1 Roland Kersting Department of Physics, Applied Physics, and Astronomy The Science of Information Technology Computing with Light the processing.

Slides:



Advertisements
Similar presentations
Optical sources Lecture 5.
Advertisements

Photoreflectance of Semiconductors Tyler A. Niebuhr.
Chapter 1 Electromagnetic Fields
Interaction of Electromagnetic Radiation with Matter
Early Quantum Theory and Models of the Atom
Shaping the color Optical property of photonic crystals Shine.
Chapter 11: Electromagnetic Waves
Ruby Laser Crystal structure of sapphire: -Al2O3 (aluminum oxide). The shaded atoms make up a unit cell of the structure. The aluminum atom inside the.
All-Optical Header Recognition M. Dagenais Department of Electrical and Computer Engineering, University of Maryland, College Park, MD 20742, USA
Integrated Optic Components  Passive: Requires no input power, like directional couplers, beam splitters, isolators, filters, lenses and prisms  Active:
2. High-order harmonic generation in gases Attosecond pulse generation 1. Introduction to nonlinear optics.
Optical Interconnects Speeding Up Computing Matt Webb PICTURE HERE.
Some quantum properties of light Blackbody radiation to lasers.
Part A: Controlling Oscillation Frequency with Capacitors and Resistors Part B: Diodes and Light Experiment Timer.
INTRO TO SPECTROSCOPIC METHODS (Chapter 6) NATURE OF LIGHT AND INTERACTION WITH MATTER Electromagnetic Radiation (i.e., “light”) –Wave-particle duality.
Fiber-Optic Communications
9. Semiconductors Optics Absorption and gain in semiconductors Principle of semiconductor lasers (diode lasers) Low dimensional materials: Quantum wells,
Optical Devices An Overview of Terms from Optical Computing.
Optical Interconnects Speeding Up Computing Matt Webb PICTURE HERE.
Solar Cells Outline. Single-Junction Solar Cells. Multi-Junction Solar Cells.
Training materials for wireless trainers Radio Physics.
3.1Introduction to CPU Central processing unit etched on silicon chip called microprocessor Contain tens of millions of tiny transistors Key components:
Properties of ElectroMagnetic Radiation (Light)
P6 – The Wave Model of Radiation
SARAN THAMPY D SARAN THAMPY D S7 CSE S7 CSE ROLL NO 17 ROLL NO 17 Optical computing.
Workshop on the Chemistry of Information Technology Welcome! Acknowledgements The American Chemical Society Petroleum Research Fund Type H Grant Program.
Communicating by Light Dr Martin Ams MQ Photonics Research Centre Centre for Ultrahigh bandwidth Devices for Optical Systems (CUDOS) Department of Physics.
KM3NeTmeeting Pylos, Greece, April of 12 Mar van der Hoek et al. electronic department PROGRESS ON OPTICAL MODULATORS FOR KM3NeT Mar van der.
MODULATION AIDA ESMAEILIAN 1. MODULATION  Modulation: the process of converting digital data in electronic form to an optical signal that can be transmitted.
Light and Optics. Unit 8: Light and Optics Chapter 23: The Physical Nature of Light 23.1 Electromagnetic Spectrum 23.2 Interference, Diffraction, and.
McGill Photonic Systems Group Andrew Kirk Micro and nano-optics Optical interconnects Applications of MEMS Lawrence Chen Optical.
Photonic (Optical) Computing Jason Plank. Topics to be Addressed What is photonic computing? How does it compare to conventional electronic computing?
Light and Matter Tim Freegarde School of Physics & Astronomy University of Southampton Classical electrodynamics.
Lecture 7. Tunable Semiconductor Lasers What determines lasing frequency: Gain spectrum A function of temperature. Optical length of cavity Mirror reflectance.
Abstract Although the sine-Gordon equation was originally obtained for the description of four wave-mixing in transmission geometry, it describes self-diffraction.
All-optical control of light on a silicon chip Vilson R. Almeida, Carlos A. Barrios, Roberto R. Panepucci & Michal Lipson School of Electrical and Computer.
Optical telecommunication networks.  Introduction  Multiplexing  Optical Multiplexing  Components of Optical Mux  Application  Advantages  Shortcomings/Future.
Kerr Effect  n = KE a 2 Applied field Kerr effect term An applied electric field, via the Kerr effect, induces birefringences in an otherwise optically.
Terahertz Applications by THz Time Domain Spectroscopy
Surface Plasmon Resonance
1 RF (Radio Frequency) technology BASIC TELECOMMUNICATIONS.
Modulators and Semiconductors ERIC MITCHELL. Acousto-Optic Modulators Based on the diffraction of light though means of sound waves travelling though.
§9.6 High-Frequency Modulation Considerations Lecture 16 In practice, the modulation signal is often at very high frequencies and may occupy a large bandwidth,
Optoelectronics.
Plan for Today (AP Physics 2) Ch 24, 27, and 28 Review Day More Review Materials.
Modelling and Simulation of Passive Optical Devices João Geraldo P. T. dos Reis and Henrique J. A. da Silva Introduction Integrated Optics is a field of.
1 Discussion about the mid-term 4. A high voltage generator is made of a metal sphere with a radius of 6 cm sits on an insulating post. A wire connects.
Optical Computing. Objectives  Definition of Optical computing  Advantages of Optical computing  Optical components for binary digital computer  Misconceptions,
Measurements of High-Field THz Induced Photocurrents in Semiconductors Michael Wiczer University of Illinois – Urbana-Champaign Mentor: Prof. Aaron Lindenberg.
教育部顧問室光通訊系統教育改進計畫台科大 師大 淡江 東南 萬能 教育部顧問室光通訊系統教育改進計畫 台科大 師大 淡江 東南 萬能 3. 光調變器之性能量測 (Modulation Measurements) Modulation measurement is essential in characterizing.
Integrated Coordinated Science End of Year Review.
Light and Optics  The Electromagnetic Spectrum  Interference, Diffraction, and Polarization Wave Properties of Light.
WAVES SP4. Students will analyze the properties and applications of waves. a. Explain the processes that result in the production and energy transfer.
Free Electron Laser Studies
Chapter 1 Electromagnetic Fields
Kankeshwaridevi institute of technology
Optoelectronic Integration
Government engineering college ramgarh
Modelling & Simulation of Semiconductor Devices
Electromagnetic Waves
Optical and Terahertz Spectroscopy of CdSe/ZnS Quantum Dots
The Role of Light in High Speed Digital Design
Origin of The Electromagnetic (EM) Waves
Photonics and Electro-Optical Engineering
Coherent Nonlinear Optics
3.1 Introduction to CPU Central processing unit etched on silicon chip called microprocessor Contain tens of millions of tiny transistors Key components:
Fiber Optic Transmission
Fibre Optic Transmission
Anything that can carry information from a source to a destination.
Presentation transcript:

