Crystal detector
A crystal detector is an obsolete
The "asymmetric conduction" of electric current across electrical contacts between a crystal and a metal was discovered in 1874 by
The unamplified radio receivers that used crystal detectors are called crystal radios.[16] The crystal radio was the first type of radio receiver that was used by the general public,[14] and became the most widely used type of radio until the 1920s.[17] It became obsolete with the development of vacuum tube receivers around 1920,[1][14] but continued to be used until World War II and remains a common educational project today thanks to its simple design.
Operation
The contact between two dissimilar materials at the surface of the detector's semiconducting crystal forms a crude
- (A) This graph shows the amplitude modulated radio signal from the receiver's tuned circuit, which is applied as a voltage across the detector's contacts. The rapid oscillations are the radio frequency carrier wave. The audio signal (the sound) is contained in the slow variations (modulation) of the size of the waves. If this signal were applied directly to the earphone, it could not be converted to sound, because the audio excursions are the same on both sides of the axis, averaging out to zero, which would result in no net motion of the earphone's diaphragm.
- (B) This graph shows the current through the crystal detector which is applied to the earphone and bypass capacitor. The crystal conducts current in only one direction, stripping off the oscillations on one side of the signal, leaving a pulsing direct current whose amplitude does not average zero but varies with the audio signal.
- (C) This graph shows the current which passes through the earphone. A bypass capacitor across the earphone terminals, in combination with the intrinsic forward resistance of the diode, creates a low-pass filter that smooths the waveform by removing the radio frequency carrier pulses and leaving the audio signal. When this varying current passes through the earphone piezoelectric crystal, it causes the crystal to deform (flex), deflecting the earphone diaphragm; the varying deflections of the diaphragm cause it to vibrate and produce sound waves (acoustic waves). If instead a voice-coil type headphone is used, the varying current from the low-pass filter flows through the voice coil, generating a varying magnetic field which pulls and pushes the earphone diaphragm, again causing it to vibrate and produce sound.
Crystal radios had no amplifying components to increase the loudness of the radio signal; the sound power produced by the earphone came solely from the radio waves of the radio station being received, intercepted by the antenna. Therefore, the sensitivity of the detector was a major factor determining the sensitivity and reception range of the receiver, motivating much research into finding sensitive detectors.
In addition to its main use in crystal radios, crystal detectors were also used as radio wave detectors in scientific experiments, in which the DC output current of the detector was registered by a sensitive
Types
The crystal detector consisted of an electrical contact between the surface of a
Another type used two crystals of different minerals with their surfaces touching, the most common being the "Perikon" detector. Since the detector would only function when the contact was made at certain spots on the crystal surface, the contact point was almost always made adjustable. Below are the major categories of crystal detectors used during the early 20th century:Cat whisker detector
Patented by Karl Ferdinand Braun and Greenleaf Whittier Pickard[5] in 1906, this was the most common type of crystal detector, mainly used with galena[21][22] but also other crystals. It consisted of a pea-size piece of crystalline mineral in a metal holder, with its surface touched by a fine metal wire or needle (the "cat whisker").[2][4][20][23] The contact between the tip of the wire and the surface of the crystal formed a crude unstable point-contact metal–semiconductor junction, forming a Schottky barrier diode.[4][24] The wire whisker is the anode, and the crystal is the cathode; current can flow from the wire into the crystal but not in the other direction.
Only certain sites on the crystal surface functioned as rectifying junctions.
The detector consisted of two parts mounted next to each other on a flat nonconductive base: a
- Crystal:
- Cat whisker: Phosphor bronze wire of about 30 AWG / 0.25 mm diameter was commonly used as a cat whisker because it had the right amount of springiness.[25][27][29] It was mounted on an adjustable arm with an insulated handle so that the entire exposed surface of the crystal could be probed from many directions to find the most sensitive spot. Cat whiskers in homemade detectors usually had a simple curved shape, but most professional cat whiskers had a coiled section in the middle that served as a spring.[30] The crystal required just the right gentle pressure by the wire; too much pressure caused the device to conduct in both directions.[4] Precision detectors made for radiotelegraphy stations often used a metal needle instead of a "cat's whisker", mounted on a thumbscrew-operated leaf spring to adjust the pressure applied. Gold or silver needles were used with some crystals.
