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1 The Superlattice Story with the Esaki Tunnel Diode Leo Esaki E-mail: [email protected] President, Yokohama College of Pharmacy Chairman, The Science & Technology Promotion Foundation of Ibaraki
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Leo Esaki- The Superlattice Story with the Esaki Tunnel Diode

Oct 13, 2014

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Page 1: Leo Esaki- The Superlattice Story with the Esaki Tunnel Diode

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The Superlattice Story with the Esaki Tunnel Diode

Leo Esaki

E-mail: [email protected]

President, Yokohama College of Pharmacy Chairman, The Science & Technology Promotion Foundation of Ibaraki

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Standard Form 298 (Rev. 8-98) Prescribed by ANSI Std Z39-18

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Giaever Esaki Schwinger Dirac1973 1973 1965 1933

Lamb Bloch Wigner Rabi Ting Kantorovic1955 1952 1963 1944 1976 1975

1979 Cockchafer����������Speech at Lindau

Participants in the Quantum Revolution

from Science at First Hand – 50 years of the Meetings of Nobel Laureates in Lindau on Lake Constance

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QUANTUM PRINCIPLES INTO PRACTICE Quantum Tunneling –

The Esaki Diode, Double-Barrier ResonantTunnel Diodes, etc.

Quantum Nano-structures � Man-made Superlattices, Wires, Dots, etc.

Quantum Informatics � Quantum Teleportation, Quantum Computers, etc.

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Quantum-Mechanical Effect

Electron Tunneling

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6�����Tunnel Diode 1957

Zener Effect

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8W. Brattain (55 yrs) visited Leo Esaki (32 yrs) at Sony in 1957

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Crystals, Electronics, and Man’s Conquest of Nature W. SHOCKLEY

Shockley Semiconductor Laboratory of Beckman Instruments, Inc. Introduction

It is particularly appropriate that solid state physics and its applications toelectronics should be the subject of an international symposium at theBrussels World’s Fair. The Exposition is dedicated to showing man’sprogress in molding his environment to his liking, and electronics is one of hismost powerful new tools in this endeavor. Furthermore, an importantsymbol of the Fair is the atomic arrangement of a crystal, and crystals are thesubject-matter of solid state physics.

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xxii W. SHOCKLEY The most beautiful demonstration of the Zener effect so farachieved is presented at this symposium by L. Esaki of Tokyo. Esaki has studied p-n junctions which are very heavily doped onboth sides, so that there is a built-in field of the order of 5 x 105

volt/cm. Under these conditions, current flows by the Zenermechanism even at zero voltage. Esaki finds that as forwardbias is increased across the junction, this possibility of directtunneling disappears and, as a consequence, he observes apredictable negative resistance region. The Zener effect is alsodealt with from a theoretical point of view at this meeting by G.H. Wannier of Bell Telephone Laboratories.

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12W. Shockley (48 yrs), Leo Esaki (33 yrs) in 1958

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Examples in 1-D Mathematical Physics: Resonant Electron Tunneling (1930s) Kronig-Penney Bands (1931) Tamm Surface States (1932) Zener Band-to-Band Tunneling (1934) * Stark Ladders including Bloch Oscillations(1940s)* Those which had remained textbook exercises,could for the first time, be practiced in alaboratory: Do-It-Yourself Quantum Mechanics with MBE This approach makes a “gedanken-experiment” a reality and offers a new degree of freedom in semiconductor research. * not observable at ordinary circumstances

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Resonant Tunneling

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Total Energy and Transverse MomentumShould be conserved.

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Chang, Esaki and Tsu (1974)

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IEEE SOLID STATE DEVICE RESEARCH CONFERENCE

Rochester, New York June 23� 26, 1969

Session 4 � Junction and Other Devices Morning Session

Tuesday, June 24, 1969

Chairman: L. Esaki Organizer: R. Stratton IBM Watson Research Center Texas Instruments Inc.

