Semiconductors Stocks List

Recent Signals

Date Stock Signal Type
2019-11-15 ACLS New 52 Week Closing High Bullish
2019-11-15 ACLS Pocket Pivot Bullish Swing Setup
2019-11-15 AMKR Shooting Star Candlestick Bearish
2019-11-15 AMKR Doji - Bearish? Reversal
2019-11-15 AMKR Lizard Bearish Bearish Day Trade Setup
2019-11-15 APD Calm After Storm Range Contraction
2019-11-15 APD New 52 Week Closing High Bullish
2019-11-15 APD New 52 Week High Strength
2019-11-15 ASX Crossed Above 20 DMA Bullish
2019-11-15 ASX Bollinger Band Squeeze Range Contraction
2019-11-15 ATOM Doji - Bullish? Reversal
2019-11-15 ATOM NR7 Range Contraction
2019-11-15 ATOM Narrow Range Bar Range Contraction
2019-11-15 ATOM Stochastic Buy Signal Bullish
2019-11-15 AVT Crossed Above 20 DMA Bullish
2019-11-15 CPSH 20 DMA Resistance Bearish
2019-11-15 CPSH MACD Bearish Signal Line Cross Bearish
2019-11-15 CPSH Non-ADX 1,2,3,4 Bullish Bullish Swing Setup
2019-11-15 CVV Narrow Range Bar Range Contraction
2019-11-15 CVV Crossed Above 20 DMA Bullish
2019-11-15 CVV Crossed Above 200 DMA Bullish
2019-11-15 ETB 1,2,3 Pullback Bullish Bullish Swing Setup
2019-11-15 ETB Calm After Storm Range Contraction
2019-11-15 ETB Non-ADX 1,2,3,4 Bullish Bullish Swing Setup
2019-11-15 ETB Spinning Top Other
2019-11-15 HIMX 20 DMA Support Bullish
2019-11-15 HTGC Calm After Storm Range Contraction
2019-11-15 HTGC NR7 Range Contraction
2019-11-15 IMOS Non-ADX 1,2,3,4 Bullish Bullish Swing Setup
2019-11-15 IMOS Calm After Storm Range Contraction
2019-11-15 KLIC New 52 Week High Strength
2019-11-15 KLIC Non-ADX 1,2,3,4 Bullish Bullish Swing Setup
2019-11-15 KLIC MACD Bearish Signal Line Cross Bearish
2019-11-15 KLIC 1,2,3 Pullback Bullish Bullish Swing Setup
2019-11-15 KLIC Wide Range Bar Range Expansion
2019-11-15 KLIC Volume Surge Other
2019-11-15 KLIC Fell Below 20 DMA Bearish
2019-11-15 MX Pocket Pivot Bullish Swing Setup
2019-11-15 NVMI NR7 Range Contraction
2019-11-15 NVMI New 52 Week High Strength
2019-11-15 NVMI NR7-2 Range Contraction
2019-11-15 NVMI Narrow Range Bar Range Contraction
2019-11-15 NVMI New 52 Week Closing High Bullish
2019-11-15 NVMI Calm After Storm Range Contraction
2019-11-15 OLN Stochastic Reached Oversold Weakness
2019-11-15 PLAB Pocket Pivot Bullish Swing Setup
2019-11-15 PSCT Pocket Pivot Bullish Swing Setup
2019-11-15 PSCT 180 Bullish Setup Bullish Swing Setup
2019-11-15 PSCT MACD Bearish Signal Line Cross Bearish
2019-11-15 PSI New 52 Week Closing High Bullish
2019-11-15 PSI New 52 Week High Strength
2019-11-15 PSI Volume Surge Other
2019-11-15 PSI Gilligan's Island Sell Setup Bearish Swing Setup
2019-11-15 PSI Pocket Pivot Bullish Swing Setup
2019-11-15 PTF Narrow Range Bar Range Contraction
2019-11-15 ROM New 52 Week Closing High Bullish
2019-11-15 ROM New 52 Week High Strength
2019-11-15 SMIT Non-ADX 1,2,3,4 Bullish Bullish Swing Setup
2019-11-15 SMIT 1,2,3 Pullback Bullish Bullish Swing Setup
2019-11-15 SMIT Upper Bollinger Band Walk Strength
2019-11-15 SMIT Calm After Storm Range Contraction
2019-11-15 SNE Stochastic Sell Signal Bearish
2019-11-15 SNSR New 52 Week Closing High Bullish
2019-11-15 SNSR Pocket Pivot Bullish Swing Setup
2019-11-15 SNSR New 52 Week High Strength
2019-11-15 SNSR 180 Bullish Setup Bullish Swing Setup
2019-11-15 SVVC Narrow Range Bar Range Contraction
2019-11-15 SVVC NR7 Range Contraction
2019-11-15 SVVC Bollinger Band Squeeze Range Contraction
2019-11-15 SVVC New 52 Week Closing Low Bearish
2019-11-15 SWKS Non-ADX 1,2,3,4 Bullish Bullish Swing Setup
2019-11-15 SWKS Calm After Storm Range Contraction
2019-11-15 SWKS MACD Bearish Signal Line Cross Bearish
2019-11-15 SWKS 1,2,3 Pullback Bullish Bullish Swing Setup
2019-11-15 SWKS Boomer Buy Setup Bullish Swing Setup
2019-11-15 TAIT Bollinger Band Squeeze Range Contraction
2019-11-15 TAIT Crossed Above 20 DMA Bullish
2019-11-15 TDY New 52 Week Closing High Bullish
2019-11-15 TDY Pocket Pivot Bullish Swing Setup
2019-11-15 TDY New 52 Week High Strength
2019-11-15 TDY Shooting Star Candlestick Bearish
2019-11-15 TECL New 52 Week Closing High Bullish
2019-11-15 TECL New 52 Week High Strength
2019-11-15 TECL NR7 Range Contraction
2019-11-15 TECL Narrow Range Bar Range Contraction
2019-11-15 TECS New 52 Week Closing Low Bearish
2019-11-15 TECS Narrow Range Bar Range Contraction
2019-11-15 TECS NR7-2 Range Contraction
2019-11-15 TECS NR7 Range Contraction
2019-11-15 TECS New 52 Week Low Weakness
2019-11-15 TSEM Three Weeks Tight Range Contraction
2019-11-15 TSEM Narrow Range Bar Range Contraction
2019-11-15 TSEM Calm After Storm Range Contraction
2019-11-15 TSEM Non-ADX 1,2,3,4 Bullish Bullish Swing Setup
2019-11-15 TXN NR7 Range Contraction
2019-11-15 USD New 52 Week Closing High Bullish
2019-11-15 USD Pocket Pivot Bullish Swing Setup
2019-11-15 USD Gilligan's Island Sell Setup Bearish Swing Setup
2019-11-15 USD New 52 Week High Strength
2019-11-15 VSH Crossed Above 20 DMA Bullish
2019-11-15 WISA NR7 Range Contraction
2019-11-15 WISA Narrow Range Bar Range Contraction
2019-11-15 WISA Non-ADX 1,2,3,4 Bearish Bearish Swing Setup
2019-11-15 XNTK Narrow Range Bar Range Contraction
2019-11-15 XNTK NR7 Range Contraction
2019-11-15 XSD New 52 Week High Strength

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.

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