Superconductivity
Yesterday
"Superconductivity:
The Day Before Yesterday - Yesterday - Today - Tomorrow,"
V. L. Ginzburg, Physics - Uspekhi 43, 573 (2000).
[A marvelous review of
the ghosts of superconductivity, past, present and future,
written in the style only Vitaly Ginzburg can create.
The reference bibliography spans the entire scientific
history of superconductivity to its date of publication.] |
"Further
Experiments with Liquid Helium...The Resistance of Pure
Mercury at Helium Temperatures," as reported by H. Kamerlingh
Onnes, Director of the Physical Laboratory of the Unversity
of Leiden, Commun. Leiden 120b (1911).
[Arguably the first report,
at least in English, of the observation of "zero resistance"
in mercury. Because of the unusual nature and vagaries
(at least from a modern viewpoint) of "publication
lexicography" in The Netherlands at the time, it can be
difficult to actually sort out the time series of events
(hopefully, all this will be sorted out by the 100th
anniversary in 2011!). Toward this end, one should
also consult the following sources (please observe the
inserted comments and Acrobat Bookmarks):
Through Measurement to Knowledge
(a perspective),
KAWA 120b,122b,124c (124c contains the "famous" Hg R vs.
T plot),
KAWA 133a-d (Observation of Ic in Hg, and Tc in Sn and
Pb. The detection of relatively low levels of
"critical current" dashed immediate hopes of lossless
transmission lines, which were being touted right from "t=0"
1911). For an overall summary of work at Onnes'
laboratory from 1910 to 1924, see
CL S34b (A good discussion of the experimental apparati
available at Leiden (photos of representative equipment can
be viewed on the website of
Boerhaave Museum)...and an observation that low
temperatures do not affect radioactivity!), and
CL S50a (Contains the speculation that superconductivity
may constitute a new state of matter...but it's in French!).
For a review of the properties of liquid helium and "pre-Hg"
transport measurements (e.g., Pt...we now know that Pt is
only superconducting as a powder, 0.02 K), see
CL 119, and
CL 120a for the low temperature virial properties of
argon.
CL 160b discusses the superconductivity of Tl and
suggests its transport may be "filamentary." Today we
call that "non-bulk."
An Historical Footnote
In the closing paragraph of
133d, Onnes remarks "...I wish to express my thank(s) to
Mr. G. Holst, assistant at the Physical Laboratory, for the
devotion with which he has helped me..." We now know
that it was
Gilles
Holst who proposed the purification of mercury by
distillation and performed the subsequent experiment that
first revealed superconductivity. Gilles Holst was
thus the "Georg Bednorz" of low temperature
superconductivity and in today's scientific culture would
have justly shared the fame of his better known mentor, as
indeed did Bednorz. To be fair, Holst did go on to
become the founding director of Philips Research Laboratory
and a Professor at Leiden. I find the following
remark by the late Vitaly Lazarevich Ginzburg on early
20th century publication ethics quite cogent: "...Holst
himself had not apparently thought of such a demeanor of
Kamerlingh Onnes as unjust or unusual. The situation
is not clear to me, and for our generation it is quite
unnatural; perhaps 90 years ago morals and manners in the
scientific community were totally different." The
upcoming 100th anniversary of Onnes' and Holst's shared
discovery will provide an opportunity to clarify the
record.
In that regard, the September issue of Physics Today
features a fascinating article by Dirk van Delft and Peter
Kes, both associated with Leiden today,
The Discovery of Superconductivity, containing copies of
Onnes' original notes and drawings of the "dewar" system
used in the mercury experiments. One is reminded
experiments at liquid helium those days were far more
challenging than now.] |
"Ein
neuer Effekt bei Eintritt der Supraleitfaehigkeit (A New
Effect Concerning the Ability to Penetrate a
Superconductor)", W. Meissner and R. Ochsenfeld, Die
Naturwissenshaften 44, 787 (1933).
[(In German) Discovery
that when a superconductor is cooled in an external magnetic
field, that field is expelled from within the
superconductor. It is this effect that differentiates
a superconductor from a "perfect conductor."]
|
"Measurements
of the Specific Heat of Thallium at Liquid Helium
Temperatures," W. H. Keesom and J. A. Kok, Physica 1,
175 (1934). [The first
widely circulated report of a first-order jump in specific
heat in a "Type I" superconductor, a major clue to what
would become GL theory.] |
"On
Supraconductivity I," C. J. Gorter and H. Casimir,
Physica 1, 306 (1934).
[A thermodynamic and
phenomenological treatment of the Meissner-Ochsenfeld field
expulsion effect, showing that such expulsion lowers the
overall free energy and explains the specific heat jump
observed by Keesom and collaborators at Leiden. This
paper is an anticipation of the Ginzburg-Landau theory.] |
"The
Electromagnetic Equations of the Supraconductor," F.
London and H. London, Proc Roy. Soc London A149, 71 (1935).
[An empirical
reformulation of Maxwell's equations to accommodate the
Meissner-Ochsenfeld field expulsion effect. Introduces
the key concept of a magnetic field penetration depth.] |
"The
Discovery of Type II Superconductors (Shubnikov Phase),"
A. G. Shepelev, www.intechopen.com (2010). [In
the process of obtaining the original papers of Shubnikov
and his collaborators regarding the discovery of what came
to be known as "Type II" superconductors in 1936.
Shubnikov was arrested and executed by the Stalinist police
the following year. In the meantime, please read this
excellent history of these events by Shepelev.] |
"Ginzburg-Landau
Theory (Wikipedia)," Zh. Eksp. Teor. Fiz. 20, 1064
(1950). [Can't find
the original Russian or a translation...only Wikipedia...sorry] |
"Isotope
Effect in the Superconductivity of Mercury," E. Maxwell,
Phys. Rev. 78, 477 (1950); "Superconductivity
of Isotopes of Mercury," C. A. Reynolds, B. Serin, W. H.
Wright, and L. B. Nesbitt, Phys. Rev. 78, 487 (1950).