1. The Schottky Barrier Cold C.A. Stolte, J. Vilms, and R.J. Archer Cathode Hewlett-Packard Laboratories

2. Physical Model for Burst Noise S.T. Hsu and R.J. Whittier In Semiconductor Devices Fairchild Semiconductor 3. Ultra-High Speed Power J.S. Roberts Thyristor Turn-On by Laser Triggering Westinghouse Research Laboratories 4. Field Dependence of Space R.H. Krambeck, P.T. Penousis, and Charge and Switching Effects in W.C. Johnson Semiconductors Having High Trap Bell Telephone Laboratories, Inc. Density of Amorphous Structure 5. A Thin Film Inductance Using C.N. Berglund and R.H. Walden Thermal Filaments Bell Telephone Laboratories, Inc. 6. A Superconducting Tunneling Diode W.C. Scott Texas Instruments Incorporated 7. Superlattice and Negative L. Esaki and R. Tsu Conductivity in Semiconductors IBM Watson Research Center

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Mendez, Agullo-Rueda and Hong (1988)

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Esaki, Chang, Howard and Rideout (1972)

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Historical Events of Bloch Oscillations

● Felix Bloch, Z. Physik 52, 555 (1928) “ Über die Quantenmechanik der Electronen in Kristallgittern” The quantum theory of electrons in crystal lattice, implicating Bloch oscillations. ● Clarence Zener, Proc. R. Soc. London, Ser. A145, 523 (1934) “ A Theory of the Electrical Breakdown of Solid Dielectrics”

The theoretical treatment of Zener tunneling and Bloch oscillations.

● Leo Esaki and Ray Tsu, IBM J. Res. Dev. 14, 61 (1970) “ Superlattice and Negative Conductivity in Semiconductors” The first proposal of a semiconductor superlattice with novel properties such as a negative resistance or Bloch oscillations. ● Karl Leo et.al., Solid State Communications 84, 943 (1992) “ Observation of Bloch Oscillations in a Semiconductor Superlattice” The first experimental confirmation of Bloch oscillations.

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Allowed Bands

Conduction Band

Ordinary Semiconductor

Valence Band

Man-Made Superlattice

Forbidden Bands

1�100meV

F: Electric Field

2�3eV

Bloch Oscillation Frequency :ωB = eFd� , whered : Superlattice or Lattice Period,

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Allowed Bands

Conduction Band

Bloch Oscillations

Mini-ZenerTunneling

Ordinary Semiconductor

Valence Band

Man-Made Superlattice

Forbidden Bands

1�100meV

F: Electric Field

2�3eV

Zener Tunneling

Bloch Oscillation Frequency :ωB = eFd� , whered : Superlattice or Lattice Period,

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Bloch oscillation in semiconductor superlattices isthe macroscopic quantum effect similar to theJosephson effect observed in weakly coupledsuperconductors. In both cases, if a DC electricfield is applied to the system, an AC field isgenerated. In Bloch oscillation, the frequency ν B is given byeFd/h = Fd/2Φ 0 where F is the uniform electric fieldstrength, d is the superlattice constant, h denotesPlanck’s constant and Φ 0 is the unit of the fluxquantum, whereas in the Josephson effect, thefrequency ν J is given by 2eV/h = V/Φ 0 where V isan applied voltage.

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380.01 0.1 1 10 100 1000

Out

put P

ower

(W

)

Frequency (THz)

1 μ

1m

1

10 μ

100 μ

10 m

100 m

10

100

RTDPhotomixer

Gunn

Multiplexer

Impatt

MMIC

BWO

p-Ge

THz QCL

QCL

Lead salt laser

III-V laser

FEL

Gyrotron

Technology Gap in the THz Range

Electron Devices Photonic Devices

Bloch oscillator

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39Raphael Tsu and Leo Esaki (right) in 1975

