Semiconductors Stocks List

Symbol Grade Name
ALLWF Allied Minds Plc
ASMIY Asm International Nv
BESIY BE Semiconductor Industries N.V.
DAIUF Daifuku Co. Ltd.
FELTY Fuji Electric Co., Ltd.
FJTSF Fujitsu Ltd
FJTSY Fujitsu Ltd ADR
HOCPF HOYA Corporation
HOCPY HOYA Corporation
HPHTF Hamamatsu Photonics
HTHIF Hitachi Ltd Ord
HTHIY Hitachi
IQEPF IQE plc
ISDCF Inside Secure
ISRCF Ishares V Plc MSCI World IT USD
NMGC Neomagic Corporation
OCLN Originclear Inc.
OSAGF OSRAM Licht AG
POETF Poet Technologies Inc
PRZM Prism Tech Grp Cmn
QGPLF Quest For Growth Pri
RICOY Ricoh Co Ltd SP ADR
RNECF Renesas Electronics Corporation
RNECY Renesas Electronics Corp
SEKEF Seiko Epson Corp
SEKEY Seiko Epson Unsp ADR
SIUIF Semiconductor MFG In
SLOIF Soitec S.A
SMTOF Sumitomo Electric In
SMTOY Sumitomo Electric In
SOMMF Sumitomo Chemical Co
SOMMY Sumitomo Chemical Co
STRB Strasbaugh
SUOPY Sumco Corporation
TIMNF Timminco Ltd
TOSBF Toshiba Corp
UBLXF U-Blox Hldg Ag
YAMCY Yamaha Corp Spon ADR
SESMF SÜSS MicroTec SE
BESVF BE Semiconductor Industries N.V
ZHUZF Zhuzhou Csr Times
DNXWF Dynex Power
XNGIF Xingda Intl Hldgs Ltd Ord
NINOF Nikon Corp
JIAXF Jiangxi Copper Co Ltd H
NCRBF Nippon Carbon Co Ltd
ZHUZY Zhuzhou Crrc Times Electric Co Ltd ADR
DKSHF Dksh Holding Ltd
ADTTF Advantest Corp
SMI Semiconductor Manufacturing International Corporation
HPHTY Hamamatsu Photonics
GRWXF Draper Esprit Plc
MX MagnaChip Semiconductor Corporation
TOKCF Tokyo Ohka Kogyo Co
PSI Invesco Dynamic Semiconductors ETF
RICOF Ricoh Co. Ltd [Japan]
CVV CVD Equipment Corp
IMI Intermolecular Inc
IMOS Chipmos Tech New
INTC Intel Corp
IOTS Adesto Tech
NANO Nanometrics Inc
NVMI Nova Measuring Instr
ON On Semiconductor
OXSQ Oxford Square Capital Corp
OXSQL Oxford Square Capital Corp. 6.50% Note Due 2024
PLAB Photronics Inc
PSCT S&P Smallcap Information Technology Invesco ETF
SNE Sony Corp
TPVG Triplepoint Venture Growth Bdc
TPVY Triplepoint Venture Growth Bdc Corp 5.75% Notes
VSH Vishay Intertechnology
VSM Versum Materials Inc
ELCTF Elmos Semiconductor Ag
SMICY Semiconductor Manufacturing International

