pbarp - CERN Indico
... Collider Physics in Bern, Switzerland, 5 – 8 March 1984, and published soon after. They produced much excitement and lots of theoretical papers were written to explain them, all based on new physics beyond the Standard Model. Most of these events (but not all) had hadronic jets in the final state an ...
... Collider Physics in Bern, Switzerland, 5 – 8 March 1984, and published soon after. They produced much excitement and lots of theoretical papers were written to explain them, all based on new physics beyond the Standard Model. Most of these events (but not all) had hadronic jets in the final state an ...
Particle Physics
... about Nature to the fledgling civilization that starts again. What would this be? Obviously it can’t be complicated mathematics—it has to be something simple that can be explained in plain language. Feynman’s answer was that he would tell them about atoms. Or, more precisely, he would tell them that ...
... about Nature to the fledgling civilization that starts again. What would this be? Obviously it can’t be complicated mathematics—it has to be something simple that can be explained in plain language. Feynman’s answer was that he would tell them about atoms. Or, more precisely, he would tell them that ...
Pulsed Plasma Ign.
... is not at rest: it is being continually assaulted by all manner of other particles from the vacuum." ...
... is not at rest: it is being continually assaulted by all manner of other particles from the vacuum." ...
Comments on the 2nd order bootstrap relation
... to solve it was incorrect. In this note we demonstrate that these objections are totally unfounded. They are a result of a misinterpretation of the potential used in [2], which is a different quantity as compared to the kernel used in [1,3]. We also derive the 2nd order bootstrap relation of [1] in ...
... to solve it was incorrect. In this note we demonstrate that these objections are totally unfounded. They are a result of a misinterpretation of the potential used in [2], which is a different quantity as compared to the kernel used in [1,3]. We also derive the 2nd order bootstrap relation of [1] in ...
Document
... The state of a classical particle is specified by its coordinate and momentum (x,p): phase-space – A state of classical identical particle system can be described by a phase-space distribution f(x,p). Time evolution of f(x,p) obeys the Boltzmann equation. In quantum mechanics, because of the unc ...
... The state of a classical particle is specified by its coordinate and momentum (x,p): phase-space – A state of classical identical particle system can be described by a phase-space distribution f(x,p). Time evolution of f(x,p) obeys the Boltzmann equation. In quantum mechanics, because of the unc ...
The states of matter
... Celsius, where they consist of free charged particles, usually in equal numbers, such as ions and electrons. ○ Plasma, like gas, is a state of matter that does not have definite shape or volume. ○ Unlike gases, plasmas may self-generate magnetic fields and electric currents, and respond strongly and ...
... Celsius, where they consist of free charged particles, usually in equal numbers, such as ions and electrons. ○ Plasma, like gas, is a state of matter that does not have definite shape or volume. ○ Unlike gases, plasmas may self-generate magnetic fields and electric currents, and respond strongly and ...
Strangeness production
Strangeness production is a signature and a diagnostic tool of quark–gluon plasma (or QGP) formation and properties. Unlike up and down quarks, from which everyday matter is made, strange quarks are formed in pair-production processes in collisions between constituents of the plasma. The dominant mechanism of production involves gluons only present when matter has become a quark–gluon plasma. When quark–gluon plasma disassembles into hadrons in a breakup process, the high availability of strange antiquarks helps to produce antimatter containing multiple strange quarks, which is otherwise rarely made. Similar considerations are at present made for the heavier charm flavor, which is made at the beginning of the collision process in the first interactions and is only abundant in the high-energy environments of CERN's Large Hadron Collider.