Carborundum detector
Invented in 1906 by Henry H. C. Dunwoody,[31][32] this consisted of a piece of silicon carbide (SiC, then known by the trade name carborundum), either clamped between two flat metal contacts,[4][19][23] or mounted in fusible alloy in a metal cup with a contact consisting of a hardened steel point pressed firmly against it with a spring.[33] Carborundum, an artificial product of electric furnaces produced in 1893, required a heavier pressure than the cat whisker contact.[2][4][19][33] The carborundum detector was popular[21][33] because its sturdy contact did not require readjustment each time it was used, like the delicate cat whisker devices.[2][19][23] Some carborundum detectors were adjusted at the factory and then sealed and did not require adjustment by the user.[2] It was not sensitive to vibration and so was used in shipboard wireless stations where the ship was rocked by waves, and military stations where vibration from gunfire could be expected.[4][19] Another advantage was that it was tolerant of high currents, and could not be "burned out" by atmospheric electricity from the antenna.[2] Therefore, it was the most common type used in commercial radiotelegraphy stations.[33]
Silicon carbide is a semiconductor with a wide
Silicon detector
Patented and first manufactured in 1906 by Pickard,[10][32] this was the first type of crystal detector to be commercially produced.[11] Silicon required more pressure than the cat whisker contact, although not as much as carborundum.[19] A flat piece of silicon was embedded in fusible alloy in a metal cup, and a metal point, usually brass or gold, was pressed against it with a spring.[23][34] The surface of the silicon was usually ground flat and polished. Silicon was also used with antimony[19] and arsenic[27] contacts. The silicon detector was popular because it had much the same advantages as carborundum; its firm contact could not be jarred loose by vibration and it did not require a bias battery, so it saw wide use in commercial and military radiotelegraphy stations.[19]
Crystal-to-crystal detectors
Another category was detectors which used two different crystals with their surfaces touching, forming a crystal-to-crystal contact.[4][23] The "Perikon" detector, invented 1908 by Pickard[35] was the most common. Perikon stood for "PERfect pIcKard cONtact".[4] It consisted of two crystals in metal holders, mounted face to face. One crystal was zincite (zinc oxide, ZnO), the other was a copper iron sulfide, either bornite (Cu5FeS4) or chalcopyrite (CuFeS2).[19][23] In Pickard's commercial detector (see picture), multiple zincite crystals were mounted in a fusible alloy in a round cup (on right), while the chalcopyrite crystal was mounted in a cup on an adjustable arm facing it (on left). The chalcopyrite crystal was moved forward until it touched the surface of one of the zincite crystals. When a sensitive spot was located, the arm was locked in place with the setscrew. Multiple zincite pieces were provided because the fragile zincite crystal could be damaged by excessive currents and tended to "burn out" due to atmospheric electricity from the wire antenna or currents leaking into the receiver from the powerful spark transmitters used at the time. This detector was also sometimes used with a small forward bias voltage of around 0.2V from a battery to make it more sensitive.[19][33]
Although the zincite-chalcopyrite "Perikon" was the most widely used crystal-to-crystal detector, other crystal pairs were also used. Zincite was used with carbon, galena, and tellurium. Silicon was used with arsenic,[27] antimony[19] and tellurium crystals.