[Both these papers
were submitted simultaneously on 24 March 1950, each
becoming aware of the other's work only a few weeks before
at an ONR conference. Interestingly, earlier attempts
at Leiden in 1922 to observe an isotope effect in Pb, and in
1941 in Germany, failed to give any observable effects.
These present experiments suggested the atomic mass, and
perhaps lattice vibrations, were a fundamental ingredient in
superconductivity.] |
"Theory
of the Superconducting State. I. The Ground State at the
Absolute Zero of Temperature," H. Froehlich, Phys. Rev.
79, 845 (1950).
[This paper is the
first speculation that lattice vibrations might be involved
in superconductivity. However, it deals with the scattering
of only one electron, and not pairs. It explains the earlier
discovery of the isotope effect, although Froehlich was not
aware of its existence when he first submitted this paper.] |
"An
Experimental and Theoretical Study of the Relation between
Magnetic Field and Current in a Superconductor," A.
B. Pippard, Proc. Roy. Soc. (London) A216, 547 (1953).
[In this paper, Brian
Pippard elucidates a fundamental key concept underlying all
BCS-like theories of superconductivity, whether strong or
weak coupling.] |
"On
the Theory of Superconductivity: the One-Dimensional Case,"
H. Froehlich, Proc. Roy. Soc. (London) A223, 296 (1954).
[A seminal, but often
overlooked paper, of possible relevance to eventual "room
temperature perfect conductor." It was employed by Bardeen
in 1973 to interpret the, in turned out erroneous, data by
the Heeger-Garito U. Penn group claiming observations of
superconducting fluctuations in TTF-TCNQ. It does indeed,
however, explain the phenomenon of charge density wave (Peierls)
transitions ubiquitous to quasi-1D-conductors (e.g.,
polyacetylene) and a major competitive instability to
superconductivity in such structures.] |
"Bound
Electron Pairs in a Degenerate Fermi Gas," L. N. Cooper, Phys. Rev.
104, 1189 (1956).
[Cooper's seminal
demonstration that an arbitrarily weak attractive
interaction between electrons degenerate at the Fermi
surface would lead to their pairing. He speculated that such
an attraction could arise from lattice vibrations.] |
"On
the Magnetic Properties of Superconductors of the Second
Group," A. A. Abrikosov,
Sov. Phys. JETP 5, 1174 (1957).
[Abrikosov's
elaboration of the two solutions to the G-L equations
depending on the magnitude of the parameter "kappa" which,
when less than 1/√2, leads to the formation of vortices and
all the physics we associate with Type II superconductors.
See the article by
Berlingcourt for the fascinating pre- and post Cold War
story of Type II superconductors.] |
"Theory
of Superconductivity," J. Bardeen, L. N. Cooper and J.
R. Schrieffer, Phys. Rev. 108, 1175 (1957).
[The BCS Nobel Prize
paper. Finally, an explanation of superconductivity
some 46 years after its discovery. The BCS theory is
the crowning theoretical achievement of condensed matter
physics in the 20th Century. This paper is also an
outstanding review of the past theoretical attempts to
explain superconductivity and why they failed.] |
"Interaction
between Electrons and Lattice Vibrations in a Normal Metal," A. B. Migdal, Sov.
Phys. JETP 6, 996 (1958).
[An
important elaboration of BCS which does not use a
perturbation approach to treat the electron-phonon
interaction. Instead the interaction is renomalized, showing
that pairing occurs for all values of the strength of the
e-p coupling.] |
"Microscopic
Derivation of the Ginzburg-Landau Equations in the Theory of
Superconductivity," L. P. Gorkov, Sov.
Phys. JETP 9, 1364 (1959).
[A
landmark paper proving the Ginzburg-Landau equations can be
derived from BCS theory with charge 2e.] |
"Comparison
of the Macroscopic Theory of Superconductivity with
Experimental Data," V. L. Ginzburg, Sov.
Phys. JETP (USSR) 36, 1930 (1959).
[Essentially
a comment on the paper of
Gorkov pointing out additional "thought" must be given
when using data on "small" samples relative to coherence and
penetration depths.] |
"Interactions
Between Electrons and Lattice Vibrations in a
Superconductors," G. M. Eliashberg,
Sov. Phys. JETP 11, 1364 (1959).
[This
paper continued the work of Migdal up to a value of the e-p
coupling scaled to the ratio of the Debye temperature to the
Fermi energy. Combined with the work of
McMillan, the two works form the basis of the
computational study of strong coupled superconductors.] |
"A
Research Investigation of the Factors That Affect the
Superconducting Properties of Materials," GE Report
AD480235, 15 November 1965.
[The classic GE study
done under Air Force sponsorship which contains the first
detailed study of hysteretic losses in Type II
superconductors, otherwise known at the Bean Model.] |
"Structure
and Properties of High-Field Superconductors," J.
D. Livingston, GE R&D Center Report (ca. 1969-70).
[Jim Livingston's
great little review of critical currents and pinning in Type
II superconductors, probably still the clearest exposition
of these issues and eerily relevant to anisotropic
superconductors yet to be discovered.] |
"Transition
Temperature of Strong-Coupled Superconductors," W. L.
McMillan, Phys. Rev. 167, 331 (1968).
[The "practical theory" of superconductivity which allowed
analytically relating the electron-phonon coupling to
tunneling spectroscopy, the so-called alpha-2 F(omega).] |
"The
Problem of High-Temperature Superconductivity, II," V.
L. Ginzburg, Sov. Phys. Uspekhi 13, 335 (1970).
[The original exposition of VL's "sandwich" concept as an
embodiment for RTSC, better known today as "Ginzburgers."] |
"The
Description of Superconductivity in Terms of Dielectric
Response Function,"
D. A. Kirzhnits, E. G. Maksimov, and D. I. Khomskii, J. Low
Temp. Phys. 10, 79 (1972).