1 Roland Kersting Department of Physics, Applied Physics, and Astronomy The Science of Information Technology Computing with Light the processing of signals properties of light building a photonic computer future trends ?

2 Roland Kersting Department of Physics, Applied Physics, and Astronomy Signals in IT not applicablebinary system:

3 Roland Kersting Department of Physics, Applied Physics, and Astronomy Making a Byte out of Bits understanding: computing problems can be separated into processing of single bits. tools are: transport comparison storage

4 Roland Kersting Department of Physics, Applied Physics, and Astronomy Signal Processing in IT transport of bits: switching:

5 Roland Kersting Department of Physics, Applied Physics, and Astronomy What is a Bit ? Fourier transform

6 Roland Kersting Department of Physics, Applied Physics, and Astronomy The cut-off frequency

7 Roland Kersting Department of Physics, Applied Physics, and Astronomy Electronics transport of bits: switching:

8 Roland Kersting Department of Physics, Applied Physics, and Astronomy Cut-off frequency vs. clock frequency

9 Roland Kersting Department of Physics, Applied Physics, and Astronomy Clock Frequency of Computers

10 Roland Kersting Department of Physics, Applied Physics, and Astronomy The heat problem

11 Roland Kersting Department of Physics, Applied Physics, and Astronomy Clock Frequency of Computers

12 Roland Kersting Department of Physics, Applied Physics, and Astronomy Photonics Idea: substitute electrical currents with light

13 Roland Kersting Department of Physics, Applied Physics, and Astronomy Let’s build a photonic computer

14 Roland Kersting Department of Physics, Applied Physics, and Astronomy Semiconductor laser

15 Roland Kersting Department of Physics, Applied Physics, and Astronomy Output of a laser rapidly oscillating electromagnetic field 1 fs = 10 –15 s = s

