The All Particle of Physics || the all particle physics of you

The All Particle Of Physics

Oddball is a gravitational force, which is not a quantum hypothesis at this point. However, it is so weak that it has no significant impact on the quantum level because the different energies will pass. So much of it can be taken into account in quantum measurements. However, after 100 years of rational development, we can directly produce three more forces by quantum field speculation. These theories explain how particles such as quarks and electrons connect through these three forces. Each energy is absorbed by the energy carrier, also called the go-between. Electric energy intervenes with photon, weak energy by W and Z bosons, and strong energy by gluons. In the quantum field hypothesis, we deal with all of these arbiter particles by field. For example, a photon field interferes with electrical energy between charged particles such as electrons. 



the all particle physics of you

Some basic particles of the standard model are also addressed by their individual forums. In addition, these fields can communicate with each other. Therefore, the photon field can interact with the electron field causing the shock of two electrons for example If we summarize the concept of dynamic molecules associated with different particles, we can find the whole basic molecular science molecule. We can take up space, add a quantum field to each type of fermion, such as quarks, add quantum fields of appropriate bases, such as gluons, interact with the force that the quark relies on, and we can discover how extraordinary exposures work. These ideas may be confusing, but American philosopher Richard Feynman thought of a better way to deal with this connection in what is now called Feynman's graphs. 

the all particle physics model

And surprisingly, however, these graph addresses offend numerical conditions, which can be naturally depicted and drawn into any communication that uses certain basic levels. In case you need to see all the great elements of material science with the help of these basic attributes of Feynman's nature, then Merry Christmas, because that's a modern thing… Before we explore all the molecular science I would like to pause to express my gratitude to Magellan TV for making this event imaginable. Magellan is a highly recommended free web-based feature created by the movie producers themselves. The variety of their narratives is very impressive and much broader than any other web-based feature. You can dive deeper into subjects like history, culture, science, and innovation, and see the value of them in 4K. I am eager to disclose to you that Magellan currently offers to get one, get one free, 

the all particle physics lab

a personal gift voucher for your day-to-day date you need to provide information. In the event of a teenager, you will receive the first for free of one month for Magellan. In case you are a part, you will receive an extra month whenever you purchase a gift voucher. There has never been a higher chance of distributing the gift of information. Enthusiastically I recommend Magellan TV, so be sure to disconnect the show. First, what about finding a way to make a specific Feynman chart. To do this let's start with a standard model, such as an intermediate particle table. What is remarkable here is the understanding of what different classes of particles can do. So on the left, the 12 fermions are pointed in straight lines with bolts on the Feynman charts. Bolt is important. In fact, as in the electrical circuit, the flow goes through a circuit, the bolts speak of a "stream" of fermions. No two bolts point to each other. This is the limitation of the current fermion or all of it; we should have the same number of fermions at the end as we started. 

Note that there are different texts, which use these bills in an unexpected way. If we happen to think of the x x time, we can specify that fermion bolts move forward in the system as extrusion particles, and fermion bolts reverse as antimatter particles. This is a complete guide to all fermions. At present, the fermions can be separated and continue in terms of charge rates. At the time of the litigation, I meant electricity charges and blurring. If you have no idea what a shading charge is, kindly check out my previous video on QCD. All six quarks have the cost of blurring. All particles with blurring charges claim strong atomic strength, in these lines, all quarks feel powerful. Quarks in addition have an electric charge, so they also do not feel the electric current. Another category of fermions is a lepton. This can be separated from the electron that forms the OTA, and its heavy cousins ​​the particles of muon and tau. All of these are electric charges but there are no charges for fading, so they feel the electric current is not yet strong. The last three leptons are neutrinos. 

conclusion

These have no blurring or electricity charge; in this way, they are not affected by strong or electrical energy. Also, they are low in weight, so they are simply influenced by gravity. This is something that makes it very difficult to distinguish. You may ask, hello, should it not be said that the weak and charging forces are weak? The correct answer is that all fermions transmit what many call weak isospin. This can be considered a form of "charge," for weak forces Fermions tend to be more than one-half or short-term. So all fermions connect with weak forces. However, the weak eye twist can also be 1, 0, and +1 - W-boson has weak isospin of 1, W + has +1, Higgs has - 1/2, and Z boson and photon have weak isospin of 0. Note that this zero is not equal to isospin. B

Post a Comment

Previous Post Next Post