[An alternative, and
in my view, a far more general approach to fermion-fermion
pairing than Eliashberg-McMillan which implicitly is
restricted to a phonon-boson interaction. It employs a
momentum-frequency dependent dielectric function approach
(or more exactly its inverse) similar to, and perhaps
equivalent, to the Lindhard function (see
Andrea Benassi's Thesis). This KMK formalism was
used by
Gutfreund to analytically examine
Bill Little's model for exciton-mediated
superconductivity.] |
"Transition
Temperature of Strong-Coupled Superconductors Reanalyzed,"
P. B. Allen and R. C. Dynes, Phys. Rev. B 12, 905 (1975).
[This paper applies an
important correction to the McMillan BCS Debye temperature
prefactor, involving a logarithmic average over the total
e-p coupling as measured by tunneling spectroscopy.] |
"Critical
Fields, Pauli Paramagnetic Limiting, and Material Parameters
of Nb3Sn and V3Si," T. P. Orlando,
E. J. McNiff, Jr., S. Foner and M. R. Beasley, Phys. Rev. B
19, 4545 (1978).
[The appendices of this paper
contain a tremendously useful compilation of GLAG equations
in various clean and dirty limits.] |
"Type
II Superconductivity: Quest for Understanding," T. G.
Berlincourt, IEEE Trans. Mag. MAG-23, 403 (1987).
[Probably the
definitive history of Type II (hard) superconductors.
Especially fascinating are the tribulations of Shubnikov and
the complete ignorance in the US of the achievements of
Abrikosov due to the curtain of the Cold War.] |
"The
Critical Current of a Superconductor: An Historical Review,"
D. Dew-Hughes,Low Temperature Physics 27, 713 (2001).
[Probably the most up-to-date
summary of the most important parameter for applications,
next to Tc.] |
Back to
Yesterday
Back to
All Things Superconducting
Superconductivity
Today
Con Cuidado...The links addressing the
discovery of the HTSC copper oxide perovskites emphasizes the
contributions of the three IBM Research Laboratories.
"Possibility
of Insulator to Superconductor Phase Transition," B. K.
Chakraverty, J. Physique-Lettres 40,L-99 (1978).
[Alex Mueller cites
this paper, and the following two, as his principal
inspiration to pursue mixed valent charge transition metal
complexes as possible hosts for high temperature
superconductivity.] |
"Bipolarons
and Superconductivity," B. K.
Chakraverty, J. Physique 42, 1351 (1981).
[A elaboration of the
above paper.] |
"Jahn-Teller
Effect in Itinerant Electron Systems: The Jahn-Teller
Polaron," K.-H. Hoeck, H. Nickish and H. Thomas,
Helvetica Physica Acta 56, 237 (1983).
[Mueller attributes
great importance to this paper as pointing to tetragonal
symmetry as hosting strong coupling of itinerant electrons
to a Jahn-Teller distortion such as found in mixed valent
compounds. Quite curiously, several years after the
publication of this paper, Hoeck seems to have "disappeared"
from the scientific scene.] |
"Oxygen
Intercalation in Mixed Valence Copper Oxides Related to the
Perovskites," C. Michel and B.
Raveau, Rev. Chim. Min. 21, 407 (1984).
[This is a very old
journal and has a number of continuations. I have not
been able to obtain a copy yet. It contains the first
Caen paper on LA-4-1-5-13
that Bednorz found.]
[Note added 09/24/2013: Thanks to Eric Hellstrom (ASC
Tallahassee), he and his students have found this historical
jewel...enjoy and make sure you cite them!] |
"The
Oxygen Defect Perovskite BaLa4Cu5O13.4,
a Metallic Conductor," C. Michel, L. Er-Rakho and B. Raveau,
Mat. Res. Bull. 20, 667 (1985).
[An elaboration of
measurements reported in the Revue de Chimie Mineral paper.
Shown are the thermopower and resistivity data from 200 -
550 K. Had measurements been made down to liquid
helium temperatures, it is likely the Caen Group would have
found some traces of superconductivity, especially in the
thermopower. Apparently, the main interest of these
workers in this material was for catalysis applications and
high temperature oxygen sensors for use in, for example,
cement kilns.] |
"Possible
High TC Superconductivity in the Ba-La-Cu-O
System," J. G. Bednorz and K. A. Mueller, Z. Phys B -
Condensed Matter 64, 189 (1986).
[The discovery publication.
Ironically, Bednorz chose initially the only copper oxide
perovskite that's metallic at all temperatures and
superconducting at none, but which is extremely difficult to
make single phase. It was soon recognized that it was
a minor secondary phase responsible for the appearance of
superconductivity and they were on their way. There is
quite a story behind this paper.] |
"Susceptibility
Measurements Support High TC Superconductivity in
the Ba-La-Cu-O System," J. G. Bednorz, M. Takashige and
K. A. Mueller, IBM Report RZ 1537, 19 November 1986.
[This link is actually
to a preprint received on 15 October 1986 by Rick Greene from
Alex Mueller (with autograph!). The Zuerich workers,
contrary to popular belief, in reality were the first to
confirm their own discovery.] |
"Susceptibility
Measurements Support High TC Superconductivity in
the Ba-La-Cu-O System," J. G. Bednorz, M. Takashige and
K. A. Mueller, Europhys. Lett. 3, 379 (1987). [The
paper resulting from the above preprint. Read the note added
prior to publication.] |
"High
Tc Superconductivity in La-Ba-Cu Oxides," S. Uchida, H.
Takagi, K. Kitazawa, and S. Tanaka, Jap. J. Appl. Phys. 26,
L1 (1987). [The first
"outside IBM" publication to verify the Zuerich Lab
discovery ] |
"High
Tc Superconductivity in La-Ba-Cu Oxides. II.- Specification
of the Superconducting Phase," H. Takagi, S. Uchida,
K. Kitazawa, and S. Tanaka, Jap. J. Appl. Phys. 26, L123
(1987). [A curious
paper. Appears to be a "catch-up" to cover experiments
carried out after submission of the above. ] |
|
|
"Flux
Trapping and Superconductive Glass State in La2CuO4-y:Ba,"
K. A. Mueller, M. Takashige and J. G. Bednorz, Phys. Rev.
Letters 58, 1143 (1987).
