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1 - 10 of 15 search results for KA :PC53 |u:www.damtp.cam.ac.uk where 0 match all words and 15 match some words.

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  2. solidstate

    www.damtp.cam.ac.uk/user/tong/aqm/solid4.pdf
    7 Apr 2021: m!2 = 2 eika eika. = 4sin2. ka. 2. We find the dispersion relation! = ... 2 =. mM. hm M. p(m M)2 4mM cos2(ka). i. The resulting dispersion relation is sketched in Figure 64 in the first Brillouin zone.

  3. justaqm

    www.damtp.cam.ac.uk/user/tong/aqm/justfive.pdf
    7 Apr 2021: m!2 = 2 eika eika. = 4sin2. ka. 2. We find the dispersion relation! = ... 2 =. mM. hm M. p(m M)2 4mM cos2(ka). i. The resulting dispersion relation is sketched in Figure 74 in the first Brillouin zone.

  4. solidstate

    www.damtp.cam.ac.uk/user/tong/aqm/solid3.pdf
    7 Apr 2021: structure. E = C cos(ka). Then the velocity in a constant electric field oscillates as. ... v(k) =Ca. sin(ka) = Ca. sineEa. t. The Bloch frequency is! =

  5. justaqm

    www.damtp.cam.ac.uk/user/tong/aqm/justfour.pdf
    7 Apr 2021: structure. E = C cos(ka). Then the velocity in a constant electric field oscillates as. ... v(k) =Ca. sin(ka) = Ca. sineEa. t. The Bloch frequency is! =

  6. Preprint typeset in JHEP style - HYPER VERSION Lent ...

    www.damtp.cam.ac.uk/user/tong/aqm/solidstate.pdf
    7 Apr 2021: Preprint typeset in JHEP style - HYPER VERSION Lent Term, 2017. Solid State PhysicsUniversity of Cambridge Part II Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,.

  7. solidstate

    www.damtp.cam.ac.uk/user/tong/aqm/solid2.pdf
    7 Apr 2021: value. E = E0 2t cos(ka) (2.5). The spectrum is shown in the figure for t > 0.

  8. justaqm

    www.damtp.cam.ac.uk/user/tong/aqm/justthree.pdf
    7 Apr 2021: value. E = E0 2t cos(ka) (3.5). The spectrum is shown in the figure for t > 0.

  9. Field Theory in Cosmology: Example Sheet 1 1. For ...

    www.damtp.cam.ac.uk/user/ep551/example_sheet_1_FT_in_Cosmo.pdf
    15 Apr 2021: φ(k1). φ(kn)〉 δ3D. (na=1. ka. ). (19). 7. For the metric. ... φ(k1). φ(kn)〉 = (2π)3δ3D. (na=1. ka. )Bn(k1,. ,kn). (34). must scale as.

  10. Field Theory in Cosmology (Part III) Enrico Pajer Contents ...

    www.damtp.cam.ac.uk/user/ep551/field_theory_in_Cosmology.pdf
    15 Apr 2021: Field Theory in Cosmology (Part III). Enrico Pajer. Contents. 1 A quick review of background cosmology 51.1 Classical cosmological backgrounds. 51.2 Motivations for Inflation. 101.3 A prolonged phase of quasi-de Sitter expansion. 151.4 Single field

  11. Lecture Notes on Cosmological Soft Theorems Enrico Pajera aDepartment …

    www.damtp.cam.ac.uk/user/ep551/notes_cosmo_soft_theorems.pdf
    16 Apr 2021: na=1. La〈O(k1)O(k2). O(kn)〉 = 0 , (1.1). where La = L(τa,τa, ka,ka) is some linear, possibly differential operator made of func-. ... Then (4.26) becomes[. 3(n 1) na=1. ka. ka. ]〈R(k1)R(k2). R(kn)〉′! = 0 , (4.38).

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