215,62 €
287,49 €
-25% su kodu: ENG25
Progress in Nano - Electro - Optics III
Progress in Nano - Electro - Optics III
215,62
287,49 €
  • Išsiųsime per 10–14 d.d.
Near-?eld optical recording is a promising way to realize a recording density 2 of over 1 Tb/in . In this chapter, we focused on the near-?eld optical head, which is a key device for near-?eld optical recording. First, we explained the technical issues regarding the near-?eld optical head and introduced some solutions to these issues. We focused on a highly e?cient near-?eld optical head that uses a wedge-shaped metallic plate, and described its optical pr- erties based on a simulation using a…
  • Leidėjas:
  • Metai: 2004
  • ISBN-10: 3540210504
  • ISBN-13: 9783540210504
  • Formatas: 16.2 x 24.4 x 2.4 cm, kieti viršeliai
  • Kalba: Anglų
  • Extra -25 % nuolaida šiai knygai su kodu: ENG25

Progress in Nano - Electro - Optics III (el. knyga) (skaityta knyga) | knygos.lt

Atsiliepimai

(5.00 Goodreads įvertinimas)

Aprašymas

Near-?eld optical recording is a promising way to realize a recording density 2 of over 1 Tb/in . In this chapter, we focused on the near-?eld optical head, which is a key device for near-?eld optical recording. First, we explained the technical issues regarding the near-?eld optical head and introduced some solutions to these issues. We focused on a highly e?cient near-?eld optical head that uses a wedge-shaped metallic plate, and described its optical pr- erties based on a simulation using a ?nite-di?erence time-domain method. The simulation results con?rmed that a strong optical near ?eld is generated at the apex of the metallic plate when a plasmon is excited in the metallic plate. When a TbFeCo recording medium was placed 10 nm from the ne- ?eld optical head, the size of the optical spot was 30 nm, which corresponds 2 to an areal recording density of approximately 1 Tb/in . The e?ciency was 20% if we assume that the incident beam was a Gaussian beam with a full width at half-maximum of 1u m. Furthermore, we discussed an optical head using two metallic plates. We con?rmed through our simulation that a highly localized optical near ?eld was generated at the gap when the plasmon was excited in the metallic plates. The distribution was 5 nm by 5 nm when the two apices were separated by 5 nm."

EXTRA 25 % nuolaida su kodu: ENG25

215,62
287,49 €
Išsiųsime per 10–14 d.d.

Akcija baigiasi už 1d.16:02:15

Nuolaidos kodas galioja perkant nuo 5 €. Nuolaidos nesumuojamos.

Prisijunkite ir už šią prekę
gausite 2,87 Knygų Eurų!?
Įsigykite dovanų kuponą
Daugiau
  • Leidėjas:
  • Metai: 2004
  • ISBN-10: 3540210504
  • ISBN-13: 9783540210504
  • Formatas: 16.2 x 24.4 x 2.4 cm, kieti viršeliai
  • Kalba: Anglų

Near-?eld optical recording is a promising way to realize a recording density 2 of over 1 Tb/in . In this chapter, we focused on the near-?eld optical head, which is a key device for near-?eld optical recording. First, we explained the technical issues regarding the near-?eld optical head and introduced some solutions to these issues. We focused on a highly e?cient near-?eld optical head that uses a wedge-shaped metallic plate, and described its optical pr- erties based on a simulation using a ?nite-di?erence time-domain method. The simulation results con?rmed that a strong optical near ?eld is generated at the apex of the metallic plate when a plasmon is excited in the metallic plate. When a TbFeCo recording medium was placed 10 nm from the ne- ?eld optical head, the size of the optical spot was 30 nm, which corresponds 2 to an areal recording density of approximately 1 Tb/in . The e?ciency was 20% if we assume that the incident beam was a Gaussian beam with a full width at half-maximum of 1u m. Furthermore, we discussed an optical head using two metallic plates. We con?rmed through our simulation that a highly localized optical near ?eld was generated at the gap when the plasmon was excited in the metallic plates. The distribution was 5 nm by 5 nm when the two apices were separated by 5 nm."

Atsiliepimai

  • Atsiliepimų nėra
0 pirkėjai įvertino šią prekę.
5
0%
4
0%
3
0%
2
0%
1
0%
(rodomas nebus)
[{"option":"174","probability":1,"style":{"backgroundColor":"#f2f2f2"},"image":{"uri":"\/uploads\/images\/wheel_of_fortune\/69738c2a550eb1769180202.png","sizeMultiplier":0.6,"landscape":true,"offsetX":-50}},{"option":"173","probability":1.3,"style":{"backgroundColor":"#d91e2d"},"image":{"uri":"\/uploads\/images\/wheel_of_fortune\/69738c13edaf41769180179.png","sizeMultiplier":0.6,"landscape":true,"offsetX":-50}},{"option":"172","probability":1.6,"style":{"backgroundColor":"#f2f2f2"},"image":{"uri":"\/uploads\/images\/wheel_of_fortune\/69738c00656611769180160.png","sizeMultiplier":0.6,"landscape":true,"offsetX":-50}},{"option":"171","probability":1.5,"style":{"backgroundColor":"#d91e2d"},"image":{"uri":"\/uploads\/images\/wheel_of_fortune\/6979c7e026ae11769588704.png","sizeMultiplier":0.6,"landscape":true,"offsetX":-50}},{"option":"170","probability":1.5,"style":{"backgroundColor":"#f2f2f2"},"image":{"uri":"\/uploads\/images\/wheel_of_fortune\/69738bd43f5c21769180116.png","sizeMultiplier":0.6,"landscape":true,"offsetX":-50}},{"option":"169","probability":1.6,"style":{"backgroundColor":"#d91e2d"},"image":{"uri":"\/uploads\/images\/wheel_of_fortune\/69738b882df611769180040.png","sizeMultiplier":0.6,"landscape":true,"offsetX":-50}},{"option":"167","probability":1.4,"style":{"backgroundColor":"#f2f2f2"},"image":{"uri":"\/uploads\/images\/wheel_of_fortune\/69738b6e6274b1769180014.png","sizeMultiplier":0.6,"landscape":true,"offsetX":-50}},{"option":"166","probability":0.1,"style":{"backgroundColor":"#d91e2d"},"image":{"uri":"\/uploads\/images\/wheel_of_fortune\/69738b36427321769179958.png","sizeMultiplier":0.6,"landscape":true,"offsetX":-50}}]