[This is the third
remarkable paper out of IBM Zuerich which started the whole
subsequent study of flux dynamics in these anisotropic
superconductors.] |
"Superconductivity
at 93 K in a New Mixed-Phase Y-Ba-Cu-O Compound at Ambient
Pressure," W. K. Wu, et al., Phys. Rev. Letters 58, 908
(1987).
[The Wu-Chu discovery
of YBCO...but not 1-2-3.] |
"Superconductivity
Above 90 K in the Compound YBa2Cu3Ox:
Structural, Transport, and Magnetic Properties,"
P. M. Grant, R. B. Beyers, E. M. Engler, G. Lim, S. S. P.
Parkin, M. L. Ramirez, V. Y. Lee, A. Nazzal, J. E. Vazquez
and R. J. Savoy, Phys. Rev. B35, 7242 (1987).
[First Report
of the "1-2-3" Crystal Structure and Material
Processing Conditions. More story to follow. Until
then, go here.] |
|
"Chu
Talk: Woodstock of Physics," 1987 APS March Meeting,
3/18-19/1987, Hilton NYC.
[Paul
Chu's mixed phase discovery engendered the "Woodstock of
Physics." Please watch.] |
"Mueller
Talk: Woodstock of Physics," 1987 APS March Meeting,
3/18-19/1987, Hilton NYC.
[Pay
particular attention to the Alex' last slide...there's an
interesting story within his selection.} |
"Grant
Talk: Woodstock of Physics," 1987 APS March Meeting,
3/18-19/1987, Hilton NYC.
[What we
accomplished in IBM Almaden, San Jose, 4 January 1987 to 4
March 1987. Please watch.] |
|
"Superconductivity Above Liquid Nitrogen Temperature:
Preparation and Properties of a Family of Perovskite-Based
Superconductors,"
E. M. Engler, V. Y. Lee, A. I. Nazzal, R. B. Beyers, G. Lim,
P. M. Grant, S. S. P. Parkin, M. L. Ramirez, J. E. Vazquez
and R. J. Savoy, J. Am. Chem. Soc. 109, 2848 (1987).
[The best paper hands down,
written by Ed Engler, that came out of the 1987 APS Meeting
of March, 1987, the "Woodstock of Physics." This is
the first report, which I was honored to give at
"Woodstock," on the structure, processing and properties, of
the rare earth substitutions for yttrium. There are
two retrospective "blunders" in this paper. One was
the attribution for the lack of superconductivity in
Pr-1-2-3 to the absence of the orthorhombic phase, which was
due to low oxygen concentration, later the subject of a more
comprehensive
paper. The other was reporting superconductivity
in the Ba-Ca-Sr fractional substitution which turned out to
be a blown labeling of samples! What the hell...we
were in battle!] |
"Evidence
for Superconductivity in La2CuO4,"
P. M. Grant, S. S. P. Parkin, V. Y. Lee, E. M. Engler, M.
L. Ramirez, J. E. Vazquez, G. Lim, R. D. Jacowitz and R. L.
Greene, Phys. Rev. Letters 58, 2482 (1987).
[This was a remarkable
discovery. In January, 1987, Rick Greene and I
observed zero thermopower at 41 K, a clear signature of
superconductivity, in an "undoped" sample of La2CuO4
given us by Georg Bednorz, one which was completely
insulating! Read the paper to find out what happened.
High-Temperature superconductivity could have been
discovered in 1954!] |
|
"The
Discovery of a Class of High Temperature Superconductors,"
K. A. Mueller and J. G. Bednorz, Science 237, 1133 (1987).
[Story of the
discovery by the discoverers.] |
"Critical-Current
Measurements in Epitaxial Films of YBa2Cu3O7-x
Compound," P. Chaudhari, et al., Phys. Rev. Letters 58,
2684 (1987). [The first epitaxial
films of Y-123 were made the evening of Monday,10 March
1987, the week before Woodstock, by Bob Laibowitz, using
structural and processing data supplied by IBM Almaden.] |
"Orientation
Dependence of Grain-Boundary Critical Currents in
YBa2Cu3O7-δ
Bicrystals,"
Dimos, et. al, Phys. Rev.
Letters 61, 219 (1987).
[This is the famous "Dimos"
paper that provided the science to jump start the worldwide
development of coated conductor, or Gen 2 tape.] |
"Remarks
at the Federal Conference on Commercial Applications of
Superconductivity,"
R. W. Reagan, International Ballroom,
Washington Hilton Hotel, 11:47 AM, 28 July 1987.
[I was there.
One of two (along with Praveen Chaudhari) invited
representatives from IBM. Reagan gave an absolutely
marvelous speech (he was an actor, and I learned later was
coached by Ed Teller and Ralph Gomory. What many
deemed unusual was that all of the President's senior
cabinet members attended. This was a time when there
was a fear the Japanese would again exploit another American
technology, as was supposed to have happened with VCRs. A
magic moment.] |
|
|
"Resistive
Transition of High Temperature Superconductors," M.
Tinkham, Phys. Rev. Letters 61, 1658 (1988).
[This paper scared the hell
out of us when it appeared, because it implied the newly
discovered HTSC compounds may not be practical because of
thermal depinning of the Abrikosov vortex lattice. Its
appearance engendered a column in Science by Robert Poole, "Superconductivity:
Is the Party Over?" Tinkham concludes that a future
room temperature superconductor may indeed be in the
superconducting state, but not have zero resistance!
This is a great problem for future research.] |
"Superconductivity:
Is the Party Over?," R. Poole, Science 244, 914 (1988).
[Column inspired by
Tinkham's article supported by some of David Bishop's flux
lattice melting work at Bell Labs. The piece quotes a
number of industrial leaders to the effect that "we're not
going to quit." No major corporation has a
superconductivity program today, and one of them that did now belongs
to a French company.] |
"The
Development of Superconductivity Research in Oxides," K.
