Semiconductor Stocks List

Symbol Grade Name
AIQUF L'Air Liquide Ord EU
AIXXF Aixtron Se
ASMIY Asm International Nv
ASMLF ASML Holding N.V
ASMVF Asm Pacific Technolo
ASOE Apollo Solar Energy
ASTI Ascent Solar Technologies
ATEYY Advantest Corporation
ATROB Astronics Corp
BESIY BE Semiconductor Industries N.V.
CMXX Cimetrix Incorporated
CTDT Centaurus Diamond Technologies Inc
DKILF Daikin Inds Ltd
DKILY Daikin Inds Ltd ADR
DNZOY Denso Corp Ltd ADR
DYSOF Dyesol Ltd
DYSOY Dyesol Ltd ADR
FPLSF 5N Plus Inc
GYTI Gyrotron Technology
HPHTF Hamamatsu Photonics
HTHIF Hitachi Ltd Ord
HTHIY Hitachi
IFNNF Infineon Technologie
IFNNY Infineon Tech Ads
IQEPF IQE plc
JNPKF Jenoptik Ag
JSCPY JSR Corporation
KYZN Kyzen Corp
MKTY Mechanical Technolgy
MPMQ MPM Holdings Inc
MTLK Metalink
NDCVF Nordic Vlsi As
NGKSY Ngk Spark Plug Co. Ltd. ADR
NMGC Neomagic Corporation
NNOCF Nanoco Group Plc
POCEF Photon Control Inc
POETF Poet Technologies Inc
RNECY Renesas Electronics Corp
ROHCY Rohm Co Ltd Unsp ADR
SCIA Sci Engineered Materials Inc
SGLFF SGL Carbon SE
SHECF Shin-Etsu Chemical Co., Ltd
SHECY Shin-Etsu Chemical Co., Ltd
SIEGY Siemens Ag
SLOIF Soitec S.A
SMAWF Siemens A G Register
SMMYY Sumitomo Metal
SODI Solitron Devices Inc
SOMMF Sumitomo Chemical Co
SOMMY Sumitomo Chemical Co
SOTK Sono-Tek Corp
SPRS Surge Components Inc
SPVNF Spectra7 Micro
STMEF Stmicroelectronics N
SUMCF Sumco Corporation
SUOPY Sumco Corporation
THKLY THK Co., Ltd
TOELY Tokyo Electron Ltd
TOPPY Toppan Printing
TOSCF Tosoh Corp
YAMCY Yamaha Corp Spon ADR
YASKY Yaskawa
SESMF SÜSS MicroTec SE
HCHMY Hitachi Chemical Co
XPPLF Xp Power Ltd
TOELF Tokyo Electron Ltd
INFG Infinite Graphics
BESVF BE Semiconductor Industries N.V
YASKF Yaskawa Electric Cor
SEPJY Spectris Plc
SKIGF Sanki Engineering Co
PSFT Powersafe Technology Corp
DNPCF Dai Nippon Printing
SHWDY Showa Denko Kk
STMNF Sumitomo Metal Mng C
ASMVY ASM Pacific Technolo
RNWEY REC Silicon ASA
TKCBY Tokai Carbon Co Ltd
SQTX Graphene & Solar Technologies Limited
NNCHY Nissan Chem Inds Ltd
NINOF Nikon Corp
CNHA Conihasset Cap Ptnrs
NCRBF Nippon Carbon Co Ltd
AALBF Aalberts Indus Nv Ord
HRIBF HORIBA, Ltd
HMTLY Hitachi Metals Ltd S
SHWDF Showa Denko Kk
LNTEF Lintec Corp
NGKSF Ngk Spark Plug Co Lt
SEPJF Spectris Plc [United Kingdom]
OCPNF Olympus Corp
JTEKF Jtekt Corporation
THKLF THK Co., Ltd
MCRNF Micro-Mechanics Ltd Ord
VACNY Vat Group Ag ADR
EENEF Electrocomponents Plc [Uk]
NICFF Nichias Corp [Japan]
SNIOF Sensio Technologies Inc
NPPRF Nippon Ceramic Co. Ltd
ADTTF Advantest Corp
SKSUF Sekisui Chem Co
FN Fabrinet
SSG ProShares UltraShort Semiconductors
HPHTY Hamamatsu Photonics
ALFVF Alfa Laval AB (publ)
MX MagnaChip Semiconductor Corporation
TOKCF Tokyo Ohka Kogyo Co
SLOIY Soitec Sa ADR
PKI PerkinElmer, Inc
PSI Invesco Dynamic Semiconductors ETF
QTRH Quarterhill Inc
KNIT Kinetics Group, Inc
SSLLF Siltronic Ag
MDTKF MediaTek Inc
ADKCF Adeka Corp
ROHCF Rohm Co. Ltd
JPAVF Japan Aviation Elect
MSPVF Mansei Corp
VTTGF VAT Group Ag
SGTSY Singulus Technologies Ag ADR