History
During the first three decades of radio, from 1888 to 1918, called the
The crystal detector evolved from an earlier device,
The coherer was a very poor detector, motivating much research to find better detectors.[4] It worked by complicated thin film surface effects, so scientists of the time did not understand how it worked, except for a vague idea that radio wave detection depended on some mysterious property of "imperfect" electrical contacts.[4] Researchers investigating the effect of radio waves on various types of "imperfect" contacts to develop better coherers, invented crystal detectors.[40]
Braun's experiments
The "unilateral conduction" of crystals was discovered by
Thirty years after these discoveries, after Bose's experiments, Braun began experimenting with his crystalline contacts as radio wave detectors. In 1906 he obtained a German patent on a galena cat whisker detector, but was too late to obtain patents in other countries.
Bose's experiments
Jagadish Chandra Bose used crystals for radio wave detection at the University of Calcutta in his 60 GHz microwave optics experiments from 1894 to 1900.[43][44] Like other scientists since Hertz, Bose was investigating the similarity between radio waves and light by duplicating classic optics experiments with radio waves.[45] For a receiver he first used a coherer consisting of a steel spring pressing against a metal surface with a current passing through it. Dissatisfied with this detector, around 1897 Bose measured the change in resistivity of dozens of metals and metal compounds exposed to microwaves.[44][46] He experimented with many substances as contact detectors, focusing on galena.
His detectors consisted of a small galena crystal with a metal point contact pressed against it with a thumbscrew, mounted inside a closed waveguide ending in a horn antenna to collect the microwaves.[44] Bose passed a current from a battery through the crystal, and used a galvanometer to measure it. When microwaves struck the crystal the galvanometer registered a drop in resistance of the detector. At the time scientists thought that radio wave detectors functioned by some mechanism analogous to the way the eye detected light, and Bose found his detector was also sensitive to visible light and ultraviolet, leading him to call it an artificial retina. He patented the detector 30 September 1901.[7][9] This is often considered the first patent on a semiconductor device.
Pickard: first commercial detectors
Greenleaf Whittier Pickard may be the person most responsible for making the crystal detector a practical device. Pickard, an engineer with the American Wireless Telephone and Telegraph Co. invented the rectifying contact detector,[47][48] discovering rectification of radio waves in 1902 while experimenting with a coherer detector consisting of a steel needle resting across two carbon blocks.[11][12][48] On 29 May 1902 he was operating this device, listening to a radiotelegraphy station. Coherers required an external current source to operate, so he had the coherer and telephone earphone connected in series with a 3 cell battery to provide power to operate the earphone. Annoyed by background "frying" noise caused by the current through the carbon, he reached over to cut two of the battery cells out of the circuit to reduce the current[11][12]
The frying ceased, and the signals, though much weakened, became materially clearer through being freed of their background of microphonic noise. Glancing over at my circuit, I discovered to my great surprise that instead of cutting out two of the cells I had cut out all three; so, therefore, the telephone diaphragm was being operated solely by the energy of the receiver signals. A contact detector operating without local battery seemed so contrary to all my previous experience that ... I resolved at once to thoroughly investigate the phenomenon.[11][12]
The generation of an audio signal without a DC bias battery made Pickard realize the device was acting as a rectifier. During the next four years, Pickard conducted an exhaustive search to find which substances formed the most sensitive detecting contacts, eventually testing thousands of minerals,
Use during the wireless telegraphy era
Guglielmo Marconi developed the first practical wireless telegraphy transmitters and receivers in 1896, and radio began to be used for communication around 1899. The coherer was used as detector for the first 10 years, until around 1906.[17] During the wireless telegraphy era prior to 1920, there was virtually no broadcasting; radio served as a point-to-point text messaging service. Until the triode vacuum tube began to be used around World War I, radio receivers had no amplification and were powered only by the radio waves picked up by their antennae.[11] Long distance radio communication depended on high power transmitters (up to 1 MW), huge wire antennas, and a receiver with a sensitive detector.[11]