Alex Mueller (Monograph, date uncertain, ca. 1998-99).
[The description of
the science background and Mueller's thinking that led to
the eventual discovery of high temperature superconductivity
in the copper oxide perovskites.] |
"High-Temperature
Superconductivity (History and General Review)," V. L. Ginzburg, Sov. Phys. Usp. 34,283
(1991). [Written in
Ginzburg's delightful wry English style, containing his reflection on
the recent discoveries of superconductivity in the cuprates
and implications for the future.] |
"Superconductivity
at 39 K in Magnesium Diboride," J. Nagamatsu, N.
Nakagawa, T. Muranaka, Y. Zenitani and J. Akimitsu, Nature
410, 63 (2001). [] |
|
"Ich
war wie in Trance," NZZ am Sonntag, 21 Januar 2006, p.
67. [An
interview (in German) of George Bednorz in the Swiss
National Sunday newspaper on the occasion of the 20th
anniversary of his observation of zero resistance. The
"trance" refers not to the moment of discovery, but when he
received the Nobel Prize and probably had to dance with the
Queen of Sweden.] |
Back to
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All Things Superconducting
Superconductivity
Tomorrow
"Macroscopic
Theory of Superconductivity: Introduction," F. London, Superfluids
I, (John Wiley and Sons, 1950), p.9.
[Bill Little's inspiration.
Incredible. Way before BCS and that a "bosonic field"
may be crucial to superconductivity.) |
"Possibility
of Synthesizing an Organic Superconductor," W. A.
Little, Phys. Rev. 134, A1416 (1964).
[In this paper, Little
examines and elaborates a speculation by F. London that
macromolecules might exhibit superfluid-like properties in
the context of the BSC model formulated a few years earlier.
However, in the molecular structure proposed by Little,
excitons on polarizable side group molecules replace phonons
as the "boson glue" pairing carriers on a conducting polymer
backbone. Curiously, Bill speculates that such a structure
might be capable of self-replication or "reproduction."] |
"Superconductivity
at Room Temperature," W. A. Little, Scientific American
212, 21 (1965). [This
was the paper that inspired Rick Greene and myself to begin
our (to date unsuccessful) search for the realization of
Bill's model in charge-transfer and polymer organics.
You can't always get what you want...go to
SuperTunes. ] |
"The
Problem of High-Temperature Superconductivity, II," V. L. Ginzburg, Usp. Fiz. Nauk 101,
185 (1970) [Sov. Phys. Usp. 13,335 (1970). [Mandatory
reading prior the rest of this page. Ginzburg's
formalism in this paper underlies all that follows.] |
"Dynamic
Effective Electron-Electron Interaction in the Vicinity of a
Polarizable Molecule," W. A. Little and H. Gutfreund,
Phys. Rev. B 4, 817 (1971).
[Numerical calculation of the
spatial, but not momentum, dependence of the electron-exciton
coupling.] |
"The
Description of Superconductivity in Terms of Dielectric
Response Function," D. A. Kirzhnitz, E. G. Maksimov, and
D. I. Khomskii, J. Low. Temp. Phys. 10, 80 (1973).
[This paper, received by the publishers in May, 1972, became
the base theoretical framework for the Davis, Gutfreund and
Little classic model for room temperature superconductivity.
Why has not some ambitious graduate student implemented the
KMK formalism in a DFT framework to assess any given
microscopic model based on the "Little Model"?] |
"Proposed
Model of a High-Temperature Excitonic Superconductor,"
D. Davis, H. Gutfreund, and W. A. Little, Phys. Rev. B 13,
4766 (1976). [The bottom line is that a very particular exciton-fermion
coupling k-space dispersion is required to favor
superconducting pairing over dimerization into a static
Peierls-Froehlich state.] |
"Model
for an Exciton Mechanism of Superconductivity," D.
Allender, J. Bray and J. Bardeen, Phys. Rev. B 7, 1020
(1973). [Speculation that
carries at a metal-semiconductor interface may couple to
excitons in the semiconductor leading to a Little-like
pairing (curiously there is no reference to any of Little's
papers). Many have searched for this effect, and none
(reproducible) have been found.] |
"Comment
on 'Model for an Exciton Mechanism of Superconductivity',"
J. C. Inkson and P. W. Anderson, Phys. Rev. B 8, 4429
(1973). [Claims a technical
error was made by ABB.] |
"Comment
on 'Model for an Exciton Mechanism of Superconductivity' --
A Reply," D. Allender, J. Bray and J. Bardeen, Phys.
Rev. B 8, 4433 (1973).
[Asserts the IA model
does not correspond to theirs. Still no clear experimental
one way or the other.] |
"June
2005 Notre Dame Workshop on the Possibility of RTSC,"
[Abstract List] |
"Design
for a Room Temperature Superconductor," W. E. Pickett,
BES Workshop on Superconductivity, May 2006.
[Better bone up on
Diophantine problems before reading this. A review of
Fibonacci sequences may be useful as well. I am NOT
kidding!] |
"Researchers
Find Extraordinarily High Temperature Superconductivity in
Bio-Inspired Nanopolymer," Paul M. Grant, Physics Today, May 1998.
[My whimsical SciFi
essay covering the great discovery in 2028 of an embodiment
of Bill Little's model of exciton mediated
superconductivity. You eventually "get what you need." (see
SuperTunes)] |
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Application
Surveys/Workshops
"Research
Opportunities in Superconductivity," M. Tinkham, M. R.
Beasley, D. C. Larbalestier, A. F. Clark and D. K. Finnemore,
Report on the Workshop on Problems in Superconductivity,
22-23 August 1983, Copper Mountain, CO (Sponsored by NSF,
ONR and NBS), November, 1983.
[This
workshop was held against the background of a substantial
decline in funding for superconductivity by Federal agencies
and the impending decision taken by IBM during the writing
of this report to scale back its Josephson computer project.
