373 research outputs found

    Problem Set #10

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    Blackbod

    Structure of matter, 3

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    The particle zoo Prior to the 1930s the fundamental structure of matter was believed to be extremely simple: there were electrons (each with mass about 0.5 MeV), eāˆ’ , photons (no mass), Ī³ , and protons (mass about 938 MeV), p+ . Starting in 1932 the world began to get a lot more complicated. First came Diracā€™s positron ( e+ , with same mass as the electron), postulated in 1928 but mostly ignored until Andersonā€™s accidental discovery (see SM 1). Soon after, the neutron ( n ) was identified (mass about 940 MeV). In beta decay, the neutron transforms into a proton and an electron. The energy of the electron in beta decay has a maximum cutoff and is otherwise ā€œneverā€ observed to be the sameā€“as it would be if there were only two products. It is almost as if energy is not conserved in beta decay. In 1930, Wolfgang Pauli proposed that a third, unseen, particle was also emitted and that the three products conserved energy and momentum by sharing them in a variety of unpredictable ways. The new particle would have to have spin-1/2 (because the neutron, proton, and electron all have spin-1/2 and not even the crazy rules of addition in quantum mechanics allow 1/2 +1/2 = 1/2 ) and be electrically neutral (because the neutron is neutral and the proton plus electron is also neutral). Eventually, Pauliā€™s particleā€“the neutrino, Ī½ ā€“was directly detected in the 1950s. This set of particles was all that was needed to make sense of nuclei and their properties

    Special relativity, 3

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    A few kinematic consequences of the Lorentz transformations How big is gamma

    Special relativity, 4

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    More kinematic consequences of the Lorentz transformations Light cones: A ā€œlight coneā€ is a set of world lines corresponding to light rays emanating from and/or entering into an event

    Physics 3710: Intermediate Modern Physics

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    Physics 3710 is about the principles and applications of special and general relativity and of the nuclear and sub-nuclear structures of matter. Though some of the topics of 3710 are more than 100 years old, others continue to rapidly evolveā€”and their interplay provides a fascinating, living example of science at work. Moreover, the course is predicated on, and aspires to convey, two thoroughly modern, coherent, and interconnected themes: (1) the largest (e.g., stars, galaxies, and galactic clusters) and smallest (e.g., quarks, leptons, and force-carrying bosons) observed forms of matter are intimately related to one another; and (2) dynamics, conservation laws, and symmetry are all essentially equivalent

    Special relativity, 5

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    Physics 2710: Introductory Modern Physics

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    Physics 3710 ā€“ Problem Set #12

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    Problem Set #12 Quarks and gluons In the following solid lines represent quarks or antiquarks and dotted lines represent gluons. Time increases upward

    Physics 3710 ā€“ Problem Set #5

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    Physics 3710 ā€“ Problem Set #5 Relativistic dynamics, I Problems 1-5 refer to: One mass, m1 = 1 (in some units), collides head-on with a second mass, m2 = 2 , and sticks to it, forming a composite body of mass M . There are no external forces. Observer O records m1 as initially moving with dimensionless velocity, u1 = +0.9 in the x - direction, while m2 is recorded to be at rest. Do not make unwarranted assumptions about M , please; thatā€™s the point of this set of problems

    Physics 3710 ā€“ Problem Set #6

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    Physics 3710 ā€“ Problem Set #6 Relativistic dynamics, II Problems 1-5 refer to: The mass of the neutron is 1.008664 u and that of the proton is 1.007276 u, where 1 u = 931.5 MeV
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