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Memorial Tributes: Volume 6 (1993)

Chapter: John Bardeen

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Suggested Citation:"John Bardeen." National Academy of Engineering. 1993. Memorial Tributes: Volume 6. Washington, DC: The National Academies Press. doi: 10.17226/2231.
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Suggested Citation:"John Bardeen." National Academy of Engineering. 1993. Memorial Tributes: Volume 6. Washington, DC: The National Academies Press. doi: 10.17226/2231.
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Suggested Citation:"John Bardeen." National Academy of Engineering. 1993. Memorial Tributes: Volume 6. Washington, DC: The National Academies Press. doi: 10.17226/2231.
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Suggested Citation:"John Bardeen." National Academy of Engineering. 1993. Memorial Tributes: Volume 6. Washington, DC: The National Academies Press. doi: 10.17226/2231.
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Suggested Citation:"John Bardeen." National Academy of Engineering. 1993. Memorial Tributes: Volume 6. Washington, DC: The National Academies Press. doi: 10.17226/2231.
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Suggested Citation:"John Bardeen." National Academy of Engineering. 1993. Memorial Tributes: Volume 6. Washington, DC: The National Academies Press. doi: 10.17226/2231.
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Suggested Citation:"John Bardeen." National Academy of Engineering. 1993. Memorial Tributes: Volume 6. Washington, DC: The National Academies Press. doi: 10.17226/2231.
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Suggested Citation:"John Bardeen." National Academy of Engineering. 1993. Memorial Tributes: Volume 6. Washington, DC: The National Academies Press. doi: 10.17226/2231.
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Suggested Citation:"John Bardeen." National Academy of Engineering. 1993. Memorial Tributes: Volume 6. Washington, DC: The National Academies Press. doi: 10.17226/2231.
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Suggested Citation:"John Bardeen." National Academy of Engineering. 1993. Memorial Tributes: Volume 6. Washington, DC: The National Academies Press. doi: 10.17226/2231.
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JOHN BARDEEN 1 908-1 991 BY NICK HOLONYAK, JR. IN JOHN BARDEEN'S own words: In any field there are golden ages during which advances are made at a rapid pace. In solid-state physics, three stand out. One, the early years of the present century, followed the discoveries of x rays, the electron, Planck's quantum of energy, and the nuclear atom- the discoveries that ushered in the atomic era. The Drude-Lorentz electron theory of metals and Einstein's applications of the quan- tum principle to lattice vibrations in solids and to the photoelectric effect date from this period. Von Laue's suggestion in 1912 that a crystal lattice should act as a diffraction grating for x rays and research of the W. H. and W. L. Bragg; sic] opened up the vast field of x-ray structure determination. The foundations of the field were firmly established during a second very active period, from about 1928 until the mid-thirties, which followed the discovery of quantum mechanics. Many of the world's leading theorists were involved in this effort. The Bloch theory, based on the one-electron model, introduced the concept of energy bands and showed why solids, depending on the elec- tronic structure, may be metals, insulators, or semiconductors. The fundamentals of the theory of transport of electricity and of heat in solids were established. In these same years, the importance for many crystal properties of the role of imperfections in the crystal lattice, such as vacant lattice sites, dislocations, and impurity atoms was beginning to be recognized. Some of the names prominent in the developments of solid-state theory during this period are Bloch, Brillouin, Frenkel, Landau, Mott, Peierls, Schottky, Seitz, Slater, A. 3

4 MEMORIAL TRIBUTES H. Wilson, Wigner, and Van Vleck. The third golden age has been the rapid expansion in the post-World War II years, with not only great advances in understanding but also in technology and new products. (Physics 50 Years Later Washington, D.C.: National Acad- emy of Sciences, 1973, pp. 166-167.) If we look for a specific date for the beginning of the "third golden age" of solid-state physics, the logical choice is when Bardeen identified carrier injection in a semiconductor, that is, when Bardeen and Walter Brattain first demonstrated (Decem- ber 16, 1947) the transistor and with it a new principle for an amplifying device (Physical Review 74 ~19481: 230; U.S. Patent 2,524,035, filed June 17, 1948~. Who would have believecI that the Ge band structure, which was then unknown, and carrier lifetime wouIcl have permitted carrier injection, collection, and signal amplification, even if the idea, the notion of a transistor, existed? The semiconductor sullenly took on new importance, and a revolution in electronics followed. With John Bardeen's death on January 30, 199 l, we have passed to another era, maybe now more evolutionary than revolutionary. John Bardeen was born May 23, 190S, in Madison, Wisconsin, where his father, Dr. Charles R. Bardeen, was dean of the University of`Wisconsin medical school. His mother, Althea Harmer Bardeen, was trained as an interior decorator and died in Bardeen's youth, his father later remarrying. Except for his Ph.D., all of John Bardeen's formal education occurred in Wisconsin. He was a true prodigy and at nine years of age skipped from third grade to seventh grade. It is interesting that many years later when he occasionally misspelled a word he attributed this to the drill in spelling he missed in skipping many grades of elementary school. In spite of his obvious talent for mathematics and science, he was given to normal play, mischief, and friencI- ship with his contemporaries, ant! exhibited a fondness for various sports. He learned golfvery early and played the game at a high competitive level all of his life, even into his eighties when his eyesight was failing. Maybe his interest in golf equaled or exceeded his other interests. He had a good sense of humor en c! admitted that maybe two Nobel Prizes (physics, 1956 and 1972) were better than the hole-in-one he once made. At the University