On page 12 one can find the phrase penned by Mac Beasley,
"At the extreme forefront of research in superconductivity
is the empirical search for new superconductors...," which
was quoted by Bednorz and Mueller as the first line of their
discovery paper. This report has only this one
citation in the technical literature, but what a citation!
A lesson to be learned...do not try to justify basic
research on the expectation of applications. By the
way, this report focuses overwhelmingly on electronics...the
only mention of a power application is SMES.] |
"Superconductors:
The Long Road Ahead," S. Foner and T. P. Orlando, MIT
Technology Review, February/March 1988, p. 36.
[Published the year following
the YBCO discovery, this piece expresses great caution over
the high expectations prevalent during this period.
The article is a very good survey of past superconductivity
application attempts, their successes and failures, and the
impact HTSC might or might not have in the future.] |
"Report
on Discussions with Utility Engineers about Superconducting
Generators," D. Forbes and R. Blaugher, NREL/TP-413-20668,
March 1996. [Bottom
Line: The major advantage perceived for HTSC generators was
their projected low life-cycle costs. Most respondents
did not feel a significant US market would develop earlier
than 15 - 20 years from the date of the report. As far
as I know, with the possible exception of a very small LTSC
unit in Japan, no superconducting generators are deployed or
planned for deployment anywhere in the world at present.] |
"The
US Market for High-Temperature Superconducting Wire in
Transmission Cable Applications," D. Forbes, NREL/TP-450-20667,
April 1996.
[This report summarizes a
series of interviews with utility engineers on the market
potential for HTSC cables, wires and tapes. A number
of interesting anecdotes are related which give insight into
various aspects of utility culture. The report
concludes that HTSC wire sales for cables would reach $66 M
in 2006. The future is hard to predict.] |
"Power
Applications of Superconductivity in Japan and Germany,"
D. Larbalestier, et al., WTEC Panel Final Report ISBN
1-883712-46-7, September 1997.
[The infamous male bonding
trip featuring lost colleagues and broken laptops.
This report had major impact on increasing the DOE
superconductivity appropriation thereafter by 60%.] |
"HTS
Cable -- Status, Challenge and Opportunity," A. M.
Wolsky, International Energy Agency Report, 2 December
2004.
[Alan Wolsky's
"Magnum Opus," 407 pages of everything you need or would
ever want to know about superconducting cables.
Lots of good tables on conventional HVDC transmission
lines and cables installed worldwide.] |
"IASS
Workshop -- Long Distance Transmission,"
Organized by C. Rubbia, IASS-Potsdam, 12-13 May 2011.
[This
workshop focused on a vision encompassing the
transmission of several gigawatts of solar power from
North Africa to Central Europe via a network of high
capacity HTSC dc cables running across the Mediterranean
to Italy and Spain and hence northward. It brought
together experts in many areas and represents the state
of the art at the time. This link brings you to
the program agenda and copies of the presentations
delivered.] |
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General Power
Applications Anthology
"Superconductivity
and Electric Power: Promises, Promises...Past, Present and
Future," P. M. Grant, IEEE Trans. Appl. Super. 7, 112
(1997). [Based
on a Plenary Lecture at the 1996 Applied Superconductivity
Conference held in Pittsburg. An in your face review of
where power applications have been, were at in 1997, and
where they might be going. Contains a description of
the "electricity pipe" concept of Grant, Schoenung and
Hassenzahl] |
"Cost
Projections for High Temperature Superconductors," P. M.
Grant and T. P. Sheahen,
http://arxiv.org/ftp/cond-mat/papers/0202/0202386.pdf,
Applied Superconductivity Conference, Palm Springs, CA,
1998. [An
engineering-economy based approach to estimating eventual
cost/performance of both Generation 1 (OPIT/BSCCO/Ag) and
Generation 2 coated conductor (textured YBCO) HTSC tape.
Unlike wires made from non-superconducting metals, e.g.,
copper, the cost/performance in $/kAŚm of HTSC tapes is
highly application specific and cannot be reduced to a
single number.] |
"Potential
Electric Power Applications for Magnesium Diboride,"
P. M. Grant, Mat. Res. Soc. Symp. Proc. 689, 3 (2002).
[A
quite controversial paper showing magnesium diboride
promises to be cost competitive for power transformer
application.] |
"Superconductivity
for Electric Systems 2005 Annual Peer Review," August 2-4, 2005,
L'enfant Plaza Hotel, Washington, D.C.
[Link to the latest DOE
Office of Electricity superconductivity program content,
containing downloadable pdfs of the talks.] |
"Superconductivity
Technology Center at LANL,"
[Home page at Los
Alamos, with detail on their coated conducting program and
links to other sites.] |
"High-Temperature
Superconductivity (HTS) R&D at ORNL,"
[Oak Ridge
superconductivity home page containing details of its
program in wire development and power applications.] |
"DOE
Office of Electricity Delivery & Energy Reliability -
Superconductivity Program,"
[Home page of the DOE
program in power applications of superconductivity.] |
Navigant Report: High Temperature Superconductivity Market
Readiness Review
[DOE commissioned report on
current state of HTSC technology and when market penetration
is likely to occur and where.] |
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Superconducting Cable
Anthology
"Prospect
of Employing Conductors at Low Temperature in Power Cables
and in Power Transformers,"
K. J. R. Wilkinson, Proc. IEE (London) 113, 1509 (1966).
[First
serious consideration of cryoresistive power cables,
including Nb at 4 K operating in the Meissner state!] |
"Superconducting
Lines for the Transmission of Large Amounts of Electric
Power over Great Distances," R. L. Garwin and J. Matisoo,
Proc. IEEE 55, 538 (1967).