16 Roland Kersting Department of Physics, Applied Physics, and Astronomy Desired: short pulses and pulse trains

17 Roland Kersting Department of Physics, Applied Physics, and Astronomy Let’s build a photonic computer

18 Roland Kersting Department of Physics, Applied Physics, and Astronomy Opto-electronic modulation Search : Interface between optical & electrical pulses Electro-optic modulators example liquid crystals: get dark when electrical bias is applied very slow Pockels-effect: index of refraction depends on applied voltage very fast

19 Roland Kersting Department of Physics, Applied Physics, and Astronomy Using a Mach-Zehnder interferometer

20 Roland Kersting Department of Physics, Applied Physics, and Astronomy Constructive & destructive interference

21 Roland Kersting Department of Physics, Applied Physics, and Astronomy Integration of intensity modulators material: lithiumniobate

22 Roland Kersting Department of Physics, Applied Physics, and Astronomy Let’s build a photonic computer

23 Roland Kersting Department of Physics, Applied Physics, and Astronomy All-optical switching the problem: light doesn’t interact with light

24 Roland Kersting Department of Physics, Applied Physics, and Astronomy Absorption saturation idea: use matter (electrons) to mediate the light-light interaction atom: electrons in orbits/states Pauli-rule: up to 2 electrons per state are allowed transitions by light absorption

25 Roland Kersting Department of Physics, Applied Physics, and Astronomy Optical transition of electrons

26 Roland Kersting Department of Physics, Applied Physics, and Astronomy All-optical switching by saturated absorption AND-gate:

27 Roland Kersting Department of Physics, Applied Physics, and Astronomy Excitation of bulk semiconductors

28 Roland Kersting Department of Physics, Applied Physics, and Astronomy Better: semiconductor heterostructures

29 Roland Kersting Department of Physics, Applied Physics, and Astronomy AlGaAs-Switch

30 Roland Kersting Department of Physics, Applied Physics, and Astronomy We are done: a photonic computer (???)

31 Roland Kersting Department of Physics, Applied Physics, and Astronomy Keep the information for some time Solution: bistable devices Electronics: Flip-Flop

32 Roland Kersting Department of Physics, Applied Physics, and Astronomy The SEED (self-electro-optic effect device)

33 Roland Kersting Department of Physics, Applied Physics, and Astronomy Photoinduced absorption

34 Roland Kersting Department of Physics, Applied Physics, and Astronomy Demonstration of concepts The first steps towards photonic computing: n efficient transfer of data by fibers  rates up to 30 THz n switching times as fast as 100 fs n low switching energies  close to switching energies in electronic n high repetition rates  > 100 GHz  factor 100 higher as in PCs

35 Roland Kersting Department of Physics, Applied Physics, and Astronomy Technological problems n interface electronics-optics  usually slow (10 GHz)  expensive ( ~ 100 US$) n micro integration  devices of dimension 0.03 – 10 mm  for parallel processing arrays of several cm n hybrid technologies  expensive  not acceptable

36 Roland Kersting Department of Physics, Applied Physics, and Astronomy The market n assume for 10 years:  500 Mio Computers  100 US$ for photonic components 50 billion US$ n more important:  relation between market potential and risk: 50 billion US$ risk = ?

37 Roland Kersting Department of Physics, Applied Physics, and Astronomy Research at Rensselaer n optical on chip interconnects n fiber optical connects (Persans) n terahertz optoelectronics (Zhang, Shur, Kersting)

38 Roland Kersting Department of Physics, Applied Physics, and Astronomy The electromagnetic spectrum

39 Roland Kersting Department of Physics, Applied Physics, and Astronomy THz pulses Properties: n THz pulses are information carrier  measure the field n very short light pulses possible n propagate free space & on metal wires  fibers are no longer necessary n switching medium : semiconductors  can be tailored for THz pulses  no hybrid technologies

40 Roland Kersting Department of Physics, Applied Physics, and Astronomy Logic operations with THz pulses

41 Roland Kersting Department of Physics, Applied Physics, and Astronomy THz semiconductor devices Science fiction ? our work: THz modulator 3THz

42 Roland Kersting Department of Physics, Applied Physics, and Astronomy Terahertz differentiator analog computer: calculates the first time-derivative operates at THz frequencies