoms ~0.2nm.
That would make an optical diamond fiber with a radius (or side length if square) of ~1500 carbon atoms.

Assembling such bigger structures would be straightforward with convergent assembly though.
Size scale of optical fibers for visible and far beyond is somewhere between

Difference in time-scales

Moving charges mechanically back and forth or in circles only suffices for generating and receiving radio frequencies.
See: mechanoradio and radiomechanical conversion.

This to have a bridge between the mechanical world of gemstone metamaterial technology and the optical world
other conversionmechanisms are needed.

  • (1) optomechanical conversion where a fast optical electronic excitation eventually causes a slow mechanical conformation change
  • (2) mechanooptical conversion where a machanical manipulation excites an electronic state that eventually emits a photon.

(1) is well known today (2) is pretty exotic.

Wild "photonic steampunk" implementation idea (light generation)

The idea is to

  • excite long lived (phosphorescent) electronic states on excitation carrier blocks
  • carry them over to an optical fiber via attachment chain
  • enforce a controlled deexcitation there (posibly in phase doing for lasing)

See main page: Mechanooptical conversion

Direct electromagnetic wave to mechanical conversions (light reception)

This may be:

  • to receive data
  • to recuperate power (likely more challenging)

Photoinduced conformational changes are likely typically fast and weak.
This seems to call for:

  • a photonically induced buildup of tension with many very fast very small increments
  • a collective mechanical release of big accumulated tension in a single slow step

(TODO: Investigate almost direct optical to mechanical energy conversion in more detail)

Related


  • Energy conversion – the conversions that have optical on one side
  • mechanooptical conversionthis is very new – exciting elecronic stated by force applying mechanic manipulation on bound molecules
  • optomechanical conversionbasically photochemistry – causing a conformational change through electronic structure change through optical


  • Tailored absorption spectra (aka taylored color), fluorescence, and phosphorescence in:
    Polyaromatic pigments, F-centers in gemstones, ...
  • photochromic effects – (like in self-darkening sunglasses)
  • thermochromic effects – (like in color changeing paints)

External links