[A Classic! All subsequent considerations of
superconducting dc cables derives from Garwin-Matisoo. This
paper is necessary reading for anyone interested in power
applications of superconductivity.] |
"Multiple
Use of Cryogenic Fluid Transmission Lines,"
J. R. Bartlit, F. J. Edeskuty and E. F. Hammel,
Proc. ICEC4, Eindhoven, 24/26 May 1972. [This prescient study from LANL explores the dual delivery of
methane and/or hydrogen as energy agents in a "SuperCable"
concept. However, neither serves as a cryogen...liquid
hydrogen was necessary...the discovery of high temperature
superconductivity was still 13 years in the future!]
|
"dc
Superconducting Power Transmission Line Project at LASL,"
ed. F. J. Edeskuty, US DOE Division of Electric Energy
Systems, 1 November 1972 - 30 September 1979, Progess Report
24 (Final). [Massive and inclusive study of a large capacity, 5 GW SCDC
cable employing Nb3Sn, sponsored by DOE and the
Philadelphia Electric Company (PECO) representing the
interests of several eastern utilities (this was "before
EPRI"). The project was discontinued after building
and testing a few meters of conductor due to lack of funding
and lack of utility interest (Thanks to Dean Peterson of
LANL for making this report public).] |
"Refrigeration
and Heat Transfer in Superconducting Power Lines,"
D. E. Daney and R. H. Hammond, NIST Interim Report
275.05-75-2, April 1975.
[An interesting study of the use of slush hydrogen as
cryogen for an Nb3Ge dc cable. No intention
to use the hydrogen as an energy source in and of itself is
discussed.] |
"A
Study of Refrigeration for Liquid-Nitrogen-Cooled Power
Transmission Cables," R. C. Longworth and K. F.
Schoch, Advances in Cryogenic Engineering, v.25, p.585
(1979). [An
early and classic paper on the engineering economy of
cryocooled cable designs, superconducting or otherwise.
Thanks to Bill Hassenzahl for bringing this document to
my attention.] |
"Practical
Conclusions from Field Trials of a Superconducting Cable,"
P. A. Klaudy and J. Gerhold, IEEE Trans. Mag. MAG-19, 656
(1983). [The
first superconducting cable to be installed on a grid (near
Arnstein, Austria). It used Nb at 6.5 K as the
superconductor and had a capacity of 60 kV at 1000 A and
operated continuously from 1977-80. It may be that the
Nb was operated in the Meissner state...there is no mention
of ac losses. The emphasis was on the flexible design,
rather than the superconducting properties.] |
"Performance
Summary of the Brookhaven Superconducting Power Transmission
System," E. B. Forsyth and R. A. Thomas, Cryogenics 26,
599 (1986). [A
1000 MVA, three phase ac cable built using NbTi at 4 K and
tested at Brookhaven National Laboratory in the years just
preceding the discovery of high temperature
superconductivity. The project was technically
successful, but major utilities did not think the technology
economically feasible (I know this information directly from
several "personal communications.").] |
"Design
Concepts for a Superconducting Cable," J. Engelhardt,
EPRI Research Report TR-103631, September (1994).
[This is a landmark resource focusing fundamental design
approaches to superconducting cable deploying the newly
discovered HTSC copper oxide materials. Con
cuidado...it is 534 pages...and its history chapters are
incomplete (I know...I was present at the Revelation!).] |
"Superconducting
Current Transfer Devices for Use ith a Superconducting
LVdc Mesh," B. K. Johnson, R. H. Lasseter, F.
L. Alvarado, IEEE Trans. Appl. Supercond. 4, 216 (1994).
[The original study pointing out the inherent
instability of "Kirchoff Type" networks interconnected
by "perfect conductors," proving "resistors" need to be
appropriately inserted to prevent chaotic runaway.
For the latest, go
here.] |
"A
dc Transmission Cable Prototype Using High-Temperature
Superconductors," T. P. Beales, et al., Supercond. Sci.
Technol. 9, 43 (1995).
[The first attempt at an HTSC
cable, at least a short one. The design is an interesting
one, targeting a 400 km European "ring buss" with a 400 MW,
40 kV, 10 kA capacity with cold He gas at 4.2 K blown in one
end and warming to 40 K at the other, well within the
critical parameter limits of Bi-2223 throughout that range.] |
"System
Study of Long Distance Low Voltage Transmission Using High
Temperature Superconducting Cable," S. M. Schoenung, W.
V. Hassenzahl and P. M. Grant, EPRI Report WO8065-12, March,
1997. [This
study was inspired by a talk I heard from ABB at the 1996
World Energy Conference in Yokohama, Japan, which compared
the cost effectiveness for well head generation at a vast
natural gas reserve such the Qatar region in the Persian
Gulf and transport over HVDC lines. We studied a third
alternative, that using a superconducting "e-pipe" to
transport power from Qatar to a future
Egyptian-Palestine-Israel-Syrian industrial complex, and
concluded this alternative was attractive for distances
greater than 500 miles.] |
"Superconducting
Cable Construction and Testing," D. von Dollen and J.
Daley, Final Report 1000160, November 2000.
[This project was
better known as the "EPRI/Pirelli Cable," and resulted from
studies performed by EPRI and Pirelli in the early 1990s.
The intent was the design and construction of a 50-m long US
standard "pipe type" cable to retrofit 115 kV ac cables with
an increased 3-phase capacity to 400 MVA. The design
did not have a superconducting shield which simplified the
insulation package (so-called "room temperature
dielectric"), but exposed each phase to induced co-phase ac
losses in addition to those arising from "self-current"
flow. This design was the basis for the Detroit-Edison
demonstration, NKT's Copenhagen Airport, and China's Puji
substation. It was during final testing of this cable
that the "blister/balloon" problem manifested, arising from
leakage of liquid nitrogen into the BSCCO filaments through
pinholes in the Ag tape, leading to its literal "exploding"
when the cable was warmed up. AMSC solved this by
later solder-cladding the silver tapes with stainless steel.
Since this issue was considered proprietary at the time,
there is no discussion of it in this report. |
"ac
Loss in Superconducting Power Cables," M. Daeumling, et
al., Studies of High Temperature Superconductors (ed. A.
Narlikar, Nova Science Publishers), Vol. 33, p. 73 (2000).
[Probably
the best treatise on ac losses in print. Written by
the design team of the Copenhagen Airport Cable.] |
"Copenhagen
Airport Demonstration," Dag Willen, NKT Cables Press
Release, 28 May 2001.