Recent Signals

Date Stock Signal Type
2019-09-20 ASMLF Slingshot Bullish Bullish Swing Setup
2019-09-20 ASMLF Narrow Range Bar Range Contraction
2019-09-20 ASMVY Narrow Range Bar Range Contraction
2019-09-20 ASMVY New 52 Week Closing High Bullish
2019-09-20 ASMVY New 52 Week High Strength
2019-09-20 ASTI Non-ADX 1,2,3,4 Bearish Bearish Swing Setup
2019-09-20 ASTI Narrow Range Bar Range Contraction
2019-09-20 ATEYY New 52 Week High Strength
2019-09-20 ATEYY New 52 Week Closing High Bullish
2019-09-20 ATEYY Narrow Range Bar Range Contraction
2019-09-20 ATEYY Calm After Storm Range Contraction
2019-09-20 ATROB Upper Bollinger Band Walk Strength
2019-09-20 ATROB Non-ADX 1,2,3,4 Bearish Bearish Swing Setup
2019-09-20 CMXX Narrow Range Bar Range Contraction
2019-09-20 CMXX New Uptrend Bullish
2019-09-20 DKILY Three Weeks Tight Range Contraction
2019-09-20 DKILY Slingshot Bullish Bullish Swing Setup
2019-09-20 DKILY Stochastic Sell Signal Bearish
2019-09-20 HTHIF Non-ADX 1,2,3,4 Bullish Bullish Swing Setup
2019-09-20 HTHIF Narrow Range Bar Range Contraction
2019-09-20 HTHIY Non-ADX 1,2,3,4 Bullish Bullish Swing Setup
2019-09-20 HTHIY New Downtrend Bearish
2019-09-20 IFNNY Non-ADX 1,2,3,4 Bullish Bullish Swing Setup
2019-09-20 NDCVF Narrow Range Bar Range Contraction
2019-09-20 NMGC Narrow Range Bar Range Contraction
2019-09-20 NMGC Stochastic Reached Oversold Weakness
2019-09-20 NMGC MACD Bearish Signal Line Cross Bearish
2019-09-20 NMGC Non-ADX 1,2,3,4 Bearish Bearish Swing Setup
2019-09-20 POETF Fell Below 200 DMA Bearish
2019-09-20 POETF Volume Surge Other
2019-09-20 RNECY Non-ADX 1,2,3,4 Bullish Bullish Swing Setup
2019-09-20 RNECY Stochastic Reached Oversold Weakness
2019-09-20 RNECY Narrow Range Bar Range Contraction
2019-09-20 SHECF Upper Bollinger Band Walk Strength
2019-09-20 SHECF Narrow Range Bar Range Contraction
2019-09-20 SHECF New Uptrend Bullish
2019-09-20 SIEGY Narrow Range Bar Range Contraction
2019-09-20 SMAWF Fell Below 50 DMA Bearish
2019-09-20 SMAWF Narrow Range Bar Range Contraction
2019-09-20 SMMYY Pocket Pivot Bullish Swing Setup
2019-09-20 SMMYY 180 Bullish Setup Bullish Swing Setup
2019-09-20 SOTK Narrow Range Bar Range Contraction
2019-09-20 SOTK 1,2,3 Retracement Bearish Bearish Swing Setup
2019-09-20 SOTK Golden Cross Bullish
2019-09-20 SPVNF Doji - Bearish? Reversal
2019-09-20 SPVNF Narrow Range Bar Range Contraction
2019-09-20 SPVNF 50 DMA Resistance Bearish
2019-09-20 SPVNF 20 DMA Resistance Bearish
2019-09-20 THKLF Narrow Range Bar Range Contraction
2019-09-20 TOELY Narrow Range Bar Range Contraction
2019-09-20 YAMCY 50 DMA Resistance Bearish
2019-09-20 YAMCY Stochastic Reached Overbought Strength
2019-09-20 YAMCY Non-ADX 1,2,3,4 Bearish Bearish Swing Setup

A semiconductor material has an electrical conductivity value falling between that of a metal, like copper, gold, etc. and an insulator, such as glass. Their resistance decreases as their temperature increases, which is behaviour opposite to that of a metal. Their conducting properties may be altered in useful ways by the deliberate, controlled introduction of impurities ("doping") into the crystal structure. Where two differently-doped regions exist in the same crystal, a semiconductor junction is created. The behavior of charge carriers which include electrons, ions and electron holes at these junctions is the basis of diodes, transistors and all modern electronics. Some examples of semiconductors are silicon, germanium, and gallium arsenide. After silicon, gallium arsenide is the second most common semiconductor used in laser diodes, solar cells, microwave frequency integrated circuits, and others. Silicon is a critical element for fabricating most electronic circuits.
Semiconductor devices can display a range of useful properties such as passing current more easily in one direction than the other, showing variable resistance, and sensitivity to light or heat. Because the electrical properties of a semiconductor material can be modified by doping, or by the application of electrical fields or light, devices made from semiconductors can be used for amplification, switching, and energy conversion.
The conductivity of silicon is increased by adding a small amount of pentavalent (antimony, phosphorus, or arsenic) or trivalent (boron, gallium, indium) atoms (part in 108). This process is known as doping and resulting semiconductors are known as doped or extrinsic semiconductors. Apart from doping, the conductivity of a semiconductor can equally be improved by increasing its temperature. This is contrary to the behaviour of a metal in which conductivity decreases with increase in temperature.
The modern understanding of the properties of a semiconductor relies on quantum physics to explain the movement of charge carriers in a crystal lattice. Doping greatly increases the number of charge carriers within the crystal. When a doped semiconductor contains mostly free holes it is called "p-type", and when it contains mostly free electrons it is known as "n-type". The semiconductor materials used in electronic devices are doped under precise conditions to control the concentration and regions of p- and n-type dopants. A single semiconductor crystal can have many p- and n-type regions; the p–n junctions between these regions are responsible for the useful electronic behavior.
Although some pure elements and many compounds display semiconductor properties, silicon, germanium, and compounds of gallium are the most widely used in electronic devices. Elements near the so-called "metalloid staircase", where the metalloids are located on the periodic table, are usually used as semiconductors.
Some of the properties of semiconductor materials were observed throughout the mid 19th and first decades of the 20th century. The first practical application of semiconductors in electronics was the 1904 development of the cat's-whisker detector, a primitive semiconductor diode used in early radio receivers. Developments in quantum physics in turn allowed the development of the transistor in 1947 and the integrated circuit in 1958.

More about Semiconductor