Changes

Temperature is a factor in every part of our lives; everything that we do is affected by it.  All the effects of temperature that we experience are due to the cumulative effects of the energies of trillions of particles. The temperature that we know is the consequence of thermal energies of millions and billions of particles working together to create the effects we know everyday. Statistical physics predicts the probability variation of temperature to be an exponential curve; with many particles with small energies and very few particles with large amounts of energy. This experiment uses a Silicon Photomultiplier (SiPM) to detect the thermal energy of single particles.  

Temperature is a factor in every part of our lives; everything that we do is affected by it.  All the effects of temperature that we experience are due to the cumulative effects of the energies of trillions of particles. The temperature that we experiance everyday due to the consequence of the average thermal energies of millions and billions of particles working together.

The thermal energy of a single particle is very different from average energies. Statistical physics predicts the probability variation of temperature to be an exponential curve; with many particles with small energies and very few particles with large amounts of energy. This experiment uses a Silicon Photomultiplier (SiPM) to detect the thermal energy of single particles.  

An SiPM uses the technology previously employed in the Avalanche Photodiode. A diode is reverse-biased until just before breakdown voltage and it stays at that state until a source of energy (such as thermal energy) pushes it past breakdown. It then releases all of its charge and then slowly resets. An SiPM is different in that it uses an array of many Avalanche Photodiodes [[[[[[[[[[ right into a silicon wafer. The photodiodes are so small that they can be counted as individual pixels. Therefore, an SiPM can determine how many times a particle has had enough energy to set it off, thereby detecting individual particles.  

An SiPM uses the technology previously employed in the Avalanche Photodiode. A diode is reverse-biased until just before breakdown voltage and it stays at that state until a source of energy (such as thermal energy) pushes it past breakdown. It then releases all of its charge and then slowly resets. An SiPM is different in that it uses an array of many Avalanche Photodiodes [[[[[[[[[[ right into a silicon wafer. The photodiodes are so small that they can be counted as individual pixels. Therefore, an SiPM can determine how many times a particle has had enough energy to set it off, thereby detecting individual particles.