[An RTD design like
Detroit Edison. Worked well, but no follow-on project.
The NKT superconductivity unit was later sold to Nexans.] |
"China's
30m, 35kv/2kA ac HTS Power Cable Project," Ying Xin, et
al., EUCAS 2003.
[This project was
essentially "Detroit-Edison without cryostat leaks" and
performed to its specifications perfectly.
Unfortunately, there are now plans currently in place to
follow-on.]] |
"Field
Demonstration of a 24-kV Warm Dielectric Superconducting
Cable at Detroit Edison," S. Eckroad and N. Kelly, EPRI
FY2003 Annual Progress Report 1002040,
Technical Update, March 2004.
[The Detroit-Edison
demonstration remains today the most realistic deployment of
a superconducting cable, three cables, 120-m each, threaded
though 50-year old clay ducts containing five 90-degree
bends approximately 2-m radius of curvature.
Unfortunately, the cryostat welds contained a number of
martensitic phases resulting in vacuum leaks which prevented
the cable from being fully energized at specification
voltage. However, the critical current and ac loss
properties of the superconducting tape were measured and
found to have undergone little significant degradeation
during the cablve installation. A system study
associated with the project on the impact of coaxial
(shielded) superconducting cables resulted in demonstrating
the network advantages a very low inductive reactance cable
might present in utility operation. |
"R&D
of 22.9 kV/50 MVA HTS Transmission Power Cable in Korea,"
J. Cho, Kunming Symposium, 24 June 2004.
[Review of the entire
Korean program by all participating agencies and not limited
to cables.] |
"Feasibility
of Electric Power Transmission by DC Superconducting Cables,"
P. Chowdhuri, C. Pallem, J. A. Demko and M. J. Gouge
IEEE Trans. Appl. Supercond 15, 3917 (2005).
[Study of GW and
500 MW SCDC cables. Emphasis is on cryogenics,
inverter/converter issues and harmonic control] |
"Southwire
HTS Cable Program Overview," D. Lindsay, 2005 US DOE
Peer Review, 2 August 2005
[Altogether, this is
one of earliest of US HTSC cable programs. The 30-m
installation at Southwire's Carrollton, GA plant has been in
operation almost continuously for six years. The follow-on
project will be installed in the Columbus, OH Bixby
substation. This is an adaptation of a conventional
triaxial design wherein all three phases are enclosed.
The HTSC cable will be 200-m, 13.2 kV, 1000 A/phase 69 MVA
circuit.] |
"Albany
Cable Project Progress Update," C. Weber, R. Lee and K.
Hayashi, 2005 US DOE Peer Review, 2 August 2005.
[Cable demonstration
at a Niagara Mohawk substation using Sumitomo's "3-in-1"
cable design. They plan to have a 15-m segment using Gen 2
YBCO tape.] |
"LIPA
Project Overview," 2005 US DOE Peer Review," 2 August
2005.
[Long Island Power
Authority 610-m 136 kV, 2400 A cable project with Nexans and
American Superconductor.] |
"HTS
Transmission Network Will Be the Key of 21st Century's Power
Grid," R. Hata, Kunming Symposium, 24 June 2004.[A
survey of all tape and cable programs in Japan by Ryosuke
Hata of Sumitomo Electric Industries.] |
"Getting
the Metrics Right," D. Lindsay, 2006 DOE Wire
Development Workshop, 30 January 2006, St. Petersburg, FL.
[A thoughtful
appraisal the present approach to measuring and reporting
"metric" presumed critical to commercial acceptance.
Lindsay suggests adopting a new metric with units "$/system-MVA/meter/30yr
life."] |
|
"A
Superconducting DC Cable," W. Hassenzahl, B.
Gregory, S. Eckroad, S. Nilsson, A. Daneshpooy and P.
Grant, EPRI Final Report 1020458 (Project Manager, S.
Eckroad), December 2009.
[This report
culminates almost five years of effort by the coauthors
underwritten by the Electric Power Research Institute.
It at present is the definitive study of the design and
properties of SCDV cables. For more EPRI research on
power applications of superconductivity, visit
www.epri.com.] |
"Study
on the Integration of High Temperature Superconducting
DD Cables with the Eastern and Western North American
Power Grids," T. Overbye, P. Ribeiro, and T.
Baldwin, EPRI Final Report 1020330 (Project Manager, S.
Eckroad), November 2009.
[This report
discusses a model multi-tap superconducting dc cable
system capable of carrying up to 10 GW over 1000 mile
distances, and the control of inevitable instabilities
inherent in a network of "perfect conductors."] |
"Transient
Response of a Superconducting DC Long Length Cable
System Using Voltage Source Converters," S.
Nilsson and A. Daneshpooy, EPRI Final Report 1020339
(Project Manager, S. Eckroad), December 2009.
[This report
examines the application of "voltage source converters (VSC)"
to multi-tap "relatively low voltage" SCDC cable
networks. VSC electronics are analogous to "field effect
transistors," as opposed to present "current source
controllers" used in HVDC inverter/converter stations
that are similar in operation to the original
Shockley-Bardeen junction transistors. As every
electronic engineer knows, an "infinite input impedance"
active device, like the old fashioned vacuum tube
triode, allows for far simpler circuit design and
control.] |
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SQUIDS
"Magnetocardiography,"
Cardiomag Imaging, Inc., 15 May 2006.
[SQUIDS,
"Superconducting Quantum Interference Devices," are capable of
detecting extremely small magnetic fields of the order 10^-15 T.
All nerve-generated biological functions employ electric
currents and thus generate magnetic fields in principle
detectable by SQUIDS. One notable use has to measure
magnetic fields emanating from the brain, a technique called
magnetoencephalography (MEG). In recent years, SQUID
technology has been extended to detect various heart
pathological conditions, called magnetocardiography (MCG). This
link opens an introductory pamphlet. For more detail,
including videos of actual images and medical relevance, click
here. |
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