Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

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Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato

Transcript of Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

Page 1: Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

Introduction to OptoelectronicsOptical storage (1)

Prof. Katsuaki Sato

Page 2: Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

Let’s talk on optical storages!

• Can you tell difference between storages and memories?

• There are a lot of different information storage techniques. What sort of storage devices do you know?

• Can you tell the peculiarity of optical storages in these storages?

Point of discussionDensity, capacity, transfer rate, size, removability

Page 3: Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

Storages• Old storage: stones, paper, films, photographs,

record• Advanced storage• Audio/Video use

– Analog: audio cassette, video tape– Digital: CD, MD, Digital video tape, DVD, HD

• Computer use– Magnetic: MT, FD, HD– Optical: CD-ROM, CD-R, CD-RW, MO, DVD-ROM, DVD-

R, DVD-RW– Semiconductor: Flash memory (USB memory)

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Old storages

• Woods, Bamboo• Stone: example Rosetta Stone• Paper: books, notebooks, etc.• Films: movies, photographs

Page 5: Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

Magnetic Tape (MT)

• Tape recorder

Page 6: Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

Magnetic recording

• History• Magnetic tape and magnetic disk• Recording media and recording head• GMR head for high density• Magneto-optical recording• Hybrid magnetic recording• Solid state nonvolatile magnetic memory

(MRAM)

Page 7: Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

History of magnetic recording

• 1898 V. Poulsen (Denmark) invented wire recorder; Information storage technology by control of magnetic state.

• 1900 The magnetic recorder was exhibited at the Paris EXPO and was praised as “the most interesting invention of recent years”.

• Invention of vacuum tube amplifier by L. De Forest (USA) in1921, together with development of the ring-type magnetic head and the fine magnetic powder applied tape bring about practical magnetic recorder.

Page 8: Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

Recording process

K. Sato ed., Applied Materials Science(Ohm publishing) Fig. 5.18

Recording currenttime

moving directionof recording media

Recorded wavelength

Page 9: Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

Recording process

• Signal current is applied to a coil in the magnetic head which is placed close to the recording medium to generate the magnetic flux, the intensity and direction of which is proportional to the signal.

• The medium is magnetized by the magnetic flux from the head, leading to formation of magnetic domain corresponding to the intensity and polarity of the signal.

• Recorded wavelength ( the length of recorded domain corresponding to one period of the signal) is calculated by =v/f where v is the relative velocity between head and medium, and f the signal frequency)

Page 10: Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

Read out of recorded signal ( 1 )Inductive head

• Electromagnetic inductionElectric voltage proportional to the derivative of the magnetic flux is generated

• Output has the differential form of the recorded signal

• The readout voltage is proportional to the product of the recorded wavelength and relative velocity between the head and the medium.

tE

Spacing loss

Principle of read-out

induction

K. Sato ed., Applied Materials Science(Ohm publishing) Fig. 5.19, 5.20

Running direction

Page 11: Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

Read out of recorded signal ( 2 ) MR (magneto-resistance) head

• Change of the electric resistance of the head by the magnetic flux from the medium is utilized.

• AMR (anisotropic magneto-resistance) was utilized in the early stage and was replaced to GMR (giant magneto-resistance).

N S N SN S

leakage flux

MR head

N S

Page 12: Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

Magnetization curve and GMR

• If F1 and F2 have different Hc then high resistivity state is realized for H between Hc1 and Hc2

H

M

R

H

F1

F2

F1

F2

HC2HC1

F1

F2

F1

F2

F1

F2

Resistance is high for anti-parllel configuration

Page 13: Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

What is GMR?

• Ferromag(F 1 )/Nonmag(N)/Ferromag(F2) multilayer• Small resistance for parallel spin direction of F1 and

F2, while high resistance for antiparallel direction.

Pinned layer

Free layer

Page 14: Introduction to Optoelectronics Optical storage (1) Prof. Katsuaki Sato.

Spin valve

• NiFe(free)/Cu/NiFe(pinned)/AF(FeMn) uncoupled sandwich structure

Exchange bias

Free layer

NonmagnetoclayerPinned layer

Antiferromagnetic ( 例 FeMn)

Synthetic antiferro

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Head clearance

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Increase of areal recorded density

Superparamagnetic limit

MR head

GMR head

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Limit of increase in density is coming

• Until 2000 the increase rate was 100 times per 10 years but it becomes slower.

• The reason of slowing is due to superparamagnetism due to smallness of the recorded region for one bit.

• By the use of perpendicular recording the drawback will be overcome.