Recent Signals

Date Stock Signal Type
2020-01-17 FELTY Narrow Range Bar Range Contraction
2020-01-17 FELTY Doji - Bearish? Reversal
2020-01-17 FELTY Stochastic Reached Overbought Strength
2020-01-17 FELTY Crossed Above 200 DMA Bullish
2020-01-17 FELTY MACD Bullish Centerline Cross Bullish
2020-01-17 FJTSY NR7 Range Contraction
2020-01-17 FJTSY Narrow Range Bar Range Contraction
2020-01-17 HOCPY Fell Below 20 DMA Bearish
2020-01-17 HOCPY Fell Below 50 DMA Bearish
2020-01-17 HOCPY Fell Below 200 DMA Bearish
2020-01-17 HOCPY Wide Range Bar Range Expansion
2020-01-17 HOCPY New Downtrend Bearish
2020-01-17 HOCPY Expansion Breakdown Bearish Swing Setup
2020-01-17 HOCPY MACD Bearish Centerline Cross Bearish
2020-01-17 HOCPY Expansion Pivot Sell Setup Bearish Swing Setup
2020-01-17 HTHIY Fell Below 50 DMA Bearish
2020-01-17 HTHIY 200 DMA Support Bullish
2020-01-17 HTHIY Wide Range Bar Range Expansion
2020-01-17 HTHIY MACD Bearish Centerline Cross Bearish
2020-01-17 HTHIY Expansion Pivot Sell Setup Bearish Swing Setup
2020-01-17 IQEPF Crossed Above 20 DMA Bullish
2020-01-17 IQEPF Volume Surge Other
2020-01-17 IQEPF Narrow Range Bar Range Contraction
2020-01-17 IQEPF Non-ADX 1,2,3,4 Bearish Bearish Swing Setup
2020-01-17 IQEPF Pocket Pivot Bullish Swing Setup
2020-01-17 ISRCF New 52 Week High Strength
2020-01-17 ISRCF New 52 Week Closing High Bullish
2020-01-17 ISRCF Upper Bollinger Band Walk Strength
2020-01-17 ISRCF Gilligan's Island Sell Setup Bearish Swing Setup
2020-01-17 ISRCF Expansion Breakout Bullish Swing Setup
2020-01-17 NMGC Narrow Range Bar Range Contraction
2020-01-17 NMGC Stochastic Reached Overbought Strength
2020-01-17 NMGC Bollinger Band Squeeze Range Contraction
2020-01-17 OCLN NR7 Range Contraction
2020-01-17 OCLN Narrow Range Bar Range Contraction
2020-01-17 POETF Narrow Range Bar Range Contraction
2020-01-17 POETF MACD Bearish Signal Line Cross Bearish
2020-01-17 POETF Non-ADX 1,2,3,4 Bullish Bullish Swing Setup
2020-01-17 PRZM Crossed Above 20 DMA Bullish
2020-01-17 PRZM Narrow Range Bar Range Contraction
2020-01-17 RICOY Expansion Breakout Bullish Swing Setup
2020-01-17 RICOY New 52 Week High Strength
2020-01-17 RICOY Volume Surge Other
2020-01-17 RICOY New 52 Week Closing High Bullish
2020-01-17 RICOY Pocket Pivot Bullish Swing Setup
2020-01-17 SEKEF Narrow Range Bar Range Contraction
2020-01-17 SEKEF Stochastic Reached Overbought Strength
2020-01-17 SEKEY Crossed Above 20 DMA Bullish
2020-01-17 SEKEY Crossed Above 50 DMA Bullish
2020-01-17 SEKEY NR7 Range Contraction
2020-01-17 SEKEY Narrow Range Bar Range Contraction
2020-01-17 SEKEY Cup with Handle Other
2020-01-17 SIUIF New 52 Week High Strength
2020-01-17 SIUIF Narrow Range Bar Range Contraction
2020-01-17 SIUIF New 52 Week Closing High Bullish
2020-01-17 SIUIF Upper Bollinger Band Walk Strength
2020-01-17 SIUIF Calm After Storm Range Contraction
2020-01-17 SIUIF Pocket Pivot Bullish Swing Setup
2020-01-17 SMICY Expansion Pivot Sell Setup Bearish Swing Setup
2020-01-17 SMICY Fell Below 20 DMA Bearish
2020-01-17 SMICY Fell Below 50 DMA Bearish
2020-01-17 SMICY New 52 Week High Strength
2020-01-17 SMICY Wide Range Bar Range Expansion
2020-01-17 SMICY Stochastic Sell Signal Bearish
2020-01-17 SMICY 1,2,3 Retracement Bearish Bearish Swing Setup
2020-01-17 SMICY Upper Bollinger Band Walk Strength
2020-01-17 SMICY Reversal New Lows Setup Bearish Swing Setup
2020-01-17 SMICY Expansion Breakdown Bearish Swing Setup
2020-01-17 SMICY MACD Bearish Signal Line Cross Bearish
2020-01-17 SMICY Non-ADX 1,2,3,4 Bearish Bearish Swing Setup
2020-01-17 SMICY 180 Bearish Setup Bearish Swing Setup
2020-01-17 SMTOF Narrow Range Bar Range Contraction
2020-01-17 SOMMY Expansion Pivot Buy Setup Bullish Swing Setup
2020-01-17 SOMMY Expansion Breakout Bullish Swing Setup
2020-01-17 SOMMY MACD Bullish Signal Line Cross Bullish
2020-01-17 SOMMY Crossed Above 20 DMA Bullish
2020-01-17 SOMMY Crossed Above 50 DMA Bullish
2020-01-17 SOMMY Crossed Above 200 DMA Bullish
2020-01-17 SOMMY Wide Range Bar Range Expansion
2020-01-17 SOMMY Stochastic Buy Signal Bullish
2020-01-17 SOMMY Slingshot Bearish Bearish Swing Setup
2020-01-17 STRB Slingshot Bullish Bullish Swing Setup
2020-01-17 STRB Narrow Range Bar Range Contraction
2020-01-17 YAMCY Fell Below 50 DMA Bearish
2020-01-17 YAMCY Lower Bollinger Band Walk Weakness
2020-01-17 YAMCY Stochastic Reached Oversold Weakness

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 Semiconductors