Crystal detectors were invented by several researchers at about the same time.[4] Braun began to experiment with crystal detectors around 1899, around when Bose patented his galena detector.[7] Pickard invented his silicon detector in 1906. Also in 1906 Henry Harrison Chase Dunwoody,[49] a retired general in the U.S. Army Signal Corps, patented the
and L. W. Austin invented a silicon–tellurium detector.Around 1907 crystal detectors replaced the coherer and electrolytic detector to become the most widely used form of radio detector.[17][51] Until the triode vacuum tube began to be used during World War I, crystals were the best radio reception technology, used in sophisticated receivers in wireless telegraphy stations, as well as in homemade crystal radios.[52] In transoceanic radiotelegraphy stations elaborate inductively coupled crystal receivers fed by mile long wire antennas were used to receive transatlantic telegram traffic.[53] Much research went into finding better detectors and many types of crystals were tried.[28] The goal of researchers was to find rectifying crystals that were less fragile and sensitive to vibration than galena and pyrite. Another desired property was tolerance of high currents; many crystals would become insensitive when subjected to discharges of atmospheric electricity from the outdoor wire antenna, or current from the powerful spark transmitter leaking into the receiver. Carborundum proved to be the best of these;[33] it could rectify when clamped firmly between flat contacts. Therefore, carborundum detectors were used in shipboard wireless stations where waves caused the floor to rock, and military stations where gunfire was expected.[4][19]
In 1907–1909,
Between about 1905 and 1915 new types of radio transmitters were developed which produced
Crystodyne: negative resistance diodes
Some semiconductor diodes have a property called and Pickard.[12][57] They noticed that when their detectors were biased with a DC voltage to improve their sensitivity, they would sometimes break into spontaneous oscillations.[57] However these researchers just published brief accounts and did not pursue the effect.
The first person to exploit negative resistance practically was self-taught Russian physicist Oleg Losev, who devoted his career to the study of crystal detectors. In 1922 working at the new Nizhny Novgorod Radio Laboratory he discovered negative resistance in biased zincite (zinc oxide) point contact junctions.[57][58][59][60][61] He realized that amplifying crystals could be an alternative to the fragile, expensive, energy-wasting vacuum tube. He used biased negative resistance crystal junctions to build solid-state
The negative resistance diode was rediscovered with the invention of the tunnel diode in 1957, for which Leo Esaki won the 1973 Nobel Prize in Physics. Today, negative resistance diodes such as the Gunn diode and IMPATT diode are widely used as microwave oscillators in such devices as radar speed guns and garage door openers.
Discovery of the light emitting diode (LED)
In 1907 British Marconi engineer
While investigating crystal detectors in the mid-1920s at Nizhny Novgorod, Oleg Losev independently discovered that biased carborundum and zincite junctions emitted light.[63] Losev was the first to analyze this device, investigate the source of the light, propose a theory of how it worked, and envision practical applications.[63] He published his experiments in 1927 in a Russian journal,[65] and the 16 papers he published on LEDs between 1924 and 1930 constitute a comprehensive study of this device. Losev did extensive research into the mechanism of light emission.[61][63][66] He measured rates of evaporation of benzine from the crystal surface and found it was not accelerated when light was emitted, concluding that the luminescence was a "cold" light not caused by thermal effects.[61][66] He theorized correctly that the explanation of the light emission was in the new science of quantum mechanics,[61] speculating that it was the inverse of the photoelectric effect discovered by Albert Einstein in 1905.[63][67] He wrote to Einstein about it, but did not receive a reply.[63][67] Losev designed practical carborundum electroluminescent lights, but found no one interested in commercially producing these weak light sources.