JOHN BARDEEN 5 of Wisconsin he was on the swimming team and also played billiards. One of his wartime coworkers at the Naval Ordnance Laboratory (1941-1945) commented many years later that Bardeen was also not to be challenged in bowling. In addition, he apparentlywas good at cards end was able in his youth to earn spending money playing poker. After finishing high school at age fifteen, Bardeen entered the University of Wisconsin and, in spite of his interest and ability in mathematics and physics, studied electrical engineering, receiv- ing a B.S. in 1928 and an M.S. in 1929. This is one of the first indications of another side of Bardeen, his cor~siderable appre- ciation for the practical as well as his ability to invent. It was not possible for him, however, to suppress his talent and interest in mathematics and physics, and at the University of Wisconsin in his first year as a graduate student (1928) he learned quantum mechanics from Van Vleck and later from Dirac, who deliverer! lectures in Madison based on the famous book publisher] a year later. Instead of finishing his graduate education, Bardeen followed a University of Wisconsin professor to Pittsburgh to work (1930-1933) for Gulf Research and Development Corpo- ration on problems dealing with of} exploration. He became a successful geophysicist, with some of his ideas in of} exploration still kept conficlential. Besides his work at Gulf, his golf, and attending seminars on quantum physics at the University of Pittsburgh, he became acquainted with Jane Maxwell, whom he later married (1938), and with whom he raised a family and spent his entire life. In spite of his success working on geophysical problems, John Bardeen quit his steady employrnentwith Gulfin the heart of the Great Depression to go to graduate school at Princeton Univer- sity (1933-1935~. He had heard that Einstein was coming to Princeton and thought there might be a possibility of working with him. As it turned out, Einstein did not take graduate students, and Bardeen wound up in the Princeton mathematics department (not physics) working for Eugene Wigner, one of the two brilliant young Hungarians (the other was John von Neumann) who had recently arrived in America. Frederick Seitz was Wigner's first research student, Bardeen the second, and

6 MEMORIAL TRIBUTES Conyers Herring the third, which was sufficient to identify Princeton as a center of solid-state physics. For his thesis dealing with the calculation of the work function of metals, Bardeen was awarded his Ph.D. in mathematical physics in 1936. Before his Ph.D. was completed and through the influence of Van Vleck, who had moved from Wisconsin to Harvard Univer- sity, John Bardeen took a position ~ 1935-1938) as ajunior fellow of the Society of Fellows at Harvard, where, incidentally, he overlapped with, among others, James B. Fisk (later of Bell Labs) and Stanislaw Ulam. This was the first time Bardeen was actually in a physics department. At Harvard he worked with Van Vleck and Percy Bridgman, the great high-pressure scientist, and in Cambridge interacted with John Slater and his students at the Massachusetts Institute of Technology. Slater later forgot and referred to John Bardeen as his post-doe. It was Bardeen's Princeton and Harvard years that laid the foundation for his future work. For example, in one of his Urbana seminars in 1970, he mentioned that already at Harvard he had the notion that superconductors possessed an energy gap. Before he became involved in semiconductor research in 1945, he was already deep into the study of metals and superconductors, but had not necessarily decided to pursue solid-state theory as a career. After Harvard, John Bardeen took a teaching position (assis- tant professor, 1938-1941 ~ at the University of Minnesota, ironi- cally for a salary much less than he received at Gulf. Before World War II actually began, he went on leave to the Naval Ordnance Laboratory (1941-1945) and worked on problems of ship de- gaussing and underwater ordnance. At the war's end, and with the need for increased salary for a growing family, he joined the newly formed Bell Telephone Laboratories group that set about acquiring a more fundamental understanding of solids (semi- conductors) and launched, at Kelly's urging, the search for a solid-state replacement for the vacuum tube. Because space was short, Bardeen, a theorist, wound up sharing an office with Walter Brattain and Gerald Pearson, experimentalists, and thus began an intensive collaboration of historic consequences. At Bell Labs Bardeen first checked existing calculations on the operation of a field effect device (an old idea), and agreed the

