000 03425nam a22002057a 4500
005 20220317160903.0
008 220316b ||||| |||| 00| 0 eng d
020 _a9789385998607
040 _cAL
041 _aeng
082 _223
_a539.7
_bGHOP
100 _aBipin Ghosh
_923830
245 _aParticle physics
_bIntroduction for students and scientists
260 _aNew Delhi
_bMedtech
_c2017
300 _a203p.
_bPB
_c24x18cm.
365 _2General
_aABDI/0565/22
_b₹296.25
_c
_d₹395.00
_e25%
_f7-03-2022
520 _aThis book aims to explain, to a scientific audience, the story of the microworld over the last decade. The way of telling the story is largely chronological, but with reversion to logical subject divisions where appropriate. Although the main logical connections are mentioned, no attempt has been made to keep an accurate history of the development. Part 0 takes up the story at the turn of the century when physics was first beginning to glimpse the remarkable nature of ordinary matter. Essential elements for understanding the microworld are introduced next: the theories of special relativity and quantum mechanics. Immediately the two are combined in relativistic quantum theory which is the inescapable language of modern microphysics. Part 1 examines, in turn, each of the four separate forces currently believed to govern all observed phenomena in the known universe, and goes on to describe the beginnings of particle physics proper with the discoveries of the muor.The story then progresses on to high-energy hadron physics (physics related to the pion and the proton), which dominated the world of particle physics. This was the logical extension of nuclear physics but it did not reveal any new fundamental insights (apart from the plethora of hadrons).Parts 3 and 4 describe the physics of the weak nuclear force which had been evolving from the study of nuclear β decay. The discovery of parity violation in the weak interaction provided the impetus for a better theoretical understanding and this led eventually to the modern gauge theory of the weak force, which is described in Part 5. This is the first of the essentially modern topics described in the book. The experiments, which are described in Part 6, provided a first indication of point-like objects within the proton and so led to the idea that such objects (called quarks) may be more than just mathematical constructs required to lend some order to the patterns of the multitudinous hadrons. The splendidly named `quantum chromodynamics', described in Part 7, offers a good description of the quarks' behaviour in some circumstances and benefits from sharing the same method of formulation as the earlier weak interaction gauge theory. The best class of reactions in which to observe the behaviour of quarks, and thus to test quantum chromodynamics, is electron-positron annihilation and this is described in Part 8. Over the last three decades these reactions have allowed the discovery of two new types of quark and one new lepton (a heavier relation of the electron and the muon) and have provided firm evidence for the validity of quantum chromodynamics. Part 9 then goes on to describe various theories which attempt to unify the description of the various forces of nature within the framework of a 'grand (or super) unified gauge theory.
650 _2Modern Physics
_aPhysics
_923831
942 _2ddc
_cBK
999 _c221901
_d221901