Losev died in World War II. Due partly to the fact that his papers were published in Russian and German, and partly to his lack of reputation (his upper class birth barred him from a college education or career advancement in Soviet society, so he never held an official position higher than technician) his work is not well known in the West.[63]
Use during the broadcast era
In the 1920s, the amplifying
So during the 1920s vacuum tube receivers replaced crystal radios in all except poor households.[7][16][69] Commercial and military wireless telegraphy stations had already switched to more sensitive vacuum tube receivers. Vacuum tubes temporarily put an end to crystal detector research. The temperamental, unreliable action of the crystal detector had always been a barrier to its acceptance as a standard component in commercial radio equipment[1] and was one reason for its rapid replacement. Frederick Seitz, an early semiconductor researcher, wrote:[13]
Such variability, bordering on what seemed the mystical, plagued the early history of crystal detectors and caused many of the vacuum tube experts of a later generation to regard the art of crystal rectification as being close to disreputable.
The crystal radio became a cheap alternative receiver used in emergencies and by people who could not afford tube radios:[7] teenagers, the poor, and those in developing countries.[54] Building a crystal set remained a popular educational project to introduce people to radio, used by organizations like the Boy Scouts.[16] The galena detector, the most widely used type among amateurs,[4] became virtually the only detector used in crystal radios from this point on.[21][22] The carborundum junction saw some use as a detector in early vacuum tube radios because it was more sensitive than the triode grid-leak detector. Crystal radios were kept as emergency backup radios on ships. During World War II in Nazi-occupied Europe the radio saw use as an easily constructed, easily concealed clandestine radio by Resistance groups.[54] After World War II, the development of modern semiconductor diodes finally made the galena cat whisker detector obsolete.[54]
Development of the theory of semiconductor rectification
A breakthrough came when it was realized that the rectifying action of crystalline semiconductors was not due to the crystal alone but to the presence of impurity atoms in the crystal lattice.[72] In 1930
At that time you could get a chunk of silicon... put a cat whisker down on one spot, and it would be very active and rectify very well in one direction. You moved it around a little bit-maybe a fraction, a thousandth of an inch-and you might find another active spot, but here it would rectify in the other direction.
The "metallurgical purity" chemicals used by scientists to make synthetic experimental detector crystals had about 1% impurities which were responsible for such inconsistent results.[72] During the 1930s progressively better refining methods were developed,[7] allowing scientists to create ultrapure semiconductor crystals into which they introduced precisely controlled amounts of trace elements (called doping).[72] This for the first time created semiconductor junctions with reliable, repeatable characteristics, allowing scientists to test their theories, and later making manufacture of modern diodes possible.
The theory of rectification in a metal-semiconductor junction, the type used in a cat whisker detector, was developed in 1938 independently by
The first modern diodes
The development of microwave technology during the 1930s run up to World War II for use in military radar led to the resurrection of the point contact crystal detector.[7][48][72] Microwave radar receivers required a
After the war,
See also
- Barretter detector
- Electrolytic detector
- Magnetic detector
- List of historic technological nomenclature
- Point-contact transistor
- Reginald Fessenden
References
- ^ ISBN 978-0521289030.
- ^ ISBN 978-1886606012.
- ISBN 978-0750644167.
- ^ ISBN 978-0521835268.
- ^ a b U.S. patent 1,104,073 Greenleaf Whittier Pickard, Detector for Wireless Telegraphy and Telephony, filed: 21 June 1911, granted: 21 July 1914
- ^ ISBN 978-0198530831.
- ^ ISBN 9781566771931. Retrieved 27 June 2018.
- ISBN 978-0521835268.
- ^ a b U.S. patent 755,840 Jagadis Chunder Bose, Detector for Electrical Disturbances, filed: 30 September 1901, granted 29 March 1904
- ^ a b c U.S. patent 836,531 Greenleaf Whittier Pickard, Means for Receiving Intelligence Communicated by Electric Waves, filed: 30 August 1906, granted: 20 November 1906
- ^
- ^ a b c d e f g Pickard, Greenleaf Whittier (August 1919). "How I Invented the Crystal Detector" (PDF). Electrical Experimenter. 7 (4): 325–330, 360. Retrieved 13 June 2016.
- ^ ISBN 978-0-393-31851-7.