JOHN BARDEEN 7 calculations were correct and that the failure of the device was not one of principle. Bardeen made the important suggestion that surface states on Si or Ge, the preferred experimental materials (a consequence of World War II developments), im- mobilized the carriers and thwarted conduction and field effect amplification. We cannot describe here all of Bardeen's pub- lished work, several hundred papers, but wish to mention his famousl947paper(PhysicalRe7view71 t19473:717)onsurface states, which, among other features, reveals how thoroughly Bardeen understood the symmetry in electron and hole behav- ior, that is, the importance of both. This proved later to be of some consequence in permitting recognition of carrier injec- tion. The problem with surface states led to an intensive study of surface effects with Walter Brattain. Bardeen realized that fun- damental problems existed with evaporated films then used in field effect experiments, and suggested instead, as a thin con- ducting channel, the use of inversion layers on bulk crystals of known good properties. The first working field effect device, at first on Si and then Ge, employed Barcleen's inversion layer suggestion. It should be noted that Bardeen's inversion layer idea (U.S. Patent 2,524,033, October 3,1950, filed February 26, 1948) is the basis for today's CMOS devices, now so critical in integrated circuits. Most individuals are unaware of where this iclea originated. It is a fascinating story to follow how Bardeen and Brattain, by removing the surface electrolyte (a convenientbut "slow" mecha- nism of fielcI modulation) on their field effect device and by substituting a gold field plate on the crystal, realized instead a gold injection electrode (on e-type Ge) and in the process demonstrated an entirely new device. The device, operating on entirely new principles, was the transistor. Several modifications led to the point contact version of the transistor, which was merelyan experimental simplification of Bardeen and Brattain's first transistor, the first occurring on December 16,1947, and a demonstration to the "brass" (Bardeen'sword) on December 23, 1947. Not only did Bardeen and Brattain introduce the bipolar transistor—a new idea, a new principle, a new device, a new name they also introduced a first embodiment, a direct way to

8 MEMORIAL TRIBUTES convert a crystal into an amplifying or switching crevice. Barcleen has left an account of all of this work ancl how it occurred in his June 1990 NHK Japanese television) interview. The new crevice clemonstratecI by Barcleen ancl Brattain, the transistor, the bipo- lar crevice based on carrier injection (which Barcleen iclentifiecl), served as the prototype for all bipolar anct injection crevices that followocl. A new crevice principle had been establishecI with carrier injection, ancl Barcleen ancI Brattain's transistor anct, whether it was realized or not (December 1947), the semicon- cluctor took on then a new level of importance. In fact, semicon- cluctor electronics as known tociay enjoyocl its beginning, en cl it is proper to say that the "thircl golden age" of solicl-state physics tract truly begun. It was inevitable, since he was in the same office with Brattain en c! Pearson, that John Barcleen would be drawn into semicon- cluctor work, where incleecl, his talents hac] an immediate anc} major impact. For various reasons, however, some clearing with Barcleen's broader interests (inclucling superconcluchvity), some organizational, en cl some being the opportunities that existec! elsewhere, he left Bell Labs in 1951 en cl came to the University of Illinois (Urbana), where he spent the rest of his life. Illinois was attractive to him because Seitz ancl others had already established a base in solicI-state research anct, with a joint ap- pointment in electrical engineering en c} physics, John Barcleen could expand the solicl-state research in Urbana, as he chose, into semiconductor en c] superconductivity research. In 1951 he began his teaching activities, anc! in 1952 he founclec! a semicon- cluctor research activity in electrical engineering ancI, in physics, began a further push to solve the long mysterious problem of · . superconc Sty. At Illinois, besicles continuing his work on semiconductors ancl training a new generation of engineers ancI applier! physi- cists who have themselves made major contributions to semicon- cluctor ancl solicl-state research en cl its applications to electron- ics, John Barcleen, with L. N. Cooper ancI l. R. Schrieffer, constructed ~ ~ 957) the first successful theory of superconcluctiv- ity, the so-called pairing theory. This theory, the Barcleen, Coo- per, anc} Schrieffer (BCS) theory, is universally recognized as