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Ray Tsu, who was involved in thevery early stage of thedevelopment of man-madesuperlattices, recently wrote abook entitled “Superlattice toNanoelectronics”, where he stated “ Frankly, without Esaki’sexperience and forcefulness, I would have given up ” indicating tough environment,and also mentioned what I saidto him on one occasion, “ Experts are not always right ”

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Referee’s comments, rejecting for publication in Physical Review

In summary, then, the paper is highly speculative and presents

little material not already known and understood. While one should not arbitrarily dismiss speculative papers per se, in a case such as the present where an experimental test of the speculation is close at handI believe one should incorporate the material of the paper into onewhich reports the performance of the device so constructed. Thepaper as it now stand has the flavor of a publication whose principalpurpose is to establish priority of an interesting idea. Such arguments can be settled by reference to internal laboratory reports,and already overcrowded journals should not be burdened with thesematters.

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Esaki and his coworkers’ pioneering research onsuperlattices and quantum wells in the 1970s and 1980striggered a wide spectrum of experimental and theoreticalinvestigations resulting in not only the observation of a numberof intriguing new phenomena such as

differential negative resistance, high electron mobilities, large excitonic binding energies, large Stark shifts, distinct Wannier-Stark ladders and Bloch oscillations,

but also the emergence of a new class of transport andoptoelectronic devices such as

high electron-mobility transistors (HEMT), high-speed resonant tunnel diodes, high-performance injection lasers with quantum wells, high-power cascade superlattice lasers.

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Excerpts from the Superlattice Story prepared by US Army Research Office in 1997 The superlattice concept proposed (in February, 1969)under Army sponsored research triggered a revolution insolid state physics.… … The impact of Esaki’s research has been profound. Thesuperlattice concept precipitated more than 10,000publications and is directly involved in some 465 patents inthe U.S. alone, by the end of 1996.… … The superlatticemay be regarded as the trunk of a genealogical tree ofquantum effect devices,… … The characteristic dimensionsof superlattice devices certainly served as the precursor oftoday’s “smaller and smaller” nanotechnology emphasis.

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A list of “five don’ts” which anyone with an interest inrealizing his or her creative potential should follow. Whoknows, it may even help you win a Nobel Prize. Rule number one: Don’t allow yourself to be trapped byyour past experiences. If you allow yourself to get caughtup in social conventions or circumstances, you will notnotice the opportunity for a dramatic leap forward when itpresents itself. Looking back at the history of the NobelPrize, you will notice that most of the laureates havereceived the Nobel Prize for work they had done duringtheir thirties. In my case, I was 32 years old when Ideveloped the “Esaki tunnel diode.” The point that I amtrying to make is that younger people are able to look at things with a clearer vision, one that is not clouded bysocial conventions and past history.

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Rule number two: Don’t allow yourself to become overlyattached to any authority in your field – the great professorperhaps. By becoming closely involved with the greatprofessor, you risk losing sight of yourself and forfeiting thefree spirit of youth. Although the great professor may beawarded the Nobel Prize, it is unlikely that hissubordinates will ever receive it.

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Rule number three: Don’t hold on to what you don’t need.The information-oriented society facilitates easy access toan enormous amount of information. The brain can be compared to a personal computer with an energyconsumption of about 25 watts. In terms of memorycapacity or computing speed, the human brain has notreally changed much since ancient times. Therefore, wemust constantly be inputting and deleting information, andwe should save only the truly vital and relevantinformation. As the president of a university, I have theopportunity to meet with many people and to exchangemeishi (name card) with them. I try to discard the namecards as soon as possible, so that I always leave maximummemory space open. I’m kidding, of course.

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Rule number four: Don’t avoid confrontation. I myselfbecame embroiled in some trouble with the company I was working for many years ago. At times, it is necessary toput yourself first and to defend your own position. Mypoint is that fighting is sometimes unavoidable for the sakeof self-defense. Rule number five: Don’t forget your spirit of childhoodcuriosity. It is the vital component for imagination. Having listed the five rules, let me say that they do notconstitute the sufficient conditions for success. They aremerely suggested guidelines. Good Luck!

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