- ^ ISBN 978-0-521-29681-6.
- ISBN 978-1315512198.
- ^ ISBN 978-1135176846.
- ^ S2CID 51644366. Retrieved 2010-01-19.
- ^ US National Bureau of Standards (March 1918). Circular No. 74: Radio Instruments and Measurements. Washington DC: United States Government Printing Office. p. 105.
- ^ a b c d e f g h i j k l m n o p q r s t u v Ould, Richard Sheldon (1922). The Principles Underlying Radio Communication, 2nd Ed. (Radio communication pamphlet no. 40). Written by the US Bureau of Standards for US Army Signal Corps. pp. 433–439.
- ^ a b Bucher, Elmer Eustice (1920). The Wireless Experimenters Manual. New York: Wireless Press. p. 167.
- ^ a b c d e f g h Hirsch, William Crawford (June 1922). "Radio Apparatus - What is it made of?". The Electrical Record. 31 (6): 393–394. Retrieved 10 July 2018.
- ^ a b c Cockaday, Laurence M. (1922). Radio-telephony for Everyone. New York: Frederick A. Stokes Co. p. 94.
- ^ a b c d e f g h i Stanley, Rupert (1919). Textbook of Wireless Telegraphy Volume 1: General theory and practice. London: Longmans, Green and Co. pp. 311–318.
- ^ "The cat’s-whisker detector is a primitive point-contact diode. A point-contact junction is the simplest implementation of a Schottky diode, which is a majority-carrier device formed by a metal-semiconductor junction." Shaw, Riley (April 2015). "The cat's-whisker detector". Riley Shaw's personal blog. Retrieved 1 May 2018.
- ^ a b c Lescarboura, Austin C. (1922). Radio for Everybody. New York: Scientific American Publishing Co. pp. 144–146.
- ^ Bucher, Elmer Eustice (1920). The Wireless Experimenter's Manual. Wireless Press. p. 164.
- ^ a b c d Morgan, Alfred Powell (1914). Wireless Telegraph Construction for Amateurs, 3rd Ed. New York: D. Van Nostrand Co. pp. 198–199.
- ^ a b Edelman, Phillip E. (1920). Experimental Wireless Stations. New York: Norman W. Henly Publishing Co. pp. 258–259.
- ^ Cole, Arthur B. (1913). The Operation of Wireless Telegraph Apparatus. New York: Cole and Morgan. p. 15.
- ISBN 978-1-886606-01-2.
- ^ a b U.S. patent 837,616 Henry H. C. Dunwoody, Wireless Telegraph System, filed: 23 March 1906, granted: 4 December 1906
- ^ . Retrieved 31 July 2020.
- ^ a b c d e f g Bucher, Elmer Eustice (1921). Practical Wireless Telegraphy: A Complete Text Book for Students of Radio Communication. New York: Wireless Press, Inc. pp. 135, 139–140.
- ^ Pierce, George Washington (1910). Principles of Wireless Telegraphy. New York: McGraw-Hill Book Co. pp. 160–162.
- ^ a b U.S. patent 912,726 Greenleaf Whittier Pickard, Oscillation receiver, filed: 15 September 1908, granted: 16 February 1909
- ^ A. P. Morgan, Wireless Telegraph Construction for Amateurs, 3rd ed. New York: D. Van Nostrand Co., 1914, p. 135, Fig. 108
- (PDF) from the original on 6 October 2022. Retrieved 8 August 2023.
In any event, we can see how the modern symbol for the diode evolved from a depiction of this physical arrangement, with the arrow representing the catwhisker point contact, as seen in the figure.
- ^ a b c d
Phillips, Vivian J. (1980). Early Radio Wave Detectors. London: Inst. of Electrical Engineers. pp. 18–21. ISBN 978-0906048245.
- ^
Aitken, Hugh G.J. (2014). The Continuous Wave: Technology and American Radio, 1900-1932. Princeton University Press. pp. 4–7, 32–33. ISBN 978-1400854608.