JOHN BARDEEN 9 providing the correct account of the superconductivity of met- als, a phenomenon discovered nearly fifty years earlier (1911~. From the time of its discovery, superconductivity remained unexplained and was studied by a long list of outstanding physicists, including such great men as Felix Bloch, Niels Bohr, Richard Feynman, Werner Heisenberg, Lev Landau, Fritz Lon- don, and Wolfgang Pauli. This gives some idea of the importance attacher! to this long~unsolved problem and of the genius of John Bardeen in recognizing how to go about attacking it. No one else had a better understanding of the problem and how it might be solved. A solution for the problem of superconductivity ranks as one of the major achievements of physics and technology of this century. Superconductivity, of course, has important practical applications (e.g., high-field magnets) and is perceived as offer- ing even a wider range of important uses now that a new family of so-called high Tc oxide superconductors has been discovered. The BCS theory is considered the standarcl for judging and explaining superconductivity in all of its various manifestations, and has provided also the basis for major advances in related fields. It has been used to explain a number of puzzling facts concerning the structure of nuclei. The "pairing" ideas charac- teristic of the BCS theory play nearly as basic of a role in theories of nuclear structure as they do in the explanation of the super- concluctivity of metals. BCS ideas have influenced also the theory of elementary particles and superfluid helium. John Bardeen had a unique influence on the technical and scientific life of our time. As aIreacly mentioned, he, with Brattain, identified minority carrier injection in semiconductors en cl invented the transistor. This event started a revolution in elec- tronics and computer technology that is unparalleled ant! that continues to grow. No other invention of our time has had such a profound effect on society. John Barcleen had an equally profound influence on contemporary physics with the creation of the BCS theory of superconductivity, ant! its far-reaching influence on superconductivity itself and on various related problems. Bardeen was regarded as one of the worId's great solid-state theorists. He was equally renowned as, andwas first, an engineer and inventor. His work shed light on nearly every

10 MEMORIAL TRIBUTES corner of the field of solid-state physics and the conductivity of solids (metals, semiconductors, superconductors, photoconduc- tors, and linear conductors). The foundation of modern elec- tronics rests on much of John Bardeen's work on the conductiv- ity of solids. Even the light emitters and lasers of present-clay optoelectronics rely on the mechanism of carrier injection that begins with Bardeen and Brattain's original bipolar transistor. John Bardeen spoke in a soft voice and at times could be inaudible, particularly when he was tired, deep in thought, or in a long, involved discussion. Some students dubbed him "silent John" or "whispering John, " which was a little unfair considering how generously and fairly Bardeen treated students, and simi- larly colleagues, coworkers, and everyone in general. Everyone sought his advice. In fact, legend held that he was infallible, which, of course, was untrue, but which, of course, had much substance considering his great talent and success as a scientist and engineer. Itwas known that he didn't say much, but whet he said was carefully thought out and important to hear. He was in heavy demand for advice, talks, seminars, committee service, and university, government, and industrial consulting. For ex- ample, itwas well known that he had no small part in helping the Xerox Corporation in the development of several aspects of the xerographic process. He always gave the best possible advice, and was never intimidated, not even by presidential committees. John Bardeen was a man of the highest integrity and never allowed his name to be used improperly or falsely. On difficult doctoral examinations he often was the voice of reason that could see where the canclidate had ability and was apt to make a contribution. He always looked for the best in others, not the worst. The standards he set for himself, for example, were not what he imposed on others. It was amusing to see him smile when he received a preprint, sometimes wrong, from someone coming into an area of work Bardeen initiated. Prob- lems he worked on quickly drew others. It is hard to estimate the total number of students, post-does, visitors, and advisees of all sorts that owed their start to John Bardeen. He was a teacher of the highest order, by example and accomplishment, not by popularity vote. It is also hard to estimate how often he was

JOHN BARDEEN 11 approached to write letters of recommendation for awards, academy memberships, etc., and the burden that this created. John Bardeen was kind and very generous and gave much of himself to others. It seemed his time was never his own. Never- theless, he somehow managed to be a productive scientist and engineer even as his health was failing. In fact, over the years his publication rate did not change, in spite of his great fame and all the demands on his time. Only a month before his death he published a paper in Physics Today (December 1990) on his most recent thoughts and work. Right up to the end of his life, he regularly gave talks and seminars on the "early days of solid-state and transistor research" as well as on superconductivity. Just before his death, he was sorting and assembling material to prepare an account of the history and development of supercon- ductivity, which perhaps no one knew as did John Bardeen. John Bardeen was a rarely gifted person (cf., Physics Today, April 1992) and, of course, received many honors, including the unprecedented award of two Nobel Prizes in physics. His math- ematical and analytical skills were of the highest order, and his intuition for "right and wrong physics" incomparable. He was able to untangle and simplify problems important, difficult (even messy) problems that stopped the best minds. With the transistor and BCS theory of superconductivity, not to mention his other work, he left science and technology, and indeed, the world, much richer than he found it. He, more than anyone else, can be said to be the "godfather" of modern electronics. We will always be inspired by him and be in his debt.

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