- ^ a b
Phillips, Vivian J. (1980). Early Radio Wave Detectors. London: Inst. of Electrical Engineers. pp. 205–209, 212. ISBN 978-0906048245.
- ^ a b c Pierce, George W. (July 1907). "Crystal rectifiers for electric currents and electric oscillations, Part 1: Carborundum". Physical Review. 25 (1): 31–60. . Retrieved 25 July 2018.
- doi:10.1109/22.643830. Retrieved 29 July 2018. also reprinted on IndianDefense Archived 2018-08-09 at the Wayback Machine
- ^ ISBN 978-0471783015.
- ^ Sarkar, et al (2006) History of Wireless, pp. 477–483
- ^
Bose, Jagadish Chandra (January 1899). "On electric touch and the molecular changes produced in matter by electric waves". Proceedings of the Royal Society of London. 66 (424–433): 452–474. S2CID 121203904.
- ^ "Greenleaf Whittier Pickard". Encyclopaedia Britannica online. Encyclopaedia Britannica Inc. 2018. Retrieved 31 July 2018.
- ^ a b c
Roer, T.G. (2012). Microwave Electronic Devices. Springer Science and Business Media. pp. 5–7. ISBN 978-1461525004.
- ^ Some biographical information on General Henry H.C. Dunwoody is available at Arlington National Cemetery.
- ^ German patent 178871 Karl Ferdinand Braun, Wellenempfindliche Kontaktstel, filed: 18 February 1906, granted: 22 October 1906
- ^ The 1911 edition of the US Navy's manual of radio stated: "There are but two types of detectors now in use: crystal or rectifying detectors and the electrolytic. Coherers and microphones [another type of coherer detector] are practically obsolete, and comparatively few of the magnetic and Audion or valve [triode] detectors have been installed."Robison, Samuel Shelburne (1911). Manual of Wireless Telegraphy for the Use of Naval Electricians, 2nd Ed. Washington DC: United States Naval Institute. p. 128.
- ISBN 978-0906048245.
- ISBN 978-0852967928.
- ^ a b c d e Craddock, Christine D. (24 March 1987). "Crystal Radio: An historical survey" (PDF). Honors Thesis. Ball State University, Muncie, Indiana. Retrieved 2 August 2018.
- ^ a b
Grebennikov, Andrei (2011). RF and Microwave Transmitter Design. John Wiley & Sons. p. 4. ISBN 978-0470520994. Archivedfrom the original on 2016-09-17.
- ^ Pickard, Greenleaf W. (January 1925). "The Discovery of the Oscillating Crystal" (PDF). Radio News. 6 (7): 1166. Retrieved July 15, 2014.
- ^ a b c White, Thomas H. (2003). "Section 14 – Expanded Audio and Vacuum Tube Development (1917–1924)". United States Early Radio History. earlyradiohistory.us. Retrieved September 23, 2012.
- ^ Losev, O. V. (January 1925). "Oscillating Crystals" (PDF). Radio News. 6 (7): 1167, 1287. Retrieved July 15, 2014.
- ^ a b Gabel, Victor (October 1, 1924). "The Crystal as a Generator and Amplifier" (PDF). The Wireless World and Radio Review. 15: 2–5. Archived (PDF) from the original on October 23, 2014. Retrieved March 20, 2014.
- ^
Ben-Menahem, Ari (2009). Historical Encyclopedia of Natural and Mathematical Sciences, Vol. 1. Springer. p. 3588. ISBN 978-3540688310. Archivedfrom the original on 2017-11-23.
- ^ a b c d e f g Lee, Thomas H. (2004) The Design of CMOS Radio-Frequency Integrated Circuits, 2nd Ed., p. 20
- ^ a b Gernsback, Hugo (September 1924). "A Sensational Radio Invention". Radio News: 291. and "The Crystodyne Principle", Radio News, September 1924, pages 294-295, 431.
- ^ a b c d e f g
Zheludev, Nikolay (April 2007). "The life and times of the LED – a 100-year history" (PDF). doi:10.1038/nphoton.2007.34. Archived from the original(PDF) on 2017-03-31. Retrieved 2007-04-11.
- ^ Round, Henry J. (9 February 1907). "A note on carborundum". Electrical World. 49 (6): 309. Retrieved September 1, 2014.
- ^ Losev, O. V. (1927). "Светящийся карборундовый детектор и детектирование с кристаллами" [Luminous carborundum detector and detection with crystals]. Телеграфия и Телефония без Проводов (Wireless Telegraphy and Telephony). 5 (44): 485–494. English version published as Lossev, O. V. (November 1928). "Luminous carborundum detector and detection effect and oscillations with crystals". .
- ^ a b
Schubert, E. Fred (2003). Light-emitting Diodes. Cambridge University Press. pp. 2–3. ISBN 978-0521533515.
- ^ a b
Graham, Loren (2013). Lonely Ideas: Can Russia Compete?. MIT Press. pp. 62–63. ISBN 978-0262019798.
- ^ The 1918 edition of the US Navy's manual of radio stated: "There are two types of detectors now in use: the Audion [triode] and the crystal or rectifying detector. Coherers and microphones [another type of coherer detector] are practically obsolete... but the use of Audions...is increasing."Robison, Samuel Shelburne (1918). Manual of Wireless Telegraphy for the Use of Naval Electricians, 4th Ed. Washington DC: United States Naval Institute. p. 156.
- ISBN 978-0906048245.
- ^ a b c d e
Lukasiak, Lidia; Jakubowski, Andrzej (January 2010). "History of Semiconductors" (PDF). Journal of Telecommunications and Information Technology. ISSN 1509-4553. Retrieved 2 August 2018.
- ^ a b c d "1931: "The Theory Of Electronic Semi-Conductors" is Published". The Silicon Engine. Computer History Museum. 2018. Retrieved 1 August 2018.
- ^ a b c d e f g h Michael Riordan, Lillian Hoddeson (1998) Crystal Fire: The Invention of the Transistor and the Birth of the Information Age, p. 89-93
- ^ Schottky, W. "Halbleitertheorie der Sperrsschicht." Naturwissenschaften Vol. 26 (1938) pp. 843. Abstract in English as "Semiconductor Theory of the Blocking Layer" in Sze, S.M. Semiconductor Devices: Pioneering Papers. (World Scientific Publishing Co., 1991) pp. 381
- ^
Mott, Neville F. (1 May 1939). "The theory of crystal rectifiers". Proceedings of the Royal Society of London, Series A. 171 (944): 27–38. ISBN 978-9810222529.
External links
- Crystal and Solid Contact Rectifiers 1909 publication describes experiments to determine the means of rectification (PDF file).
- Radio Detector Development from 1917 The Electrical Experimenter
- The Crystal Experimenters Handbook 1922 London publication devoted to point-contact diode detectors (PDF file courtesy of Lorne Clark via earlywireless.com)
- Gardner, Arthur C. (August 1945). "Rectifying Crystals" (PDF). Radio. 29 (8): 48–50, 68–69.
- Patents
- U.S. patent 906,991 - Oscillation detector (multiple metallic sulfide detectors), Clifford D. Babcock, 1908
- U.S. patent 912,613 - Oscillation detector and rectifier ("plated" silicon carbide detector with DC bias), G.W. Pickard, 1909
- U.S. patent 912,726 - Oscillation receiver (fractured surface red zinc oxide (zincite) detector), G.W. Pickard, 1909
- U.S. patent 933,263 - Oscillation device (iron pyrite detector), G.W. Pickard, 1909
- U.S. patent 1,118,228 - Oscillation detectors (paired dissimilar minerals), G.W. Pickard, 1914